Updated on 2026/05/06

写真a

 
KUROSAWA Shunsuke
 
Organization
Graduate School of Engineering Energy Engineering 2 Professor
Undergraduate School
School of Engineering Energy Science and Engineering
Title
Professor
 

Papers 660

  1. Remote gamma-ray detection system with Mo-doped Cs2ZrCl6 near-infrared emission scintillators and optical fibers

    Fujiwara C., Kurosawa S., Yamaji A., Yoshikawa A.

    Nuclear Instruments and Methods in Physics Research Section A Accelerators Spectrometers Detectors and Associated Equipment   Vol. 1089   2026.9

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    Publisher:Nuclear Instruments and Methods in Physics Research Section A Accelerators Spectrometers Detectors and Associated Equipment  

    Accurate remote radiation monitoring in high dose rate conditions is often hampered by stem effects (Cherenkov radiation and emission) generated within optical fibers. To achieve accurate remote radiation monitoring with scintillator and optical fiber under ultra-high dose rate condition, we developed a near-infrared (NIR) scintillator, molybdenum (Mo)-doped Cs<inf>2</inf>​ZrCl<inf>6</inf>​. The Mo: Cs<inf>2</inf>ZrCl<inf>6</inf> crystal exhibits a strong radioluminescence peak at 900 nm, originating from the Mo<sup>4+</sup> activator under X-ray and Gamma-ray excitation. This emission is well-separated from the fiber noise-region (below 800 nm), resulting in a high signal-to-noise ratio. In addition, we developed the detector with Mo: Cs<inf>2</inf>ZrCl<inf>6</inf> and optical fiber and evaluated the gamma-ray detection ability as a dosimeter. The signal value of the scintillator could be fitted by a linear-law function to the calibrated dose rate, and the fitting accuracy of signal was (R<sup>2</sup> = 0.99) over a wide range gamma-ray dose rate. These results establish Mo: Cs<inf>2</inf>​ZrCl<inf>6</inf>​ as a promising candidate for robust remote dosimetry in extreme radiation environments, such as nuclear decommissioning.

    DOI: 10.1016/j.nima.2026.171548

    Web of Science

    Scopus

  2. Optical and electronic properties of zero-dimensional-type lithium hafnium iodide scintillator Open Access

    Fujiwara C., Kurosawa S., Yamaji A., Yoshikawa A., Matsubayashi N., Takata T., Tanaka H.

    Journal of Luminescence   Vol. 293   2026.5

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    Zero-dimensional (0D) halides with the general formula A<inf>2</inf>BX<inf>6</inf> (such as Cs<inf>2</inf>HfI<inf>6</inf>) have emerged as a promising class of next-generation scintillator materials characterized by their high luminescence efficiency. This study investigated the novel 0D halide Li<inf>2</inf>HfI<inf>6</inf>, where A-site Li<sup>+</sup> substitution induces a structural transition to a rhombohedral structure. Comprehensive experimental and density functional theory (DFT) analyses reveal that Li<sup>+</sup> substitution facilitates carrier delocalization. Temperature-dependent photoluminescence identified a shallow 17 meV de-trapping barrier from the self-trapped exciton (STE) to the free exciton (FE) state. This thermally induced transition, paralleling phenomena well-observed in 2D perovskites, results in a coexistence of high-energy FE and low-energy STE emissions at room temperature. The emergence of the FE component enables a rapid scintillation decay time of less than 100 ns. In addition, Li<inf>2</inf>HfI<inf>6</inf> achieves a high thermal neutron light yield of 17,000 photons/neutron, which is approximately three times higher than commercial <sup>6</sup>Li-glass. These characteristics demonstrate that Li<inf>2</inf>HfI<inf>6</inf> is a promising candidate for <sup>3</sup>He-alternative technologies. This work establishes A-site cation engineering as an effective design principle for controlling the structure and luminescence properties of 0D halide neutron scintillators.

    DOI: 10.1016/j.jlumin.2026.121784

    Open Access

    Scopus

  3. Development and experimental validation of a neutron detector system for accelerator-based BNCT irradiation fields Open Access

    Zhao, L; Tanaka, H; Hu, NNR; Takata, T; Kawabata, S; Kurosawa, S; Yamaji, A; Masuda, A; Matsumoto, T

    JAPANESE JOURNAL OF APPLIED PHYSICS   Vol. 65 ( 8 )   2026.4

  4. Evidence for Itinerant Ferromagnetic Flat Bands Producing Large Transverse Responses. Open Access

    Minami S, Wang Y, Souma S, Nakamura H, Sakai A, Osumi T, Su H, Watanabe H, Kurosawa S, Oiwa R, Nishio-Hamane D, Nakayama K, Nomoto T, Arita R, Sato T, Nakatsuji S

    Advanced materials (Deerfield Beach, Fla.)     page: e17521   2026.4

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    Language:English  

    DOI: 10.1002/adma.202517521

    PubMed

  5. Polycomb repressive complex 2 insufficiency underlies myeloid leukemia in Down syndrome.

    Suzuki Y, Nakajima-Takagi Y, Oshima M, Ochi Y, Tsuchiya A, Koide S, Yokomizo-Nakano T, Kurosawa S, Rizq O, Kon A, Miyano S, Rahmutulla B, Kaneda A, Nakayama M, Koseki H, Yu E, Toki T, Ito E, Ogawa S, Iwama A

    Blood     2026.4

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    Language:English  

    DOI: 10.1182/blood.2025032083

    PubMed

  6. Photo- and X-ray excited luminescence, thermoluminescence and scintillation characteristics of LuGd2Al3Ga2O12:Ce,Mo single crystal scintillators: Influence of Mo co-doping

    Chewpraditkul W., Pattanaboonmee N., Chewpraditkul W., Sakthong O., Yoshino M., Horiai T., Kurosawa S., Kamada K., Kucerkova R., Beitlerova A., Li T., Wang Y., Hu C., Li J., Babin V., Nikl M., Yoshikawa A.

    Journal of Luminescence   Vol. 292   2026.4

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    Mo co-doped LuGd<inf>2</inf>Al<inf>3</inf>Ga<inf>2</inf>O<inf>12</inf>:Ce,Mo (Mo = 0, 300, 600 ppm) single crystals were grown by the micro-pulling-down method. The optical absorption and X-ray excited luminescence spectra, temperature dependence of photoluminescence decay kinetics, afterglow and thermoluminescence (TL) intensity, and scintillation properties (light yield, LY, and decay time) were investigated. The quenching temperature of 355 K was determined from temperature-dependent photoluminescence decay kinetics in the temperature range of 77–487 K under excitation in the 4f - 5d<inf>1</inf> absorption band of the Ce<sup>3+</sup> ions. Under excitation of 662 keV γ rays, the LuGd<inf>2</inf>Al<inf>3</inf>Ga<inf>2</inf>O<inf>12</inf>:Ce,Mo600 sample showed high LY value of 32,900 photons/MeV, energy resolution of 7.6 %, and scintillation decay time of 119 ns (38 %) + 475 ns (62 %). The lower LY value together with higher contribution of slower scintillation decay component among the samples studied was observed for LuGd<inf>2</inf>Al<inf>3</inf>Ga<inf>2</inf>O<inf>12</inf>:Ce,Mo300 sample, consistently with its higher afterglow intensity and longer de-trapping time of the dominant TL glow peak at 356 K.

    DOI: 10.1016/j.jlumin.2026.121737

    Scopus

  7. Corrosion Resistance of Ru-Mo-W-Fe Alloy in Inorganic Acids Open Access

    Murugesan N., Murakami R., Itoi S., Kamada K., Hanada T., Yamaji A., Ishizawa S., Yoshino M., Sato H., Kurosawa S., Yokota Y., Yoshikawa A.

    Journal of the Electrochemical Society   Vol. 173 ( 6 )   2026.3

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    Publisher:Journal of the Electrochemical Society  

    In this study, we examined the corrosion resistance of Ru<inf>57</inf>Mo<inf>14.25</inf>W<inf>23.75</inf>Fe<inf>5</inf>, Ru<inf>54</inf>Mo<inf>13.5</inf>W<inf>22.5</inf>Fe<inf>10</inf>, and Ru<inf>48</inf>Mo<inf>12</inf>W<inf>20</inf>Fe<inf>20</inf> alloys in inorganic acids. The alloys were fabricated using the dewetting micro-pulling-down and plasma-melt stamping methods. Immersion tests in H<inf>2</inf>SO<inf>4</inf> at 300 °C for 24 h indicated that Ru-Mo-W-Fe alloys exhibit better corrosion resistance (<0.17 mm y<sup>−1</sup>), compared to conventional corrosion-resistant materials (>10 mm y<sup>−1</sup>). Immersion tests at 25 °C in 5% HCl for 72 h and at 100 °C in 50% HF for 24 h also indicated that Ru-Mo-W-Fe alloys are highly corrosion resistant. Electrochemical tests in 1 M HCl and 1 M H<inf>2</inf>SO<inf>4</inf> revealed an increase in the anodic current and the formation of a low charge transfer resistance passive layer corresponding to alloying Fe. XPS analysis revealed that the primary corrosion product formed during polarization of Ru-Mo-W-Fe alloys in 1 M H<inf>2</inf>SO<inf>4</inf> was WO<inf>3</inf>. Notably, WO<inf>3</inf> is kept passivated on pure W during the corrosion in H<inf>2</inf>SO<inf>4</inf>; however, it is not kept passivated when present on Ru-Mo-W-Fe alloys.

    DOI: 10.1149/1945-7111/ae4cd0

    Open Access

    Scopus

  8. Orthogonal Biosynthesis of Pyrrolamides through Dehydration by a Pathway-Specific Glycoside Hydrolase-Like Enzyme in Gram-Positive Bacteria Open Access

    Kanki D., Kurosawa S., Yoshida A., Awakawa T., Kosono S., Nishiyama M.

    Journal of the American Chemical Society   Vol. 148 ( 9 ) page: 10037 - 10048   2026.3

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    Language:English   Publisher:Journal of the American Chemical Society  

    Pyrrolamides, defined by a pyrrole-2-carboxamide core, represent a family of natural products produced by Streptomyces species. They exhibit potent yet promiscuous bioactivities, including antimicrobial, antifungal, antiviral, and anticancer effects. The characteristic pyrrole moiety is derived from 4-acetamidopyrrole-2-carboxylate, which was previously proposed to originate most likely from N-acetylglucosamine-1-phosphate. This unusual transformation of a primary metabolite sugar into an aromatic peptide building block is of interest mechanistically; however, the pathway preceding pyrrole formation remains unclear. We herein report the discovery of manlipyrrolamides A–F from Bacillus manliponensis, a new class of pyrrolamides with distinctive structural features. Gene disruption and in vitro assays allowed us to identify the functions of key enzymes in the pyrrole formation pathway. Man17, a nucleotidyltransferase, functions as a gatekeeper that activates the precursor N-acetylglucosamine-1-phosphate, through guanosine diphosphate (GDP) derivatization for subsequent modifications. Man18, a glycosyltransferase-like enzyme, and Man15, a glycoside hydrolase-like enzyme, function as a hydrolase and dehydratase, respectively, forming a pyrrole from a mature GDP-linked sugar. After pyrrole formation, a xanthine dehydrogenase-like enzyme complex is utilized in oxidation to produce carboxylate, distinct from the previously proposed Streptomyces pathway. The pathway-specific enzyme Man15, which is widely distributed in Gram-positive bacteria, is encoded in diverse biosynthetic gene clusters, indicating that this unprecedented transformation is utilized for unknown classes of pyrrolamides. The use of a GDP derivative suggests an orthogonal strategy distinct from that of the canonical UDP-linked sugar pathway. The present study reveals novel sugar skeletal conversion in secondary metabolism, which provides novel insights into bacterial metabolic strategies.

    DOI: 10.1021/jacs.5c23027

    Open Access

    Scopus

    PubMed

  9. 1H polarization above 60 % at room temperature by triplet dynamic nuclear polarization

    Tateishi K., Otsuka S., Yamaji A., Kurosawa S., Uesaka T.

    Chemical Physics Letters   Vol. 885   2026.2

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    Publisher:Chemical Physics Letters  

    We achieved 61 % <sup>1</sup>H polarization at room temperature and in 0.64 T via Dynamic Nuclear Polarization using photoexcited triplet electrons (Triplet-DNP). Dibenz[ a, h ]anthracene was introduced as a new host for pentacene- d <inf>14</inf>, providing a long spin-lattice relaxation time ( T <inf>1</inf>) exceeding 2 h. Single crystals doped with 0.05 mol% pentacene- d <inf>14</inf> were grown by the Bridgman method and cut to ∼1 mg for experiments. The <sup>1</sup>H polarization buildup and relaxation measurements indicated that paramagnetic relaxation dominates over spin-lattice relaxation. Finally, potential applications of room-temperature hyperpolarization, i.e. , nuclear ordering and radiation-tolerant polarized targets, were discussed.

    DOI: 10.1016/j.cplett.2025.142606

    Scopus

  10. Novel zero-dimensional halide perovskite Li2Hf(Br,I)6 with red/NIR emission wavelength for thermal neutron detection Open Access

    Fujiwara C., Kurosawa S., Yamaji A., Yoshikawa A., Matsubayashi N., Takata T., Tanaka H.

    Materials Today Physics   Vol. 60   2026.1

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    Publisher:Materials Today Physics  

    Novel neutron Li<inf>2</inf>Hf(Br,I)<inf>6</inf> scintillators were developed, and their luminescence and scintillation properties were investigated both experimentally and via density functional theory calculations. The development of conventional neutron scintillators has been dominated by materials with emission wavelengths in the range of 400–500 nm that have wavelength sensitivity of photomultiplier tubes (PMTs). However, with the recent emergence of detectors having higher quantum efficiencies than PMTs, such as Si-based photodetectors, there is a need for neutron scintillators with red-to-near-infrared (red/NIR) emission wavelengths that match the wavelength sensitivity of these detectors. Therefore, this study demonstrates that Li<inf>2</inf>Hf(Br,I)<inf>6</inf> exhibits self-trapped exciton emission under both X-ray and thermal neutron irradiation, with an emission peak at approximately 650 nm, which is 100–200 nm longer than the corresponding peak wavelength of conventional neutron scintillators. The emission wavelength of Li<inf>2</inf>Hf(Br,I)<inf>6</inf> matches the wavelength sensitivity of Si-APD. In addition, Li<inf>2</inf>HfBr<inf>4</inf>I<inf>2</inf> is the first neutron scintillator to combine emission in the red/NIR region with a high light output of approximately 40,000 photons per thermal neutron, which is six to seven times that observed in commercial Ce:Li-glass (GS20). Furthermore, the pulse shape discrimination (PSD) Figure of Merit (FOM) was found to be 2.47, indicating excellent neutron/gamma-ray discrimination capability. This study opens a new avenue for both red/NIR emission and high-light-output neutron scintillators.

    DOI: 10.1016/j.mtphys.2025.101997

    Open Access

    Scopus

  11. Fundamental properties of novel zero-dimensional halide Na<sub>2</sub>HfI<sub>6</sub> and application for neutron detection by Li doping Open Access

    Fujiwara Chihaya, Kurosawa Shunsuke, Yamaji Akihiro, Yoshikawa Akira, Matsubayashi Nishiki, Takata Takushi, Tanaka Hiroki

    Journal of the Ceramic Society of Japan   Vol. advpub ( 0 )   2026

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    Language:English   Publisher:The Ceramic Society of Japan  

    <p>Zero-dimensional (0D) metal halide scintillators have attracted considerable attention owing to their exceptional emission properties derived from strongly localized self-trapped excitons. In this paper, we report the development of a novel thermal neutron scintillator—Na<sub>2−</sub><i><sub>x</sub></i>Li<i><sub>x</sub></i>HfI<sub>6</sub> (0 ≤ <i>x</i> ≤ 2)—achieved by strategically substituting lithium for the Na of the 0D Na<sub>2</sub>HfI<sub>6</sub> host. The Na<sub>2</sub>HfI<sub>6</sub> host material has a 0D structure with an [HfI<sub>6</sub>]<sup>2−</sup> octahedral unit, exhibiting broad red-to-near-infrared (NIR) emission with a large stokes shift, driven by strong electron–phonon coupling (<i>S</i> = 56.7) and high exciton binding energy (<i>E</i><sub>b</sub> = 200 meV). Density functional theory calculations revealed that the A site cations (Na<sup>+</sup> and Li<sup>+</sup>) did not contribute to the valence or conduction band edges. This indicated that the fundamental electronic structure was preserved upon Li substitution; consequently, the Li-alloyed Na<sub>2−</sub><i><sub>x</sub></i>Li<i><sub>x</sub></i>HfI<sub>6</sub> also exhibited the characteristic broad red-to-NIR emission. Remarkably, the Na<sub>1.5</sub>Li<sub>0.5</sub>HfI<sub>6</sub> crystal demonstrated a light yield of 37,000 ph./n<sub>th</sub> under thermal neutron irradiation, approximately six times higher than that of the standard <sup>6</sup>Li glass scintillator (GS20). With the fast decay time (650 ns) as red/NIR emission, high light output, and red/NIR emission wavelength, Na<sub>2−</sub><i><sub>x</sub></i>Li<i><sub>x</sub></i>HfI<sub>6</sub> offers a robust and high-performance alternative material to conventional scintillators.</p>

    DOI: 10.2109/jcersj2.25178

    Open Access

    CiNii Research

  12. Scintillation Properties of Tl+ and Sr2+ Co-doped Cs3Cu2I5

    Urano Y., Kurosawa S., Yamaji A., Yoshikawa A., Wu Y.

    IEEE Transactions on Nuclear Science     2026

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    Tl<sup>+</sup>-doped Cs3Cu2I5 (Tl:CCI) scintillator is reported to have a light output of 98,200 photons/MeV and energy resolution of 3.3% (FWHM, 662 keV), while the energy resolution is expected to be improved due to high light output compared to other bright scintillators such as Ce:LaBr3 with an FWHM energy resolution of 3.0% at 662 keV and light output of around 60,000 photons/MeV. The energy resolution is related to nonproportional response (NPR), and NPR and energy resolution for Tl:NaI was improved by co-doping with Sr<sup>2+</sup> and Ca<sup>2+</sup>. Therefore, we grew Tl:CCI and Sr<sup>2+</sup> co-doped Tl:CCI (Tl,Sr:CCI) crystals by the vertical Bridgman-Stockbarger method to investigate the Sr<sup>2+</sup> co-doping effect on the scintillation properties. The result shows the NPR was improved with Sr<sup>2+</sup> co-doping, and the observed energy resolution was improved; Tl:CCI, 0.1 and 0.5% Sr-codoped Tl:CCI had energy resolutions of 4.9±0.1, 4.5±0.1 and 4.3±0.1% (FWHM, 662 keV), respectively. In addition, their intrinsic energy resolutions (FWHM) at 662 keV were estimated to be 2.1±0.2, 1.1±0.2 and 1.0±0.2%, respectively, so that Sr<sup>2+</sup> co-doping effect for the energy resolution was observed.

    DOI: 10.1109/TNS.2025.3649272

    Scopus

  13. Development status of the SMILE-3 balloon experiment Open Access

    Nakamori T., Takada A., Abe M., Deguchi S., Hamaguchi K., Iiyama H., Kurosawa S., Kushida J., Miuchi K., Mizumura Y., Mori M., Munakata Y., Oka T., Okamoto K., Sakata M., Sato T., Sawano T., Tanimori T., Tsukamoto H., Yaegashi D., Yoshioka R.

    Proceedings of Science   Vol. 501   2025.12

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    MeV gamma-ray astronomy remains relatively underexplored, despite extensive worldwide efforts to investigate this crucial energy range. To address this challenge, we have demonstrated the high-performance capabilities of an electron-tracking Compton camera (ETCC) during the Sub-MeV/MeV gamma-ray Imaging Loaded-on-balloon Experiment (SMILE) missions. The ETCC employs a gaseous time-projection chamber (TPC) as the primary scatterer, surrounded by pixelated scintillator arrays (PSAs) that function as absorbers. The gas TPC measures the momentum vector of the recoil electron, while the PSAs simultaneously determine the energy of the scattered gamma ray. This capability enables a bijective reconstruction of both the direction and energy of the incident gamma ray, which enhances the sensitivity compared to classical Compton reconstruction that constrains the incident direction only by a circular region. The SMILE-2+ experiment, which consisted of a 26-hour balloon flight over Australia, successfully detected the Crab Nebula and Galactic diffuse emissions around the Galactic Center at a significance level exceeding 4σ. Following this achievement, we have initiated the successor project, SMILE-3, to enable a more detailed investigation of diffuse emissions. The detector design has been upgraded to achieve a larger effective area and a wider dynamic range, thereby increasing photon collection power. The first flight for SMILE-3 is currently planned for early 2027. In this paper, we present an overview of the SMILE-3 experiment and report the current status of our R&D efforts.

    DOI: 10.22323/1.501.0777

    Open Access

    Scopus

  14. Investigation of the intrinsic detector background for SMILE-3 balloon experiment Open Access

    Iiyama H., Nakamori T., Yaegashi D., Ikeda T., Oka T., Takada A., Abe M., Tsukamoto H., Sato T., Deguchi S., Sawano T., Sakata M., Munakata Y., Okamoto K., Mizumura Y., Kurosawa S., Mori M., Kushida J., Hamaguchi K., Miuchi K., Tanimori T., Yoshioka R.

    Proceedings of Science   Vol. 501   2025.12

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    MeV gamma-ray observations are a probe for uncovering various physical phenomena, such as the search for dark matter and primordial black holes, and the study of the nucleosynthesis in the Universe. To achieve high sensitivity in this band, we are developing an electron-tracking Compton camera (ETCC), which combines a gaseous time projection chamber (TPC) and pixelated GSO(Ce) scintillator arrays (PSAs). The ETCC tracks recoil electrons in the TPC and reconstructs Compton events to uniquely determine gamma-ray arrival directions. We are now planning the Sub-MeV/MeV gamma-ray Imaging Loaded-on-balloon Experiment 3 (SMILE-3), which will use an upgraded ETCC from the previous balloon experiment, SMILE-2+, with improved dynamic range and effective area. The first one-day flight of SMILE-3 is scheduled for spring 2027 in Australia” The ETCC has background events originating from radioactive isotopes contained in the GSO(Ce) scintillators. Therefore, we measured the intrinsic background of all GSO(Ce) scintillators to be used in SMILE-3 and investigated their properties to evaluate the feasibility of selecting low-background scintillators.

    DOI: 10.22323/1.501.0690

    Open Access

    Scopus

  15. Ce3+:CaHfO3 thick film scintillators epitaxially grown on SrTiO3, YAlO3, and MgO substrates using chemical vapor deposition Open Access

    Oga T., Kurosawa S., Ito A.

    Journal of Luminescence   Vol. 288   2025.12

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    Alkaline earth hafnate perovskite is a promising inorganic scintillator due to its high density and high stopping power; however, its high melting point and phase transitions at elevated temperatures make its crystal growth difficult. We apply chemical vapor deposition method to prepare Ce<sup>3+</sup>-doped CaHfO<inf>3</inf> (Ce<sup>3+</sup>:CaHfO<inf>3</inf>) thick films on the SrTiO<inf>3</inf>, YAlO<inf>3</inf>, and MgO substrates. Ce<sup>3+</sup>:CaHfO<inf>3</inf> thick films were epitaxially grown on each substrate with deposition rates of 44–77 μm h<sup>−1</sup>. The luminescence spectra of the films at the excitation wavelength of 340 nm showed peaks at 423 nm and 463 nm, which were attributed to the Ce<sup>3+</sup> 5d → <sup>2</sup>F<inf>5/2</inf> and 5d → <sup>2</sup>F<inf>7/2</inf> transitions, respectively. The scintillation light yield of the Ce<sup>3+</sup>:CaHfO<inf>3</inf> thick film grown on the MgO substrate was 2900 photons per 5.5 MeV with fast decay constant of 32.1 ns.

    DOI: 10.1016/j.jlumin.2025.121568

    Open Access

    Scopus

  16. Crystal growth and characterization of 1-inch GTAGG: Ce single crystal for sub-micron resolution synchrotron radiation X-ray imaging Open Access

    Omuro K., Yoshino M., Gushchina L., Yamamoto S., Nakanishi K., Kamada K., Bartosiewicz K., Kim K.J., Horiai T., Murakami R., Yamaji A., Hanada T., Yokota Y., Kurosawa S., Ohashi Y., Sato H., Kataoka J., Yoshikawa A.

    Scientific Reports   Vol. 15 ( 1 ) page: 12993   2025.12

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    A high-performance Ce<sup>3+</sup>-doped (Gd, Tb)<inf>3</inf>(Ga, Al)<inf>5</inf>O<inf>12</inf> (GTAGG: Ce) single crystal was engineered and characterized, demonstrating a high application potential for advanced X-ray imaging. A transparent 1-inch diameter single crystal was grown using the Czochralski method, demonstrating a significant advancement in large-scale scintillator production. Comprehensive characterization using X-ray diffraction and electron probe micro-analysis confirmed the crystal’s structural integrity. Photoluminescence and radioluminescence spectroscopy demonstrated efficient bidirectional energy transfer between Ce<sup>3+</sup> and Tb<sup>3+</sup> ions, a critical mechanism enhancing the performance of the scintillator. X-ray imaging tests were performed using crystals with a thickness of 100 μm at the Aichi Synchrotron Radiation Center. Comparison with the industry-standard LuAG: Ce scintillator showed that the GTAGG: Ce crystal produced 2.4 times higher light output and achieved a high spatial resolution of 0.85 μm. The results indicated that GTAGG: Ce is suitable for the next generation of high-performance X-ray imaging detectors in scientific and medical imaging applications.

    DOI: 10.1038/s41598-025-96031-5

    Open Access

    Scopus

    PubMed

  17. Chromatin accessibility in stem cells unveils progressive transcriptional alterations in myelodysplastic syndrome Open Access

    Oshima M., Takayama N., Nakajima-Takagi Y., Shinoda D., Itokawa N., Kurosawa S., Kaito S., Kamiya T., Yamada Y., Andoh S., Kayamori K., Paul S.K., Kanashiro M.A., Muto T., Tsukamoto S., Sakaida E., Sato E., Yusa N., Yokoyama K., Nannya Y., Imoto S., Rahmutulla B., Kaneda A., Yamaguchi K., Furukawa Y., Doki N., Eto K., Nishikawa K., Ding Y., Myojo T., Harada Y., Harada H., Iwama A.

    Nature Communications   Vol. 16 ( 1 ) page: 10726   2025.12

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    Language:English   Publisher:Nature Communications  

    Myelodysplastic syndrome (MDS) originates from hematopoietic stem cell (HSC) clones with acquired gene mutations. However, the molecular characteristics of MDS stem cells remain poorly understood. Here, we show that the chromatin accessibility profiles of MDS stem cells more accurately reflect disease status than those of progenitor cells and reveal the process of stem cell alterations during disease progression. Characterization of differentially accessible regions (DARs) shows that MDS stem cells acquire progenitor-like chromatin accessibility during disease progression, leading to disruption of the normal stem-progenitor hierarchy. Profiling of transcription factor-binding motifs at DARs further uncovers precocious activation of myeloid transcriptional networks in MDS stem cells, with a concurrent loss of HSC-associated regulatory programs. In particular, increased chromatin accessibility at CEBP target sites represents the myeloid reprogramming status of MDS stem cells. Newly developed “progenitor scores” based on chromatin accessibility stratify disease status and correlate well with prognosis. These findings indicate that chromatin landscapes of MDS stem cells define their cell-autonomous behavior and contribute to disease progression.

    DOI: 10.1038/s41467-025-65753-5

    Open Access

    Scopus

    PubMed

  18. Differential impact of graft-versus-host disease on post-transplant outcomes of chronic myelomonocytic leukemia according to transplant procedures Open Access

    Itonaga H., Miyazaki Y., Fujioka M., Kurosawa S., Nagata Y., Shimazu Y., Ueda T., Uchida N., Doki N., Nishida T., Asada N., Tanaka M., Takada S., Sakurai M., Kurokawa M., Yoshimitsu M., Kanda Y., Ichinohe T., Atsuta Y., Tachibana T.

    Leukemia Research   Vol. 159   page: 108134   2025.12

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    Language:English   Publisher:Leukemia Research  

    Allogeneic hematopoietic stem cell transplantation (allo-HSCT) provides curative outcomes for chronic myelomonocytic leukemia (CMML). We conducted a retrospective study to clarify the protective impact of acute and chronic graft-versus-host disease (aGVHD and cGVHD) on relapse by transplant procedures in 314 CMML patients. Interaction effects of conditioning intensity were observed with aGVHD (P<inf>interaction</inf>=0.181) and cGVHD (P<inf>interaction</inf>=0.256) for the cumulative incidence of relapse (CIR), whereas interaction effects of donor type were not detected with GVHD. In patients with the myeloablative conditioning regimens, the multivariate analysis showed that the development of aGVHD was not associated with overall survival (OS). The development of limited cGVHD correlated with better OS (HR [95 % CI], 0.34 [0.14–0.81]; P = 0.015); and that of extensive cGVHD correlated with better OS (HR, 0.44 [0.21–0.91]; P = 0.026) and lower CIR (HR, 0.28 [0.08–0.94]; P = 0.040). In patients with the reduced-intensity conditioning regimens, the development of grade I-II aGVHD correlated with better OS (HR, 0.39 [0.20–0.76]; P = 0.005) and lower CIR (HR, 0.30 [0.13–0.70]; P = 0.006). The development of extensive cGVHD correlated with better OS (HR, 0.44 [0.20–0.96]; P = 0.039). The present results suggest that the type and severity of GVHD mediating graft-versus-leukemia effects against relapse were influenced by conditioning intensity in CMML patients.

    DOI: 10.1016/j.leukres.2025.108134

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    PubMed

  19. Yb3+:Lu2O3 thick film scintillators with dense and columnar structures grown via chemical vapor deposition Open Access

    Nakayama T., Kurosawa S., Ito A.

    Journal of Luminescence   Vol. 288   2025.12

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    Thick film scintillators enhance the spatial resolution of nondestructive X-ray testing. This study investigates thick-film phosphors with dense and uniform microstructure, which smoothly transmit scintillation light, and with columnar-structured phosphors expected to exhibit waveguide effects. We demonstrated the preparation of Yb<sup>3+</sup>:Lu<inf>2</inf>O<inf>3</inf> thick films with both dense and columnar structures using chemical vapor deposition. High deposition temperature and high Lu vaporization temperature yielded dense films, whereas reduced temperatures produced columnar microstructures. Increasing the Yb vaporization temperature increased the lattice constant of the Yb<sup>3+</sup>:Lu<inf>2</inf>O<inf>3</inf> films, suggesting an increase in the Yb concentration in the film. The resulting Yb<sup>3+</sup>:Lu<inf>2</inf>O<inf>3</inf> films exhibited Yb<sup>3+</sup> charge-transfer luminescence at 300–600 nm and f–f transition emission at 900–1100 nm. For 5.5 MeV-α-particle-excited scintillation, the scintillation light yields of the Yb<sup>3+</sup>:Lu<inf>2</inf>O<inf>3</inf> columnar and dense films with 0.6–9.4 mol%Yb<inf>2</inf>O<inf>3</inf> were ranged from 880 to 1290 photons per 5.5 MeV with a fast decay constant of 1.9–2.2 ns.

    DOI: 10.1016/j.jlumin.2025.121589

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  20. Tb3+and Ce3+as a functional couple for enhanced luminescence in YAG ceramics for X-ray imaging and high-power white LEDs and laser diodes Open Access

    Markovskyi A., Chewpraditkul W., Gołębiewski P., Socha P., Węglarz H., Szysiak A., Jary V., Kučerková R., Tomala R., Yoshikawa A., Kurosawa S., Buczyński R., Chewpraditkul W., Bartosiewicz K.

    Materials Advances   Vol. 6 ( 22 ) page: 8464 - 8478   2025.11

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    The exposure of luminescent materials to X-ray radiation and high-power laser excitation results in significant heating, leading to thermal quenching and a corresponding reduction in phosphor efficiency. This study aimed to address this limitation by enhancing material efficiency while maintaining high thermal stability. YAG:Ce,Tb transparent ceramics were successfully fabricated via vacuum reactive sintering method, with moderate concentrations of Tb<sup>3+</sup> ions (1, 5 and 10 at%) codopants. These ceramics exhibited a dense microstructure without micropores, achieving high transparency of 77–80% at 900 nm. The incorporation of Tb<sup>3+</sup> ions, is evidenced by the systematic increase in lattice constants from 12.608 Å (YAG:Ce) to 12.615 Å (YAG:Ce,Tb10%) in accordance with Vegard's law. The phonon-assisted Ce<sup>3+</sup> ↔ Tb<sup>3+</sup> bidirectional resonance mechanism, which facilitated energy transfer between Ce<sup>3+</sup> and Tb<sup>3+</sup> ions, was observed. The optimal transfer rate was observed at approximately 480 K. Beyond this temperature, the rate progressively accelerated, leading to accelerated decay times. Notably, YAG:Ce,Tb10% ceramics demonstrated a two-fold increase in radioluminescence intensity compared to uncodoped YAG:Ce ceramics. This substantial improvement in luminescence performance highlights the potential of YAG:Ce,Tb ceramics as highly efficient phosphors for X-ray imaging applications, offering enhanced brightness and energy transfer efficiency under high-temperature operating conditions. The Tb<sup>3+</sup> codoping also enhanced Ce<sup>3+</sup> emission, allowing for tuning of the correlated color temperature to a maximum of 6013 K, while maintaining a stable color rendering index of 69–73 and luminous efficacy of ∼123 lm W<sup>−1</sup>. It was shown that the luminous efficacy was not a constant parameter, but depended on the excitation laser power, initially increasing with power up to 0.5 W and then saturating. These results establish YAG:Ce,Tb transparent ceramics as highly promising materials for white LEDs due to their good thermal stability, tunable optical properties, and enhanced luminescence performance.

    DOI: 10.1039/d5ma00464k

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  21. Tolerance of Corundum-Structured Tin-Doped Indium Oxide Thin Films to Gamma-ray Irradiation

    Shimazoe K., Kurosawa S., Tanaka H., Takata T., Nishinaka H.

    Physica Status Solidi B Basic Research   Vol. 262 ( 11 )   2025.11

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    Corundum-structured Sn-doped indium oxide (rh-ITO) is investigated as a novel transparent conductive oxide. Herein, its gamma-ray tolerance up to a total dose of 77 kGy is examined for potential applications in harsh environments, such as space. The investigations are conducted on rh-ITO with Sn concentrations of 0 and 5 at%. X-ray diffraction 2θ-ω scan analysis reveals that no phase separation occurs due to gamma-ray irradiation. The carrier concentration in undoped rh-In<inf>2</inf>O<inf>3</inf> increases after irradiation, indicating that the gamma rays displace the oxygen atoms and form oxygen defects that generate donors. The high visible light transparency of rh-In<inf>2</inf>O<inf>3</inf> and rh-ITO is maintained after irradiation. This study demonstrates the high stability of rh-ITO to gamma-ray irradiation until 77 kGy dose. This work contributes to the application of rh-ITO as an electrode in high-radiation environments.

    DOI: 10.1002/pssb.202400368

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  22. Concept of high-z gamma-ray bursts unraveling the dark ages and extreme space-time mission—HiZ-GUNDAM Open Access

    Yonetoku D., Doi A., Mihara T., Matsuhara H., Sakamoto T., Tsumura K., Ioka K., Arimoto M., Ando Y., Enoto T., Fujimoto K., Goto H., Hiraga J., Kawai N., Kondo R., Kurosawa S., Maeda Y., Mitsuishi I., Murakami T., Nagataka I., Nakagawa Y., Nakajima H., Ogino N., Sato M., Sato T., Sawano T., Serino M., Shen H.C., Sugita S., Sugizaki M., Takahashi S., Tamagawa T., Tamura K., Tanaka T., Tanimori T., Tashiro M.S., Tomida H., Uchida H., Ueda S., Yamaoka K., Yamauchi M., Yatsu Y., Yoshida A., Akitaya H., Fukui A., Fukui H., Hashimoto R., Hori T., Ita Y., Kageyama R., Kawabata K., Matsuura S., Miyasaka A., Motohara K., Narita N., Noda H., Okita H., Sano K., Shinozaki K., Tajima S., Urata Y., Wada T., Yamashita H., Yanagisawa K., Yoshida M., Gunji S., Togashi T., Sato R., Watanabe K., Niinuma H., Bando N., Jikuya I., Minesugi K., Miyazaki Y., Kono Y., Takase N., Nakatsubo S., Kaga T., Asano K., Inayoshi K., Inoue S., Ito H., Izumiura H., Kawanaka N., Kinugawa T., Kisaka S., Kiuchi K., Kyutoku K., Matsumoto J., Mizuta A., Murase K., Nagakura H., Nagataki S., Nakada Y., Nakamura T., Niino Y., Suwa Y., Takahashi K., Tanaka T., Toma K.

    Journal of Astronomical Telescopes Instruments and Systems   Vol. 11 ( 4 )   2025.10

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    HiZ-GUNDAM is a candidate for JAXA’s competitive medium-class mission program, with its concept approved by ISAS/JAXA in 2018. This proposed satellite aims to play a leading role in time-domain astronomy in the 2030s by pursuing two primary scientific goals: (1) probing the early universe through the detection of high-redshift gamma-ray bursts (GRBs) and (2) enabling the rapid identification of X-ray and optical-near-infrared counterparts of multimessenger sources. To achieve these objectives, HiZ-GUNDAM is equipped with two key instruments. A wide-field X-ray monitor, EAGLE, utilizes a micropore optics array and a focal plane imaging sensor to observe transients across ∼0.5sr in the 0.4 to 4 keV energy range. To follow up on this observation, an optical–near-infrared telescope, MONSTER, features a 30 cm aperture and conducts simultaneous five-band photometry over the 0.5 to 2.5μm wavelength range. It employs a Kösters-type prism for multi-band photometry to follow up on transients detected by the EAGLE. A sun-synchronous dawn–dusk orbit has been selected to ensure thermal stability for the MONSTER. We present a comprehensive overview of the HiZ-GUNDAM mission concept. The mission is expected to make a significant contribution to our understanding of cosmic evolution through observations of high-redshift GRBs, as well as to the identification of the multiwavelength properties of multimessenger sources by enhancing the observational capabilities for transient searches. The specifications and concepts discussed herein are subject to refinement as the mission progresses.

    DOI: 10.1117/1.JATIS.11.4.044002

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  23. Effect of the pringle maneuver on patient status index during total intravenous anesthesia with propofol Open Access

    Honda J., Yoshida K., Obara S., Inoue S., Kurosawa S.

    Journal of Anaesthesiology Clinical Pharmacology   Vol. 41 ( 4 ) page: 754 - 755   2025.10

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    DOI: 10.4103/joacp.joacp_533_24

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  24. Outcomes of Allogeneic Hematopoietic Stem Cell Transplantation in Elderly Patients with Myeloid Malignancies Over 70 Years Old: A Retrospective Analysis of the Japanese Nationwide Registry

    Kobayashi S., Itonaga H., Kurosawa S., Yanada M., Miyazaki Y., Najima Y., Aoki J., Uchida N., Miyakoshi S., Doki N., Tanaka M., Uehara Y., Eto T., Anzai N., Onizuka M., Sawa M., Fukuda T., Asada N., Katayama Y., Kawakita T., Yoshimitsu M., Kanda J., Ohbiki M., Atsuta Y., Ishiyama K.

    Transplantation and Cellular Therapy   Vol. 31 ( 10 ) page: 822 - 822.e11   2025.10

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    Although allogeneic hematopoietic stem cell transplantation (SCT) remains a potentially curative treatment option for several myeloid malignancies, despite the fact that the average age at disease onset for myeloid malignancies is approximately 70 years of age, its applicability in elderly patients is challenging. We retrospectively evaluated the outcomes of elderly SCT patients with acute myeloid leukemia (AML) or myelodysplastic syndrome (MDS), using a nationwide Japanese registry database. We analyzed the data of 3609 patients ranging from 65 to 79 years of age with AML or MDS who underwent initial SCT between 2003 and 2022, while focusing on those 70 to 74 (n = 645) and 75 to 79 years old (n = 65). The 2-year overall survival (OS) and relapse-free survival rates for patients aged 65 to 69, 70 to 74, and 75 to 79 years were 40.9%, 38.0%, and 22.7%, and 48.4%, 47.2%, and 18.5%, respectively. Among patients categorized as low-risk at SCT, no significant differences were observed in the cumulative incidence of grade III to IV acute graft-versus-host disease (aGVHD), extensive chronic GVHD (cGVHD), non-relapse mortality, or relapse across all age groups. A multivariate analysis revealed that sex (male), diagnosis (AML), disease status (high-risk), SCT year (2003 to 2007), performance status (2-4), hematopoietic cell transplantation-specific comorbidity index (≥3), development of grade III to IV III–IV aGVHD, and extensive chronic GVHD significantly affected the OS. An older age (75 to 79) and the intensity of conditioning (reduced intensity) were factors indicating a trend toward an adverse prognosis. In these subgroups, significant interactions were observed between OS and SCT years, the time from diagnosis to SCT, and aGVHD. These findings suggest that SCT may be a potential curative option for selected elderly patients up to the mid-70s; however, careful patient selection and vigilant management of aGVHD are crucial factors for improving outcomes.

    DOI: 10.1016/j.jtct.2025.06.032

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  25. Evaluation of photon-counting capability for silicon photomultiplier-based photon-counting CT using Ce-doped SrHfO3 scintillator

    Sato D., Kurosawa S., Harata K., Fujioka K., Yamaji A., Urano Y., Arimoto M., Lucyana F., Tomoda T.

    Radiation Measurements   Vol. 187   2025.9

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    Cross-sectional images were obtained using photon-counting computed tomography (PCCT) for medical applications, incorporating a silicon photomultiplier (SiPM) and Ce-, Mg- and Al-codoped SrHfO<inf>3</inf> transparent-ceramic scintillator (Mg/Al/Ce:SHO). A maximum counting rate of 8 MHz was achieved with our PCCT system equipped with this scintillator. Enhancing the maximum counting rate is crucial for short-time imaging, and further advancements in counting capability are essential for clinical applications. The Mg/Al/Ce:SHO scintillator, which has a shorter decay time (∼20 ns) and higher density (7.6 g/cm<sup>3</sup>) compared to the Ce:(Y, Gd)<inf>3</inf>(Al, Ga)<inf>5</inf>O<inf>12</inf> scintillator used in earlier PCCT systems, was prepared via spark plasma sintering and integrated into the PCCT. The maximum counting rate was estimated by varying the intensity of incident X-ray photons using an X-ray tube and applying a non-paralyzable dead-time model, yielding approximately 8 MHz–double the photon-counting capability of our previous system. Additionally, static phantom imaging with iodine and gadolinium contrast agents was performed at X-ray tube current of 0.5, 1.0 and 2.0 mA. The image quality remained consistent within the standard deviation of CT values despite increasing the tube current. These findings suggest that the Mg/Al/Ce:SHO scintillator offers superior potential for clinical PCCT applications compared to conventional systems.

    DOI: 10.1016/j.radmeas.2025.107456

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  26. Fabrication and Characterization of Ce-Doped LiCaAlF6–CaF2–Li3AlF6 and CaF2–LiF–Li3AlF6 Scintillators for Thermal Neutron Detection Open Access

    Matsuyama T., Kamada K., Murugesan N., Yoshino M., Murakami R., Yamaji A., Sato H., Kim K.J., Ishizawa S., Kurosawa S., Hanada T., Yokota Y., Yoshikawa A.

    Crystals   Vol. 15 ( 9 )   2025.9

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    In this study, we developed and characterized novel scintillators with Ce: LiCaAlF<inf>6</inf>–CaF<inf>2</inf>–Li<inf>3</inf>AlF<inf>6</inf> and Ce: CaF<inf>2</inf>–LiF–Li<inf>3</inf>AlF<inf>6</inf> ternary systems for thermal neutron detectors. The eutectics were grown by the vertical Stochbarger-Bridgman (VB) technique, and their constituent phases were identified using powder X-ray diffraction and scanning electron microscopy. Radioluminescence spectra irradiated under an Ag-target X-ray tube and confirmed the 5d-4f and self-trapped exciton luminescence derived from Ce<sup>3+</sup>. Scintillation decay and pulse height measurements were performed using <sup>252</sup>Cf and <sup>60</sup>Co sources. The Ce: CaF<inf>2</inf>–LiF–Li<inf>3</inf>AlF<inf>6</inf> sample exhibited approximately 5.6 times higher effective neutron sensitivity compared with a Ce: LiCaAlF<inf>6</inf> single crystal. A favorable decrease in the neutron discrimination threshold level (Q<inf>th</inf>) due to reduced γ-ray emission was observed. <sup>6</sup>Li-enriched Ce: CaF-based scintillators hold potential for nuclear decommissioning applications.

    DOI: 10.3390/cryst15090761

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  27. Fatal Eosinophilia-Associated Thrombotic Microangiopathy and the Role of Renal Charcot-Leyden Crystals Open Access

    Kurosawa S., Hizuka K., So Y., Yoshimura Y., Minami H., Idetsuka T., Hayashi H., Shimomura R., Yamaguchi Y., Hayami H., Inoue T., Kawamoto Y., Matsumoto K., Kambara T., Hirano M., Maruyama S., Kato N., Tatematsu Y., Ueki S., Nakazato T.

    Kidney International Reports   Vol. 10 ( 8 ) page: 2864 - 2868   2025.8

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    DOI: 10.1016/j.ekir.2025.05.015

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  28. Magnetic Field Switching of Exchange Bias in a Metallic FM/AFM Heterostructure at Room Temperature

    Asakura M., Higo T., Matsuo T., Tsushima Y., Kurosawa S., Uesugi R., Nishio-Hamane D., Nakatsuji S.

    Nano Letters   Vol. 25 ( 26 ) page: 10294 - 10302   2025.7

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    The exchange bias effect, which causes a shift in the ferromagnetic hysteresis loop due to magnetic coupling with an adjacent antiferromagnetic layer, has been a key area of study for fundamental research and spintronic applications. This effect is known to be static once established through a field cooling procedure and is difficult to manipulate isothermally. Here we present the first room temperature field switching of interlayer magnetic coupling at the metallic heterointerface between a ferromagnet and antiferromaget. Specifically, we demonstrate that the exchange bias can be systematically switched by manipulating the global time-reversal-symmetry-broken antiferromagnetic order of Mn<inf>3</inf>Sn via both magnetic field sweeping and field cooling. Furthermore, we confirm that the magnitude and sign of the interlayer coupling can be tuned by selecting the ferromagnet. These findings provide a novel approach for controlling the magnetic state of ferromagnets and functional antiferromagnets, paving the way for advancing spintronic technologies using antiferromagnets.

    DOI: 10.1021/acs.nanolett.5c00988

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  29. Study on the optimization of an ambient dose detector in an accelerator-based BNCT irradiation field Open Access

    Zhao L., Matsubayashi N., Nojiri M., Hu N., Takata T., Kawabata S., Kurosawa S., Masuda A., Tanaka H.

    Japanese Journal of Applied Physics Part 1 Regular Papers and Short Notes and Review Papers   Vol. 64 ( 6 )   2025.6

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    Accelerator-based boron neutron capture therapy (AB-BNCT) systems that utilize various neutron production methods have been developed in recent years. As the AB-BNCT system is a novel radiation production system, accurately measuring the neutron ambient dose is crucial for evaluating its performance and ensuring its safety. In this study, we designed a neutron detector system capable of measuring the neutron ambient dose H* in a cyclotron-based epithermal neutron source irradiation field using the particle and heavy ion transport code system 3.34 Monte Carlo simulation code. This neutron detector system comprises slow and fast neutron detectors, which are sensitive to energy ranges of 10<sup>−9</sup>-10<sup>−2</sup> MeV and 10<sup>−2</sup>-28 MeV, respectively. The response function of this neutron detector system exhibited satisfactory agreement with the conversion coefficients h*, and the dose measurement accuracy was within 6.5%.

    DOI: 10.35848/1347-4065/add593

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  30. X-ray performance evaluation and vibration testing of the wide-field X-ray monitor with Lobster Eye Optics

    Goto H., Yonetoku D., Arimoto M., Sawano T., Nagataka I., Mihara T., Sakamoto T., Maeda Y., Matsuhara H., Doi A., Takase N., Kaga T., Nakatsubo S., Kurosawa S., Komatsuzaki T.

    Journal of Instrumentation   Vol. 20 ( 6 )   2025.6

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    The future satellite HiZ-GUNDAM will be equipped with a wide-field X-ray monitor using Lobster Eye Optics (LEO), covering a wide field of view of ∼ 0.6 steradian in the 0.4-4 keV energy range. LEO, an X-ray optics system, achieves both a wide field of view and high sensitivity by focusing soft X-rays through spherically curved SiO<inf>2</inf> plates with heavy-metal-coated micropores. This design significantly enhances sensitivity by reducing cosmic X-ray background events, outperforming conventional non-focusing detectors. As a prototype, we developed a breadboard frame capable of holding nine LEO segments, aligning them on a single spherical surface to achieve a wide field of view. Given LEO's brittleness, there are concerns about potential damage from launch vehicle vibrations. In addition, the system must be structurally robust, avoiding strong resonances at expected vibration frequencies. To address these concerns, we performed vibration tests simulating launch conditions to assess the structural integrity of the combined LEO and breadboard frame. X-ray performance, particularly angular resolution, was evaluated before and after the tests. The results demonstrate that the system is structurally robust and capable of maintaining imaging performance after simulated rocket launch vibrations.

    DOI: 10.1088/1748-0221/20/06/C06044

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  31. Center effect on outcomes of second allogeneic hematopoietic stem cell transplantation for B-cell acute lymphoblastic leukemia: a nationwide retrospective study

    Kurosawa S., Fukuda T., Ichinohe T., Hashii Y., Kanda J., Goto H., Kato K., Ishimaru F., Yoshimitsu M., Hino M., Matsuo K., Ito Y., Yanagisawa A., Ohbiki M., Tabuchi K., Atsuta Y., Arai Y.

    Cytotherapy   Vol. 27 ( 6 ) page: 733 - 743   2025.6

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    We evaluated the impact of center volume on outcomes in patients with B-cell acute lymphoblastic leukemia following their second allogeneic hematopoietic stem cell transplantation (allo-HSCT). Our cohort included 299 patients with relapse and 68 patients with graft failure after their first allo-HSCT between 2003 and 2017. Patients were stratified into low- and high-volume groups based on the number of allo-HSCT performed at each center. The primary endpoint was 5-year overall survival (OS) following the second allo-HSCT. In the relapse cohort, the high-volume group demonstrated significantly better 5-year OS (21.1% vs 13.6%, P = 0.0062) and progression-free survival (16.1% vs 10.6%, P = 0.010). Multivariate analysis showed that high-volume group was a favorable factor for OS (hazard ratio [HR]: 0.72, 95% confidence interval [CI]: 0.56–0.94, P = 0.016). This survival benefit was consistent in both Philadelphia chromosome-negative (HR: 0.71, 95% CI: 0.51–0.99, P = 0.042) and positive (HR: 0.61, 95% CI: 0.39–0.95, P = 0.030) subcohorts. In the graft failure cohort, the high-volume group showed a trend toward better 5-year OS (41.6% vs 24.4%, P = 0.098) and lower 5-year nonrelapse mortality (NRM) (55.9% vs 75.6%, P = 0.067). Multivariate analysis confirmed the protective effect of the high-volume group on NRM (HR: 0.55, 95% CI: 0.30–0.99, P = 0.044). Our findings demonstrate that center volume significantly impacts outcomes after the second allo-HSCT regardless of indication, highlighting the need for inter-center collaboration and standardized management strategies for this high-risk population.

    DOI: 10.1016/j.jcyt.2025.03.002

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  32. Effects of alkali earth metal doping on the luminescence and scintillation properties of Cs2HfCl6 single crystals

    Cheng S., Beitlerova A., Kucerkova R., Nikl M., Kurosawa S., Ren G., Wu Y.

    Radiation Measurements   Vol. 184   2025.6

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    In recent years, intrinsic self-trapped exciton (STE) emission materials have been developed as promising scintillators due to their bright and self-absorption free luminescence. Among these materials, cesium hafnium chloride (Cs<inf>2</inf>HfCl<inf>6</inf>, CHC) has received attention for its high light yield, remarkable energy resolution, high radiation-stopping capability, absence of radioactive background, and low non-proportionality. This study investigated the luminescence and scintillation properties of both the undoped and alkali earth metals (AE)-doped CHC. The findings revealed that undoped and AE-doped CHC exhibited four emission peaks at 368, 383, 435, and 465 nm, corresponding to intrinsic STE emission, defect-related emission, Zr-related emission, and I-related emission, respectively. The corresponding decay time were about 1.5, 5.5, 11, and 2.3 μs. Notably, AE doping did not introduce any new emission centers, as confirmed by photoluminescence and radioluminescence spectra. The light yield and energy resolution for undoped CHC and CHC:AE were measured to be 34,000–37,000 ph/MeV and 3.5–4.1 % at 662 keV, respectively. Although AE doping did not enhance scintillation properties of CHC, this study elucidated several sources of luminescence centers in CHC, providing valuable insights for future optimization of its scintillation properties.

    DOI: 10.1016/j.radmeas.2025.107438

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  33. Correlating Structural Disorder and Pr3+ Emission Dynamics in Lu3Al2.5-xScxGa2.5O12 Crystals: A Comprehensive Structure-Property Investigation Open Access

    Bartosiewicz K., Dewo W., Nagirnyi V., Runka T., Kirm M., Horiai T., Szymanski D., Yamaji A., Kurosawa S., Socha P., Pejchal J., Babin V., Kral R., Kotlov A., Yoshikawa A., Nikl M.

    ACS Omega   Vol. 10 ( 19 ) page: 19817 - 19831   2025.5

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    This study explored the influence of Sc<sup>3+</sup> ions incorporation on the structural, vibrational, luminescent, and scintillation properties of Pr<sup>3+</sup>-doped Lu<inf>3</inf>(Al, Sc)<inf>2.5</inf>Ga<inf>2.5</inf>O<inf>12</inf> garnet crystals. Addressing the limited research on Sc-admixed and Pr<sup>3+</sup> doped garnet systems, this work successfully demonstrated the crystallization of garnet crystals from the melt, overcoming the substantial atomic mismatch between Sc and Al while preserving the thermodynamic stability of the garnet phase. Importantly, Sc-admixing enhanced atomic homogeneity and allowed for increased doping concentrations of Pr<sup>3+</sup> ions, which is crucial for tailoring the functional properties of advanced optical materials. The trap depths ranged from 1.63 eV (deep traps) to 0.22 eV (shallow traps) across all samples, with frequency factors predominantly between 1 × 10<sup>7</sup> and 1 × 10<sup>11</sup> s<sup>-1</sup>, consistent with first-order thermoluminescent kinetics. From a materials design perspective, Sc<sup>3+</sup> ions substitution induced beneficial host lattice disorder, enhancing the emission intensity of 4f<sup>1</sup>5d<inf>1</inf><sup>1</sup> → 4f<sup>2</sup> interconfigurational and 4f<sup>2</sup> → 4f<sup>2</sup> intraconfigurational transitions. This effect highlighted the potential of Sc as a promising substituent for enhancing the luminescence intensity of rare earth elements. Synchrotron radiation experiments provided insights into the impact of Sc on band gap energy and energy transfer efficiency toward Pr<sup>3+</sup> ions offering new opportunities for engineering scintillators and phosphors with tunable optical properties.

    DOI: 10.1021/acsomega.5c01062

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  34. Application of the Deconvolution Method to Alpha-Ray Energy Spectrum to Improve the Performance of a Radiation Airborne Particulate Monitor Open Access

    Sasano M., Hayashi M., Yanagawa Y., Kai M., Nakano Y., Osawa Y., Kurosawa S., Morishita Y.

    Journal of Radiation Protection and Research   Vol. 50   page: S86 - S94   2025.5

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    Background: At nuclear facilities and decommissioning sites, monitoring radioactivity concentrations in airborne particulates is crucial to prevent worker exposure. To avoid internal exposure, alpha-decay radionuclides must be detected. When monitoring alpha-decay radionuclides in airborne dust, we want to measure the concentration of only artificial radionuclides (e.g., <sup>238</sup>Pu, <sup>239</sup>Pu, <sup>240</sup>Pu, <sup>235</sup>U, <sup>238</sup>U, <sup>241</sup>Am, and <sup>244</sup>Cm). The radioactivity concentration must be measured separately for artificial (4.3–5.8 MeV) and natural radionuclides (<sup>212</sup>Bi, <sup>214</sup>Po, and <sup>212</sup>Po at 6.0, 7.7, and 8.8 MeV, respectively). Materials and Methods: We created response functions for various alpha-ray energies using a radiation simulation toolkit. Utilizing these response functions, we deconvolved the alpha-ray energy spectra measured while collecting dust on filter paper. To ensure the precision of the response function, we prepared a model including the distance between the filter and the detector and the structure of the light shield in detail. Results and Discussion: The deconvolved spectra had three clear peaks at 6.0, 7.7, and 8.8 MeV. These energies were consistent with those of <sup>212</sup>Bi, <sup>214</sup>Po, and <sup>212</sup>Po. The deconvolved energy spectra showed that only a few measurements (4.0–5.8 MeV) were included in the energy range due to artificial radionuclides. From these measurements, the decision threshold for artificial radionuclides was determined to be about 1.5×10<sup>−7</sup> Bq/cm<sup>3</sup>. Conclusion: Our findings demonstrated that we could measure artificial and natural radionuclides separately with the deconvolved alpha-ray energy spectra. Specifically, we were able to monitor artificial radionuclides down to low radioactivity concentrations in 10-minute measurements.

    DOI: 10.14407/jrpr.2023.00444

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  35. Crystal growth and evaluating luminescent properties of Eu-doped (Y, Lu, Sc)2O3 for optical thermometry Open Access

    Abe Y., Horiai T., Yokota Y., Yoshino M., Pejchal J., Kucerkova R., Murakami R., Hanada T., Yamaji A., Sato H., Ohashi Y., Kurosawa S., Kamada K., Nikl M., Yoshikawa A.

    Journal of Luminescence   Vol. 280   2025.5

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    Optical thermometry is one of the promising methods of detecting temperature under harsh environments. In this study, for the development of a novel optical thermometer, we focused on Eu-doped (Y, Lu, Sc)<inf>2</inf>O<inf>3</inf> and grew single crystals using the micro-pulling-down method. Crystal growth was performed by systematically changing the ratio of Y to Lu, and the crystalline system and space group were identified to be cubic and Ia–3, respectively, by the powder X-ray diffraction analysis. From the photoluminescence emission spectra, the emission peaks attributed to Eu<sup>3+</sup> <sup>5</sup>D<inf>0</inf>–<sup>7</sup>F<inf>1</inf> and <sup>5</sup>D<inf>1</inf>–<sup>7</sup>F<inf>1</inf> transitions were observed. The temperature dependence of these emission peaks was measured and evaluated using the fluorescence intensity ratio method to estimate the performance as the optical thermometer. It was found that Eu-doped (Y, Lu, Sc)<inf>2</inf>O<inf>3</inf> can be used as the optical thermometer in the temperature range from 430 K to 790 K. The relative sensitivity reached a maximum of 0.22 %K<sup>−1</sup> at 760 K.

    DOI: 10.1016/j.jlumin.2025.121118

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  36. Long-Term Survival After Allogeneic Hematopoietic Stem Cell Transplantation for BCR::ABL1-Negative Atypical Chronic Myeloid Leukemia: A Nationwide Retrospective Study by Adult CML/MPN and MDS Working Groups of the Japanese Society for Transplantation and Cellular Therapy Open Access

    Itonaga H., Miyazaki Y., Kondo T., Shimazu Y., Aoki J., Kurosawa S., Ikeda T., Eto T., Uchida N., Nakazawa H., Kawamura K., Kanda J., Atsuta Y., Tachibana T.

    American Journal of Hematology   Vol. 100 ( 5 ) page: 917 - 921   2025.5

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    DOI: 10.1002/ajh.27641

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  37. Limits on the Low-energy Electron Antineutrino Flux from the Brightest Gamma-Ray Burst of All Time Open Access

    Abe S., Araki T., Chauhan S., Chiba K., Eda T., Eizuka M., Funahashi Y., Furuto A., Gando A., Gando Y., Goto S., Hachiya T., Hata K., Ichimura K., Ikeda H., Inoue K., Ishidoshiro K., Kamei Y., Kawada N., Kishimoto Y., Koga M., Marthe A., Matsumoto Y., Mitsui T., Miyake H., Morita D., Nakajima R., Nakamura K., Nakamura R., Nakane J., Ono T., Ozaki H., Saito K., Sakai T., Shimizu I., Shirai J., Shiraishi K., Suzuki A., Tachibana K., Tamae K., Watanabe H., Watanabe K., Kurosawa S., Urano Y., Yoshida S., Umehara S., Fushimi K., Kotera K., Berger B.E., Fujikawa B.K., Learned J.G., Maricic J., Fu Z., Ghosh S., Smolsky J., Winslow L.A., Efremenko Y., Karwowski H.J., Markoff D.M., Tornow W., Dell’Oro S., O’Donnell T., Detwiler J.A., Enomoto S., Decowski M.P., Weerman K.M., Grant C., Penek , Song H., Li A., Axani S.N., Garcia M., Sarfraz M.

    Astrophysical Journal   Vol. 981 ( 2 )   2025.3

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    Publisher:Astrophysical Journal  

    The electron antineutrino flux limits are presented for the brightest gamma-ray burst (GRB) of all time, GRB221009A, over a range of 1.8-200 MeV using the Kamioka Liquid Scintillator Antineutrino Detector. Using multiple time windows ranging from minutes to days surrounding the event to search for electron antineutrinos coincident with the GRB, we set an upper limit on the flux under the assumption of several power-law neutrino source spectra, with power-law indices ranging from 1.5 to 3 in steps of 0.5. No excess was observed in any time windows ranging from seconds to days around the event trigger time T<inf>0</inf>. For a power-law index of 2 and a time window of T<inf>0</inf> ± 500 s, a flux upper limit of 2.34 × 10<sup>9</sup> cm<sup>−2</sup> was calculated. The limits are compared to the results presented by IceCube.

    DOI: 10.3847/1538-4357/ad9c36

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  38. Crystal growth and temperature dependence of luminescence characteristics of Pr3+ and Tb3+ doped solid-solution sesquioxide single crystals Open Access

    Abe Y., Horiai T., Yokota Y., Yoshino M., Murakami R., Hanada T., Yamaji A., Sato H., Ohashi Y., Kurosawa S., Kamada K., Yoshikawa A.

    Journal of Materials Chemistry C   Vol. 13 ( 16 ) page: 8032 - 8042   2025.3

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    Publisher:Journal of Materials Chemistry C  

    In recent decades, optical thermometry has gained significant attention due to its promising properties, such as non-contact measurement, temperature mapping and immunity to electromagnetic interference. It overcomes the limitations of conventional temperature measurement methods and offers additional benefits. However, the widespread adoption of optical thermometry requires an expanded operating temperature range and improved sensitivity. Therefore, in this study, we focused on solid-solution sesquioxides, which are expected not only to enable the growth of single crystals with a cubic structure but also to allow for a wider selection of luminescence centers. We evaluated the applicability of (Lu, Y, Sc)<inf>2</inf>O<inf>3</inf> single crystals doped with Pr<sup>3+</sup> and Tb<sup>3+</sup>, which exhibit different temperature dependent behaviors, for optical thermometry. The optical temperature sensing properties evaluated using the fluorescence lifetime method revealed a maximal relative sensitivity of 1.53% K<sup>−1</sup> in the temperature range of 78-790 K for Pr<sup>3+</sup>, Tb<sup>3+</sup>:(Lu, Y, Sc)<inf>2</inf>O<inf>3</inf>. These results suggest that (Lu, Y, Sc)<inf>2</inf>O<inf>3</inf> co-doped with Pr<sup>3+</sup> and Tb<sup>3+</sup> is a promising candidate for optical thermometry.

    DOI: 10.1039/d5tc00156k

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  39. Crystal Growth and Energy Transfer Study in Ce3+ and Pr3+ Co-Doped Lu2Si2O7 Open Access

    Abe Y., Horiai T., Yokota Y., Yoshino M., Murakami R., Hanada T., Yamaji A., Sato H., Ohashi Y., Kurosawa S., Kamada K., Yoshikawa A.

    Crystals   Vol. 15 ( 3 )   2025.3

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    Publisher:Crystals  

    Ce-doped Lu<inf>2</inf>Si<inf>2</inf>O<inf>7</inf> has a high density, high luminescence efficiency even at high temperatures, and a high effective atomic number, making it a promising candidate for use as a radiation detector in medical devices and resource exploration equipment. In this study, we grow and characterize Pr<sup>3+</sup> and Ce<sup>3+</sup>-doped Lu<inf>2</inf>Si<inf>2</inf>O<inf>7</inf> single crystals by systematically varying the Ce<sup>3+</sup> to Pr<sup>3+</sup> ratio to further improve scintillation properties. The optical characterization results show a bidirectional energy transfer: from the Pr<sup>3+</sup> 5d levels to the Ce<sup>3+</sup> 5d levels and from the Ce<sup>3+</sup> 5d levels to the Pr<sup>3+</sup> 4f levels. Consistently with this result, the PL decay time of emission from the Pr<sup>3+</sup> 5d–4f transition tends to become faster as the Ce<sup>3+</sup>/Pr<sup>3+</sup> ratio increases, due to the energy transfer from the Pr<sup>3+</sup> 5d levels to the Ce<sup>3+</sup> 5d levels. Additionally, (Ce<inf>0.0022</inf> Pr<inf>0.0016</inf> Lu<inf>0.9962</inf>)<inf>2</inf>Si<inf>2</inf>O<inf>7</inf> exhibits a high light yield comparable to Ce-doped Lu<inf>2</inf>Si<inf>2</inf>O<inf>7</inf> and a slightly faster decay time than Ce-doped Lu<inf>2</inf>Si<inf>2</inf>O<inf>7</inf>.

    DOI: 10.3390/cryst15030202

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  40. Development of a method for distinguishing alpha particles from other types of radiation using a high-resolution alpha imager

    Morishita Y., Sagawa N., Fujisawa M., Kurosawa S., Sasano M., Hayashi M., Tanaka H.

    Radiation Measurements   Vol. 181   2025.2

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    Publisher:Radiation Measurements  

    The effects of different types of radiation on a high-resolution alpha imager developed using an electron multiplying charge-coupled device (EMCCD) camera were investigated. This imager was originally developed to visualize alpha particles from Pu oxide particles at decommissioning sites. Other types of radiation such as beta particles, gamma rays, and neutrons are also present. The purpose of this study is to investigate the effects of these background radiations on the imager and to develop a method to discriminate between alpha particles and other types of radiation. When measuring gamma rays, and neutrons, the sensor of the EMCCD camera generated high intensity signals due to gamma rays and neutrons. These radiations were identified by image processing. The image values were binarized and the findContours function for detecting edges in an image was applied to count the number of alpha particle spots. The results showed that alpha and gamma (neutron) radiation can be discriminated by using differences in intensity. This method will be useful for visualizing alpha particles at decommissioning sites.

    DOI: 10.1016/j.radmeas.2024.107371

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  41. Outcome of donor lymphocyte infusion after allogeneic hematopoietic stem cell transplantation in relapsed myelodysplastic syndrome

    Marumo A., Nagata Y., Fujioka M., Kurosawa S., Najima Y., Sakaida E., Doki N., Fukushima K., Ota S., Shono K., Ito A., Uchida N., Nishida T., Sawa M., Tsunemine H., Matsuoka K.i., Makoto O., Kanda Y., Fukuda T., Atsuta Y., Itonaga H.

    Cytotherapy   Vol. 27 ( 2 ) page: 222 - 228   2025.2

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    Background aims: Allogeneic hematopoietic stem cell transplantation (HSCT) improves outcomes for myelodysplastic syndrome (MDS) patients, but relapse rates remain high, and postrelapse treatment options are limited. Therefore, this study aimed to identify the factors contributing to the response to donor lymphocyte infusion (DLI) in relapsed MDS patients post-HSCT. Methods: This study included 107 patients with relapsed and DLI-treated MDS who underwent their first HSCT between 2002 and 2022 and were registered in the Transplant Registry Unified Program. Univariate and multivariate survival analyses were conducted using log-rank tests and Cox proportional hazards models. Overall survival (OS) and response rates to DLI were also analyzed. Results: The 1-year OS was 30.0% and univariate analysis identified poor prognostic factors: age ≥58 years (P = 0.003), complex karyotype (P = 0.026), hematologic relapse (P = 0.026) and early relapse (P = 0.004). Azacitidine plus DLI also improved prognosis (P < 0.001). Multivariate analysis confirmed age ≥58 years, hematologic relapse, and early relapse as poor prognostic factors. The adjusted OS for patients aged ≥58 years who relapsed <110 days post-transplant showed that the 1-year OS in patients with cytogenetic/molecular relapse was 43.6%, compared to 9.4% for those with hematologic relapse. Acute graft-versus-host disease (GVHD) occurred in 62.3% of patients, and chronic GVHD in 30.8%, with manageable outcomes. Conclusions: DLI may improve OS in younger patients, those with cytogenetic/molecular relapse, and those with late relapse. Despite the risk of GVHD, its impact on prognosis is minimal. Given the limited treatment options, DLI should be considered for relapsed MDS patients post-HSCT.

    DOI: 10.1016/j.jcyt.2024.09.006

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  42. Enfortumab Vedotin-Induced Diabetic Ketoacidosis and Acute Tubulointerstitial Nephritis Requiring Intensive Care in the Treatment of Advanced Urothelial Carcinoma: A Case Report Open Access

    Matsui R., Kawasaki Y., Satake Y., Takahashi K., Kurosawa S., Sato T., Katayama H., Sato T., Kawamorita N., Yamashita S., Katagiri H., Ito A.

    Case Reports in Oncology   Vol. 18 ( 1 ) page: 675 - 682   2025.1

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    Abstract – Introduction: Enfortumab vedotin (EV) has been approved for the treatment of many types of cancer, and its use is still expanding. It is an essential drug used as a standard treatment for advanced and metastatic urothelial carcinoma but is known to cause various adverse events (AEs). Case Presentation: We report a patient with metastatic urothelial carcinoma who experienced multiple AEs associated with diabetic ketoacidosis (DKA) during EV treatment. The onset of DKA during EV treatment has been reported to be associated with poor prognosis. Although strict management was required in the intensive care unit, we were able to save the patient’s life. Conclusion: Although the detailed mechanism that induced insulin resistance remains unclear, the patient required high-dose insulin because of a marked increase in insulin resistance. If hyperglycemia is observed during EV therapy, DKA may lead to the occurrence of serious AEs. We report on the pathogenesis and management of drug-induced DKA caused by EV based on our case and a literature review.

    DOI: 10.1159/000545957

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  43. Feasibility and usefulness of symptom monitoring with electronic patient-reported outcomes: an experience at single-center outpatient oncology clinic

    Kurosawa S., Koike K., Arai T., Yoshida S., Ito M., Kuriyama Y., Kitahara M., Rokuhara T., Yamaguchi T., Takeuchi N.

    Supportive Care in Cancer   Vol. 33 ( 1 ) page: 3   2025.1

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    Purpose: The benefit of patient-reported outcomes (PRO) in routine oncology practice is increasingly recognized. This study aimed to develop a team-based monitoring and intervention system using electronic PRO (ePRO) and to evaluate its impact at an outpatient oncology clinic. Methods: Patients receiving chemotherapy at our department were eligible for this study. Those who had access to a smartphone or tablet (Bring Your Own Device [BYOD]) and consented participated, and reported 28 symptoms weekly via 3H P-guardian downloaded on their BYOD. E-mail alerts were sent to attending healthcare providers when participants reported at least grade 3 severity for any of nine symptoms (decreased appetite, nausea, vomiting, diarrhea, shortness of breath, pain, insomnia, fatigue, and sadness), which prompted interventions. Comparisons of overall survival (OS), emergency room visits, and hospitalizations were conducted using propensity scores. Results: Among 203 patients who received chemotherapy from September 2021 to August 2023, 77 participated in ePRO monitoring. The overall response rate was 55% (1991 valid responses out of a total of 3597 expected time points), and the median individual response rate was 66% (range, 0–100%). Of 1991 valid responses, 250 (13%) prompted alerts, and most interventions were initiated by making telephone calls. OS and other clinical outcomes were better in ePRO participants compared with non-participants, but these outcomes did not differ significantly between the ePRO and pre-ePRO eras. Conclusions: It was feasible to develop a multi-professional team-based monitoring and intervention system using ePRO at a single-center outpatient oncology clinic. Our results indicate that weekly monitoring of ePRO, along with corresponding interventions, may benefit patients receiving chemotherapy.

    DOI: 10.1007/s00520-024-09062-5

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  44. Temperature dependence of photoluminescence kinetics, scintillation properties, and coincidence time resolution of Mo co-doped Y1.5Gd1.5Al2Ga3O12:Ce (Mo = 0, 300, 600 ppm) multicomponent garnet crystals

    Chewpraditkul W., Sakthong O., Chewpraditkul W., Yoshino M., Horiai T., Kurosawa S., Kucerkova R., Beitlerova A., Szczesniak T., Grodzicka-Kobyłka M., Nikl M., Yoshikawa A.

    Optical Materials   Vol. 158   2025.1

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    Luminescence and scintillation properties of Mo co-doped Y<inf>1.5</inf>Gd<inf>1.5</inf>Al<inf>2</inf>Ga<inf>3</inf>O<inf>12</inf>:Ce,Mo (Mo = 0, 300, 600 ppm) multicomponent garnet crystals grown by the micro-pulling-down method were investigated. To investigate temperature stability, temperature dependence of photoluminescence decay time was measured from 77 to 487 K and thermal activation energy was determined. Y<inf>1.5</inf>Gd<inf>1.5</inf>Al<inf>2</inf>Ga<inf>3</inf>O<inf>12</inf>:Ce,Mo (300, 600 ppm) samples showed faster scintillation decay time with a similar LY value compared to Mo-free Y<inf>1.5</inf>Gd<inf>1.5</inf>Al<inf>2</inf>Ga<inf>3</inf>O<inf>12</inf>:Ce one. Y<inf>1.5</inf>Gd<inf>1.5</inf>Al<inf>2</inf>Ga<inf>3</inf>O<inf>12</inf>:Ce,Mo (600 ppm) showed a light yield value of 34,300 photons/MeV along with fast scintillation decay times of 45.2 ns (55 %) +153 ns (45 %) and time resolution of 313 ps. Radioluminescence and afterglow signal were also measured at RT and discussed.

    DOI: 10.1016/j.optmat.2024.116494

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  45. Feasibility study of reactor radiation photon spectroscopy in Fugen for nuclear decommissioning Open Access

    Kaburagi M., Miyamoto Y., Mori N., Iwai H., Tezuka M., Kurosawa S., Tagawa A., Takasaki K.

    Journal of Nuclear Science and Technology   Vol. 62 ( 3 ) page: 308 - 316   2025

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    Nuclear decommissioning is crucial as nuclear facilities become old. This trend has recently accelerated, particularly following the accident at Fukushima Daiichi Nuclear Power Station, Tokyo Electric Power Holdings. New nuclear decommissioning technologies are required to improve safety, save time, and reduce costs. An example is γ-ray/X-ray (radiation photon) spectroscopy, which provides information on the types of radionuclides with radiation photon emissions. A feasibility study of radiation photon spectroscopy in conjunction with reactor dosimetry in a control rod guide tube positioned at the center of Fugen (a prototype advanced thermal reactor under decommissioning) was conducted. Fugen is a prototype advanced thermal reactor with 165 MWe electric power generation that is being decommissioned. The dose rates measured in a control rod guide tube positioned at the center of the reactor of FUGEN were 4.1–9.1 Gy/h. The dose rate considerably increased at a position close to a tank that contained <sup>60</sup>Co caused by the radioactivation of stainless steel. Radiation photon spectroscopy was performed without radiation shielding, identifying <sup>60</sup>Co with an energy resolution better than 5.4% at 1333 keV and <sup>94</sup>Nb with an energy resolution better than 5.9% at 871 keV.

    DOI: 10.1080/00223131.2024.2417786

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  46. Research on estimating snow distribution using AI technology

    Kurosawa S., Kazama S.

    Proceedings of the IAHR World Congress     page: 672 - 675   2025

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    Publisher:Proceedings of the IAHR World Congress  

    In recent years, more accurate flood forecasting information has been needed to contribute to flood prevention activities and damage minimization in the event of flood disasters that exceed the planned scale. However, many of the flood forecasting systems used in Japan are designed to target summer floods caused by rainfall and cannot be applied to snowmelt floods in early spring. For this reason, research is being conducted to enable year-round flood forecasting, including snowmelt floods. In this paper, we apply AI technology to snow distribution estimation to ensure the accuracy of snowmelt flood forecasting and demonstrate its practicality through verification results.

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  47. Recent Study on Red and Infrared Scintillation Crystals Open Access

    Kurosawa Shunsuke

    Journal of the Japanese Association for Crystal Growth   Vol. 52 ( 2 ) page: n/a   2025

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    Language:Japanese   Publisher:The Japanese Association for Crystal Growth  

    <p>  Real dose monitors under the high dose-rate condition are required to remove the debris in the Fukushima Daiichi Nuclear Power Plant as the decommissioning step, and I have proposed a dose-rate monitor consisting of a scintillator, optical fiber and photo detector. To realize such monitor, scintillation materials are required to have the long-emission-wavelength (550 - 1000 nm) and high light output. From this reason, several novel materials such as Cs<sub>2</sub>HfI<sub>6</sub> and Rb<sub>2</sub>HfI<sub>6</sub> for gamma-ray detection have been developed, and Li<sub>2</sub>HfBr<sub>6</sub> had sensitive to both gamma ray and neutrons. These scintillators had an emission wavelengths of 600 to 750 nm, and I review the detail of such red and infrared emitting scintillator.</p>

    DOI: 10.19009/jjacg.52-2-03

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  48. Tailoring scintillation and luminescence through Co-doping engineering: A comparative study of Ce,Tb Co-doped YAGG and GAGG garnet crystals Open Access

    Omuro K., Yoshino M., Bartosiewicz K., Horiai T., Murakami R., Kim K.J., Kamada K., Kucerkova R., Babin V., Nikl M., Yamaji A., Hanada T., Yokota Y., Kurosawa S., Ohashi Y., Sato H., Yoshikawa A.

    Journal of Alloys and Compounds   Vol. 1008   2024.12

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    The development of scintillators with co-doping mechanisms has received significant attention due to the resulting enhancements in luminescence and scintillation properties. Scintillators such as Ce-doped (Gd,Tb)<inf>3</inf>(Al,Ga)<inf>5</inf>O<inf>12</inf> have been recognized for their improved performance, attributed to the effective energy transfer between Ce<sup>3+</sup> and Tb<sup>3+</sup> ions. Nevertheless, the presence of Gd<sup>3+</sup> introduced complexities, as its absorption lines strongly overlap with those of Tb<sup>3+</sup>, thus masking the details of mechanisms of the Tb<sup>3+</sup>↔Ce<sup>3+</sup> energy transfer. This study endeavored to elucidate this mechanism by comparing the luminescence characteristics of Ce,Tb co-doped Y<inf>3</inf>Al<inf>2</inf>Ga<inf>3</inf>O<inf>12</inf> (YAGG) and Gd<inf>3</inf>A<inf>2</inf>Ga<inf>3</inf>O<inf>12</inf> (GAGG) single crystals. Through detailed photoluminescence spectral analysis, it was discerned that GAGG exhibited a more robust Tb<sup>3+</sup>↔Ce<sup>3+</sup> energy transfer, as evidenced by a marked extension in the decay time of Ce<sup>3+</sup> luminescence. Furthermore, GAGG demonstrated superior integrated radioluminescence intensity across all compositions which is a result of efficient energy transfer from Gd<sup>3+</sup> to the luminescence centers. Additionally, comparative thermally stimulated luminescence glow curves, revealed distinctive spectral features between YAGG and GAGG, underscoring the complexity of their luminescence mechanisms. This comparative study not only augmented our comprehension of the intricate energy transfer processes in Ce, Tb co-doped garnet scintillators but also underscored the potential for tailored scintillator development through strategic ion co-doping.

    DOI: 10.1016/j.jallcom.2024.176550

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  49. Temperature dependence of photo- and radio-luminescence, scintillation and photoconversion properties of Lu0.6Gd2.4(Al5-xScx)O12:Ce garnet crystals grown by micro-pulling-down method

    Chewpraditkul W., Sakthong O., Horiai T., Kurosawa S., Witkowski M.E., Makowski M., Bartosiewicz K., Tomala R., Szymański D., Drozdowski W., Chewpraditkul W., Yoshikawa A.

    Journal of Alloys and Compounds   Vol. 1008   2024.12

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    The luminescence, scintillation and photoconversion properties of Ce<sup>3+</sup>-doped Lu<inf>0.6</inf>Gd<inf>2.4</inf>(Al<inf>5-x</inf>Sc<inf>x</inf>)O<inf>12</inf> (x = 1.2, 1.5, 2) garnet crystals grown by micro-pulling-down method were investigated. Increasing Sc<sup>3+</sup> concentration induced lattice strain and cracking due to ionic radius mismatch. At low Sc<sup>3+</sup> concentration, the strain caused core-concentrated cracks and radial inhomogeneity. At higher Sc<sup>3+</sup> concentration, extensive cracking occurred throughout crystals, improving radial homogeneity. With the increase of Sc<sup>3+</sup> concentration, the Ce<sup>3+</sup> 5d<inf>1</inf> → 4f luminescence was slightly blue-shifted due to the decrease in crystal field splitting of the 5d levels. At room temperature (RT), the increase of light yield with increasing Sc<sup>3+</sup> concentration was attributed to the decrease in the bandgap value. Above RT, the decrease of photo- and radio-luminescence for all samples was due to the thermal ionization process. The decrease of radioluminescence at low-temperature regions can be caused by the localization of electrons at intrinsic shallow traps. Photoluminescence measurements disclosed that variations in scandium concentration can effectively modulate the correlated color temperature (CCT), color rendering index (CRI), and luminous efficiency (LE) of these luminescent materials. The incorporation of a micro-perovskite phase in the Lu<inf>0.6</inf>Gd<inf>2.4</inf>(Al<inf>3.8</inf>Sc<inf>1.2</inf>)O<inf>12</inf>:Ce crystal resulted in a notable enhancement of the luminous efficiency, exhibiting a 38 % increase when compared to the sample devoid of micro-inclusions (e.g. x = 2.0).

    DOI: 10.1016/j.jallcom.2024.176586

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  50. Center effect on allogeneic hematopoietic stem cell transplantation outcomes for B-cell acute lymphoblastic leukemia

    Kurosawa S., Fukuda T., Ichinohe T., Hashii Y., Kanda J., Goto H., Kato K., Yoshimitsu M., Ishimaru F., Sato A., Onizuka M., Matsuo K., Ito Y., Yanagisawa A., Ohbiki M., Tabuch K., Atsuta Y., Arai Y.

    Cytotherapy   Vol. 26 ( 10 ) page: 1185 - 1192   2024.10

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    This nationwide study retrospectively examined the center effect on allogeneic hematopoietic stem cell transplantation (allo-HSCT) for adult B-cell acute lymphoblastic leukemia. The cohort analyses were separated into Philadelphia chromosome (Ph)-positive and -negative cases. The patients were divided into low- and high-volume groups according to the number of allo-HSCTs at each facility. The primary endpoint was 5-year overall survival (OS). This study included 1156 low-volume and 1329 high-volume Ph-negative and 855 low-volume and 926 high-volume Ph-positive cases. In Ph-negative cases, 5-year OS was significantly higher in the high-volume centers at 52.7% (95% confidence interval [CI]: 49.9–55.5) versus 46.8% (95% CI: 43.8–49.7) for the low-volume centers (P < 0.01). Multivariate analysis identified high volume as a favorable prognostic factor (hazard ratio [HR]: 0.81 [95% CI: 0.72–0.92], P < 0.01). Subgroup analysis in Ph-negative cases revealed that the center effects were more evident in patients aged ≥40 years (HR: 0.72, 95% CI: 0.61–0.86, P < 0.01) and those receiving cord blood transplantation (HR: 0.62, 95% CI: 0.48–0.79, P < 0.01). In Ph-positive cases, no significant difference was observed between the high and low-volume centers for 5-year OS (59.5% [95% CI: 56.2–62.7] vs. 54.9% [95% CI: 51.3–58.3], P = 0.054). In multivariate analysis, center volume did not emerge as a significant prognostic indicator. This study showed center effects on survival in Ph-negative but not in Ph-positive cases, highlighting the heterogeneity of the center effect in allo-HSCT for B-cell acute lymphoblastic leukemia. Collaborative efforts among transplant centers and further validation are essential to improve outcomes.

    DOI: 10.1016/j.jcyt.2024.05.004

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  51. Results of the SMILE-2+ balloon experiment

    Ikeda T., Takada A., Abe M., Kobayashi K., Tahara K., Yoshikawa K., Ogio S., Tsuda M., Yoshida Y., Mizumura Y., Nakamori T., Kurosawa S., Sawano T., Hamaguchi K., Mori M., Kushida J., Tanimori T.

    Proceedings of Science   Vol. 444   2024.9

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    The cosmic MeV gamma-ray observation is a promising diagnostic tool to address the universe. While INTEGRAL and COMPTEL unveiled the MeV gamma-ray sky, the outstanding issue, like the origin of the gamma-ray and positron excesses toward the galactic inner region, remained. Furthermore, the conventional nonlinear imaging with the superposition of the Compton circles and the coded mask aperture system cannot discriminate the background from the signal. To overcome such difficulties, we developed an Electron-Tracking Compton Camera (ETCC), which has a linear imaging system. The balloon experiment on April 2018 in Australia, the so-called SMILE-2+, was carried out, and we observed the galactic diffuse gamma-rays with a significance of 4.3σ in the energy range of 150–600 keV. The gamma-ray flux was consistent with the point-source emission and the annihilation radiation from the positronium observed from INTEGRAL/SPI.

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  52. Insights into luminescence and energy transfer processes in Ce3+- and Tb3+ co-doped (Gd, Y)3Al2Ga3O12 garnet single crystals

    Omuro K., Yoshino M., Bartosiewicz K., Horiai T., Murakami R., Kim K.J., Kamada K., Kucerkova R., Babin V., Nikl M., Yamaji A., Hanada T., Yokota Y., Kurosawa S., Ohashi Y., Sato H., Yoshikawa A.

    Journal of Luminescence   Vol. 273   2024.9

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    Publisher:Journal of Luminescence  

    Driven by the pursuit of optimizing the luminescent properties of garnet-based single crystals for X-ray imaging applications, this work reports on the successful synthesis and in-depth characterization of GYAGG crystals doped with Ce³⁺ or Tb³⁺ ions, and doubly-doped with both of them. Micro-pulling down synthesis yielded crystals with a single cubic phase confirmed by X-ray diffraction. Photoluminescence (PL) and radioluminescence (RL) measurements on Ce³⁺,Tb³⁺ co-doped GYAGG revealed bidirectional energy transfer processes. Characteristic broadband 5d<inf>1</inf>→4f emission of Ce³⁺ centers peaking at 530 nm and narrow 4f→4f emission lines of Tb³⁺ ions starting from <sup>5</sup>D<inf>4</inf> level within 480–630 nm were observed. At higher doping levels, cross-relaxation in Tb³⁺ pairs resulted depleted <sup>5</sup>D<inf>3</inf> state and only the emission from <sup>5</sup>D<inf>4</inf> one was observed in the spectra. Analysis of PL decay characteristics corroborated the spectral observations, confirming progressively decreasing Ce³⁺ decay time (down to 40 ns at 15 % Tb<sup>3+</sup>) due to enhanced Ce³⁺→Tb³⁺ energy transfer. Similarly, the Tb³⁺ decay time accelerated by more than 60 % after the Ce³⁺ co-doping. Notably, co-doping with 0.5 % Ce³⁺ and 10–15 % Tb³⁺ doubled the luminescence intensity of RL spectra compared to 0.5 % Ce³⁺-doping alone, attributed to the increased density of emitting centers.

    DOI: 10.1016/j.jlumin.2024.120663

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  53. Flux growth and evaluation of optical properties of Ce doped Li<sub>2</sub>CaSiO<sub>4</sub> as a candidate for noble neutron scintillator Open Access

    Kodama Shohei, Nishii Taiga, Urano Yusuke, Kurosawa Shunsuke, Yanase Ikuo, Takeda Hiroaki, Sodeno Miki

    Journal of the Ceramic Society of Japan   Vol. 132 ( 7 ) page: 369 - 374   2024.7

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    <p>This study focuses on the growth of transparent single crystals of Li<sub>2</sub>CaSiO<sub>4</sub> (LCS) doped with Ce as neutron scintillator candidates. LCS is a light material with a high melting point and chemical stability; thus, LCS is applicable for use in high-flux neutron environments. However, the growth of transparent single crystals from the melt has been difficult owing to the phase transitions. In this study, the LiF/LiCl eutectic was used as a flux with a lower melting point and less decomposition than LiCl, and Ce was selected as the luminescent center. The phase diagram of the LiF/LiCl-LCS system was determined, and the conditions for crystal growth were optimized, consequently, transparent non-doped LCS and Ce:LCS crystals were successfully obtained. The alpha-ray-excited scintillation spectrum and scintillation decay time of Ce:LCS were measured in a feasibility study for neutron detection. The results showed that Ce:LCS has potential as a neutron scintillator, with a significantly fast decay time of 28.46 ns.</p>

    DOI: 10.2109/jcersj2.23214

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    CiNii Research

  54. Highly efficient In(I) doped Cs3Cu2I5 single crystals for light-emitting diodes and gamma spectroscopy applications Open Access

    Wen X., Gao Q., Wang Q., Chewpraditkul W., Korjik M., Kurosawa S., Buryi M., Babin V., Wu Y.

    Optical Materials X   Vol. 23   2024.7

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    Publisher:Optical Materials X  

    High-quality Cs<inf>3</inf>Cu<inf>2</inf>I<inf>5</inf>:In single crystals with a 7 mm diameter were grown by using the vertical Bridgman method. These crystals have a high optical transmittance (>75 %) and emit a bright red-orange light under both UV and X-ray irradiation. The Cs<inf>3</inf>Cu<inf>2</inf>I<inf>5</inf>:In crystals can exhibit a high photoluminescence quantum efficiency (PLQY) of 79.5 %, thus we explored the potential applications for light-emitting diodes (LED). The fabricated LED demonstrated CIE color coordinates of (0.553, 0.431) with a color rendering index (Ra) of 77, making it suitable for supplementary light in plant growth. Moreover, we evaluated their gamma-ray spectroscopy capability by using an avalanche photodiode (APD) detector. Under <sup>137</sup>Cs gamma-ray irradiation, the gamma scintillation yield and energy resolution gradually degraded as the In concentration increased, which can be attributed to an enhanced afterglow after In doping.

    DOI: 10.1016/j.omx.2024.100335

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  55. Effects of rare earth codoping on the optical and scintillation properties of Cs3Cu2I5:Tl single crystals

    Gao Q., Wang Q., Li W., Gao A., Korzhik M., Kurosawa S., Ren G., Wu Y.

    Journal of Crystal Growth   Vol. 636   2024.6

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    Publisher:Journal of Crystal Growth  

    In this work, the effects of rare earth ion codoping on the optical and scintillation performance of Cs<inf>3</inf>Cu<inf>2</inf>I<inf>5</inf>:Tl single crystals were studied. Cs<inf>3</inf>Cu<inf>2</inf>I<inf>5</inf>:Tl single crystals codoped with different concentrations of Sc<sup>3+</sup>, Y<sup>3+</sup>, and La<sup>3+</sup> ions were grown by the Bridgman method. It was found that rare earth ion codoping reduces the optical transmittance of the as-grown crystals, in particular the coloring caused by Sc<sup>3+</sup>codoping. The luminescence mechanism associated with self-trapped exciton (STE) and Tl-related emissions has not been affected by the introduction of rare earth ion. The gamma scintillation yield and energy resolution are degraded after rare earth ion codoping.

    DOI: 10.1016/j.jcrysgro.2024.127717

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  56. High-energy extension of the gamma-ray band observable with an electron-tracking Compton camera Open Access

    Oka T., Ogio S., Abe M., Hamaguchi K., Ikeda T., Kubo H., Kurosawa S., Miuchi K., Mizumura Y., Nakamura Y., Sawano T., Takada A., Takemura T., Tanimori T., Yoshikawa K.

    Nuclear Instruments and Methods in Physics Research Section A Accelerators Spectrometers Detectors and Associated Equipment   Vol. 1063   2024.6

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    Although the MeV gamma-ray band is a promising energy-band window in astrophysics, the current situation of MeV gamma-ray astronomy significantly lags behind those of the other energy bands in angular resolution and sensitivity. An electron-tracking Compton camera (ETCC), a next-generation MeV detector, is expected to revolutionize the situation. An ETCC tracks each Compton-recoil electron with a gaseous electron tracker and determines the incoming direction of each gamma-ray photon; thus, it has a strong background rejection power and yields a better angular resolution than classical Compton cameras. Here, we study ETCC events in which the Compton-recoil electrons do not deposit all energies to the electron tracker but escape and hit the surrounding pixel scintillator array (PSA). The PSA provides additional information on the electron-recoil direction, which enables us to improve significantly the angular resolution. We developed an analysis method for this untapped class of events and applied it to laboratory and simulation data. We found that the energy spectrum obtained from the simulation agreed with that of the actual data within a factor of 1.2. We then evaluated the detector performance using the simulation data. The angular resolution for the new-class events was found to be twice as good as in the previous study at the energy range 1.0–2.0 MeV, where both analyses overlap. We also found that the total effective area is dominated by the contribution of the double-hit events above an energy of 1.5 MeV. Notably, applying this new method extends the sensitive energy range with the ETCC from 0.2–2.1 MeV in the previous studies to up to 3.5 MeV. Adjusting the PSA dynamic range should improve the sensitivity in even higher energy gamma-rays. The development of this new analysis method would pave the way for future observations by ETCC to fill the MeV-band sensitivity gap in astronomy.

    DOI: 10.1016/j.nima.2024.169242

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  57. Micro-Inclusion Engineering via Sc Incompatibility for Luminescence and Photoconversion Control in Ce3+-Doped Tb3Al5−xScxO12 Garnet Open Access

    Bartosiewicz K., Tomala R., Szymański D., Albini B., Zeler J., Yoshino M., Horiai T., Socha P., Kurosawa S., Kamada K., Galinetto P., Zych E., Yoshikawa A.

    Materials   Vol. 17 ( 11 )   2024.6

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    Aluminum garnets display exceptional adaptability in incorporating mismatching elements, thereby facilitating the synthesis of novel materials with tailored properties. This study explored Ce<sup>3+</sup>-doped Tb<inf>3</inf>Al<inf>5−x</inf>Sc<inf>x</inf>O<inf>12</inf> crystals (where x ranges from 0.5 to 3.0), revealing a novel approach to control luminescence and photoconversion through atomic size mismatch engineering. Raman spectroscopy confirmed the coexistence of garnet and perovskite phases, with Sc substitution significantly influencing the garnet lattice and induced A<inf>1g</inf> mode softening up to Sc concentration x = 2.0. The Sc atoms controlled sub-eutectic inclusion formation, creating efficient light scattering centers and unveiling a compositional threshold for octahedral site saturation. This modulation enabled the control of energy transfer dynamics between Ce<sup>3+</sup> and Tb<sup>3+</sup> ions, enhancing luminescence and mitigating quenching. The Sc admixing process regulated luminous efficacy (LE), color rendering index (CRI), and correlated color temperature (CCT), with adjustments in CRI from 68 to 84 and CCT from 3545 K to 12,958 K. The Ce<sup>3+</sup>-doped Tb<inf>3</inf>Al<inf>5−x</inf>Sc<inf>x</inf>O<inf>12</inf> crystal (where x = 2.0) achieved the highest LE of 114.6 lm/W and emitted light at a CCT of 4942 K, similar to daylight white. This approach enables the design and development of functional materials with tailored optical properties applicable to lighting technology, persistent phosphors, scintillators, and storage phosphors.

    DOI: 10.3390/ma17112762

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    PubMed

  58. Updated comparable efficacy of cord blood transplantation for chronic myelomonocytic leukaemia: a nationwide study

    Kurosawa S., Shimomura Y., Ishiyama K., Fuse K., Shimazu Y., Doki N., Uchida N., Tanaka M., Takahashi S., Sakurai M., Kobayashi H., Katayama Y., Takada S., Ozeki K., Nakamae H., Ishimaru F., Kanda Y., Ichinohe T., Atsuta Y., Itonaga H.

    Bone Marrow Transplantation   Vol. 59 ( 6 ) page: 742 - 750   2024.6

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    Chronic myelomonocytic leukaemia (CMML) is a haematological malignancy with a poor prognosis. Allogeneic haematopoietic stem cell transplantation remains the only curative approach. Without human leucocyte antigen-matched related sibling donors, the optimal alternative donor has yet to be established. Although unrelated bone marrow transplantation (UBMT) has been extensively studied, cord blood transplantation (CBT) for CMML remains largely unexplored. This nationwide retrospective study compared the outcomes of UBMT and single-unit umbilical CBT in patients with CMML. This study included 118 patients who underwent their first allo-HSCT during 2013–2021. Of these, 50 received BMT (UBMT group), while 68 underwent CBT (CBT group). The primary endpoint was the 3-year overall survival (OS). There were comparable 3-year OS rates between the UBMT (51.0%, 95% confidence interval [CI]: 34.1–65.5%) and CBT (46.2%, 95% CI: 33.2–58.1%; P = 0.60) groups. In the inverse probability of treatment weighting analysis, CBT did not show significantly improved outcomes compared with UBMT regarding the 3-year OS rate (hazard ratio 0.97 [95% CI: 0.57–1.66], P = 0.91). Thus, CBT may serve as an alternative to UBMT for patients with CMML. Further research is necessary to optimise transplantation strategies and enhance outcomes in patients with CMML undergoing CBT.

    DOI: 10.1038/s41409-024-02223-4

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  59. Engineering atomic size mismatch in Pr3+, La3+ codoped Lu3Al5O12 garnet single crystals for tailored structure and functional properties

    Bartosiewicz K., Albini B., Szymański D., Socha P., Horiai T., Yoshino M., Yamaji A., Kurosawa S., Kucerkova R., Galinetto P., Yoshikawa A.

    Journal of Alloys and Compounds   Vol. 985   2024.5

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    This study provided the first in-depth investigation of the effects of large dopant incompatibility (Pr<sup>3+</sup> and La<sup>3+</sup> ions) on the small host lattice element (Lu<sup>3+</sup>) in Lu<inf>3</inf>Al<inf>5</inf>O<inf>12</inf> (LuAG) single crystal. The growth of such complex crystals from the melt presented many challenges. By engineering the ionic radius ratio of RE- and M-site cations, a single-crystal phase stabilized by configurational entropy was achieved. This investigation elucidated the crystallization behavior of configurationally disordered rare-earth aluminum garnet oxide (Lu<inf>1−x−y</inf>Pr<inf>x</inf>La<inf>y</inf>)<inf>3</inf>Al<inf>5</inf>O<inf>12</inf> from the melt and characterized its functional properties, including microstructural, optical, photoluminescence, and scintillation properties, between 5 and 300 K. Relaxation of the imposed strain energy led to local perturbations and destabilization of the garnet structure. Multielemental EDS mapping, micro-Raman spectroscopy, and thermoluminescence revealed the mechanism by which atomic size mismatch drove a smooth transition from the garnet to the perovskite phase in high entropy garnets. The optical, photoluminescence, and scintillation measurements provided fundamental insights into property changes driven by incompatibility doping. Standard and modified Judd-Ofelt theory analysis of absorption spectra determined the phenomenological Judd-Ofelt parameters Ω<inf>λ</inf> and radiative lifetimes. Atomic size mismatch engineering offers a promising approach to overcoming the limitations of conventional eutectic synthesis methods.

    DOI: 10.1016/j.jallcom.2024.174078

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  60. Advances in Ce3+ doped Y1±xAlO3 (x≠0) single crystal perovskite scintillators through nonstoichiometric engineering Open Access

    Bartosiewicz K., Pejchal J., Kucerkova R., Beitlerova A., Babin V., Vanecek V., Kurosawa S., Kamada K., Yoshikawa A.

    Optical Materials X   Vol. 22   2024.5

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    Publisher:Optical Materials X  

    The influence of nonstoichiometric engineering on the scintillation properties of Ce<sup>3+</sup> doped yttrium aluminum perovskite (YAP:Ce) crystals was investigated. Crystals with slight yttrium excess (Y<inf>1</inf> <inf>·</inf> <inf>004</inf>AlO<inf>3</inf>:Ce), yttrium deficiency (Y<inf>0</inf> <inf>·</inf> <inf>994</inf>AlO<inf>3</inf>:Ce), and stoichiometric composition (YAlO<inf>3</inf>:Ce) were synthesized using the micro-pulling down method. Structural characterization confirmed crystallization in the pure orthorhombic Pnma space group for all compositions. Optical absorption spectroscopy revealed an extensive background in the nonstoichiometric crystals due to the increased degree of light scattering centers associated with the defects. The photoluminescence excitation and emission spectra of Ce<sup>3+</sup> ions were unaffected by nonstoichiometry. However, the scintillation decay kinetics and light yield exhibited marked improvements in the Y<inf>1±x</inf>AlO<inf>3</inf>:Ce (x≠0) crystals. The light yield increased by 22 % and 15 % and the slower component of the decay accelerated from 171 ns to 106 and 131 ns compared to the stoichiometric crystal. Thermoluminescence glow curves revealed that nonstoichiometry significantly altered the concentrations of antisite defects and oxygen vacancies. The EPR spectroscopy investigations revealed a correlation between the Ce<sup>3+</sup> ions concentration and the degree of nonstoichiometry. Strategic engineering of nonstoichiometry in Y<inf>1±x</inf>AlO<inf>3</inf>:Ce (x≠0) scintillators may have provided an effective approach to optimizing scintillation performance.

    DOI: 10.1016/j.omx.2024.100295

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  61. Comparison of Melphalan Dose in Patients with Myelodysplastic Syndrome Undergoing Allogeneic Transplantation with Reduced-Intensity Conditioning

    Kurosawa S., Shimomura Y., Itonaga H., Katayama Y., Onizuka M., Tanaka M., Kobayashi H., Ozawa Y., Sawa M., Kanda J., Doki N., Fujisawa S., Uchida N., Fukuda T., Atsuta Y., Ishiyama K.

    Transplantation and Cellular Therapy   Vol. 30 ( 5 ) page: 510 - 510.e10   2024.5

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    The present study compared lower-dose melphalan (80 mg/m<sup>2</sup>, FM80) and higher-dose melphalan (140 mg/m<sup>2</sup>, FM140) when administering reduced-intensity conditioning with fludarabine in adult patients with myelodysplastic syndrome (MDS) undergoing allogeneic hematopoietic stem cell transplantation (allo-HSCT). We retrospectively analyzed nationwide registry data (2006 to 2019) and compared transplant outcomes between the 2 groups. Ninety-two patients (median age, 61 [interquartile range, 56 to 65] years) were assigned to the FM80 and FM140 groups by propensity score matching. The 3-year overall survival (OS) rate in the FM140 group (63.9%; 95% confidence interval [CI], 52.9% to 73.0%) was significantly higher than that in the FM80 group (54.2%; 95% CI, 37.1% to 52.1%) (P = .038). The FM140 group had a nonsignificantly (P = .095) lower 3-year cumulative incidence of relapse (15.5%; 95% CI, 8.9% to 23.8% versus 26.0%; 95% CI, 17.3% to 35.5%). The 3-year cumulative incidences of nonrelapse mortality were 22.3% (95% CI, 14.1% to 31.8%) and 23.7% (95% CI, 15.4% to 33.2%) in the FM80 and FM140 groups, respectively (P = .49). The beneficial effect of FM140 was more evident in patients with a poor cytogenetic risk. Our findings suggest the superiority of FM140 in patients with MDS undergoing allo-HSCT, especially in high-risk patients.

    DOI: 10.1016/j.jtct.2024.01.083

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    PubMed

  62. Large spontaneous magneto-thermoelectric effect in epitaxial thin films of the topological kagome ferromagnet Fe3Sn

    Kurosawa S., Higo T., Saito S., Uesugi R., Nakatsuji S.

    Physical Review Materials   Vol. 8 ( 5 )   2024.5

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    Publisher:Physical Review Materials  

    Recent intensive studies in metallic kagome systems have revealed various correlated topological and electronic states, leading to their spintronic applications. The kagome ferromagnetic metal Fe3Sn has been found to host a topological nodal plane near the Fermi energy and exhibits large transverse transport responses. Here we report the fabrication of the epitaxial thin films of Fe3Sn and the observation of its large anomalous Nernst effect (ANE). Structural and magnetic measurements reveal (0001)-orientated epitaxial growth of kagome D019 Fe3Sn and the magnetic easy plane along the substrate plane. Moreover, transport measurements confirm the large ANE of 2.4 μV/K at room temperature, comparable to that of the bulk polycrystalline samples. The obtained Fe3Sn film should be useful for thermoelectric applications, because the binary compound based on inexpensive elements exhibits large spontaneous ANE voltage under an out-of-plane heat current due to the magnetic and electronic states stabilized by the magnetic anisotropy.

    DOI: 10.1103/PhysRevMaterials.8.054206

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  63. Optical and scintillation properties of Pr3+-doped (La, Y)2Si2O7 single crystals Open Access

    Abe Y., Horiai T., Pejchal J., Yokota Y., Yoshino M., Murakami R., Hanada T., Yamaji A., Sato H., Ohashi Y., Kurosawa S., Kamada K., Yoshikawa A., Nikl M.

    Optical Materials X   Vol. 22   2024.5

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    Publisher:Optical Materials X  

    Pr-doped scintillators are attracting attention because of their potential applications in medical devices. In this study, we focused on Pr-doped (La, Y)<inf>2</inf>Si<inf>2</inf>O<inf>7</inf> scintillators to grow single crystals by the micro-pulling-down method and to evaluate their optical and scintillation properties. From the powder XRD results, the crystal structure and the space group were identified to be monoclinic and P2<inf>1</inf>/n, respectively. The results of optical and scintillation characterization show that the luminescence from the Pr<sup>3+</sup> 5d<inf>1</inf>–4f transition increases with increasing Pr<sup>3+</sup> concentration. The maximum light yield was also obtained for the sample with the highest Pr<sup>3+</sup> concentration. The Pr-doped (La, Y)<inf>2</inf>Si<inf>2</inf>O<inf>7</inf> single crystal shows promising properties for application in radiation detection.

    DOI: 10.1016/j.omx.2024.100318

    Open Access

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  64. 「次世代放射線シンポジウム 2023(第 35 回 放射線夏の学校)」 の特集号に寄せて

    黒澤 俊介

    放射線   Vol. 49 ( 1 ) page: 1   2024.3

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    Language:Japanese   Publisher:公益社団法人 応用物理学会  

    DOI: 10.11470/houshasen.49.1_1

    CiNii Research

  65. Demonstration of Tl-208 background reduction using topological information of Cherenkov light and observation of Zr-96 two neutrino double beta decay

    Fukuda Y., Moriyama S., Hiraide K., Ogawa I., Gunji T., Kurosawa S.

    Proceedings of Science   Vol. 441   2024.3

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    An experiment has been planned to measure the half-life of double beta decay with two-neutrino emission for <sup>96</sup>Zr nuclei. A newly designed 2ν-ZICOS detector will observe about 100 events of <sup>96</sup>Zr double beta decay. The detector will use an ultra-pure quartz flask and 20 Hamamatsu H3378-50 photomultipliers in order to distinguish the signal shape of Cherenkov lights. The liquid scintillator containing 0.4 g of <sup>96</sup>Zr will be filled in the ETFE cubic bag. The transparency of 50 µm thickness ETFE sheet for scintillation light was 97.5% at minimum. The constructions of a radiation shield using Pb blocks and the setup of 2ν-ZICOS detector will start in May 2024 at LAB-A in Kamioka mine, and the observation will start in next summer or autumn at the latest.

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  66. Quenching factor measurement of low-energy Na recoils in ultra-pure NaI(Tl) crystal

    Urano Y., Fushimi K., Hata K., Kawai Y., Konishi S., Kotera K., Kurosawa S., Mukai K., Ogino Y., Orito R., Sakabe T.

    Proceedings of Science   Vol. 441   2024.3

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    The Weakly Interacting Massive Particles (WIMPs) are considered to be the hypothetical particles that have been the leading candidate for dark matter for decades. The PICOLON project is directly searching for WIMPs dark matter using ultra-pure NaI(Tl) crystals at the Kamioka underground laboratory. To determine the WIMP sensitivity, it is necessary to know the quenching factor (QF) of NaI(Tl), which is the scintillation light yield ratio of nuclear recoil and electron recoil at the same energy deposit. Several groups reported the QF absolute values and its energy dependence in the low energy region (less than 100 keV), however the results are not in good agreement. It is still unsolved whether the disagreement is due to the individual crystal differences or the effect of systematic errors. In this paper, we report the QF of ultra-pure NaI(Tl) crystal developed by PICOLON group. To measure the QF, the crystal was irradiated with 2.45-MeV monochromatic neutrons generated by a discharge-type compact D-D fusion neutron source at the Institute of Advanced Energy, Kyoto University. The QFs of Na were obtained at six points in the range of 19-101 keV<inf>nr</inf>

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  67. Relationship of single crystal growth and luminescence properties of Cr-doped gadolinium gallium garnet crystals for radiation dose-rate monitoring systems

    Matsukura D., Kurosawa S., Yamaji A., Ohashi Y., Yokota Y., Kamada K., Sato H., Toyoda S., Yoshino M., Hanada T., Murakami R., Horiai T., Yoshikawa A.

    Journal of Crystal Growth   Vol. 630   2024.3

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    For the decommissioning of Fukushima Daiichi Nuclear Plants, a novel real-time dose-rate monitor consisting of a scintillator, 100-m long optical fiber and CCD spectrometer has been proposed, and this scintillation material is required to have an emission wavelength of longer than approximately 650 nm. In this paper, as a candidate material for the system, we focused on Ce/Cr co-doped Gd<inf>3</inf>Ga<inf>5</inf>O<inf>12</inf> (Ce/Cr:GGG) single crystals grown by the micro-pulling down method. Since the light output of this material was expected to depend on the Cr<sup>3+</sup> concentration, we investigated the relationship between Cr segregation and luminescence properties in Ce/Cr:GGG crystal. Generally, a single photon counting method is not available to evaluate its light output accurately due to the long decay time, we used a novel technique “emission-intensity two-dimensional- mapping method” (2D-image method) to verify the light intensity at each point of the sample. This method realized estimation of the light intensity within the sample, though segregation of Cr<sup>3+</sup> is observed. The results showed that Cr was concentrated in the center part along the radial direction in the grown crystals, while all parts had an emission wavelength of approximately 730 nm excited by X-ray. Using the 2D-image method, emission intensity was found to correspond to the Cr concentration, and its correlation coefficients between emission intensity and Cr concentration were over 0.8. We found that our material is available for the monitoring system when the Cr dense part of the crystal is cut and used.

    DOI: 10.1016/j.jcrysgro.2024.127581

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  68. Proposal of Change from SPECT to PET Aiming at Highly Reliable Diagnosis

    Takahashi Miwako, Yamaya Taiga, Ito Kimiteru, Kurosawa Shunsuke, Higuchi Takahiro, Tsuji Atsushi

    RADIOISOTOPES   Vol. 73 ( 1 ) page: 109 - 116   2024.3

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    <p>Early diagnosis based on pathophysiology enables optimal treatment. Nuclear medicine is one of the methods for visualizing organ functions and leading to early diagnosis. single photon emission computed tomography (SPECT) is widely used and supports clinical practice. However, the performance of SPECT is not sufficient to meet recent diagnostic needs. In this paper, we argue that the prospects and challenges of replacing part of SPECT with positron emission tomography.</p>

    DOI: 10.3769/radioisotopes.73.109

    CiNii Research

  69. Development of calculation model for designing temperature characteristics of double-layered thickness-shear resonator Open Access

    Ohashi Y., Noguchi T., Yokota Y., Murakami R., Kurosawa S., Kamada K., Horiai T., Yamaji A., Yoshino M., Yoshikawa A.

    Japanese Journal of Applied Physics   Vol. 63 ( 3 )   2024.3

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    Publisher:Japanese Journal of Applied Physics  

    A calculation model for predicting the temperature characteristics of the double-layered resonator (DRL) was developed by using the total strain ratio including the influence of the waves reflected at the bonding boundary. The validity of the model proposed was examined from the comparison between the measured and calculated results for a DRL specimen consisting of 129.55°Y- and 0°Y-quartz substrates. The calculation results of the model proposed demonstrated that it is possible to predict the trends of changes in experimental values of temperature characteristics not only in the 1st-order mode but also in the higher-order modes. In addition, the changes in the particle displacement distribution and temperature characteristics of the DLR obtained by the model proposed were also in good agreement with the results of finite element method analysis. The proposed model is expected to greatly contribute to the design of DLRs with high excitation efficiency and excellent temperature characteristics.

    DOI: 10.35848/1347-4065/ad1fb1

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  70. Investigation of the phase diagram of the CsI-LiBr system and fabrication of the eutectic scintillator for thermal neutron detection

    Sasaki R., Kamada K., Yoshino M., Jin Kim K., Murakami R., Horiai T., Yamaji A., Kurosawa S., Yokota Y., Sato H., Ohashi Y., Hanada T., Yoshikawa A.

    Journal of Crystal Growth   Vol. 628   2024.2

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    <sup>3</sup>He gas detectors have been commonly used in applied technology related to thermal neutron detectors; however, owing to the depletion of <sup>3</sup>He, applications using solid-state scintillators are expanding. In recent years, our group has reported a novel Tl:CsI/<sup>6</sup>LiBr eutectic scintillator for thermal neutron detection, which has excellent light yield and (n,γ) discrimination ability. In practical applications of eutectic scintillators, achieving eutectic production precisely at the eutectic point is crucial to ensure a high production yield and the development of a uniform eutectic structure. However, the phase diagram of the CsI-LiBr system has not yet been reported. In this study, the phase diagram obtained from calorimetry was investigated. Furthermore, eutectic fabrication was performed at the eutectic point, and the neutron response was evaluated.

    DOI: 10.1016/j.jcrysgro.2023.127543

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  71. Feasibility study of one-dimensional imaging with an optical fiber for radiation dose-rate monitoring system in the decommissioning process Open Access

    Matsukura D., Kurosawa S., Fujiwara C., Yamaji A., Ohashi Y., Yokota Y., Kamada K., Sato H., Masao Y., Hanada T., Murakami R., Horiai T., Yoshikawa A., Takata T., Tanaka H.

    Journal of Instrumentation   Vol. 19 ( 2 )   2024.2

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    Publisher:Journal of Instrumentation  

    Real-time dose-rate monitoring system under the high dose-rate situation is required for the decommissioning of Fukushima Daiichi Nuclear Plants to remove the debris remaining inside the plants. We have proposed a dose-rate monitor consisting of a scintillator, over 100-m long optical fiber and CCD spectrometer. Some noises with a dominant emission wavelength of below 550 nm originating from the optical fiber itself must be separated from the signal from the scintillator, and the signal region has been defined as 650–1000 nm to use significant data, up to now. In this paper, we investigated if the noise region defined as below 550 nm can be supporting data for the monitoring system, because such noises are expected to include position information through the fiber. In the emission spectrum, the intensities of the noise emission or absorption band are expected to depend on the position of the fiber, and we demonstrated such dependence, “one-dimensional dose-rate distribution”, with 20 m-long optical fiber and CCD spectrometer. Optical fiber was placed around a <sup>60</sup>Co source with an activity of approximately 60 TBq, and emission spectra of the fiber were acquired with different dose-rate conditions from 10 to 700 Gy/h. The noise intensities were well fitted with the power function as a function of the product of fiber length and dose rate, and we found that fiber noise has rate information in one-dimensional imaging.

    DOI: 10.1088/1748-0221/19/02/C02053

    Scopus

  72. Growth of Mg2Si thermoelectric eutectics by unidirectional solidification

    Hayashi N., Yokota Y., Horiai T., Yoshino M., Yamaji A., Murakami R., Hanada T., Sato H., Ohashi Y., Kurosawa S., Kamada K., Yoshikawa A.

    Journal of Crystal Growth   Vol. 627   2024.2

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    Publisher:Journal of Crystal Growth  

    Mg<inf>2</inf>Si/Si eutectics are grown from melt by the Vertical Bridgman method using a carbon crucible at three pulling rates. All the Mg<inf>2</inf>Si/Si eutectics are composed of Mg<inf>2</inf>Si and Si phases, and the eutectic structure becomes finer with an increase in the pulling rate. Increasing the pulling rate systematically decreases the thermal conductivities of the Mg<inf>2</inf>Si/Si eutectics, suggesting that a decrease in the thermal conductivity is attributed to an increase in phonon scattering at the boundaries between the two phases. The power factor and figure of merit of the Mg<inf>2</inf>Si/Si eutectics are larger than those of Mg<inf>2</inf>Si above 400 °C because of the increase in the Seebeck coefficient. The figure of merit, ZT, of the Mg<inf>2</inf>Si/Si eutectics solidified at a 10<sup>3</sup> mm/min pulling rate reached 0.076 at 600 °C.

    DOI: 10.1016/j.jcrysgro.2023.127533

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  73. Fabrication and Properties for Thermal Neutron Detection of 6LiCl/Rb2CeCl5 Eutectic Scintillator Open Access

    Sasaki R., Kamada K., Yoshino M., Kim K.J., Murakami R., Horiai T., Yamaji A., Kurosawa S., Yokota Y., Sato H., Ohashi Y., Hanada T., Yoshikawa A.

    Crystals   Vol. 14 ( 2 )   2024.2

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    Publisher:Crystals  

    The <sup>3</sup>He gas is commonly used for the detection of thermal neutrons. However, with the depletion of <sup>3</sup>He gas, there is a need to develop new solid scintillators for thermal neutron detection. Solid scintillators containing <sup>6</sup>Li, which have large neutron capture cross-sections and a large amount of energy released by transmutation reactions, are commonly used as alternative candidates. However, only single-crystal scintillators are currently used, and their <sup>6</sup>Li concentration is limited by their chemical composition. In this study, we designed, grew, and evaluated a new eutectic scintillator, Rb<inf>2</inf>CeCl<inf>5</inf>/LiCl, which can improve the <sup>6</sup>Li concentration compared with single-crystal scintillators. Rb<inf>2</inf>CeCl<inf>5</inf>, which was selected as the scintillator phase, has excellent scintillator properties (light yield: 36,000 photons/MeV, decay time: mostly 24 ns, slightly 153 ns), and is less deliquescent than other halide scintillators. The crystal grown using the vertical Bridgman method exhibited a eutectic phase composed of Rb<inf>2</inf>CeCl<inf>5</inf> and LiCl. The eutectic crystals exhibited Ce<sup>3+</sup> 5d-4f emissions, with a peak between 360 and 370 nm. The Rb<inf>2</inf>CeCl<inf>5</inf> phase was identified as the luminescent phase via cathodoluminescence mapping, and 16,000 photons/neutron of the light yield and 56.1 ns of the decay time were observed. This study indicates that the Rb<inf>2</inf>CeCl<inf>5</inf>/LiCl eutectic scintillator is a promising candidate for use in thermal neutron detectors.

    DOI: 10.3390/cryst14020154

    Open Access

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  74. Highly Efficient and Flexible Scintillation Screen Based on Organic Mn(II) Halide Hybrids toward Planar and Nonplanar X-Ray Imaging

    Li W., Li Y., Wang Y., Zhou Z., Wang C., Sun Y., Sheng J., Xiao J., Wang Q., Kurosawa S., Buryi M., John D., Paurová K., Nikl M., OuYang X., Wu Y.

    Laser and Photonics Reviews   Vol. 18 ( 2 )   2024.2

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    Publisher:Laser and Photonics Reviews  

    The urgency for cost-effective, high-resolution, flexible X-ray imaging detectors is generating great demand for scintillators with low-temperature processability, high scintillation yield, and negligible afterglow. X-ray imaging materials are currently dominated by inorganic scintillators in the form of rigid films and bulk crystals, which have inherent limitations including high-temperature, complex synthesis, and considerable challenges toward advanced nonplanar imaging. Here, high-performance and flexible X-ray scintillators based on novel zero-dimensional (0D) (BTPP)<inf>2</inf>MnX<inf>4</inf> (BTPP = benzyltriphenylphosphonium; X = Cl, Br) halides are reported. They emit bright green light originating from the <sup>4</sup>T<inf>1</inf>-<sup>6</sup>A<inf>1</inf> transition of Mn<sup>2+</sup> under X-ray excitation. In particular, (BTPP)<inf>2</inf>MnBr<inf>4</inf> single crystals exhibit excellent air- and radiation-stability, a high scintillation yield of 53 000 photons MeV<sup>−1</sup>, a low detection limit of 89.9 nGy<inf>air</inf> s<sup>−1</sup>, and an ultralow afterglow comparable to commercial Bi<inf>4</inf>Ge<inf>3</inf>O<inf>12</inf> (BGO) single crystals. Moreover, the (BTPP)<inf>2</inf>MnCl<inf>4</inf>@polydimethylsiloxane (PDMS) flexible scintillation screens achieve a high spatial resolution of 14.1 lp mm<sup>−1</sup> and realize high-quality imaging results of nonplanar objects. This study demonstrates that the flexible scintillation screens based on low-dimensional Mn(II) hybrid halides have significant potential for low-dose and high-resolution X-ray imaging applications.

    DOI: 10.1002/lpor.202300860

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  75. The prognosis and risk factors for patients with complex karyotype myelodysplastic syndrome undergoing allogeneic haematopoietic stem cell transplantation Open Access

    Shimomura Y., Komukai S., Kitamura T., Tachibana T., Kurosawa S., Itonaga H., Tsukamoto S., Doki N., Katayama Y., Ito A., Sawa M., Ueda Y., Nakamae H., Nawa Y., Tanaka M., Arai Y., Ota S., Kataoka K., Nishida T., Kanda J., Fukuda T., Atsuta Y., Ishiyama K.

    British Journal of Haematology   Vol. 204 ( 2 ) page: 612 - 622   2024.2

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    Language:English   Publisher:British Journal of Haematology  

    Allogeneic haematopoietic stem cell transplantation (HCT) is the curative treatment for myelodysplastic syndrome with a complex karyotype (CK-MDS). However, only a few studies have been limited to patients with CK-MDS undergoing allogeneic HCT. This study aimed to identify the risk factors for patients with CK-MDS undergoing allogeneic HCT. We included 691 patients with CK-MDS who received their first allogeneic HCT. The overall survival (OS) was the primary end-point, estimated using the Kaplan–Meier method. Prognostic factors were identified using a Cox proportional hazards model. The 3-year OS was 29.8% (95% confidence interval [CI]: 26.3–33.3). In the multivariable analysis, older age (hazard ratio [HR]: 1.44, 95% CI: 1.11–1.88), male sex (HR: 1.38, 95% CI: 1.11–1.71), poor haematopoietic cell transplant comorbidity index (HR: 1.47, 95% CI: 1.20–1.81), red blood cell transfusion requirement (HR: 1.58, 95% CI: 1.13–2.20), platelet transfusion requirement (HR: 1.85, 95% CI: 1.46–2.35), not-complete remission (HR: 1.55, 95% CI: 1.16–2.06), a high number of karyotype abnormality (HR: 1.63, 95% CI: 1.18–2.25) and monosomal karyotype (HR: 1.49, 95% CI: 1.05–2.12) were significantly associated with OS. Thus, the 3-year OS of allogeneic HCT was 29.8% in patients with CK-MDS, and we identified risk factors associated with poor OS.

    DOI: 10.1111/bjh.19139

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    PubMed

  76. Thermal multiferroics in all-inorganic quasi-two-dimensional halide perovskites

    Zhu T., Lu X.Z., Aoyama T., Fujita K., Nambu Y., Saito T., Takatsu H., Kawasaki T., Terauchi T., Kurosawa S., Yamaji A., Li H.B., Tassel C., Ohgushi K., Rondinelli J.M., Kageyama H.

    Nature Materials   Vol. 23 ( 2 ) page: 182 - 188   2024.2

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    Language:English   Publisher:Nature Materials  

    Multiferroic materials, particularly those possessing simultaneous electric and magnetic orders, offer a platform for design technologies and to study modern physics. Despite the substantial progress and evolution of multiferroics, one priority in the field remains to be the discovery of unexplored materials, especially those offering different mechanisms for controlling electric and magnetic orders<sup>1</sup>. Here we demonstrate the simultaneous thermal control of electric and magnetic polarizations in quasi-two-dimensional halides (K,Rb)<inf>3</inf>Mn<inf>2</inf>Cl<inf>7</inf>, arising from a polar–antipolar transition, as evidenced using both X-ray and neutron powder diffraction data. Our density functional theory calculations indicate a possible polarization-switching path including a strong coupling between the electric and magnetic orders in our halide materials, suggesting a magnetoelectric coupling and a situation not realized in oxide analogues. We expect our findings to stimulate the exploration of non-oxide multiferroics and magnetoelectrics to open access to alternative mechanisms, beyond conventional electric and magnetic control, for coupling ferroic orders.

    DOI: 10.1038/s41563-023-01759-y

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    PubMed

  77. Structure analysis and luminescence properties of red-emitting iodide scintillators with potassium-hexachloroplatinate(IV) type structure

    Kodama S., Kurosawa S., Fujii K., Yashima M., Yamaji A., Yoshikawa A.

    Journal of Alloys and Compounds   Vol. 970   2024.1

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    Publisher:Journal of Alloys and Compounds  

    Halide compounds with chemical formula A<inf>2</inf>MX<inf>6</inf> (A: alkali metal or Tl, M: tetravalent metal, X: halogen) have previously been reported as intrinsic scintillators. However, some application fields e.g., utilizing waveguides, require novel scintillators with emission wavelengths longer than that of Cs<inf>2</inf>HfI<inf>6</inf> as bright and red/infrared scintillators. Thus, in this study, cation-substituted Cs<inf>2</inf>HfI<inf>6</inf> crystals (Rb<inf>2</inf>HfI<inf>6</inf>, K<inf>2</inf>HfI<inf>6</inf>, Cs<inf>2</inf>ZrI<inf>6</inf>, Rb<inf>2</inf>ZrI<inf>6</inf>, and K<inf>2</inf>ZrI<inf>6</inf>) were grown using the vertical Bridgman method, and their crystal structures were analyzed via single-crystal X-ray diffraction. The crystal structures of Cs<inf>2</inf>HfI<inf>6</inf> and Cs<inf>2</inf>ZrI<inf>6</inf> were determined to be cubic (space group: Fm3̅m), Rb<inf>2</inf>HfI<inf>6</inf> and Rb<inf>2</inf>ZrI<inf>6</inf> were tetragonal (space group: P4/mnc), and K<inf>2</inf>HfI<inf>6</inf> and K<inf>2</inf>ZrI<inf>6</inf> were monoclinic (space group P2<inf>1</inf>/c). In addition, the emission spectra of Rb<inf>2</inf>HfI<inf>6</inf>, K<inf>2</inf>HfI<inf>6</inf>, Rb<inf>2</inf>ZrI<inf>6</inf>, and K<inf>2</inf>ZrI<inf>6</inf> showed that their peaks exhibited a 25 nm red-shift in comparison with that of Cs<inf>2</inf>HfI<inf>6</inf>, whereas those of Cs<inf>2</inf>ZrI<inf>6</inf> did not. For A<inf>2</inf>MI<inf>6</inf> compounds, the emission was effectively determined by A-site cation substitution. Moreover, the pulse-height spectra were successfully measured for A<inf>2</inf>HfI<inf>6</inf>. The scintillation light outputs of Cs<inf>2</inf>HfI<inf>6</inf>, Rb<inf>2</inf>HfI<inf>6</inf>, and K<inf>2</inf>HfI<inf>6</inf> were estimated to be approximately 60,000, 40,000, and 33,000 photons/MeV, respectively.

    DOI: 10.1016/j.jallcom.2023.172506

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  78. Celestial MeV gamma-ray observation using electron-tracking Compton camera loaded on long duration balloons (SMILE-3)

    Takada A., Ikeda T., Abe M., Tsukamoto H., Yoshioka R., Tanimori T., Takemura T., Yoshikawa K., Mizumura Y., Kurosawa S., Miuchi K., Sawano T., Nakamori T., Iiyama H., Oka T., Mori M., Hamaguchi K., Kushida J.

    Proceedings of SPIE the International Society for Optical Engineering   Vol. 13093   2024

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    Publisher:Proceedings of SPIE the International Society for Optical Engineering  

    MeV gamma-ray observations provide unique information about nucleosynthesis, diffusion in our galaxy, low-energy cosmic rays, particle acceleration, and other phenomena. However, the detection sensitivity in this band is significantly lower than that in other bands due to a large background contamination. To address this issue, we are developing an electron-tracking Compton camera (ETCC) with powerful background rejection tools based on Compton recoil electron tracks. This will enable future observations to be conducted with greater sensitivity. We have successfully demonstrated the detection technology and performance of the ETCC with two balloon experiments. We are preparing for the next balloon flight, SMILE-3, to observe galactic diffusion gamma rays and some bright celestial objects.

    DOI: 10.1117/12.3016872

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  79. High-z gamma-ray bursts unraveling the dark ages and extreme space-time mission - HiZ-GUNDAM Open Access

    Yonetoku D., Doi A., Mihara T., Matsuhara H., Sakamoto T., Tsumura K., Ioka K., Arimoto M., Enoto T., Fujimoto K., Goto H., Gunji S., Hiraga J., Ikunaga S., Kawai N., Kondo R., Kurosawa S., Li J., Maeda Y., Mitsuishi I., Murakami T., Nagataka I., Nakagawa Y., Ogino N., Owari T., Sato R., Sato M., Sato T., Sawano T., Serino M., Shen H.C., Sugita S., Takahashi S., Tamagawa T., Tamura K., Tanaka T., Tanimori T., Tashiro M.S., Togashi T., Tomida H., Watanabe K., Yamaoka K., Yamauchi M., Yatsu Y., Yoshida A., Akitaya H., Fukui A., Fukui H., Ita Y., Kawabata K., Matsuura S., Miyasaka A., Motohara K., Narita N., Noda H., Okita H., Sano K., Shinozaki K., Tajima S., Urata Y., Wada T., Yanagisawa K., Yoshida M., Bando N., Jikuya I., Minesugi K., Miyazaki Y., Kono Y., Takase N., Nakatsubo S., Kaga T., Asano K., Inayoshi K., Inoue S., Ito H., Izumiura H., Kawanaka N., Kinugawa T., Kisaka S., Kiuchi K., Kyutoku K., Matsumoto J., Mizuta A., Murase K., Nagakura H., Nagataki S., Nakada Y., Nakamura T., Niino Y., Suwa Y., Takahashi K., Tanaka T., Toma K., Totani T., Yamazaki R., Yokoyama J., Harikane Y., Tanaka M., Kimura S., Kimura M.

    Proceedings of SPIE the International Society for Optical Engineering   Vol. 13093   2024

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    Publisher:Proceedings of SPIE the International Society for Optical Engineering  

    HiZ-GUNDAM is a future satellite mission whose mission concept was approved by ISAS/JAXA, and it is one of the future satellite candidates of JAXA's competitive medium-class mission. HiZ-GUNDAM will lead time-domain astronomy in 2030s, and its key sciences are (1) exploration of the early universe with high-redshift gamma-ray bursts, and (2) contribution to the multi-messenger astronomy. Two mission payloads are aboard HiZ-GUNDAM to realize these two scientific issues. The wide field X-ray monitors which consist of Lobster Eye optics array and focal imaging sensor, monitor ~0.5 steradian field of view in 0.5-4 keV energy range. The near infrared telescope with an aperture size of 30 cm in diameter performs simultaneous 5-band photometric observation in 0.5-2.5 µm wavelength with Koester's prism for X-ray transients discovered by Wide Field X-ray Monitor. In this paper, we introduce the mission overview of HiZ-GUNDAM while the information contained herein may change in future studies.

    DOI: 10.1117/12.3018571

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  80. Modification of Ce3+luminescence in Li+and Mg2+codoped GAGG:Ce scintillators: A comparative study using synchrotron radiation Open Access

    Bartosiewicz K., Kurosawa S., Yamaji A., Zorenko Y., Yoshikawa A.

    Journal of Physics Conference Series   Vol. 2712 ( 1 )   2024

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    Publisher:Journal of Physics Conference Series  

    The luminescence characteristics of Gd3Al2Ga3O12:Ce3+ garnet scintillator crystals codoped with Li+ and Mg2+ ions were investigated. The excitation and emission spectra were obtained within the energy range of 3.6-21.6 eV, at both liquid helium and room temperature conditions to examine the effects of Li+ and Mg2+ codoping on cerium valence states, gadolinium-cerium energy transfer, and defect formation. Codoping with Mg2+ was found to efficiently convert Ce3+ to Ce4+, evidenced by significant changes in the shapes of the excitation spectra profile for Ce3+ luminescence in the exciton range, while Li+ had little impact. The presence of the high concentration of Ce4+ ions hampered the Gd3+→Ce4+ energy transfer. Redshifts in Ce3+ emission peaks indicated codopant-induced perturbations to the crystal field environment. The significant changes in the location of the Ce3+ excitation bands of Ce3+ luminescence in the exciton range further suggested alterations in the elemental distributions by the creation of complex defect clusters, particularly with Mg2+ codoping. The results demonstrate that Li+ and Mg2+ uniquely impact cerium valence, energy transfer processes, and structural properties in GAGG:Ce crystals.

    DOI: 10.1088/1742-6596/2712/1/012011

    Open Access

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  81. Thermophysical Properties of Molten Fe–Cu Alloy Measured Using the Electrostatic Levitation Furnace Aboard the International Space Station (ISS-ELF) under Microgravity Conditions Open Access

    Seimiya Y., Kobatake H., Tono-Oka K., Sugahara R., Kurosawa S., Shiratori S., Sugioka K.I., Ishikawa T., Koyama C., Watanabe Y., Shimonishi R., Ozawa S.

    ISIJ International   Vol. 64 ( 15 ) page: 2253 - 2261   2024

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    Publisher:ISIJ International  

    The thermophysical properties of molten Fe–Cu alloys, including density, surface tension, and viscosity, were measured using the electrostatic levitation furnace aboard the International Space Station (ISS-ELF) under microgravity conditions, which provided an environment that facilitated accurate measurements. The densities of the molten Fe–25at%Cu and Fe–50at%Cu alloys decreased linearly with increasing temperature, and higher copper compositions resulted in increased density. The surface tension of the molten alloys exhibited a unique up-convex temperature dependence curve that initially increased and then decreased as the temperature increased. Viscosity measurements indicated that the viscosity of the molten Fe–Cu alloys decreased with increasing temperature, following a quadratic curve, and that an increase in the copper composition resulted in lower viscosity.

    DOI: 10.2355/isijinternational.ISIJINT-2024-277

    Open Access

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  82. Feasibility Study on One-Dimensional Dose Rate Distribution Measurement Using Fiber Noise Data from the Fiber-Optic Radiation Dose Rate Monitoring System

    Matsukura Daisuke, Kurosawa Shunsuke, Tanaka Hiroki, Takata Takushi, Yamaji Akihiro

    Ionizing Radiation   Vol. 49 ( 1 ) page: 18 - 22   2024

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    Language:Japanese   Publisher:The Japan Society of Applied Physics  

    Real-time dose-rate monitoring system under the high dose-rate situation is required for the decommissioning of the Fukushima Daiichi Nuclear Plants to remove the debris remaining inside the plants. We have proposed a dose-rate monitor consisting of a scintillator, over 100-m long optical fiber and CCD spectrometer. Some noises with a dominant-emission wavelength band of below 550 nm originating from the optical fiber itself must be separated from the scintillator emission light in 650-1000 nm, which is used as signal data, up to now. In this paper, we investigated if the noise region defined as below 550 nm is available for the position estimation of the hot spot through the fiber. The intensities of the noise emission or absorption band of such fiber-emission spectra are expected to depend on the hot-spot position through the fiber, and we demonstrated such dependence, “one-dimensional dose-rate distribution”, with a 20 m-long optical fiber and CCD spectrometer. Two types of optical fibers (High OH and Low OH) were tested under several length conditions of the fiber from the CCD spectrometer to 60Co source. The results of the emission spectra showed the intensity ratio of absorption to maximum intensity peak decreased as such length condition increased. We found that fiber noise is available for the position estimation for the hotspots (debris).

    DOI: 10.11470/houshasen.49.1_18

    CiNii Research

  83. Novel optical-guiding crystal scintillator composed of an Eu-doped SrI2 core and glass cladding

    Yajima R., Kamada K., Takizawa Y., Kutsuzawa N., Sasaki R., Yoshino M., Horiai T., Murakami R., Kim K.J., Kochurikhin V.V., Yamaji A., Kurosawa S., Yokota Y., Sato H., Toyoda S., Ohashi Y., Takashi H., Yoshikawa A.

    Ceramics International   Vol. 49 ( 24 ) page: 41259 - 41263   2023.12

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    Publisher:Ceramics International  

    Scintillators are used not only as single crystals in radiation detection systems but also as arrays, columns, and fibers. In this study, a novel optical-guiding crystal scintillator (OCS) was fabricated using an Eu:SrI<inf>2</inf> crystal as the core and borosilicate glass as the cladding. The OCS has an elongated shape and can be flexibly processed like an optical fiber. Furthermore, because inorganic scintillator crystals are used as the core, the OCS has high sensitivity to high-energy radiation, such as γ- and X-ray radiation, unlike plastic scintillators. In this study, by observing the cross section of the fabricated OCS, identifying the crystal structure, and investigating the radioluminescence spectrum under X-ray irradiation, OCS fabrication in accordance with the OCS design specifications was confirmed, and the SrI<inf>2</inf> crystal structure and Eu<sup>2+</sup> 5d–4f luminescence were maintained. The γ-ray responses, such as light yield and decay time, were also investigated.

    DOI: 10.1016/j.ceramint.2022.12.264

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  84. Alpha-ray imaging with alkali copper halide scintillator

    Urano Y., Kurosawa S., Yamaji A., Yoshikawa A., Wu Y.

    Journal of Instrumentation   Vol. 18 ( 12 )   2023.12

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    Publisher:Journal of Instrumentation  

    Internal exposure for decommissioning workers at the Fukushima Daiichi Nuclear Power Plant must be prevented, and we have developed a monitoring system for alpha-ray emitting dust (alpha dust). When the dust size is less than several tens of micrometers, a dust protection mask does not work effectively to prevent internal exposure. Since no devices have been operated to observe alpha-dust images in real-time up to now, we have developed an alpha-ray imaging detector consisting of a scintillation material and imaging detector. Scintillators are required to have high light output and chemical stability. Cs<inf>3</inf>Cu<inf>2</inf>I<inf>5</inf> (CCI) scintillator was found to be one of the candidates, and an imaging test was operated with this material. The CCI crystal was grown by the Bridgman-Stockberger method, and a scintillation sheet for alpha-ray imaging was prepared by CCI microcrystals with a thickness of approximately 70 μm on a 200-μm thickness transparent polyethylene terephthalate film as a first imaging test. The sheet was irradiated with 5.5-MeV alpha rays from an <sup>241</sup>Am source, and scintillation photons were detected with a CMOS camera through an optical lens. We succeeded in visualizing alpha rays, and a position resolution of our system achieved approximately 16.2 ± 2.6 μm (10-90 %). This resolution was similar value to other imaging devices with Ag:ZnS powder scintillator, and a CCI single crystal sheet was expected to reach better resolution.

    DOI: 10.1088/1748-0221/18/12/C12009

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  85. Scintillator-oriented near-infrared emitting Cs4SrI6:Yb2+, Sm2+ single crystals via sensitization strategy Open Access

    Wen X., Kucerkova R., Babin V., Prusa P., Kotykova M., Nikl M., Li W., Wang Q., Kurosawa S., Wu Y.

    Journal of the American Ceramic Society   Vol. 106 ( 11 ) page: 6762 - 6768   2023.11

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    Publisher:Journal of the American Ceramic Society  

    In this study, a new Cs<inf>4</inf>SrI<inf>6</inf>:Yb<sup>2+</sup>,Sm<sup>2+</sup> near-infrared (NIR) emitting scintillator was developed using sensitization strategy. It was found that Yb<sup>2+</sup> sensitization significantly enhances the NIR radioluminescence (RL) of Sm<sup>2+</sup>, providing a new approach of designing highly emissive sensitized NIR scintillators. By studying the optical spectra and decay kinetics of Cs<inf>4</inf>SrI<inf>6</inf>:Yb<sup>2+</sup>,Sm<sup>2+</sup>, it was revealed that the energy transfer pathways involve both radiative and nonradiative processes. The gamma spectroscopy performance of Cs<inf>4</inf>SrI<inf>6</inf>:Yb<sup>2+</sup>,Sm<sup>2+</sup> single crystals was studied by using the high-quantum-efficiency avalanche photodiode (APD) as the readout. Our results highlight the importance of using sensitization strategy of achieving NIR emitting scintillators and demonstrate the significant potential for radiation detection applications.

    DOI: 10.1111/jace.19302

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  86. Li2HfBr6 scintillator for neutron and gamma-ray dual detection Open Access

    Fujiwara C., Kurosawa S., Yamaji A., Yoshikawa A.

    Applied Physics Express   Vol. 16 ( 10 )   2023.10

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    Publisher:Applied Physics Express  

    Li<inf>2</inf>HfBr<inf>6</inf> with host emission was grown as a gamma-ray- and neutron-sensitive scintillator. Decay time of Li<inf>2</inf>HfBr<inf>6</inf> was estimated to be less than 5 μs, and single-photon counting is available to evaluate its light output. The emission wavelength under X-ray excitation was approximately 570 nm, which is a longer wavelength than that of commonly used neutron scintillators, e.g. Li-glass. The light output excited by thermal neutrons was estimated to be 52000 photons per thermal neutron, which is approximately eight to nine times higher than that of Li-glass. Additionally, neutrons and gamma rays were discriminated using the pulse-shaped discrimination technique for Li<inf>2</inf>HfBr<inf>6</inf>

    DOI: 10.35848/1882-0786/ad03ab

    Open Access

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  87. Purification of CaF2crystal for double beta decay experiments

    Fushimi K., Imagawa K., Kishida Y., Kurosawa S., Orito R., Sakaue A., Takihira Y., Umehara S., Yamaji A., Yamamoto Y., Yasuda K., Yoshida T.

    Aip Conference Proceedings   Vol. 2908 ( 1 )   2023.9

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    Publisher:Aip Conference Proceedings  

    We report on inorganic crystal purification for the search for the neutrinoless double-beta decay of 48Ca using CaF2 crystals. We are working on the purification of CaF2 crystal, which is made from water-insoluble raw materials. The goal of the purity in this crystal is ≤1 μBq/kg. We measured the impurities in the crucible and CaF2 powder before we made a molten product of the CaF2. We will consider the correlation between the purity contained in the materials around the crystal growth and the purity of the molten product. The material-selection policy and prospects for the large-volume detector system will be discussed.

    DOI: 10.1063/5.0161258

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  88. Designing TOGAXSI: Telescope for inverse-kinematics cluster-knockout reactions

    Tanaka J., Tsuji R., Higuchi K., Baba H., Böhmer M., Furuno T., Gernhäuser R., Hijikata Y., Ishimoto S., Kawabata T., Kawase S., Kubota Y., Kurosawa S., Takeshige S., Uesaka T., Yahiro K., Zenihiro J.

    Nuclear Instruments and Methods in Physics Research Section B Beam Interactions with Materials and Atoms   Vol. 542   page: 4 - 6   2023.9

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    Publisher:Nuclear Instruments and Methods in Physics Research Section B Beam Interactions with Materials and Atoms  

    We have launched a new research project named “ONOKORO” to elucidate the formation mechanism of clusters in atomic nuclei. The project comprehensively investigates clustering phenomena in the medium-to-heavy mass region with inverse-kinematics cluster-knockout reactions at the intermediate energy facilities. The new detector array named “TOGAXSI” is under construction for this purpose. It measures scattering angles and the energies of deuterons, tritons, <sup>3</sup>He, and α particles emitted at forward angles from the cluster-knockout reactions. It also measures the recoil protons emitted from the scattering events at large angles. High-angular and high-energy resolutions with wide solid angles are required to achieve a good cluster separation energy resolution and a reasonably high yield. The designed telescope consists of silicon trackers and GAGG:Ce calorimeters. This paper shows the required conditions and design concepts of TOGAXSI.

    DOI: 10.1016/j.nimb.2023.05.054

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  89. Optical and scintillation properties of Yb-doped La2Hf2O7 crystal grown by core heating method for fiber reading remote-dosimetry system

    Ishizawa S., Kurosawa S., Kurashima Y., Kodama S., Morishita Y., Yamaji A., Ohno M., Ishikawa S., Hayashi M., Sasano M., Makita T., Fujiwara C., Kochurikhin V., Yoshikawa A., Takata T., Tanaka H.

    Optical Materials   Vol. 142   2023.8

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    Publisher:Optical Materials  

    (La<inf>0.99</inf>Yb<inf>0.01</inf>)<inf>2</inf>Hf<inf>2</inf>O<inf>7</inf> (Yb:LaHO) crystal has been developed by the core heating method as a near-infrared-emitting oxide scintillator for a fiber reading remote-dosimetry system under the high-dose-rate region. This system consists of a scintillator, a long silica optical fiber and a detector unit. Near-infrared-emitting photons can be separated from significant fiber-derived noise mainly observed in the UV–blue range. The noise is generated in the optical fiber itself by gamma-rays and charged particles. The Yb:LaHO crystal had a maximum emission peak at 975 nm when excited by X-rays and a transmittance of approximately 29% at 977 nm. The afterglow intensity of the Yb:LaHO crystal under X-rays was 11% that of Cr:α-Al<inf>2</inf>O<inf>3</inf> (ruby) crystal. We demonstrated the applicability of the remote-dosimetry system with the Yb:LaHO crystal irradiated with gamma rays from a <sup>60</sup>Co source with an activity of ∼77 TBq. The signal-to-noise ratio (SNR) of the Yb:LaHO crystal was 1.9 times higher than that of the ruby crystal at ∼ 1 kGy/h, and the lowest limit of the dynamic range was comparable between the Yb:LaHO and ruby crystals. The results of the SNR and afterglow intensity showed that the Yb:LaHO crystal is a more suitable scintillator than the ruby crystal for fiber reading remote-dosimetry systems.

    DOI: 10.1016/j.optmat.2023.113941

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  90. Growth and Scintillation Properties of 6Li Containing Ce:LaCl3-Based Eutectic Scintillator for Neutron Detection

    Sasaki R., Kim K.J., Kamada K., Yajima R., Kutsuzawa N., Yoshino M., Murakami R., Horiai T., Yamaji A., Kurosawa S., Yokota Y., Sato H., Toyoda S., Ohashi Y., Hanada T., Takahashi I., Tomida T., Kochurikhin V.V., Yoshikawa A.

    IEEE Transactions on Nuclear Science   Vol. 70 ( 7 ) page: 1337 - 1341   2023.7

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    Publisher:IEEE Transactions on Nuclear Science  

    In this study, Ce:6LiCl/LaCl3 with a high 6Li concentration was developed as a novel thermal neutron scintillator, in which Ce3+ serves as an activator for the LaCl3 phase. The Ce:6LiCl/LaCl3 eutectic was grown in a quartz ampoule (inner diameter: 4.0 mm) using the Bridgman-Stockbarger technique. The grown eutectic contained 0.038 mol/cm36Li, which is greater than that found in commercially available scintillators such as LiCaAlF6 single crystals and Li glass. The Ce:6LiCl/LaCl3 eutectic has a lamellar eutectic structure and is optically transparent. A 350-nm emission due to Ce3+ 4f-5d transition was observed. The light yield under neutron irradiation was estimated to be 5.0 times higher than that of Li glass. In this eutectic, the 6Li ( n , a 3 H reaction made the 6LiCl phase to act as the neutron capture phase and LaCl3 to act as the scintillator phase.

    DOI: 10.1109/TNS.2023.3271639

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  91. Tl-Doped CsI/LiBr Scintillator for Thermal Neutron Detection With Ultrahigh Light Yield

    Yajima R., Kamada K., Yoshino M., Sasaki R., Horiai T., Murakami R., Kim K.J., Kochurikhin V.V., Ohashi Y., Yamaji A., Kurosawa S., Yokota Y., Sato H., Toyoda S., Hanada T., Yoshikawa A.

    IEEE Transactions on Nuclear Science   Vol. 70 ( 7 ) page: 1331 - 1336   2023.7

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    Publisher:IEEE Transactions on Nuclear Science  

    In this study, a novel thermal neutron scintillator of Tl:CsI/LiBr was developed. The eutectics were fabricated at various growth rates and investigated their scintillation properties. As a material design guideline, Tl:CsI, which has an excellent ratio, was selected as the scintillator phase to realize high light yield at the energy of rays and tritons generated by the nuclear transmutation reaction with 6Li and LiBr, which has a refractive index close to that of CsI, was selected as the neutron capture phase. Radioluminescence (RL) measurement under X-ray irradiation was also performed to obtain the emission spectrum of the eutectics. The light yield and decay time for thermal neutron were measured using 252Cf and were much higher than those of conventional scintillators for thermal neutron. Furthermore, fabricated eutectic can have the higher sensitivity to thermal neutron due to the high 6Li concentration compared to conventional single-crystal scintillators. Therefore, we have succeeded in developing a promising scintillator material.

    DOI: 10.1109/TNS.2023.3278465

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  92. Incidence and predictors of recurrent sick leave in survivors who returned to work after allogeneic hematopoietic cell transplantation

    Kurosawa S., Yamaguchi T., Mori A., Matsuura T., Masuko M., Murata M., Tashiro H., Kako S., Satake A., Hagihara M., Ota S., Saito T., Kagawa K., Matsuo Y., Itonaga H., Uoshima N., Yamaguchi H., Naito K., Takahashi M., Fukuda T.

    Journal of Cancer Survivorship   Vol. 17 ( 3 ) page: 781 - 794   2023.6

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    Background: Although rather favorable probabilities of return to work have been reported after allogeneic hematopoietic cell transplantation (allo-HCT), survivors often have difficulty continuing to work because of their immunocompromised status and diverse late effects after allo-HCT. We evaluated the incidence of and risk factors for recurrent sick leave in allo-HCT survivors after they initially returned to work. Methods: We targeted allo-HCT survivors who were employed at diagnosis, aged 20–64 at survey, and survived for ≥ 2 years without relapse. Of the 1904 survivors who were informed of the study, 1148 returned the questionnaire (60%), and 1048 eligible participants were included in the overall analysis. In the present study that considered recurrent sick leave after return to work, we targeted 896 participants who returned to work at least once after allo-HCT. Participants stated if they had recurrent sick leave after returning to work and its reasons, as well as associated patient-, HCT/HCT center–, and work-related factors and clinical events after allo-HCT. A logistic regression analysis was conducted to explore correlated factors for recurrent sick leave. Results: In survivors who returned to work, 30% required recurrent sick leave. The most frequent causes of recurrent leave were physical issues (72%), and analysis of free descriptions demonstrated that these were mainly associated with graft-versus-host disease, infection, or readmission. Other reasons included work-related issues such as gap between physical and working conditions. Multivariate analysis showed that cord blood transplantation, longer employment duration, and counseling from healthcare professionals were associated with a lower risk of recurrent leave. Readmission, immunosuppressant use, and symptoms involving the respiratory system, gut, and joints and muscles were associated with a higher risk. Conclusions: Our results drawn from a large cohort study should help healthcare professionals identify and assist at-risk patients. Multi-professional teams that provide continuous support and effective communication with the workplace are necessary to improve long-term outcomes after allo-HCT. Implications for Cancer Survivors: In order to continue working after the initial return to work, it is important to receive counseling from healthcare professionals and obtain reasonable accommodation from workplace.

    DOI: 10.1007/s11764-022-01250-8

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  93. Development of Performance Measurement Methods for Medical Compton Camera

    AKAMATSU Go, TASHIMA Hideaki, TAKYU Sodai, YAMAGUCHI Mitsutaka, KAWACHI Naoki, SAKAI Makoto, KUROSAWA Shunsuke, SHIMAZOE Kenji, FURUKAWA Jun, MOTOMURA Shinji, NISHIKIDO Fumihiko, YAMAYA Taiga, YOSHIDA Eiji, TAKAHASHI Miwako

    Medical Imaging Technology   Vol. 41 ( 3 ) page: 117 - 123   2023.5

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    Language:Japanese   Publisher:The Japanese Society of Medical Imaging Technology  

    <p>Compton cameras have the potential to become a novel imaging modality in nuclear medicine. One of the key issues in the medical application of Compton camera is the lack of performance measurement methods. In the case of SPECT and PET, there are standard performance measurement methods that are utilized in research and development of new imaging systems. Defining the standard performance measurement methods may facilitate research and development of a clinical Compton camera. We have organized an interdisciplinary research group and work towards developing performance measurement methods for medical Compton cameras. This report overviews this work.</p>

    DOI: 10.11409/mit.41.117

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  94. Towards deliberate design of persistent phosphors: a study of La-Ga admixing in LuAG:Ce crystals to engineer elemental homogeneity and carrier trap depths Open Access

    Bartosiewicz K., Fritz V., Van der Heggen D., Szymanski D., Zeler J., Pejchal J., Yamaji A., Kucerkova R., Beitlerova A., Kurosawa S., Yoshikawa A., Smet P.F., Zych E., Nikl M.

    Journal of Materials Chemistry C   Vol. 11 ( 26 ) page: 8850 - 8865   2023.5

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    Publisher:Journal of Materials Chemistry C  

    This research investigated the crystal chemical principles related to the incorporation of incompatible atoms into a garnet host lattice. These considerations might be used to guide and drive the design of new garnet compounds with novel properties. The strongly incompatible La atoms at the Lu sites of the Lu<inf>3</inf>Al<inf>2</inf>Ga<inf>3</inf>O<inf>12</inf>:Ce host lattice served as a research model. This study showed the possibility of designing material properties by exploiting atom mismatches in a crystal lattice. Lu<inf>3</inf>Al<inf>2</inf>Ga<inf>3</inf>O<inf>12</inf>:Ce0.075% crystals with increasing concentrations of La<sup>3+</sup> ions were grown from the melt using the micro-pulling down method. The concentration of La<sup>3+</sup> ions above 0.300 at% imposed physical and chemical boundary conditions on the crystallization process. The radial distributions of the chemical elements were studied as a function of the concentration of La<sup>3+</sup> ions. It was revealed that La<sup>3+</sup> codoping significantly reduced the cross-sectional fluctuation of the Ga and Al atoms. Persistent green-yellow luminescence due to the inter-configurational 5d → 4f transition of Ce<sup>3+</sup> was observed after the blue-light excitation. The LuAGG:Ce0.075%,La0.015% phosphor showed long persistent luminescence for more than 14 h above 0.32 mcd m<sup>−2</sup>, the detection limit of a human eye. The thermoluminescence glow curves revealed that the addition of La<sup>3+</sup> ions increased the concentration of traps.

    DOI: 10.1039/d3tc01304a

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  95. Prototype fabrication of optical-guiding Tl:CsI crystal scintillators and investigation of the crystallization process Open Access

    Yajima R., Kamada K., Murakami R., Kutsuzawa N., Sasaki R., Yoshino M., Horiai T., Kim K.J., Kochurikhin V.V., Yamaji A., Kurosawa S., Yokota Y., Sato H., Toyoda S., Ohashi Y., Hanada T., Yoshikawa A.

    Japanese Journal of Applied Physics   Vol. 62   2023.4

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    Publisher:Japanese Journal of Applied Physics  

    In this study, optical-guiding crystal scintillator (OCS) and bundled plates were fabricated. Considering the performance and melting point of halide scintillators and the softening point of glass, Tl:CsI was selected as the fiber core and borosilicate glass as the cladding. Thus, the fabricated OCS had a scintillator in the core and glass in the cladding. The scintillator was remelted and unidirectionally solidified to remove the voids in the OCS and form a single crystal. Consequently, the OCS served as a scintillator fiber with excellent optical-guiding performance and high sensitivity to γ- and X-rays. An OCS plate was also fabricated using bundles of OCSs with diameters of several tens of microns. The developed OCS plate is expected to be a high-resolution and high-sensitivity imaging plate because of its excellent optical-guiding performance.

    DOI: 10.35848/1347-4065/acb3d1

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  96. Downslope variation in hemipelagic sedimentation in an active margin basin: An example from the lower Pleistocene Kiwada and Takamizo formations on the Boso Peninsula, Japan

    Kurosawa S., Furota S., Mitsui M., Sawada K., Seike K., Furukawa N., Ito M.

    Sedimentology   Vol. 70 ( 3 ) page: 705 - 727   2023.4

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    Publisher:Sedimentology  

    Hemipelagites are widespread fine-grained sediments found from shelf margin to deep-water environments, and they are considered to have been formed as background sedimentation by vertical settling and slow lateral advection of clastic and biogenic fine-grained particles. Downflow variation in hemipelagic sedimentation, however, is not yet clearly understood, and was investigated in the lower Pleistocene Kiwada and Takamizo formations in the Kazusa forearc basin on the Boso Peninsula, Japan. Mapping of three tephra key beds enabled detailed correlation of two hemipelagite beds over a distance of ca 30 km from shelf-margin to basin-plain environments. The sedimentation rates decreased gradually in the downslope direction, but increased locally in response to turbidite sedimentation. This downslope variation indicates that hemipelagic sedimentation is not necessarily constant and varies in response to progradation and retrogradation of deep-water depositional systems, as well as additional input of fine-grained sediments from turbidity currents. In contrast, the grain size, magnetic susceptibility, clay-mineral composition, total organic carbon contents relative to total nitrogen contents (carbon/nitrogen), and δ<sup>13</sup>C values of organic carbon do not exhibit distinct downslope variation. This downslope consistency indicates that hemipelagites document temporal perturbations of geological and palaeoclimatic conditions in hinterlands, regardless of spatial and temporal variations in deep-water depositional environments. The concentrations of total organic carbon, total nitrogen and five biomarkers were lower values in turbiditic mudstones and hemipelagites that formed above a turbidite bed than in those of the other hemipelagites. This variation suggests that an additional supply of fine-grained sediments from turbidity currents likely diluted the organic matter in the hemipelagites. In addition, hemipelagites for which deposition was affected by turbidity currents exhibit slightly lower δ<sup>13</sup>C values, and may also document an additional contribution of terrestrial organic matter from turbidity currents.

    DOI: 10.1111/sed.13055

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  97. Mutational analysis of DNMT3A improves the prognostic stratification of patients with acute myeloid leukemia Open Access

    Wakita S., Marumo A., Morita K., Kako S., Toya T., Najima Y., Doki N., Kanda J., Kuroda J., Mori S., Satake A., Usuki K., Ueki T., Uoshima N., Kobayashi Y., Kawata E., Nakayama K., Nagao Y., Shono K., Shibusawa M., Tadokoro J., Hagihara M., Uchiyama H., Uchida N., Kubota Y., Kimura S., Nagoshi H., Ichinohe T., Kurosawa S., Motomura S., Hashimoto A., Muto H., Sato E., Ogata M., Mitsuhashi K., Ando J., Tashiro H., Sakaguchi M., Yui S., Arai K., Kitano T., Miyata M., Arai H., Kanda M., Itabashi K., Fukuda T., Kanda Y., Yamaguchi H.

    Cancer Science   Vol. 114 ( 4 ) page: 1297 - 1308   2023.4

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    Nucleophosmin1 (NPM1) mutations are the most frequently detected gene mutations in acute myeloid leukemia (AML) and are considered a favorable prognostic factor. We retrospectively analyzed the prognosis of 605 Japanese patients with de novo AML, including 174 patients with NPM1-mutated AML. Although patients with NPM1-mutated AML showed a high remission rate, this was not a favorable prognostic factor for overall survival (OS); this is contrary to generally accepted guidelines. Comprehensive gene mutation analysis showed that mutations in codon R882 of DNA methyltransferase 3A (DNMT3A<sup>R882</sup> mutations) were a strong predicative factor indicating poor prognosis in all AML (p < 0.0001) and NPM1-mutated AML cases (p = 0.0020). Furthermore, multivariate analysis of all AML cases showed that DNMT3A<sup>R882</sup> mutations and the co-occurrence of internal tandem duplication in FMS-like tyrosine kinase 3 (FLT3-ITD), NPM1 mutations, and DNMT3A<sup>R882</sup> mutations (triple mutations) were independent factors predicting a poor prognosis related to OS, with NPM1 mutations being an independent factor for a favorable prognosis (hazard ratios: DNMT3A<sup>R882</sup> mutations, 1.946; triple mutations, 1.992, NPM1 mutations, 0.548). Considering the effects of DNMT3A<sup>R882</sup> mutations and triple mutations on prognosis and according to the classification of NPM1-mutated AML into three risk groups based on DNMT3A<sup>R882</sup>/FLT3-ITD genotypes, we achieved the improved stratification of prognosis (p < 0.0001). We showed that DNMT3A<sup>R882</sup> mutations are an independent factor for poor prognosis; moreover, when confounding factors that include DNMT3A<sup>R882</sup> mutations were excluded, NPM1 mutations were a favorable prognostic factor. This revealed that ethnological prognostic discrepancies in NPM1 mutations might be corrected through prognostic stratification based on the DNMT3A status.

    DOI: 10.1111/cas.15720

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  98. Growth and scintillation properties of Ce 3+:LuAG-Al2O3 chemically deposited eutectics Open Access

    Matsumoto Shogen, Kurosawa Shunsuke, Yokoe Daisaku, Kimura Teiichi, Ito Akihiko

    Optical Materials   Vol. 138   page: 113674   2023.3

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    Directionally solidified eutectics (DSEs) in Al2O3-based systems have been studied as high-temperature structural ceramics, also recently attracting attention as a phosphor screen for high-resolution radiation imaging. However, it is difficult to obtain uniform and thinly processed DSE in large areas. Here, we report a chemically deposited eutectic (CDE) of Lu3Al5O12 (LuAG)-Al2O3 using a laser-assisted chemical vapor deposition method. The Ce3+- doped LuAG lamella were epitaxially grew with an alpha-Al2O3 matrix on an r-cut sapphire substrate. The Ce3+: LuAG-alpha-Al2O3 CDE film exhibited green emissions due to the 5d-4f transitions of the Ce3+ center under UV light and alpha-/X-ray irradiations. The alpha-ray dose in the Ce3+:LuAG phase was estimated with Monte Carlo simulations to study a scintillation light yield of the CDE film. The X-ray radiograph of the semiconductor storage device was successfully obtained using a 15-mu m-thick Ce3+:LuAG-alpha-Al2O3 CDE film as an X-ray phosphor screen.

    DOI: 10.1016/j.optmat.2023.113674

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  99. Red-Emitting Organic–Inorganic Hybrid Manganese(II) Halides for X-Ray Imaging Open Access

    Li W., Zhou Z., Wang C., Li Y., Kurosawa S., Ren G., OuYang X., Wu Y.

    Advanced Sensor Research   Vol. 2 ( 3 )   2023.3

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    Publisher:Advanced Sensor Research  

    Low-dimensional organic–inorganic hybrid manganese(II) halides are emerging as a highly promising class of candidate materials for X-ray imaging due to their excellent radioluminescence performance. Here, a red-emitting (Gua)<inf>2</inf>MnCl<inf>4</inf> (Gua = guanidine, CH<inf>6</inf>N<inf>3</inf><sup>+</sup>) single crystal scintillator grown by a simple solution-processing method is reported. (Gua)<inf>2</inf>MnCl<inf>4</inf> crystallizes into a zero-dimensional (0D) crystal structure consisting of trimeric [Mn<inf>3</inf>Cl<inf>12</inf>]<sup>6−</sup> units. It has a high PLQY of 76% and a large Stokes shift of 125 nm. (Gua)<inf>2</inf>MnCl<inf>4</inf> flexible scintillation screen demonstrates a decent X-ray detection limit of 145.3 nGy<inf>air</inf> s<sup>−1</sup> and a superior imaging resolution of 8 lp mm<sup>−1</sup>. These results highlight the potential of low-dimensional red-emitting Mn-based hybrids for X-ray imaging applications.

    DOI: 10.1002/adsr.202200083

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  100. Synthesis and Characterization of All-Inorganic Perovskite CsEuBr3 Single-Crystal Scintillator

    Wen X., Wang Q., Li W., Li Y., Cheng S., Wang J., Kurosawa S., Wu Y.

    Physica Status Solidi Rapid Research Letters   Vol. 17 ( 3 )   2023.3

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    Publisher:Physica Status Solidi Rapid Research Letters  

    All-inorganic halide perovskites appear as a promising class of scintillators for radiation detection applications due to their excellent optoelectronic properties. Herein, a self-activated perovskite CsEuBr<inf>3</inf> single crystal is developed as an efficient X- and γ-ray scintillator. Single crystals of CsEuBr<inf>3</inf> are grown by the Bridgman method. The phase structure, stability, photophysics properties, and scintillation performance of CsEuBr<inf>3</inf> single crystals are studied. Under X-ray irradiation, its emission peaks at 445 and 510 nm, associated with Eu<sup>2+</sup> 5d–4f and defect-related emission, respectively, are studied. Under <sup>137</sup>Cs gamma irradiation, it has a decent light yield of 22 000 ± 2000 photons MeV<sup>−1</sup> and an energy resolution of 6.2 ± 0.4% at 662 keV with a scintillation decay of 510 ns.

    DOI: 10.1002/pssr.202200341

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  101. Mechanisms of Sugar Aminotransferase-like Enzymes to Synthesize Stereoisomers of Non-proteinogenic Amino Acids in Natural Product Biosynthesis

    Kurosawa S., Okamura H., Yoshida A., Tomita T., Sone Y., Hasebe F., Shinada T., Takikawa H., Kosono S., Nishiyama M.

    ACS Chemical Biology   Vol. 18 ( 2 ) page: 385 - 395   2023.2

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    (2,6)-Diamino-(5,7)-dihydroxyheptanoic acid (DADH), a non-proteinogenic amino acid, is converted to 1-azabicyclo[3.1.0]hexane ring-containing amino acids that are subsequently incorporated into ficellomycin and vazabitide A. The present study revealed that the sugar aminotransferase-like enzymes Fic25 and Vzb9, with a high amino acid sequence identity (56%) to each other, synthesized stereoisomers of DADH with (6S) and (6R) configurations, respectively. The crystal structure of the Fic25 complex with a PLP-(6S)-N<sup>2</sup>-acetyl-DADH adduct indicated that Asn45 and Gln197 (Asn205 and Ala53 in Vzb9) were located at positions that affected the stereochemistry of DADH being synthesized. A modeling study suggested that amino acid substitutions between Fic25 and Vzb9 allowed the enzymes to bind to the substrate with almost 180° rotation in the C5-C7 portions of the DADH molecules, accompanied by a concomitant shift in their C1-C4 portions. In support of this result, the replacement of two corresponding residues in Fic25 and Vzb9 increased (6R) and (6S) stereoselectivities, respectively. The different stereochemistry at C6 of DADH resulted in a different stereochemistry/orientation of the aziridine portion of the 1-azabicyclo[3.1.0]hexane ring, which plays a crucial role in biological activity, between ficellomycin and vazabitide A. A phylogenic analysis suggested that Fic25 and Vzb9 evolved from sugar aminotransferases to produce unusual building blocks for expanding the structural diversity of secondary metabolites.

    DOI: 10.1021/acschembio.2c00823

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  102. Irradiation Tests of Silicon Photomultipliers for Use in Space

    Saito Y., Gunji S., Nakamori T., Mihara T., Yonetoku D., Sawano T., Kurosawa S., Kodaira S.

    IEEE Transactions on Nuclear Science   Vol. 70 ( 2 ) page: 150 - 155   2023.2

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    For using silicon photomultipliers (SiPMs) in space experiments, we conducted irradiation experiments of SiPMs with protons and iron ions. In particular, the relationship between leakage current and radiation dose was investigated under various irradiation conditions to determine techniques of mitigating damage caused by radiation. The leakage current was approximately proportional to dose; however, the proportionality constant did not significantly vary with irradiation conditions. The effects of annealing after irradiation tests indicated no substantial decrease in leakage current. Conversely, while the leakage current increased with dose, the SiPMs continued to operate even after 5 krad of irradiation, which corresponds to several years of radiation exposure in space at altitudes of 400-500 km. The results obtained from these irradiation tests are used to characterize a hard X-ray (>60 keV) detector for space-based applications. This detector couples an inorganic scintillator with a high light yield, such as CsI(Tl), to an SiPM.

    DOI: 10.1109/TNS.2022.3162788

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  103. Fabrication and scintillation properties of a flexible optical-guiding crystal scintillator Open Access

    Yajima R., Kamada K., Murakami R., Kutsuzawa N., Sasaki R., Yoshino M., Horiai T., Kim K.J., Kochurikhin V.V., Yamaji A., Kurosawa S., Yokota Y., Sato H., Toyoda S., Ohashi Y., Hanada T., Yoshikawa A.

    Applied Physics Express   Vol. 16 ( 2 )   2023.2

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    Publisher:Applied Physics Express  

    Scintillation properties of a flexible optical-guiding crystal scintillator with a thallium-doped CsI (Tl:CsI) crystal and borosilicate glass as the core and cladding, respectively, are reported. The as-fabricated optical-guiding crystal scintillator exhibits a light yield of 31,000 photons MeV<sup>−1</sup> under 662 keV γ-ray irradiation. The recrystallized sample is transparent and provides a higher light yield of 54,000 photons MeV<sup>-1</sup>, which is comparable to that of single-crystal Tl:CsI. The decay times are 400 ns (28%) and 1,350 ns (72%). This material can serve as a scintillator fiber with high sensitivity to γ- and X-rays, high light yield, and energy discrimination.

    DOI: 10.35848/1882-0786/acb891

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  104. Identifying the optimal conditioning intensity for stem cell transplantation in patients with myelodysplastic syndrome: a machine learning analysis

    Shimomura Y., Komukai S., Kitamura T., Sobue T., Kurosawa S., Doki N., Katayama Y., Ozawa Y., Matsuoka K.i., Tanaka T., Kako S., Sawa M., Kanda Y., Nakamae H., Nakazawa H., Ueda Y., Kanda J., Fukuda T., Atsuta Y., Ishiyama K.

    Bone Marrow Transplantation   Vol. 58 ( 2 ) page: 186 - 194   2023.2

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    A conditioning regimen is an essential prerequisite of allogeneic hematopoietic stem cell transplantation for patients with myelodysplastic syndrome (MDS). However, the optimal conditioning intensity for a patient may be difficult to establish. This study aimed to identify optimal conditioning intensity (reduced-intensity conditioning regimen [RIC] or myeloablative conditioning regimen [MAC]) for patients with MDS. Overall, 2567 patients with MDS who received their first HCT between 2009 and 2019 were retrospectively analyzed. They were divided into a training cohort and a validation cohort. Using a machine learning-based model, we developed a benefit score for RIC in the training cohort. The validation cohort was divided into a high-score and a low-score group, based on the median benefit score. The endpoint was progression-free survival (PFS). The benefit score for RIC was developed from nine baseline variables in the training cohort. In the validation cohort, the hazard ratios of the PFS in the RIC group compared to the MAC group were 0.65 (95% confidence interval [CI]: 0.48–0.90, P = 0.009) in the high-score group and 1.36 (95% CI: 1.06–1.75, P = 0.017) in the low-score group (P for interaction < 0.001). Machine-learning-based scoring can be useful for the identification of optimal conditioning regimens for patients with MDS.

    DOI: 10.1038/s41409-022-01871-8

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  105. Scintillation Properties of Red-emitting Li<sub>2</sub>Hf(I, Br)<sub>6</sub> Scintillators for Remote Real-time Neutron and Gamma-ray Monitors to Apply into Decommissioning of Nuclear Power Plants

    Fujiwara Chihaya, Kurosawa Shunsuke, Yamaji Akihiro

    Ionizing Radiation   Vol. 48 ( 2 ) page: 49 - 53   2023

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    Language:Japanese   Publisher:The Japan Society of Applied Physics  

    <p>  A radiation detector consisting of a scintillator and optical fiber has been proposed for the decommissioning of nuclear power plants to determine the dose rate in real-time. Inside the plant, gamma-ray and neutron emitting debris can remain, and the scintillator is required to have gamma-ray and neutron sensitivity. Moreover, red or near-infrared emission scintillators have the advantage to obtain higher sensitivity. In such demand, we have developed Li<sub>2</sub>Hf(Br, I)<sub>6</sub> scintillator with an emission wavelength of around 650 nm under visible light excitation and X-ray excitation. The light outputs of this material excited by thermal neutron and 662-keV gamma-ray excitation were evaluated to be 18,000 photons/(thermal neutron) and 16,000 photons/MeV, respectively. Therefore, we found this material has a potential to apply such a real-time monitor.</p>

    DOI: 10.11470/houshasen.48.2_49

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  106. Li+ incorporation and defect-creation processes imposed by X-ray and UV irradiation in Li-codoped Y3Al5O12:Ce scintillation crystals

    Laguta V., Buryi M., Babin V., Machek P., Zazubovich S., Bartosiewicz K., Kurosawa S., Yamaji A., Yoshikawa A., Uličná K., Chlan V., Štěpánková H., Nikl M.

    Journal of Materials Chemistry C   Vol. 11 ( 4 ) page: 1346 - 1359   2022.12

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    Cerium-doped rare-earth aluminum garnets represent an important class of scintillation and luminescent materials that are widely used in different technical fields, including medical imaging and solid-state white light sources, whose performances have to be further improved. One of the most effective tools for improving the light yield and timing characteristics of these materials is codoping with optically inactive ions. Herein, we investigate the Li<sup>+</sup> incorporation, as well as defect formation processes imposed by X-ray and UV irradiation, in Li<sup>+</sup>-codoped Y<inf>3</inf>Al<inf>5</inf>O<inf>12</inf>:Ce garnet scintillation crystals with the use of electron paramagnetic resonance (EPR), <sup>7</sup>Li nuclear magnetic resonance, and thermally stimulated luminescence (TSL) methods. The EPR study showed that the Ce<sup>3+</sup> content in the Li<sup>+</sup>-codoped crystals does not depend visibly on the Li concentration. The EPR spectra of X-ray-irradiated Li<sup>+</sup>-codoped YAG crystals revealed the presence of both isolated O<sup>−</sup> centers (a hole trapped at the oxygen ion) and O<sup>−</sup> centers stabilized by the neighboring Li<sup>+</sup> ions. The latter centers are responsible for the TSL peak at 320 K. Our data also show that at low Li concentrations in the melt, the Li<sup>+</sup> ions mainly substitute for Y<sup>3+</sup> ions. However, at high Li<sup>+</sup> ion concentrations (∼1 at% in melt), the Li<sup>+</sup> ions also substitute for Al<sup>3+</sup> ions. A strong increase in the oxygen vacancy concentration in the Li<sup>+</sup>-codoped crystals suggests that oxygen vacancies serve as effective compensators for the negative excess charge introduced into the crystal lattice by Li<sup>+</sup> ions, thus suppressing the Ce<sup>3+</sup> → Ce<sup>4+</sup> conversion process, which plays an important role in the acceleration of the scintillation decay. The obtained data suggest that the decrease in a slow component in the scintillation decay of the Li<sup>+</sup> ion-codoped crystals is caused, at least partly, by the redistribution of trapped charge carriers to more thermally stable centers.

    DOI: 10.1039/d2tc04520f

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  107. Development of Hf-Containing Halide and Ce-Doped Gd-Containing Oxide Scintillators Open Access

    Kurosawa Shunsuke

    RADIOISOTOPES   Vol. 71 ( 3 ) page: 255 - 264   2022.11

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    <p>High effective atomic-numbers (Z<sub>eff</sub>) and light outputs are required for gamma-ray scintillator, and we have developed novel materials such as Cs<sub>2</sub>HfI<sub>6</sub> (Z<sub>eff</sub>:58) and Ce<sup>3+</sup>-doped (Gd, La)<sub>2</sub>Si<sub>2</sub>O<sub>7</sub> (Z<sub>eff</sub>:56) with high light outputs of approximately 64,000 photons/MeV and 50,000–60,000 photons/MeV, respectively.</p>

    DOI: 10.3769/radioisotopes.71.255

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  108. Water vapor plasma-assisted low-temperature bonding of cyclo-olefin polymer for microchannel with integrated leak detector

    Tsukamoto M., Terai H., Tsumaya M., Kurosawa S., Tsuji O., Sato M., Inoue Y., Kawano K., Matsushima T., Tsuchiya T.

    MRS Advances   Vol. 7 ( 31 ) page: 905 - 910   2022.11

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    Cyclo-olefin polymer (COP) has attracted much attention as substrate material for microfluidic devices because of its excellent optical properties, processability, and lower cost than glass materials. We have previously reported surface modification using water vapor plasma as a method of bonding COP substrates at low temperature. In this study, water feeding and bonding strength of this method was investigated using a microfluidic device equipped with fluid leak detectors. Water was fed by capillary flow in microchannels bonded at room temperature. Water leak was visually detected by the detectors, using an optical microscope. The withstanding pressure was 200 kPa or higher.

    DOI: 10.1557/s43580-022-00346-8

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  109. Resignation and return to work in patients receiving allogeneic hematopoietic cell transplantation close up

    Kurosawa S., Yamaguchi T., Mori A., Matsuura T., Mori T., Tanaka M., Kondo T., Umemoto Y., Goto H., Yoshioka S., Machida S., Sato T., Katayama Y., Kato S., Shono K., Mizuno I., Fujiwara S.i., Kohno A., Takahashi M., Fukuda T.

    Journal of Cancer Survivorship   Vol. 16 ( 5 ) page: 1004 - 1015   2022.10

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    Purpose: To characterize the issues regarding work and employment specific to allogeneic hematopoietic cell transplantation (allo-HCT) survivors, we conducted a nationwide cross-sectional questionnaire survey. Methods: We targeted allo-HCT survivors employed at diagnosis, aged 20–64 at survey, and survived ≥2 years without relapse. The questionnaire included the timing of and reasons for resignation (termination of employment contract), and patient-related, HCT-related, work-related, and HCT center-related factors. Results: A total of 1048 eligible participants were included in the analysis (response rate, 60%). The median time after allo-HCT was 5 years (range, 2–30) at the time of survey. After diagnosis, 41% of participants resigned from work throughout the course of treatment. The most frequent timing of the first resignation was “after discharge post-HCT” (46%), followed by “from diagnosis to initial treatment” (27%). Factors significantly associated with resignation included female gender, older age, and part-time employment. Favorable factors included the presence of occupational health staff at the workplace, employment of ≥10 years, and self-employed/freelance. After resignation, the overall incidence of return to work with some accommodations was 76% at 5 years after HCT, but it was 52% without any accommodation. Conclusions: Overall, the rate of resignation was 41%, and the most frequent timing of resignation was after discharge post-HCT, accounting for approximately half of the resignations (46%). Workplace accommodations increased the rate of return to work from 52% to 76%. Implications for Cancer survivors: Early detection of employment-related concerns and support throughout the treatment process are necessary for patients receiving allo-HCT.

    DOI: 10.1007/s11764-021-01092-w

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  110. Molecular Basis for Enzymatic Aziridine Formation via Sulfate Elimination

    Kurosawa S., Hasebe F., Okamura H., Yoshida A., Matsuda K., Sone Y., Tomita T., Shinada T., Takikawa H., Kuzuyama T., Kosono S., Nishiyama M.

    Journal of the American Chemical Society   Vol. 144 ( 35 ) page: 16164 - 16170   2022.9

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    Natural products containing an aziridine ring, such as mitomycin C and azinomycin B, exhibit antitumor activities by alkylating DNA via their aziridine rings; however, the biosynthetic mechanisms underlying the formation of these rings have not yet been elucidated. We herein investigated the biosynthesis of vazabitide A, the structure of which is similar to that of azinomycin B, and demonstrated that Vzb10/11, with no similarities to known enzymes, catalyzed the formation of the aziridine ring via sulfate elimination. To elucidate the detailed reaction mechanism, crystallization of Vzb10/11 and the homologous enzyme, AziU3/U2, in the biosynthesis of azinomycin B was attempted, and the structure of AziU3/U2, which had a new protein fold overall, was successfully determined. The structural analysis revealed that these enzymes adjusted the dihedral angle between the amino group and the adjacent sulfate group of the substrate to almost 180° and enhanced the nucleophilicity of the C6-amino group temporarily, facilitating the S<inf>N</inf>2-like reaction to form the aziridine ring. The present study reports for the first time the molecular basis for aziridine ring formation.

    DOI: 10.1021/jacs.2c07243

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  111. Temperature dependence of radio- and photoluminescence and scintillation properties of Y0.6Gd2.4Al2Ga3O12:Ce,Mg single crystal

    Chewpraditkul W., Pattanaboonmee N., Chewpraditkul W., Kim K.J., Yoshikawa A., Kamada K., Kurosawa S., Beitlerova A., Kucerkova R., Babin V., Nikl M.

    Optical Materials   Vol. 131   2022.9

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    Mg<sup>2+</sup>-codoped Y<inf>0.6</inf>Gd<inf>2.4</inf>Al<inf>2</inf>Ga<inf>3</inf>O<inf>12</inf>:Ce (YGAGG:Ce,Mg) single crystal was grown by the Czochralski method and its luminescence and scintillation properties were investigated. Temperature dependence of radioluminescence (RL) yield and photoluminescence (PL) decay time was measured, and activation energy of thermal ionization process was determined from temperature-dependent PL decay time measurement. YGAGG:Ce,Mg exhibited high X-ray excited RL yield almost 5 times higher than BGO reference scintillator. Its light yield of 41,500 ph/MeV and scintillation decay times of 12 ns (2%) + 52 ns (65%) + 207 ns (33%) were measured under excitation with 662 keV γ rays from <sup>137</sup>Cs source. Afterglow and thermally stimulated luminescence characteristics are also investigated.

    DOI: 10.1016/j.optmat.2022.112662

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  112. Growth of thallium-doped CsI/CsCl/KCl eutectics and their scintillation properties Open Access

    Takizawa Y., Kamada K., Yoshino M., Kim K.J., Kutsuzawa N., Yamaji A., Kurosawa S., Yokota Y., Sato H., Toyoda S., Ohashi Y., Hanada T., Kochurikhin V., Yoshikawa A.

    Optical Materials X   Vol. 15   2022.8

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    In this study, Tl:CsI/CsCl/KCl ternary eutectic scintillators were grown using the vertical Bridgman–Stockbarger method by unidirectional solidification. The CsI and KCl phases were elongated along the growth direction, based on backscattered electron imaging (BEI) observations. The Tl:CsI scintillator phase grew as a matrix, which can be used to create optical waveguides for scintillation light. The expected Tl<sup>+</sup> emission peak was observed at 550 nm under X-ray excitation. This emission was attributed to the self-trapped excitons perturbed by TI<sup>+</sup> in Tl:CsI. The decay time of the Tl:CsI/CsCl/KCl eutectic was 285 ns, and its light output was estimated to be 10,800 photons/MeV.

    DOI: 10.1016/j.omx.2022.100159

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  113. Influence of reflected waves at the bonded boundary in double-layered thickness-shear resonator using α-quartz Open Access

    Noguchi T., Ohashi Y., Omote M., Yokota Y., Kurosawa S., Kamada K., Sato H., Toyoda S., Yoshino M., Yamaji A., Yoshikawa A.

    Japanese Journal of Applied Physics   Vol. 61 ( SG )   2022.7

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    The influence of the reflected waves at the bonding boundary on the resonance waveform and temperature characteristics was investigated using α-quartz (QZ). The double-layered resonator specimen was fabricated using 129.55°Y-and 0°Y-cut QZ substrates with the thickness ratio x = 0.520. The temperature characteristic of the 1st and 2nd resonance modes at the range from 100 °C to 300 °C was deviated from the calculated values estimated by the equations considering thickness ratio and electric flux density ratio proposed in the previous work. Considering the phase matching conditions, it was clarified that the reflected waves at the bonding boundary are in phase in the lower acoustic impedance substrate and out of phase in the other substrate for the 1st mode, so the temperature characteristics are mainly dominated by that of the lower acoustic impedance substrate. In contrast, these relationships are reversed for the 2nd mode.

    DOI: 10.35848/1347-4065/ac4a03

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  114. Allogeneic Hematopoietic Stem Cell Transplantation for Adult Philadelphia Chromosome-Negative B-Cell Acute Lymphoblastic Leukemia in Second Complete Remission

    Kaito S., Kurosawa S., Najima Y., Sakaida E., Shingai N., Fukuda T., Tachibana T., Uchida N., Ozawa Y., Sawa M., Nakazawa H., Ota S., Kato J., Nakamae H., Katayama Y., Eto T., Tanaka J., Kanda Y., Atsuta Y., Arai Y., Kako S.

    Transplantation and Cellular Therapy   Vol. 28 ( 6 ) page: 326 - 326.e10   2022.6

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    Even in the era of high-intensity chemotherapy, disease recurrence remains a major cause of treatment failure in adult patients with Philadelphia chromosome-negative B-cell acute lymphoblastic leukemia (Ph-negative B-ALL). For patients who achieved second complete remission (CR2) with salvage chemotherapy, allogeneic hematopoietic stem cell transplantation (allo-HSCT) could be the best curative treatment. However, limited data are available on the outcomes of allo-HSCT for adult Ph-negative B-ALL in CR2 in the high-intensity chemotherapy era. We evaluated the transplantation outcomes of adult patients with Ph-negative B-ALL in CR2 compared with those in CR1. We also clarified the prognostic factors among adult allo-HSCT recipients with Ph-negative B-ALL in CR2. We conducted a nationwide retrospective study using the data form Japanese transplant registry database. Patients aged ≥16 years and underwent their first allo-HSCT between 2003 and 2017 were included. The 3-year overall survival (OS) rate of the patients in CR2 (n = 382) was significantly lower than that in first complete remission (n = 1375) (51.8% versus 68.1%; P < .001), accompanied by a higher relapse rate (34.2% versus 17.6% at 3 years; P < .001). In a multivariate analysis among CR2 patients, time from diagnosis to allo-HSCT (≤2 years) was a significant factor for OS (hazard ratio [HR] 1.87; P < .001) and relapse (HR = 1.88; P < .001), whereas age at allo-HSCT (≥30 years) was a significant factor for OS (HR = 2.10, P < .001) and nonrelapse mortality (HR = 2.68; P < .001). By assigning a score of 1 to each factor, the 3-year OS rate of CR2 patients significantly stratified: 70.7% in patients with score 0, 56.4% with score 1, and 28.4% with score 2 (P < .001). The survival outcomes of allo-HSCT in adult Ph-negative B-ALL patients in CR2 were inferior to those in CR1 in the high-intensity chemotherapy era, mainly because of the higher relapse rate. Among the CR2 patients, the short time between diagnosis and allo-HSCT was a significant risk factor for disease recurrence and overall mortality. Better disease control with novel treatment strategies may be needed for early relapse. In addition, the nonrelapse mortality rate in patients over 30 years of age was particularly high among CR2 patients, suggesting the need for improved supportive care for these patients. Further studies are warranted on the outcomes of allo-HSCT after achieving CR2 with novel drugs, such as inotuzumab ozogamicin and blinatumomab.

    DOI: 10.1016/j.jtct.2022.03.017

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  115. Myeloablative Versus Reduced-Intensity Conditioning With Fludarabine/Busulfan for Myelodysplastic Syndrome: A Propensity Score-Matched Analysis

    Kurosawa S., Shimomura Y., Itonaga H., Najima Y., Kobayashi T., Ozawa Y., Kanda Y., Kako S., Kawakita T., Matsuoka K.i., Maruyama Y., Ota S., Nakazawa H., Imada K., Kimura T., Kanda J., Fukuda T., Atsuta Y., Ishiyama K.

    Transplantation and Cellular Therapy   Vol. 28 ( 6 ) page: 323 - 323.e9   2022.6

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    There are limited data comparing myeloablative conditioning with fludarabine/busulfan (Flu/Bu4) and reduced-intensity conditioning with fludarabine/busulfan (Flu/Bu2) in patients with myelodysplastic syndrome (MDS) undergoing allogeneic hematopoietic stem cell transplantation (allo-HSCT). We retrospectively analyzed nationwide registry data and compared the outcomes of adult patients with MDS receiving Flu/Bu4 and Flu/Bu2 by propensity score (PS) matching. Patients who met the following criteria were eligible for enrollment: (1) age ≥16 years; (2) diagnosis of de novo MDS; (3) first allo-HSCT between 2006 and 2018; (4) related bone marrow transplantation (BMT) or peripheral blood stem cell transplantation from an HLA-matched donor, unrelated BMT from an HLA-matched or HLA-1 allele–mismatched donor, or unrelated cord blood transplantation; and (5) receiving Flu/Bu4 or Flu/Bu2 as a conditioning regimen. Flu/Bu4 comprised intravenous busulfan (total dose, 12.8 mg/kg) combined with fludarabine (total dose, 125–180 mg/m<sup>2</sup>). Flu/Bu2 comprised intravenous busulfan (total dose, 6.4 mg/kg) combined with the same dose of fludarabine. To minimize selection bias and confounding factors, we performed a propensity score (PS)-matched analysis. The primary endpoint was overall survival (OS) after allo-HSCT. A total of 3386 patients with de novo MDS underwent their first allo-HSCT between 2006 and 2018. Among them, 202 patients were assigned each to the Flu/Bu4 and Flu/Bu2 groups after PS-matched analysis. The median age was 61 (interquartile, 57-65) years. The 3-year OS rates were 44.8% (95% confidence interval [CI], 37.1–52.1%) and 46.9% (95% CI, 39.2–54.2%) in the Flu/Bu4 and Flu/Bu2 groups, respectively (P = .67). The 3-year rates of graft-versus-host disease (GVHD)–free survival, relapse-free survival (GRFS) were 28.8% (95% CI, 22.2–35.7%) and 33.0% (95% CI, 26.2–40.0%), respectively (P = .36). The 3-year cumulative incidence rates of relapse were 28.9% (95% CI, 22.6–35.6%) and 30.0% (95% CI, 23.6–36.6%), respectively (P = .47). The 3-year cumulative incidence rates of non-relapse mortality (NRM) were 28.2% (95% CI, 21.7–35.0%) and 27.1% (95% CI, 20.6–33.9%), respectively (P = .60). The 100-day cumulative incidence rate of grade II–IV acute GVHD was significantly higher in the Flu/Bu4 group than in the Flu/Bu2 group (41.7% [95% CI, 34.8%–48.4%] versus 29.3% [95% CI, 23.2%-35.7%], P = 0.012). To identify patients who had more favorable outcomes with 1 of the 2 regimens, we compared the outcomes between the 2 groups after stratifying by age, hematopoietic cell transplantation-comorbidity index, cytogenetic risk, disease status at allo-HSCT, stem cell source, and donor type. OS, GRFS, relapse, and NRM did not differ between the 2 groups in any subgroup analyses. There were no significant interactions between the choice of conditioning regimens and any other factors. There are no differences in survival between Flu/Bu4 and Flu/Bu2, although our study population was highly selected by PS matching. Data from more patients and prospective studies are needed to determine the optimal intensity of conditioning regimens in patients with MDS.

    DOI: 10.1016/j.jtct.2022.03.011

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  116. First Observation of the MeV Gamma-Ray Universe with Bijective Imaging Spectroscopy Using the Electron-tracking Compton Telescope on Board SMILE-2+ Open Access

    Takada Atsushi, Takemura Taito, Yoshikawa Kei, Mizumura Yoshitaka, Kubo Hidetoshi, Kurosawa Shunsuke, Ikeda Tomonori, Hamaguchi Kenji, Sawano Tatsuya, Saito Kaname, Nakamura Yuta, Miuchi Kentaro, Abe Mitsuru, Tanimori Toru, Onozaka Ken

    The Astrophysical Journal   Vol. 930 ( 1 ) page: 6   2022.5

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    MeV gamma-rays provide a unique window for the direct measurement of line emissions from radioisotopes, but observations have made little significant progress since COMPTEL on board the Compton Gamma-ray Observatory (CGRO). To observe celestial objects in this band, we are developing an electron-tracking Compton camera (ETCC) that realizes both bijective imaging spectroscopy and efficient background reduction gleaned from the recoil-electron track information. The energy spectrum of the observation target can then be obtained by a simple ON–OFF method using a correctly defined point-spread function on the celestial sphere. The performance of celestial object observations was validated on the second balloon SMILE-2+ , on which an ETCC with a gaseous electron tracker was installed that had a volume of 30 × 30 × 30 cm³. Gamma-rays from the Crab Nebula were detected with a significance of 4.0σ in the energy range 0.15–2.1 MeV with a live time of 5.1 hr, as expected before launch. Additionally, the light curve clarified an enhancement of gamma-ray events generated in the Galactic center region, indicating that a significant proportion of the final remaining events are cosmic gamma-rays. Independently, the observed intensity and time variation were consistent with the prelaunch estimates except in the Galactic center region. The estimates were based on the total background of extragalactic diffuse, atmospheric, and instrumental gamma-rays after accounting for the variations in the atmospheric depth and rigidity during the level flight. The Crab results and light curve strongly support our understanding of both the detection sensitivity and the background in real observations. This work promises significant advances in MeV gamma-ray astronomy.

    DOI: 10.3847/1538-4357/ac6103

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  117. Growth and scintillation properties of LiBr/CeBr3eutectic scintillator for neutron detection Open Access

    Yajima R., Kamada K., Takizawa Y., Yoshino M., Kim K.J., Kochurikhin V.V., Yamaji A., Kurosawa S., Yokota Y., Sato H., Toyoda S., Ohashi Y., Hanada T., Yoshikawa A.

    Japanese Journal of Applied Physics   Vol. 61 ( SC )   2022.5

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    A 6LiBr/CeBr3 eutectic thermal-neutron scintillator, with a high 6Li concentration, was developed using the vertical Bridgman method. The grown eutectic contained an 6Li molar ratio of 35%, which is higher than those of the commercial neutron scintillators such as Ce:LiCaAlF6 and Ce:Cs2LiYCl6. Furthermore, it showed optical transparency and a lamellar eutectic structure elongating along the growth direction. The synthesized eutectic showed emission peaks at 360 and 380 nm, originating from the Ce3+ 5d-4f transition in the CeBr3 scintillation phase. The scintillation performance of 6LiBr/CeBr3 was evaluated under X-ray, γ-ray, and neutron irradiation to corroborate its neutron detection potential.

    DOI: 10.35848/1347-4065/ac4076

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  118. Growth of Zn3Ta2O8 crystal scintillator by a novel melt growth technique named shielded arc melting method Open Access

    Yajima R., Kamada K., Takizawa Y., Yoshino M., Murakami R., Kim K.J., Horiai T., Yamaji A., Kurosawa S., Yokota Y., Sato H., Toyoda S., Ohashi Y., Hanada T., Yoshikawa A.

    Optical Materials X   Vol. 14   2022.5

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    In this study, it was demonstrated that Zn<inf>3</inf>Ta<inf>2</inf>O<inf>8</inf> crystals containing zinc oxide with high vapor pressure can grow in melt by the shielded arc melting method. The radiation response characteristics of the crystals were evaluated. The grown crystals showed an emission peak at 410 nm, ascribed to self-trapped excitation, Ta<sup>4+</sup>–O<sup>2−</sup>. The full width at half maximum of the X-ray rocking curve was 655 arcsec. The light output under 662 keV gamma-ray irradiation of Zn<inf>3</inf>Ta<inf>2</inf>O<inf>8</inf> was approximately 4,700 photons/MeV. The decay time was 17.3 μs? Thus, the shielded arc melting method was shown to be a quick and economic growth technique for the survey of new scintillator materials containing high-vapor-pressure starting components.

    DOI: 10.1016/j.omx.2022.100149

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  119. Large size growth of terbium doped BaCl2/NaCl/KCl eutectic for radiation imaging

    Takizawa Y., Kamada K., Kim K.J., Yoshino M., Yamaji A., Kurosawa S., Yokota Y., Sato H., Toyoda S., Ohashi Y., Hanada T., Kochurikhin V.V., Yoshikawa A.

    Japanese Journal of Applied Physics   Vol. 61 ( SC )   2022.5

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    In this study, a large-size eutectic scintillator of Tb-doped BaCl2/NaCl/KCl was grown using the Czochralski (Cz) and halide vertical Bridgman methods (H-VB). The suitability of these two growth methods for growing the eutectic was compared. Finally, 1 inch diameter eutectic bulks were obtained using the H-VB method. The Tb3+-derived strongest intensity peak at approximately 550 nm was observed by X-ray irradiation. An approximately 3 × 3 mm transparent eutectic wafer was cut and polished from the grown eutectic bulk. An imaging test using α-ray was performed using the grown eutectic, a fiber optic plate, and an electron-multiplying CCD camera. The resolution performance for radiation-imaging applications was evaluated.

    DOI: 10.35848/1347-4065/ac3b23

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  120. Growth and scintillation properties of directionally solidified Ce:LaCl3/AECl2 (AE = Mg, Ca, Sr) eutectic Scintillators

    Kim K.J., Kamada K., Murakami R., Yoshino M., Kurosawa S., Yamaji A., Shoji Y., Kochurikhin V.V., Sato H., Toyoda S., Ohashi Y., Hanada T., Yokota Y., Yoshikawa A.

    Journal of Crystal Growth   Vol. 584   2022.4

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    Ce-doped LaCl<inf>3</inf>/AECl<inf>2</inf> (AE = Mg, Ca, Sr) system eutectics were explored. Ce-doped LaCl<inf>3</inf>/ AECl<inf>2</inf> (AE = Mg, Ca, Sr) eutectics were grown using the Bridgman–Stockbarger method in quartz ampoules. In the case of AE = Mg, Ca, eutectics with submicron-diameter phase-separated scintillator fibers (PSSFs) structure were observed. In the case of AE = Sr sample, a solid solution of La<inf>0.708</inf>Sr<inf>0.292</inf>Cl<inf>2.708</inf> was observed. The plate sample from the grown eutectics has some transparency. The grown eutectic structure showed a mixture of rods and plates shape. This mixed structure was aligned with a length of around 100–400 μm. The Ce:LaCl<inf>3</inf>/CaCl<inf>2</inf> eutectic showed 345 nm emission ascribed to Ce<sup>3+</sup> 4f-5d transition under X-ray excitation. The Ce:LaCl<inf>3</inf>/CaCl<inf>2</inf> sample resulted in the highest light output of 9,000 photon/MeV, which is comparable to the previously reported eutectic scintillator Ce:GdAlO<inf>3</inf>/α-Al<inf>2</inf>O<inf>3</inf>, 9500 photon/MeV. Scintillation decay time of the Ce:LaCl<inf>3</inf>/CaCl<inf>2</inf> sample under 662 keV gamma-ray excitation was 26.8 ns (26%) and 282 ns (74%).

    DOI: 10.1016/j.jcrysgro.2022.126549

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  121. A study of Mg2+ ions effect on atoms segregation, defects formation, luminescence and scintillation properties in Ce3+ doped Gd3Al2Ga3O12 single crystals

    Bartosiewicz K., Markovskyi A., Horiai T., Szymański D., Kurosawa S., Yamaji A., Yoshikawa A., Zorenko Y.

    Journal of Alloys and Compounds   Vol. 905   2022.4

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    The undoped, Mg<sup>2+</sup> doped, Ce<sup>3+</sup> doped as well as Mg<sup>2+</sup>:Ce<sup>3+</sup> codoped Gd<inf>3</inf>Al<inf>2</inf>Ga<inf>3</inf>O<inf>12</inf> crystals were grown from the melt by the micro-pulling down method. Ce<sup>3+</sup> and Mg<sup>2+</sup> ions were codoped in a wide concentration range. A study of Mg<sup>2+</sup> ion concentration effect on the luminescence and scintillation properties as well as segregation of atoms and defects creation processes were carried out. Mg<sup>2+</sup> doping in Gd<inf>3</inf>Al<inf>2</inf>Ga<inf>3</inf>O<inf>12</inf> led to the creation of O<inf>O</inf><sup>•</sup> defects localized next to Mg<sup>2+</sup> sites due to charge imbalance compensation. Consequently, neutral (Mg<inf>Ga/Al/Gd</inf>O<inf>O</inf>)<sup>x</sup> defects were formed. In Ce<sup>3+</sup> doped crystals, Mg<sup>2+</sup> codoping changed the valence state from Ce<sup>3+</sup> to Ce<sup>4+</sup> to maintain charge neutrality. Hence, additional neutral (Ce<inf>Gd</inf><sup>•</sup>-Mg<inf>Ga/Al/Gd</inf>′)<sup>x</sup> and (Ce<inf>Gd</inf>-Mg<inf>Ga/Al/Gd</inf>O<inf>O</inf>)<sup>x</sup> defects appeared. Moreover, Mg<sup>2+</sup> induced charge imbalance in GAGG crystal might also be compensated by the formation of oxygen vacancies (V<inf>O</inf><sup>••</sup>). The Mg<sup>2+</sup> ions imposed defects deteriorated the segregation of atoms. Accordingly the radial inhomogeneity of the crystals was diminished. The presence of stable Ce<sup>4+</sup> and defects imposed by Mg<sup>2+</sup> ions codoping were proved by absorption, photoluminescence, and scintillation decay time analysis. Hence, Mg<sup>2+</sup> codoping resulted in quenching of the Ce<sup>3+</sup> luminescence, acceleration of scintillation response, reduction of light yield, and thermally stimulated luminescence. The mechanism explaining a strong luminescence quenching with increasing Mg<sup>2+</sup> ions concentration was proposed.

    DOI: 10.1016/j.jallcom.2022.164154

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  122. Crystal growth of La2Hf2O7 by micro-pulling-down method using W crucible

    Suda T., Yokota Y., Horiai T., Yamaji A., Yoshino M., Hanada T., Sato H., Toyoda S., Ohashi Y., Kurosawa S., Kamada K., Yoshikawa A.

    Journal of Crystal Growth   Vol. 583   2022.4

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    La<inf>2</inf>Hf<inf>2</inf>O<inf>7</inf> crystals with a melting point of ∼2418 °C were grown by the micro-pulling-down method using a W crucible and deoxygenated ZrO<inf>2</inf> insulators. A La<inf>2</inf>Hf<inf>2</inf>O<inf>7</inf> crystal grown at a rate of 0.07 mm/min (LHO[0.07 mm/min]) showed a high transparency without any visible cracks and inclusions, while a La<inf>2</inf>Hf<inf>2</inf>O<inf>7</inf> crystal grown at a rate of 2.00 mm/min had some cracks. The LHO[0.07 mm/min] crystal had a transmittance of over 70% in the wavelength range of 450–800 nm. The X-ray rocking curve of the LHO[0.07 mm/min] crystal showed a symmetric sharp peak with a full width at half maximum of 138 arcsec. The Laue image revealed that the grown crystals were single crystals.

    DOI: 10.1016/j.jcrysgro.2022.126547

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  123. Growth and scintillation properties of Ce doped 6LiBr/LaBr3 eutectic scintillator for neutron detection

    Takizawa Y., Kamada K., Yoshino M., Kim K.J., Yamaji A., Kurosawa S., Yokota Y., Sato H., Toyoda S., Ohashi Y., Hanada T., Kochurikhin V.V., Yoshikawa A.

    Nuclear Instruments and Methods in Physics Research Section A Accelerators Spectrometers Detectors and Associated Equipment   Vol. 1028   2022.4

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    In this study, Ce:<sup>6</sup>LiBr/LaBr<inf>3</inf> eutectic with a high Li concentration was developed as a novel thermal neutron scintillator. Ce served as an activator for the LaBr<inf>3</inf> phase, and Ce:<sup>6</sup>LiBr/LaBr<inf>3</inf> eutectics were grown via the vertical Bridgman method in quartz ampoules (inner diameter = 4 mm). In the eutectic, the <sup>6</sup>LiBr phase worked as the neutron capture phase by the <sup>6</sup>Li (n, a) <sup>3</sup>H reaction, and Ce:LaBr<inf>3</inf> worked as the scintillator phase. The Ce:<sup>6</sup>LiBr/LaBr<inf>3</inf> eutectic exhibited a lamellar eutectic structure and optical transparency, as well as 350 and 380 nm emission due to Ce<sup>3+</sup> 5d-4f transition. The light yield under neutrons excitation was estimated to be 74000 photons/neutron. The scintillation decay time was 18.7 ns.

    DOI: 10.1016/j.nima.2022.166384

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  124. Crystal growth and luminescence properties of phenanthrene for neutron detection

    Yamaji A., Kurosawa S., Yoshikawa A.

    Journal of Crystal Growth   Vol. 581   2022.3

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    Phenanthrene crystals were grown by the self-seeding vertical Bridgman technique as a neutron scintillation material and their luminescence properties were evaluated. As-grown crystals had no secondary phases from the results of the powder X-ray Diffraction and Fourier transform infrared spectrometer measurements. The radioluminescence emission spectrum had a peak at 408 nm and its profile was similar to that of the photoluminescence emission spectrum. The relative light yield under 5.5-MeV alpha-ray was 1.15 times higher than that of lithium glass GS-20. The light yield of phenanthrene under 662 keV gamma-ray is estimated to be 38 ± 2% of NaI:Tl. The scintillation decay time under neutron excitation was estimated to be 7.30 ± 0.14 ns.

    DOI: 10.1016/j.jcrysgro.2021.126494

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  125. Feasibility and usefulness of recommended screenings at long-term follow-up clinics for hematopoietic cell transplant survivors

    Kurosawa S., Yamaguchi T., Mori A., Tsukagoshi M., Okuda I., Ikeda M., Ueno T., Saito Y., Aihara Y., Matsuba Y., Fuji S., Yamashita T., Ogawa C., Ito A., Tanaka T., Inamoto Y., Kim S.W., Fukuda T.

    Supportive Care in Cancer   Vol. 30 ( 3 ) page: 2767 - 2776   2022.3

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    Purpose: Advances in allogeneic hematopoietic cell transplantation (allo-HCT) have resulted in a growing number of transplant survivors; however, long-term survivors are at risk of developing late complications, and published guidelines recommend screening of this population. We conducted a single-center prospective study to evaluate the adherence to and usefulness of recommended screenings at a long-term follow-up (LTFU) clinic. Methods: We included consecutive patients who received allo-HCT at our center from 2014, as well as post-HCT patients visiting our outpatient clinic. Visits and screenings were planned at 3 months, 6 months, and 1 year after allo-HCT, and annually thereafter. Outcomes were reported by physicians including the incidence of findings at each screening that led to interventions. Results: Among the 216 participants, 95% visited the LTFU clinic, and 94% completed planned screenings. However, the rate of secondary cancer screenings targeting high-risk subjects was lower (38% to 68%). The overall percentage of screening results leading to interventions was 4.5%, with higher percentages (> 10%) for bone density testing, ophthalmological examinations, dental assessment, upper gastrointestinal endoscopy, and colonoscopy, with two patients diagnosed with secondary cancers. Conclusions: Although the overall screening rate was high, it should be possible to improve the detection rate of late complications by decreasing screening failures, especially the screening for secondary cancers limited for high-risk survivors. A nationwide effort to educate HCT survivors and health practitioners using standardized nationwide LTFU tools may be effective, along with the development of institutional, local, and nationwide networks to maintain effective follow-up systems.

    DOI: 10.1007/s00520-021-06698-5

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  126. Specifics of Spectroscopic Features of Yb3+-Doped Lu2O3 Laser Transparent Ceramics

    Boulon G., Guyot Y., Guzik M., Toci G., Pirri A., Patrizi B., Vannini M., Yoshikawa A., Kurosawa S., Ikesue A.

    Physica Status Solidi B Basic Research   Vol. 259 ( 3 )   2022.3

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    Some specifics of spectroscopic and laser properties of Yb<sup>3+</sup> dopant are shown in Yb<sup>3+</sup>-doped Lu<inf>2</inf>O<inf>3</inf> cubic sesquioxide transparent ceramics, a very important laser material, fabricated by Akio Ikesue using the method based on solid-state mixing of oxides and sintering by hot isostatic pressing (HIP) technique. For instance, despite the simplicity of Yb<sup>3+</sup> electronic configuration, it is emphasized that a lot of precautions need to be considered during the evaluation and the assignment of Yb<sup>3+</sup> experimental data in this sample and also in all Yb<sup>3+</sup>-doped materials. First, we focus our discussion on the position of <sup>2</sup>F<inf>7/2</inf> (ground state) and <sup>2</sup>F<inf>5/2</inf> (excited state) Stark levels of the most populated C<inf>2</inf> symmetry site, and on the presence of the magnetic dipole transitions from the C<inf>3i</inf> (S<inf>6</inf>) inversion symmetry site. Then, we point out the strong influence of the self-trapping and the self-quenching processes on the measurement of the <sup>2</sup>F<inf>5/2</inf>(5) upper level decay time which needs the pin-hole method. Finally, we comment on the spectrum of the tuneable laser emission behaviour near 1033 nm with respect to the losses of the laser cavity without the laser emission near 1080 nm, as observed in other laser materials.

    DOI: 10.1002/pssb.202100521

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  127. Direct measurement of topological information for Cherenkov lights using HUNI-ZICOS detector Open Access

    Fukuda Y., Moriyama S., Hiraide K., Ogawa I., Gunji T., Hayami R., Tsukada S., Kurosawa S.

    Journal of Physics Conference Series   Vol. 2156 ( 1 )   2022.2

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    The topological information of Cherenkov light emitted from low energy electron was directly measured by HUNI-ZICOS detector. A 1.484 MeV electron with fixed direction to the center of hemispherical surface of the detector was generated by Compton back scattering with 100 degree from <sup>88</sup>Y 1.836 MeV gamma. The observed averaged angle of Cherenkov light emitted from this electron was clustered around 40 degree assuming the vertex position to be at the center of truncated icosahedron photomultiplier jig. It was not Cherenkov angle around 47 degree as obtained by old simulation and the vertex to be the center of light yield for hitted photomultiplier. According to the HUNI-ZICOS simulation, the averaged angle of Cherenkov light was also clustered around 40 degree. On the other hands, the simulated averaged angle of scintillation was clustered around 49 degree, which is consistent with the averaged value of angle between the direction to center of hemisphere surface and each photomultiplier from the center of the jig. The obtained hitmap seemed to have same non flat structure as that of simulation due to Cherenkov ring. This is an evidence that Cherenkov lights emitted from 1.484 MeV electron should really have their topology. Therefore, we concluded that we will be able to reduce <sup>208</sup>Tl background using the averaged angle for <sup>96</sup>Zr neutrinoless double beta decay search.

    DOI: 10.1088/1742-6596/2156/1/012116

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  128. Growth of Tb-doped BaCl2/NaCl/KCl ternary eutectic and its luminescence properties

    Takizawa Y., Kamada K., Jin Kim K., Yoshino M., Yamaji A., Kurosawa S., Yokota Y., Sato H., Toyoda S., Ohashi Y., Hanada T., Kochurikhin V.V., Yoshikawa A.

    Journal of Crystal Growth   Vol. 580   2022.2

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    In this study, Tb:BaCl<inf>2</inf> and NaCl/KCl ternary eutectics were grown using quartz ampoules via the vertical Bridgman–Stockbarger method. Each crystal phase had a polygonal columnar shape with a length of 300 µm along the growth direction. The Tb:BaCl<inf>2</inf> scintillator phase grew in the columnar phase. The BaCl<inf>2</inf> scintillator phase is expected to make optical waveguides of the scintillation light. The expected Tb<sup>3+</sup> emission peak was observed at approximately 360–630 nm under X-ray irradiation. This emission is mainly attributed to the Tb<sup>3+5</sup>D<inf>4</inf>→<sup>7</sup>F<inf>6</inf>, <sup>7</sup>F<inf>6</inf>, <sup>7</sup>F<inf>5</inf>, <sup>7</sup>F<inf>4</inf>, and <sup>7</sup>F<inf>3</inf> transitions and BaCl<inf>2</inf> host emission transition. The photoluminescence decay times of the Tb:BaCl<inf>2</inf>/NaCl/KCl eutectics was 0.49 ms (7.5%) and 6.64 ms (92.5%).

    DOI: 10.1016/j.jcrysgro.2021.126467

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  129. Temperature Characteristics of Resonance Frequency for Double-Layered Thickness-Shear Resonator

    Ohashi Y., Owada Y., Yokota Y., Yoshikawa A., Kurosawa S., Kamada K., Sato H., Toyoda S., Yamaji A., Yoshino M., Hanada T.

    IEEE Transactions on Ultrasonics Ferroelectrics and Frequency Control   Vol. 69 ( 2 ) page: 870 - 877   2022.2

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    The effect of the difference in the thickness ratio of the double-layered thickness-shear resonator on the temperature characteristics of the resonance frequency was investigated using a Ca<sub>3</sub>TaGa<sub>3</sub>Si<sub>2</sub>O<sub>14</sub> (CTGS) single crystal. Three specimens with thickness ratios of <inline-formula> <tex-math notation="LaTeX">${x} =0.25$ </tex-math></inline-formula>, 0.33, and 0.50 were prepared using <inline-formula> <tex-math notation="LaTeX">$122^{\circ } ~{Y}$ </tex-math></inline-formula>- and <inline-formula> <tex-math notation="LaTeX">$171^{\circ }~{Y}$ </tex-math></inline-formula>-cut CTGS substrates. For the specimens with <inline-formula> <tex-math notation="LaTeX">${x} =0.25$ </tex-math></inline-formula> and 0.33, the temperature characteristics varied depending on the order of the resonance mode. For the specimen with <inline-formula> <tex-math notation="LaTeX">${x} =0.50$ </tex-math></inline-formula>, on the other hand, almost the same temperature characteristics were observed regardless of the order of the resonance mode. To interpret this phenomenon, a new equation for predicting the temperature characteristics of the fundamental mode (first mode) for the double-layered resonator was created using the electric flux density ratio generated in the two substrates. The expected values using this equation were in good agreement with the result of the first mode temperature characteristics.

    DOI: 10.1109/TUFFC.2021.3121782

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  130. Prognostic impact of CEBPA bZIP domain mutation in acute myeloid leukemia Open Access

    Wakita S., Sakaguchi M., Oh I., Kako S., Toya T., Najima Y., Doki N., Kanda J., Kuroda J., Mori S., Satake A., Usuki K., Ueki T., Uoshima N., Kobayashi Y., Kawata E., Tajika K., Nagao Y., Shono K., Shibusawa M., Tadokoro J., Kayamori K., Hagihara M., Uchiyama H., Uchida N., Kubota Y., Kimura S., Nagoshi H., Ichinohe T., Kurosawa S., Motomura S., Hashimoto A., Muto H., Sato E., Ogata M., Mitsuhashi K., Ando J., Marumo A., Omori I., Fujiwara Y., Terada K., Yui S., Arai K., Kitano T., Miyata M., Kurosawa A., Mizoguchi A., Komatsu N., Fukuda T., Ohashi K., Kanda Y., Inokuchi K., Yamaguchi H.

    Blood Advances   Vol. 6 ( 1 ) page: 238 - 247   2022.1

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    Mutations of CCAAT/enhancer–binding protein alpha (CEBPAmu) are found in 10% to 15% of de novo acute myeloid leukemia (AML) cases. Double-mutated CEBPA (CEBPAdm) is associated with a favorable prognosis; however, single-mutated CEBPA (CEBPAsm) does not seem to improve prognosis. We investigated CEBPAmu for prognosis in 1028 patients with AML, registered in the Multi-center Collaborative Program for Gene Sequencing of Japanese AML. It was found that CEBPAmu in the basic leucine zipper domain (bZIP) was strongly associated with a favorable prognosis, but CEBPAmu out of the bZIP domain was not. The presence of CEBPAmu in bZIP was a strong indicator of a higher chance of achieving complete remission (P, .001), better overall survival (OS; P, .001) and a lower risk of relapse (P, .001). The prognostic significance of CEBPAmu in bZIP was also observed in the subgroup with CEBPAsm (all patients: OS, P 5 .008; the cumulative incidence of relapse, P 5 .063; patients aged #70 years and with intermediate-risk karyotype: OS, P 5 .008; cumulative incidence of relapse, P 5 .026). Multivariate analysis of 744 patients aged #70 years showed that CEBPAmu in bZIP was the most potent predictor of OS (hazard ratio, 0.3287; P, .001). CEBPAdm was validated as a cofounding factor, which was overlapping with CEBPAmu in bZIP. In summary, these findings indicate that CEBPAmu in bZIP is a potent marker for AML prognosis. It holds potential in the refinement of treatment stratification and the development of targeted therapeutic approaches in CEBPA-mutated AML.

    DOI: 10.1182/bloodadvances.2021004292

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  131. Evaluation of Inner Phase of ZnAl2O4 Thin Film for Ultra Violet Emission

    Inoue K., Adachi S., Kominami H., Hara K., Kurosawa S.

    Proceedings of the International Display Workshops   Vol. 29   page: 412 - 415   2022

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    ZnO films were deposited on sapphire substrates by magnetron sputtering and annealed to produce zinc aluminate (ZnAl2O4) deep ultraviolet emitting phosphor thin films by mutual thermal diffusion between film and substrate. Etching was applied to the annealed samples to change the film thickness of ZnAl2O4. the samples after etching were subjected to emission characteristics evaluation by cathodoluminescence (CL) and crystal structure analysis by X-ray diffraction (XRD), and elemental mapping by field emission-scanning electron microscope analysis (FE-SEM) to estimate the range where Zn was distributed and the distribution of high quality emitting layer.

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  132. Development of particle identification method by waveform analysis of GAGG scintillator (2) Open Access

    Fujikawa Y., Inaba K., Okamoto S., Itoh M., Matsuda Y., Kurosawa S., Yamaji A., Tsuji S., Kawabata T., Furuno T., Adachi S., Murata M., Sakanashi K., Himi K.

    Meeting Abstracts of the Physical Society of Japan   Vol. 77.1 ( 0 ) page: 405 - 405   2022

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    DOI: 10.11316/jpsgaiyo.77.1.0_405

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  133. Reduction of Tl-208 background for Zr-96 neutrinoless double beta decay experiment using topological information of Cherenkov light

    Fukuda Y., Moriyama S., Hiraide K., Ogawa I., Gunji T., Hayami R., Tsukada S., Kurosawa S.

    Proceedings of Science   Vol. 414   2022

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    The topological information (averaged angle) of Cherenkov light was measured by UNI-ZICOS detector. We have retuned the pulse shape discrimination for a selection of the photomultiplier which receives Cherenkov light for Hamamatsu H3164-12, and have developed a method of the vertex reconstruction. An averaged angle for fixed energy fixed direction electron generated by Compton scattering from <sup>88</sup>Y was used for the validity checking of the selection of PMT, and the obtained peak was found around 50 degree which was reproduced by Monte Carlo simulation. A pseudo background events of simultaneous beta and Compton electron scattered by gamma from the decay of <sup>208</sup>Tl was simulated by <sup>60</sup>Co β source. Obtained data indicated that the averaged angle of simultaneous beta with E ≤ 1.48 MeV plus gamma events should have a peak around 60 degree, and the value is different from 48 degree for an usual electron. In conclusion, the averaged angle will be able to use as a reduction method for <sup>208</sup>Tl beta decay backgrounds even though they have an energy around 3.35 MeV which is Q-value of <sup>96</sup>Zr neutrinoless double beta decay.

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  134. Crystal growth of La2Zr2O7 by micro-pulling-down method using Mo and W crucibles

    Suda T., Yokota Y., Horiai T., Yamaji A., Yoshino M., Hanada T., Sato H., Toyoda S., Ohashi Y., Kurosawa S., Kamada K., Yoshikawa A.

    Journal of Crystal Growth   Vol. 575   2021.12

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    La<inf>2</inf>Zr<inf>2</inf>O<inf>7</inf> crystals with a melting point of 2283 °C are grown via the micro-pulling-down (μ-PD) method using Mo and W crucibles to expand the possibility of material research of functional single crystals with high melting points by the μ-PD method. La<inf>2</inf>Zr<inf>2</inf>O<inf>7</inf> crystals grown using Mo and W crucibles under an Ar + 3% H<inf>2</inf> atmosphere are composed of a La<inf>2</inf>Zr<inf>2</inf>O<inf>7</inf> main phase, which includes Mo and W. However, a La<inf>2</inf>Zr<inf>2</inf>O<inf>7</inf> crystal without W can be grown under an Ar atmosphere using the μ-PD method using a W crucible and deoxygenated ZrO<inf>2</inf> insulators. After post-annealing in air at 1000 °C, the La<inf>2</inf>Zr<inf>2</inf>O<inf>7</inf> crystal without W becomes colorless and transparent, indicating a transmittance exceeding 70% in wavelengths ranging from 450 to 800 nm.

    DOI: 10.1016/j.jcrysgro.2021.126357

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  135. Fludarabine/busulfan versus busulfan/cyclophosphamide as myeloablative conditioning for myelodysplastic syndrome: a propensity score-matched analysis

    Kurosawa S., Shimomura Y., Itonaga H., Najima Y., Kobayashi T., Ozawa Y., Kanda Y., Kako S., Kawakita T., Matsuoka K.i., Maruyama Y., Ota S., Nakazawa H., Imada K., Kanda J., Fukuda T., Atsuta Y., Aoki J.

    Bone Marrow Transplantation   Vol. 56 ( 12 ) page: 3008 - 3015   2021.12

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    Myeloablative conditioning with fludarabine/busulfan (Flu/Bu4) prior to allogeneic hematopoietic stem cell transplantation (allo-HSCT) is effective for acute myeloid leukemia. However, the effectiveness of Flu/Bu4 for myelodysplastic syndrome (MDS) remains poorly understood. Therefore, we retrospectively analyzed nationwide registry data in Japan from 2006 to 2018 and compared transplant outcomes of adult MDS patients receiving Flu/Bu4 and busulfan/cyclophosphamide (Bu4/Cy) using propensity score (PS) matching. The primary endpoint was overall survival (OS). Among 2,482 MDS patients, 153 patients were assigned each to the Flu/Bu4 and Bu4/Cy groups. The 3-year OS rates were 52.7% (95% confidence interval [CI], 43.8–60.8%) and 49.5% (95% CI, 40.8–57.6%) in the Flu/Bu4 and Bu4/Cy group, respectively (P = 0.548). The 3-year progression-free survival (P = 0.858), the cumulative incidence of relapse (P = 0.536), and cumulative incidence of non-relapse mortality (P = 0.684) were not significantly different between the two groups. According to the findings of subgroup analyses, no patient had a favorable OS when using either of the two regimens. In conclusion, although our PS-matched cohort mainly comprised older patients who had a low hematopoietic cell transplantation-comorbidity index and low-risk disease status, Flu/Bu4 could be an alternative to Bu4/Cy for MDS patients prior to allo-HSCT.

    DOI: 10.1038/s41409-021-01447-y

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  136. Luminescence and scintillation properties of Mo co-doped Y0.8Gd2.2(Al5-xGax)O12: Ce multicomponent garnet crystals

    Sakthong O., Chewpraditkul W., Chewpraditkul W., Kurosawa S., Yoshikawa A., Kamada K., Kim K.J., Drozdowski W., Witkowski M.E., Makowski M., Kucerkova R., Beitlerova A., Nikl M.

    Optical Materials   Vol. 122   2021.12

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    Mo co-doped Y<inf>0.8</inf>Gd<inf>2.2</inf>(Al<inf>5-x</inf>Ga<inf>x</inf>)O<inf>12</inf>:Ce (x = 2.6 and 3) multicomponent garnet crystals were grown by the micro-pulling down method and the luminescence and scintillation properties were investigated. The temperature dependences of radioluminescence yield and photoluminescence decay time were measured to investigate the temperature stability of these crystals. Under excitation with 662 keV γ rays at room temperature, Y<inf>0.8</inf>Gd<inf>2.2</inf>(Al<inf>2.4</inf>Ga<inf>2.6</inf>)O<inf>12</inf>:Ce,Mo shows a higher light yield of 53,800 ph/MeV whereas Y<inf>0.8</inf>Gd<inf>2.2</inf>(Al<inf>2</inf>Ga<inf>3</inf>)O<inf>12</inf>:Ce,Mo shows a faster scintillation decay times of 50 ns (56%) + 275 ns (44%). A decrease of radioluminescence yield at low temperature observed in correlation with an appearance of the large thermoluminescence peaks can be attributed to the localization of charge carriers at shallow traps.

    DOI: 10.1016/j.optmat.2021.111783

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  137. Plutonium dioxide particle imaging using a high-resolution alpha imager for radiation protection Open Access

    Morishita Y., Kurosawa S., Yamaji A., Hayashi M., Sasano M., Makita T., Azuma T.

    Scientific Reports   Vol. 11 ( 1 ) page: 5948   2021.12

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    The internal exposure of workers who inhale plutonium dioxide particles in nuclear facilities is a crucial matter for human protection from radiation. To determine the activity median aerodynamic diameter values at the working sites of nuclear facilities in real time, we developed a high-resolution alpha imager using a ZnS(Ag) scintillator sheet, an optical microscope, and an electron-multiplying charge-coupled device camera. Then, we designed and applied a setup to measure a plutonium dioxide particle and identify the locations of the individual alpha particles in real time. Employing a Gaussian fitting, we evaluated the average spatial resolution of the multiple alpha particles was evaluated to be 16.2 ± 2.2 μmFWHM with a zoom range of 5 ×. Also, the spatial resolution for the plutonium dioxide particle was 302.7 ± 4.6 µmFWHM due to the distance between the plutonium dioxide particle and the ZnS(Ag) scintillator. The influence of beta particles was negligible, and alpha particles were discernible in the alpha–beta particle contamination. The equivalent volume diameter of the plutonium dioxide particle was calculated from the measured count rate. These results indicate that the developed alpha imager is effective in the plutonium dioxide particle measurements at the working sites of nuclear facilities for internal exposure dose evaluation.

    DOI: 10.1038/s41598-021-84515-z

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  138. Development of an Electron-Tracking Compton Camera

    KUROSAWA Shunsuke

    Medical Imaging Technology   Vol. 39 ( 5 ) page: 217 - 222   2021.11

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    Language:Japanese   Publisher:The Japanese Society of Medical Imaging Technology  

    <p>Electron-Tracking Compton Camera is one of the gamma-ray imaging devices, and the gamma-ray direction and energy can be determined event by even with this camera. I show the camera structure, short history of the camera, improvement of each part and medical application.</p>

    DOI: 10.11409/mit.39.217

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  139. Cs2HfCl6 doped with Zr: Influence of tetravalent substitution on scintillation properties

    Vaněček V., Páterek J., Král R., Buryi M., Babin V., Zloužeová K., Kodama S., Kurosawa S., Yokota Y., Yoshikawa A., Nikl M.

    Journal of Crystal Growth   Vol. 573   2021.11

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    Homeland security is an emerging application field for inorganic scintillators. Detection and identification of radioactive materials in both individual and cargo transport requires scintillators with excellent energy resolution and high light output. On the other hand, the time characteristics of the scintillation are less crucial. Furthermore, price is a key parameter due to the large volume of the detectors. State-of-the-art halide scintillators e. g. SrI<inf>2</inf>:Eu or LaBr<inf>3</inf>:Ce can satisfy the requirements for light yield and energy resolution, but the production costs are very high due to complicated crystal growth and the high prices of rare earth metals. Cesium hafnium chloride (Cs<inf>2</inf>HfCl<inf>6</inf>) is a promising intrinsic scintillator with high light yield and excellent resolution. Moreover, its low hygroscopicity and cubic crystal structure could allow lower production costs compared to SrI<inf>2</inf> or LaBr<inf>3</inf>. Intrinsic luminescence of Cs<inf>2</inf>HfCl<inf>6</inf> is commonly attributed to self-trapped excitons. However, the luminescence of Cs<inf>2</inf>HfCl<inf>6</inf> shows complex structure and temperature dependence. This might be explained by the presence of zirconium which is a common impurity in hafnium compounds. We present a study of the influence of zirconium doping on the scintillation properties of Cs<inf>2</inf>HfCl<inf>6</inf>. Single crystals of Cs<inf>2</inf>HfCl<inf>6</inf> with zirconium doping from 0 to 1 mol% were grown by the vertical Bridgman method. Their phase purity, radioluminescence, scintillation decay, light yield, and afterglow were evaluated. Results show that zirconium doping can affect the scintillation properties of Cs<inf>2</inf>HfCl<inf>6</inf> even at concentrations comparable to impurity levels of zirconium in hafnium compounds.

    DOI: 10.1016/j.jcrysgro.2021.126307

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  140. Growth and scintillation properties of Tl-doped CsI/KI/KCl ternary eutectics

    Takizawa Y., Kamada K., Kutsuzawa N., Jin Kim K., Yoshino M., Yamaji A., Kurosawa S., Yokota Y., Sato H., Toyoda S., Ohashi Y., Hanada T., Kochurikhin V.V., Yoshikawa A.

    Journal of Crystal Growth   Vol. 573   2021.11

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    In this study, Tl:CsI/KI/KCl eutectic scintillators were grown using the Bridgman–Stockbarger method by unidirectional solidification. The eutectic phases were uniformly distributed in the transverse direction and were slightly aligned along the growth direction. The Tl:CsI scintillator phase was grown as a matrix, which was then used for creating optical waveguides of the scintillation light. The expected Tl<sup>+</sup> emission peak was observed at 486 nm under X-ray excitation and cathodoluminescence; this was attributed to the self-trapped exciton perturbed by TI<sup>+</sup> in Tl:CsI. The decay time of the Tl:CsI/KI/KCl eutectic was 313 ns, and its light output was estimated to be 22,000 photons/MeV.

    DOI: 10.1016/j.jcrysgro.2021.126287

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  141. Prognostic Impact of Pretransplantation Quality of Life and Its Post-Transplantation Longitudinal Change after Allogeneic Hematopoietic Cell Transplantation: A Prospective Study That Administered the Short-Form Health Survey (SF-12) and EuroQol 5

    Kurosawa S., Yamaguchi T., Mori A., Tsukagoshi M., Okuda I., Ikeda M., Fuji S., Yamashita T., Ogawa C., Ito A., Tanaka T., Inamoto Y., Kim S.W., Fukuda T.

    Transplantation and Cellular Therapy   Vol. 27 ( 11 ) page: 935 - 935.e9   2021.11

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    In allogeneic hematopoietic cell transplantation (allo-HCT), investigator-based clinical variables have been used for pretransplantation prognostic prediction, risk adjustment, and post-transplantation long-term screenings. Although several studies have investigated the prognostic significance of pretransplantation patient-reported outcomes (PROs) and longitudinal trends in PROs after allo-HCT, few have assessed these outcomes using the Medical Outcomes Study 12-Item Short-Form Health Survey (SF-12) and EuroQol 5 Dimension (EQ-5D) index. The present study used 18 items from the SF-12 and EQ-5D index to evaluate the prognostic impact of pretransplantation quality of life (QOL) on allo-HCT outcomes and longitudinal changes in QOL in allo-HCT recipients. This single-center prospective study included consecutive patients who underwent allo-HCT at our center between October 2014 and September 2016. All participants were followed up until October 2017. The SF-12 and EQ-5D index were administered to assess patient-reported QOL before allo-HCT and at 3 months, 6 months, 1 year, and 2 years after allo-HCT when participants visited the long-term follow-up clinic. Longitudinal trends in the QOL-adjusted means were estimated using linear mixed-effects, adjusting for pretransplantation covariates and reasons for missing QOL data. Among 157 patients who underwent allo-HCT, 145 (92%) were registered in this study, and 143 with available QOL data were analyzed. The median pretransplantation scores were 45.3 for the SF-12 physical component score (PCS), 55.6 for the mental component score (MCS), 38.8 for the role/social component score (RCS), 70.0 for the visual analog scale (VAS), and 49.0 for the EQ-5D index. Overall survival (OS) was significantly improved in patients with higher pretransplantation scores on the PCS, RCS, and EQ-5D index, and multivariable analyses showed that the median pretransplantation RCS was significantly associated with OS after allo-HCT (hazard ratio, 3.66; P =.003). The longitudinal trends in the SF-12 score showed that the PCS was improved at 2 years after allo-HCT and was comparable to the normative score for the general population. The MCS remained comparable to or higher than the normative score after allo-HCT. The RCS improved significantly beginning at 6 months after allo-HCT but remained lower than the normative score at 2 years. The VAS and EQ-5D index values showed a drop at 3 months after allo-HCT. Patient-reported QOL assessed by 18 questions on the SF-12 and EQ-5D predicted prognosis, and may be used as a prognosticator to determine treatment strategies, including preparative regimens. Although we experienced a certain amount of patient attrition in the longitudinal follow-up of QOL data, we demonstrated characteristic trajectories of QOL in different domains after adjusting for background covariates and reasons for the lack of QOL data.

    DOI: 10.1016/j.jtct.2021.07.026

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  142. Scintillation characteristics and temperature quenching of radio- and photoluminescence of Mg2+-codoped (Lu,Gd)3Al2.4Ga2.6O12:Ce garnet crystals

    Chewpraditkul W., Pattanaboonmee N., Sakthong O., Chewpraditkul W., Yamaji A., Kurosawa S., Kamada K., Yoshikawa A., Makowski M., Witkowski M.E., Drozdowski W., Beitlerova A., Kucerkova R., Babin V., Nikl M.

    Optical Materials   Vol. 121   2021.11

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    Luminescence and scintillation characteristics of Mg<sup>2+</sup>-codoped (Lu<inf>x</inf>Gd<inf>3-x</inf>)Al<inf>2.4</inf>Ga<inf>2.6</inf>O<inf>12</inf>:Ce (x = 0.2–0.8) garnet crystals grown by the micro-pulling down method are investigated. The Ce<sup>3+</sup> 5d<inf>1</inf> → 4f luminescence is blue-shifted with increasing Lu content due to the decrease in crystal field splitting of the 5 d levels. With increasing Lu content, the shortening of scintillation decay time accompanied with a decrease of LY value as measured at room temperature can be explained by thermal ionization of the Ce<sup>3+</sup> 5d<inf>1</inf> excited state. Co-doping with Mg<sup>2+</sup> results in the shortening of scintillation decay time, the reduction of LY value and afterglow intensity. At low temperature the radioluminescence quenching is observed in correlation with large thermoluminescence peaks, which can be attributed to the localization of electrons at intrinsic shallow traps.

    DOI: 10.1016/j.optmat.2021.111595

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  143. Crystal growth and optical properties of Ce-doped (La,Y)2Si2O7 single crystal Open Access

    Horiai T., Paterek J., Pejchal J., Jarosova M., Rohlicek J., Kurosawa S., Hanada T., Yoshino M., Yamaji A., Toyoda S., Sato H., Ohashi Y., Kamada K., Yokota Y., Yoshikawa A., Nikl M.

    Journal of Crystal Growth   Vol. 572   2021.10

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    We have grown Ce-doped (La,Y)<inf>2</inf>Si<inf>2</inf>O<inf>7</inf> single crystal by micro-pulling-down method and investigated its optical and scintillation properties. We have successfully prepared the single crystal with (Ce<inf>0.015</inf>La<inf>0.600</inf>Y<inf>0.385</inf>)<inf>2</inf>Si<inf>2</inf>O<inf>7</inf> composition. The observed thermal quenching process could be characterized by the quenching temperature (T<inf>50%</inf>) of 526 K and its activation energy was determined to be 0.62 eV. Further considering the thermal quenching factors, it was found that the thermal quenching was caused by at least the thermal ionization and maybe also by classical thermal quenching. The light output and scintillation decay time were evaluated to be ~12,000 photons/MeV and ~42 ns, respectively. These results indicate that (Ce<inf>0.015</inf>La<inf>0.600</inf>Y<inf>0.385</inf>)<inf>2</inf>Si<inf>2</inf>O<inf>7</inf> has a great potential for application in scintillation materials.

    DOI: 10.1016/j.jcrysgro.2021.126252

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  144. Luminescence and scintillation properties of Gd3Sc2(Al3-xGax)O12:Ce (x = 1, 2, 3) garnet crystals

    Chewpraditkul W., Pattanaboonmee N., Chewpraditkul W., Sakthong O., Kim K.J., Yoshino M., Horiai T., Kurosawa S., Yoshikawa A., Kamada K., Drozdowski W., Witkowski M.E., Makowski M., Kucerkova R., Nikl M.

    Radiation Physics and Chemistry   Vol. 187   2021.10

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    The luminescence and scintillation characteristics of Ce<sup>3+</sup> - doped Gd<inf>3</inf>Sc<inf>2</inf>(Al<inf>3-x</inf>Ga<inf>x</inf>)O<inf>12</inf> (x = 1, 2, 3) garnet crystals were investigated. The Ce<sup>3+</sup> luminescence was blue-shifted with increasing Ga content due to the decrease of the crystal field strength. A decrease of Ce<sup>3+</sup> luminescence intensity and luminescence decay time at high temperature was observed for all samples due to thermal ionization of the Ce<sup>3+</sup> 5d<inf>1</inf> excited levels. With increasing Ga content the decrease of thermal activation energies, determined from temperature dependence of decay times, was obtained. Both Gd<inf>3</inf>Sc<inf>2</inf>Al<inf>2</inf>GaO<inf>12</inf>:Ce and Gd<inf>3</inf>Sc<inf>2</inf>AlGa<inf>2</inf>O<inf>12</inf>:Ce samples exhibited a comparable light yield (LY) value of 24,000 photons/MeV while the latter sample showed faster scintillation decay time of 12 ns (11%) + 56 ns (89%) with respect to those of 55 ns (28%) + 105 ns (72%) for the former sample. An acceleration of scintillation decay time with an expense of LY value was also obtained for the Mg<sup>2+</sup>-codoped sample. At low temperature a decrease of scintillation yield was observed in correlation with the intense thermoluminescence peaks, attributing to the localization of electrons at intrinsic shallow traps.

    DOI: 10.1016/j.radphyschem.2021.109559

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  145. Response of the GAGG(Ce) scintillator to charged particles compared with the CsI(Tl) scintillator Open Access

    Furuno T., Koshikawa A., Kawabata T., Itoh M., Kurosawa S., Morimoto T., Murata M., Sakanashi K., Tsumura M., Yamaji A.

    Journal of Instrumentation   Vol. 16 ( 10 )   2021.10

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    GAGG(Ce) is a novel scintillator with a fast response and high light output without a hygroscopic nature. It is expected to be a useful detector for charged particles at high-counting rates. However, the response of the GAGG(Ce) scintillator to charged particles has not been fully examined. In the present work, the light output and energy resolution of the GAGG(Ce) scintillator were measured for protons and alpha particles at E p=5-68 MeV and E α=8-54 MeV as well as gamma rays at E γ=662 keV from a 137Cs source. The results were compared with those of the CsI(Tl) scintillator. The scintillation efficiencies dL/dE of the GAGG(Ce) and CsI(Tl) scintillators were obtained and parametrized as a function of linear energy transfer dE/dx.

    DOI: 10.1088/1748-0221/16/10/P10012

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  146. Syngeneic hematopoietic stem cell transplantation for acute myeloid leukemia: a propensity score-matched analysis Open Access

    Kurosawa S., Mizuno S., Arai Y., Masuko M., Kanda J., Kohno K., Onai D., Fukuda T., Ozawa Y., Katayama Y., Tanaka M., Ikegame K., Uchida N., Eto T., Ota S., Tanaka J., Ichinohe T., Atsuta Y., Yanada M.

    Blood Cancer Journal   Vol. 11 ( 9 ) page: 159   2021.9

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    The present study evaluated outcomes and prognostic factors in adult patients with acute myeloid leukemia (AML) after syngeneic hematopoietic stem cell transplantation (HSCT). Among patients in first complete remission (CR1), outcomes of syngeneic HSCT (Syn) were compared with those of autologous HSCT (Auto), allogeneic HSCT from human leukocyte antigen (HLA)-matched sibling donor (MSD), or allogeneic HSCT from HLA-matched unrelated donor (MUD). Among 11,866 patients receiving first HSCT, 26 in the Syn group were analyzed. The 5-year overall survival (OS) rate, the cumulative incidence of relapse, and the cumulative incidence of non-relapse mortality (NRM) were 47.8%, 59.6%, and 4.6%, respectively. The OS was significantly better in patients in CR1 (n = 13) than in patients in non-CR1 (P = 0.012). Furthermore, 39 patients in CR1 each were assigned to the Auto, MSD, and MUD groups using propensity score matching. The 5-year OS in the Syn (68.4%) was not significantly different from those in the Auto (55.9%, P = 0.265), MSD (62.4%, P = 0.419), or MUD (63.7%, P = 0.409) groups. A higher relapse in the Syn than in the MSD and MUD groups was offset by lower NRM. In summary, syngeneic HSCT might be an alternative option for AML patients in CR1.

    DOI: 10.1038/s41408-021-00553-w

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  147. Bright exciton luminescence from La doped Lu3Al5O12 single crystals

    Bartosiewicz K., Horiai T., Yamaji A., Yoshikawa A., Kurosawa S., Kim K.J., Vistovskyy V., Voloshinovskii A., Zorenko Y.

    Journal of Luminescence   Vol. 235   2021.7

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    This research dealt with the investigation of luminescence properties of undoped and La doped Lu<inf>3</inf>Al<inf>5</inf>O<inf>12</inf> single crystals using synchrotron radiation excitation. The influence of La<sup>3+</sup> doping on the exciton emission and decay kinetics properties of Lu<inf>3</inf>Al<inf>5</inf>O<inf>12</inf> single crystals was studied at 7 K and room temperature. Undoped and La<sup>3+</sup> doped samples showed bright luminescence in the UV spectral range. In undoped Lu<inf>3</inf>Al<inf>5</inf>O<inf>12</inf> crystal, the UV luminescence was associated with Lu<inf>Al</inf> antisite defects, which acted as luminescence centers in the band peaked at 295 nm La<sup>3+</sup> doping in Lu<inf>3</inf>Al<inf>5</inf>O<inf>12</inf> crystals caused the formation of La<inf>Lu</inf> luminescence centers and increased the concentration of Lu<inf>Al</inf> antisite defects. Therefore, the luminescence of La doped Lu<inf>3</inf>Al<inf>5</inf>O<inf>12</inf> crystals was a superposition of the emission coming from both La<inf>Lu</inf> and Lu<inf>Al</inf> centers. Furthermore, La<sup>3+</sup> doping significantly enhanced the intensity and shifted the UV luminescence of Lu<inf>3</inf>Al<inf>5</inf>O<inf>12</inf> crystals towards higher energy due to the dominant contribution of La<inf>Lu</inf> luminescent centers in the band peaked at 275 nm. The decay time of heavily La<sup>3+</sup> doped LuAG crystals was also significantly accelerated due to the prevailing luminescence of La<inf>Lu</inf> centers.

    DOI: 10.1016/j.jlumin.2021.118013

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  148. Optimum measurement condition for V(x) method using the line-focus-beam ultrasonic-material-characterization system

    Ohashi Y., Yokota Y., Yamaji A., Yoshino M., Kurosawa S., Kamada K., Sato H., Toyoda S., Hanada T., Yoshikawa A.

    Japanese Journal of Applied Physics   Vol. 60 ( 7 )   2021.7

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    Optimum measurement condition of the V(x) method proposed as a fast scanning technique of the line-focus-beam ultrasonic material characterization system was theoretically investigated to realize more accurate measurement. Through numerical calculation, it was clarified that the appropriate defocus position z m with higher sensitivity used in the V(x) measurement depended on the waveform attenuation of V(z) curves. It was also clarified that the measurement error caused by the focal distance change due to temperature change in the water coupler could be reduced by choosing the lower defocus position as z m. A method for measuring the surface profile of the specimen by applying the V(x) method with z m > 0 was proposed in order to correct measurement error due to warpage of specimen surface.

    DOI: 10.35848/1347-4065/ac06dc

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  149. Development of large size crystal growth technology of oxide eutectic scintillator and a proto-type Talbot-Lau imaging system

    Kamada K., Yamaguchi H., Yasui N., Ohashi R., Den T., Kim K.J., Yoshino M., Yamaji A., Kurosawa S., Shoji Y., Yokota Y., Kochurikhin V.V., Yoshikawa A.

    Japanese Journal of Applied Physics   Vol. 60 ( SB )   2021.5

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    Wafers of Tb-doped GdAlO<inf>3</inf>/α-Al<inf>2</inf>O<inf>3</inf> eutectic were fabricated by the micro-pulling-down method using an Ir crucible with a 25 × 25 mm<sup>2</sup> die. A prototype X-ray phase imaging detector was developed using a CMOS sensor with a fiber optic plate and the eutectic wafer. X-ray spots with an 8.24 μm period were observed using the detector. X-ray phase imaging of a nylon ball with a diameter of 4 mm was also carried out. It was observed that a phase change of approximately 2 μm occurs at the air-nylon interface. This technique of X-ray phase imaging can be realized in the absence of an absorption grating.

    DOI: 10.35848/1347-4065/abd708

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  150. Effect of donor type on volume of blood transfusions required after allogeneic hematopoietic cell transplantation

    Kurosawa S., Yamaguchi T., Nakabayashi S., Kasane M., Tsubokura M., Iwashita N., Minakawa Y., Ohtake R., Kawamura K., Nishioka Y., Takeda W., Hirakawa T., Aoki J., Ito A., Tanaka T., Inamoto Y., Kim S.W., Kojima M., Takanashi M., Fukuda T.

    International Journal of Hematology   Vol. 113 ( 4 ) page: 518 - 529   2021.4

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    We reviewed blood product use in 729 consecutive allogeneic hematopoietic cell transplantation (allo-HCT) recipients at our center to assess the volume of red blood cells (RBCs) and platelets required after allo-HCT. The median number of bags required by day 30 was 4 for RBCs (range 0–22) and 9.5 for platelets (0–53). Multivariate analysis showed that related peripheral blood stem cell transplantation (PBSCT) required a significantly lower RBC transfusion volume by day 30 compared to unrelated bone marrow transplantation (UBMT). PBSCT from haplo-identical related donors and cord blood transplantation (CBT) required a significantly greater RBC transfusion volume. For platelet transfusion, related and unrelated PBSCT required a significantly lower volume than UBMT, and CBT a greater volume. Other factors independently associated with greater RBC transfusion volume were male sex, disease status other than complete remission, and major ABO mismatch. For platelet transfusion, these were male sex, disease status, and HCT-specific comorbidity index of 1. Although the burden of blood transfusions may not be the most important factor when choosing a donor type, our findings may provide a foundation for nationwide strategies to prepare blood products and inform aspects of national healthcare expenditures.

    DOI: 10.1007/s12185-020-03041-2

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  151. Development of <i>Spatiotemporal</i> Measurement and Analysis Techniques in X-ray Photoelectron Spectroscopy ∼From NAP-HARPES to 4D-XPS∼ Open Access

    MINEOI Susumu, SUZUKI Satoru, MACHIDA Masatake, YOSHIGOE Akitaka, OHASHI Yuji, KAMADA Kei, YOSHIKAWA Akira, TOYODA Satoshi, HANADA Takashi, SUMIDA Hirosuke, KUROSAWA Shunsuke, YOSHINO Masao, YOKOTA Yuui, YAMAJI Akihiro, SATO Hiroki, YOKOYAMA Kazushi, YAMAMOTO Tomoki, YOSHIMURA Masashi

    Vacuum and Surface Science   Vol. 64 ( 2 ) page: 86 - 91   2021.2

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    <p>We have developed <i>spatiotemporal</i> measurement and analysis techniques in x-ray photoelectron spectroscopy. To begin with, time-division depth profiles of gate stacked film interfaces have been achieved by NAP-HARPES (<u>N</u>ear <u>A</u>mbient <u>P</u>ressure <u>H</u>ard x-ray <u>A</u>ngle-<u>R</u>esolved <u>P</u>hoto<u>E</u>mission <u>S</u>pectroscopy) data. We then have promoted our methods to quickly perform peak fittings and depth profiling from time-division ARPES data, which enables us to realize 4D-XPS analysis. It is found that the traditional maximum entropy method (MEM) combined with Jackknife averaging of sparse modeling in NAP-HARPES data is effective to perform dynamic measurement of depth profiles with high precision.</p>

    DOI: 10.1380/vss.64.86

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  152. New types of composite scintillators based on the single crystalline films and crystals of Gd3(Al,Ga)5O12:Ce mixed garnets

    Witkiewicz-Lukaszek S., Gorbenko V., Zorenko T., Syrotych Y., Kucerkova R., Mares J.A., Nikl M., Sidletskiy O., Fedorov A., Kurosawa S., Kamada K., Yoshikawa A., Zorenko Y.

    Materials Science and Engineering B   Vol. 264   2021.2

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    This work presents the results of creation of novel composite scintillators based on the Gd<inf>3</inf>Al<inf>5-x</inf> Ga<inf>x</inf>O<inf>12</inf>:Ce (x = 1.16–2.67) single crystalline films (SCF), grown by the LPE method onto Gd<inf>3</inf>Al<inf>2.5</inf> Ga<inf>2.5</inf>O<inf>12</inf>:Ce single crystal (SC) substrates. The scintillation properties of film/crystal epitaxial structures were investigated under α–particle and γ–quantum excitations. Under α–particle excitation, the light yield of mentioned SCF scintillators is significantly less than that in their substrates due to the influence of Pb<sup>2+</sup> flux contamination and formation of Pb<sup>2+</sup>-Ce<sup>4+</sup> centers. Meanwhile, these SCF scintillators under α–excitation possess significantly faster decay kinetics than that of their substrates under γ–excitation. Therefore, the Gd<inf>3</inf>Al<inf>5-x</inf>Ga<inf>x</inf>O<inf>12</inf>:Ce SCFs (x = 1.16–2.67) /Gd<inf>3</inf>Al<inf>2.5</inf>Ga<inf>2.5</inf>O<inf>12</inf>:Ce SC epitaxial structures can be used as composite scintillators for simultaneous registration of the components of mixed ionizing fluxes, specifically for detection of α–particles (SCF) and γ–quanta (substrate). The separation of the response from the SCF and substrate parts of composite scintillators under α–particle (<sup>241</sup>Am) and γ–quantum (<sup>137</sup>Cs) excitations occurs at large t<inf>γ</inf>/t<inf>α</inf> = 1.7–4.2 ratio.

    DOI: 10.1016/j.mseb.2020.114909

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  153. Novel Method of Search for Transparent Optical Materials with Extremely High Melting Point

    Kurashima Y., Kurosawa S., Murakami R., Yamaji A., Ishikawa S., Pejchal J., Kamada K., Yoshino M., Toyoda S., Sato H., Yokota Y., Ohashi Y., Yoshikawa A.

    Crystal Growth and Design   Vol. 21 ( 1 ) page: 572 - 578   2021.1

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    We propose a novel crystal growth method, "Core Heating (CH) Method", which is suitable for a search of novel materials with extremely high melting points above the melting (softening) point of an Ir crucible. As a feasibility test of the novel CH method, we fabricated the conventional material, (Y0.99Ce0.01)3Al5O12 (Ce:YAG), with a melting point of ∼1970 °C, because this material can be grown by the conventional melt growth technique like the micropulling down (μ-PD) method for the comparison. We compared scintillation properties for Ce:YAG prepared by the CH and μ-PD methods in order to find if the CH method can be applied to the material search. The crystals grown by both methods showed the YAG single-phase, and almost all their optical and scintillation properties of them were comparable for both samples. Particularly, the light output of Ce:YAG crystal grown by the CH method (20,000 ± 1,000 photons/MeV) was similar to that of the sample grown by the μ-PD method (23,000 ± 1,000 photons/MeV). Therefore, we concluded that the CH method is a useful technique for the search of scintillation materials with extremely high melting points.

    DOI: 10.1021/acs.cgd.0c01396

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  154. Allogeneic hematopoietic stem cell transplantation for adult patients with B-cell acute lymphoblastic leukemia with high hyperdiploidy: a retrospective nationwide study

    Kurosawa S., Kaito S., Uchida N., Fukuda T., Doki N., Mori T., Hasegawa Y., Takada S., Sakaida E., Tanaka M., Ikegame K., Kanda J., Atsuta Y., Kako S.

    Leukemia and Lymphoma   Vol. 62 ( 10 ) page: 2514 - 2520   2021

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    We compared the transplant outcomes of adult patients with B-cell acute lymphoblastic leukemia characterized by high hyperdiploidy (HeH; 51–65 chromosomes) (n = 29) and those with a normal karyotype (n = 87) by propensity score-matched analysis. There were no significant differences among groups in 3-year probabilities of overall survival (OS, 63.5% vs. 55.3%, p =.553), cumulative relapse incidence (28.6% vs. 28.7%, p =.982), and non-relapse mortality (10.9% vs. 21.4%, p =.303). Three-year OS was significantly worse in HeH patients with third or later complete remission (CR) or non-CR compared with those in first CR (19.0% vs. 69.9%, p =.010). Frequently gained chromosomes +21 (75.9%), +4 (69.0%), +6 (69.0%), +10 (69.0%), and +1 (69.0%) had no significant prognostic impact on the OS of patients with HeH in multivariate analyses. Patients with HeH who may benefit from allogeneic hematopoietic stem cell transplantation should be further analyzed.

    DOI: 10.1080/10428194.2021.1924374

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  155. Development of particle identification method by waveform analysis of GAGG scintillator Open Access

    Tsuji S., Adachi S., Murata M., Inaba K., Fujikawa Y., Okamoto S., Himi K., Itoh M., Matsuda Y., Sakanashi K., Kurosawa S., Furuno T., Kawabata T., Yamaji A.

    Meeting Abstracts of the Physical Society of Japan   Vol. 76.1 ( 0 ) page: 2385 - 2385   2021

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    DOI: 10.11316/jpsgaiyo.76.1.0_2385

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  156. Step-Flow Growth Model of N-polar GaN Metalorganic Vapor Phase Epitaxy Reviewed

    Hanada Takashi, Yoshino Masao, Yamaji Akihiro, Kurosawa Shunsuke, Kamada Kei, Toyoda Satoshi, Sato Hiroki, Yokota Yuui, Yoshikawa Akira, Ohashi Yuji

    Journal of the Japanese Association for Crystal Growth   Vol. 48 ( 1 ) page: n/a   2021

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    <p>  The Burton-Cabrera-Frank (BCF) theory has been applied to metalorganic vapor-phase epitaxy (MOVPE) of N-polar (000<span style="text-decoration: overline;">1</span>) GaN. Owing to the hydrogen-rich atmosphere during MOVPE, surface N atoms of the N-polar (000-1) surface are mostly covered with H atoms. Extremely small coverage of the Ga adatoms competing with the H adatoms on the terraces can be calculated using the Langmuir adsorption isotherm. The equilibrium coverage of the Ga adatoms at steps and the equilibrium pressure of the NH<sub>3</sub> gas at step kinks can be calculated from the conditions of Gibbs energy balance between the sources (Ga adatom and NH<sub>3</sub> gas molecule) and the products (GaN and 3/2 H<sub>2</sub> gas molecules) and of speed balance between Ga and N incorporation into the step kinks. Growth rates of GaN on vicinal surfaces and hexagonal spiral pyramids has been calculated as a function of the trimethylgallium flow rate and compared with experimental results.</p>

    DOI: 10.19009/jjacg.48-1-03

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  157. Tube shape-controlled crystal growth / dicing technique dedicated for scintillation materials, and its application to radiation imaging devices

    Kamada Kei, Shoji Yasuhiro, Yoshino Masao, Yokota Yuui, Kotaki Atsushi, Kurosawa Shunsuke, Hanada Takashi, Yamaji Akihiro, Ohashi Yuji, Sato Hiroki, Yoshikawa Akira

    Journal of the Japanese Association for Crystal Growth   Vol. 48 ( 1 ) page: n/a   2021

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    <p>  This article presents the development of the tube shape-controlled oxide scintillator directly grown from a melt via the micro-pulling-down method. We grew tube shape-controlled Ce doped Y<sub>3</sub>Al<sub>5</sub>O<sub>12</sub> (tube-Ce:YAG) single-crystal scintillators with shape control using the µ-PD method, which we have reported in previous paper. We also developed and evaluated the diced Eu:SrI<sub>2</sub> scintillator arrays and their scintillation properties for radiation imaging application. Using a novel dicing technique specific to halide scintillation crystals, a high-energy resolution scintillator array is developed that is cost-effective and widely applicable. Finally, these techniques and development were applied for the novel imaging method we proposed, called scintillation active collimator (SAC). These results demonstrated that the SAC could be promising imaging method for the future medical imaging application.</p>

    DOI: 10.19009/jjacg.48-1-05

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  158. Changes in avalanche amplification rate with potential difference between the upper and lower cathodes of a two-dimensional position-sensitive detector with a new electrode structure, triaxial u-PIC Open Access

    Yoshida Y., Tanimori T., Takada A., Yoshikawa K., Abe M., Ogio S., Tsuda M., Komura S., Mizumura Y., Kishimoto T., Ikeda T., Takemura T., Onozaka K., Saito K., Nakamura Y., Mizumoto T., Sonoda S., Kurosawa S., Oohigashi R., Miuchi K., Sawano T, Oota K., Kubo H., Motomura T., Hamaguchi K.

    Meeting Abstracts of the Physical Society of Japan   Vol. 76.1 ( 0 ) page: 128 - 128   2021

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    DOI: 10.11316/jpsgaiyo.76.1.0_128

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  159. Aging and leukemic evolution of hematopoietic stem cells under various stress conditions Open Access

    Kurosawa S., Iwama A.

    Inflammation and Regeneration   Vol. 40 ( 1 ) page: 29   2020.12

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    Hematopoietic stem cells (HSCs) have self-renewal capacity and differentiation potential into all lineages of blood cells throughout the lifetime of an organism. The function of HSCs gradually changes during aging. To date, various stress factors influencing HSC aging have been identified. The increased production of reactive oxygen species and DNA damage responses are causatively attributed to HSC aging. The increased apolarity is a prominent feature of aged HSCs, whereas it is less obvious in young HSCs. The bone marrow (BM) microenvironment niche is a crucial factor for HSC aging. Mesenchymal stem cells show skewed differentiation during aging, which leads to decreased bone formation and increased adipogenesis. The accumulation of adipocytes confers negative effects on hematopoiesis. Loss of sympathetic nerve fibers or adrenoreceptor β3 signaling induces premature HSC and niche aging. Epigenetic regulators such as polycomb group proteins and the sirtuin family of proteins act to prevent premature aging. Targeting these factors, several rejuvenation strategies for aged HSCs have been employed in mice. However, we still do not know whether these strategies can be extrapolated to human HSCs. Aging is frequently accompanied by the development of clonal hematopoiesis, which is called age-related clonal hematopoiesis (ARCH) or clonal hematopoiesis of indeterminate potential (CHIP). Most ARCH/CHIP mutations occur in genes encoding epigenetic regulators including DNMT3A, TET2, and ASXL1, which suggests the relevance of epigenetic drift during the aging process. ARCH/CHIP is a strong risk factor for subsequent hematologic cancer. Notably, it also has an impact on the development of non-malignant disorders such as coronary heart disease. Further studies are warranted to decipher the complete picture of molecular crosstalk that regulates HSC aging.

    DOI: 10.1186/s41232-020-00138-3

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  160. Crystal growth and scintillation properties of tube shape-controlled Ce-doped Y3Al5O12single crystals grown by micro-pulling-down method

    Kotaki A., Yoshino M., Yokota Y., Hanada T., Yamaji A., Toyoda S., Sato H., Ohashi Y., Kurosawa S., Kamada K., Yoshikawa A.

    Applied Physics Express   Vol. 13 ( 12 )   2020.12

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    Tube shape-controlled Ce-doped Y3Al5O12 (tube-Ce:YAG) single-crystal scintillators were directly grown from a melt via the micro-pulling-down method using a specially-designed iridium crucible. Back-scattering Laue images and X-ray diffraction measurements revealed the tube-Ce:YAG was a single crystal with the YAG phase. Ce distribution in the tangential direction of the tube-Ce:YAG specimen showed that Ce concentrations around the capillary positions were lower than at the corners. This was caused by the small Ce segregation coefficient in the YAG single crystal and from the small convection in the meniscus. The scintillation properties of tube-Ce:YAG specimens were comparable with previously reported Ce:YAG single crystals.

    DOI: 10.35848/1882-0786/abc8ab

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  161. Continuous glucose monitoring in patients with remission of type 2 diabetes after laparoscopic sleeve gastrectomy without or with duodenojejunal bypass

    Sawada S., Kodama S., Tsuchiya S., Kurosawa S., Endo A., Sugawara H., Hosaka S., Kawana Y., Asai Y., Yamamoto J., Munakata Y., Izumi T., Takahashi K., Kaneko K., Imai J., Imoto H., Tanaka N., Naitoh T., Ishigaki Y., Katagiri H.

    Clinical Obesity   Vol. 10 ( 6 ) page: e12409   2020.12

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    Bariatric surgery is associated with a high remission rate of type 2 diabetes mellitus. However, it is unclear whether patients showing remission of diabetes actually have normal blood glucose levels throughout the day. We therefore performed continuous glucose monitoring (CGM) in 15 ambulatory patients showing remission of diabetes after laparoscopic sleeve gastrectomy (LSG) without or with duodenojejunal bypass (DJB) at the time of diabetic remission (12.9 ± 1.8 months after bariatric surgery). The definition of remission of diabetes was based on the American Diabetes Association criteria. The mean, SD, and coefficient of variation (CV) of glucose calculated from CGM were 6.2 ± 0.6 mmol/L, 1.5 ± 0.4 mmol/L, and 23.7 ± 6.2%, respectively. These values were higher than those of healthy participants without diabetes previously reported. The percentages of time spent above 10.0 mmol/L and below 3.9 mmol/L were 2.6 (IQR 0-5.0)% and 0 (IQR 0-8.0)%, respectively. Thus, patients with remission of diabetes after LSG or LSG/DJB still had substantial periods of hyperglycemia and hypoglycemia throughout the day. Therefore, we must manage patients with diabetes carefully, even after apparent remission of type 2 diabetes in response to bariatric surgery.

    DOI: 10.1111/cob.12409

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  162. Built environment correlates of objectively-measured sedentary behaviours in densely-populated areas Open Access

    Koohsari M.J., Shibata A., Ishii K., Kurosawa S., Yasunaga A., Hanibuchi T., Nakaya T., Mavoa S., McCormack G.R., Oka K.

    Health and Place   Vol. 66   page: 102447   2020.11

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    Few studies examine associations between objectively-calculated neighbourhood built environment attributes and objectively-assessed sedentary behaviour in different geographical locations, especially in highly-populated environments. Additionally, no study, to our knowledge, has investigated associations between objective measures of neighbourhood built environment attributes and objectively-assessed sedentary behaviours in middle-aged adults, despite the fact that this is a critical stage of life when age-related functional decline begins. We examined the associations between neighbourhood built environment attributes with the total, and patterns of, objectively-assessed sedentary behaviours in a densely-populated area in Asia. Data from 866 adults (ages 40 to 64) living in Japan were included. Four classifications of sedentary behaviours, including daily total sedentary time, duration and number of long (≥30 min) sedentary bouts and breaks per sedentary hour, were estimated using hip-worn accelerometers. Individual (population density, availability of destinations, number of intersections, and distance to the nearest park) and composite (walkability and Walk Score®) neighbourhood built environment indices were calculated using geographic information systems. Covariate-adjusted multilevel linear mixed effects models were used to estimate the associations between the neighbourhood built environment attributes and sedentary behaviours. Population density and availability of destinations were positively associated with sedentary behaviours; however, the number of intersections was negatively associated with sedentary behaviours. No associations were observed between the distance to the nearest park and sedentary behaviours. There were positive associations between walkability and total sedentary time, and duration and the number of long sedentary bouts. Walk Score® was positively associated with total sedentary time and the number of long sedentary bouts. These findings suggest that urban design attributes supportive of walking (except for the number of intersections) may encourage sedentary behaviour among middle-aged adults living in densely-populated environments.

    DOI: 10.1016/j.healthplace.2020.102447

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  163. Crystal growth and optical properties of a Ce2Si2O7 single crystal Open Access

    Horiai T., Kurosawa S., Murakami R., Shoji Y., Pejchal J., Yoshino M., Yamaji A., Sato H., Ohashi Y., Kamada K., Yokota Y., Yoshikawa A.

    Optical Materials   Vol. 109   2020.11

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    The scintillators with Ce luminescent centers are widely used for radiation detection. In this study, we focused on the Ce<inf>2</inf>Si<inf>2</inf>O<inf>7</inf> pyrosilicate scintillator and evaluated its optical and scintillation properties. From the result of the temperature dependence of quantum yield of Ce<inf>2</inf>Si<inf>2</inf>O<inf>7</inf> under excitation into the Ce<sup>3+</sup> 4f-5d<inf>1</inf> transition, it was revealed that at 300°C the Ce<inf>2</inf>Si<inf>2</inf>O<inf>7</inf> had a quantum yield of approximately 40% of that at the room. In addition, Ce<inf>2</inf>Si<inf>2</inf>O<inf>7</inf> had a light output of 9,400 ± 800 photons/MeV and fast decay time (~34 ns) at room temperature, and therefore, it has potential for application in radiation detection.

    DOI: 10.1016/j.optmat.2020.110210

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  164. Effects of La doping on the crystal growth, phase stability and scintillation properties of Lu<sub>3</sub>Al<sub>5</sub>O<sub>12</sub> single crystals

    Bartosiewicz, K; Horiai, T; Yamaji, A; Yoshikawa, A; Kurosawa, S; Yoshino, M; Zorenko, Y

    MATERIALS SCIENCE AND ENGINEERING B-ADVANCED FUNCTIONAL SOLID-STATE MATERIALS   Vol. 261   2020.11

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    The growth process, crystal composition, optical and scintillation properties of Lu<inf>3</inf>Al<inf>5</inf>O<inf>12</inf>:La (La = 0–0.45%) single crystals were investigated in detail. The thermodynamical stability of the garnet phase formation was studied in the undoped and La doped Lu<inf>3</inf>Al<inf>5</inf>O<inf>12</inf> single crystals. The crystals were grown from the melt using a micro-pulling down method. Detailed composition analysis reviled the complex multiphase character of the samples. Both garnet and α-Al<inf>2</inf>O<inf>3</inf> phases were detected in the undoped and slightly La-doped samples, while heavily La-doped crystals contained the mixture of α-Al<inf>2</inf>O<inf>3</inf>, garnet and perovskites phases. The substitution La for Lu led to the formation of La<inf>Lu</inf> centers and increased the concentration of Lu<inf>Al</inf> antisite defects. Both types of centers caused a strong luminescence in the deep UV spectral range. Heavy La-doping significantly enhanced the scintillation performance of Lu<inf>3</inf>Al<inf>5</inf>O<inf>12</inf> crystals.

    DOI: 10.1016/j.mseb.2020.114677

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  165. New Efficient Scintillating and Photoconversion Materials Based on the Self-Flux Grown Tb<sub>3</sub>Al<sub>5</sub>O<sub>12</sub>:Ce Single Crystal

    Bartosiewicz, K; Markovskyi, A; Zorenko, T; Yoshikawa, A; Kurosawa, S; Yamaji, A; Zorenko, Y

    PHYSICA STATUS SOLIDI-RAPID RESEARCH LETTERS   Vol. 14 ( 11 )   2020.11

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    This research deals with a novel approach for the self-flux growth of Tb<inf>3</inf>Al<inf>5</inf>O<inf>12</inf>:Ce single crystal using the micro-pulling-down method. The self-flux method enables the fabrication of the crystals with excellent photoconversion and scintillation properties. Tb<inf>3</inf>Al<inf>5</inf>O<inf>12</inf>:Ce (TbAG:Ce) efficiently converts the blue light-emitting diode (LED) radiation into bright white light. The gradual change of crystal thicknesses (0.2–1 mm) allows for tuning white light temperature from cold to neutral white. The scintillation response is comparable with that of a high-quality single crystalline film counterpart with a light yield value of around 4500 photons MeV<sup>−1</sup> under α particle excitation from 239 Pu radioisotope. This is the highest value obtained for the TbAG:Ce crystal yet.

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  166. Stress and coping strategies among allogeneic haematopoietic stem cell transplantation survivors: A qualitative study

    Kusaka, K; Inoguchi, H; Nakahara, R; Kurosawa, S; Fukuda, T; Satomura, K; Shimizu, K

    EUROPEAN JOURNAL OF CANCER CARE   Vol. 29 ( 6 ) page: e13307   2020.11

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    Objective: The aim of this qualitative study was to explore allogeneic haematopoietic stem cell transplantation (allo-HSCT) survivors' perspectives of stresses and their coping strategies, in order to attain a deeper understanding of their experience. Methods: We conducted semi-structured interviews with 20 Japanese allo-HSCT survivors about the stresses they experienced and how they coped. We then conducted a content-driven thematic analysis of the interview results. The interview questions probed stresses and coping strategies related to allo-HSCT. Results: We identified 74 stresses across 7 domains: symptoms after transplantation, limitations in daily life, appearance changes, relationship anxieties, work impairment and financial issues, uncertainty and disappointed expectations. In addition, 21 coping strategies were identified across 3 domains: direct efforts to manage problems, adaptive attitude, and seeking and using social support. Conclusion: By identifying a broad range of stressors associated with allo-HSCT, insight was gained as to the impact of allo-HSCT on survivors' lives. These results provide a foundation for the future development of resources for survivors, their significant others and clinicians. Stressors and coping strategies among allo-HSCT survivors were comprehensively characterised, which will provide useful information for patients and enable healthcare practitioners to provide better care.

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  167. Dog ownership and adults' objectively-assessed sedentary behaviour and physical activity Open Access

    Koohsari, MJ; Shibata, A; Ishii, K; Kurosawa, S; Yasunaga, A; Hanibuchi, T; Nakaya, T; McCormack, GR; Oka, K

    SCIENTIFIC REPORTS   Vol. 10 ( 1 ) page: 17487   2020.10

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    Evidence suggests a positive effect of dog ownership on physical activity. However, most previous studies used self-reported physical activity measures. Additionally, it is unknown whether owning a dog is associated with adults’ sedentary behaviour, an emerging health risk factor. In this study, physical activity and sedentary behaviour were objectively collected between 2013 and 2015 from 693 residents (aged 40–64 years) living in Japan using accelerometer devices. Multivariable linear regression models were used, adjusted for several covariates. The means of total sedentary time and the number of long (≥ 30 min) sedentary bouts were 26.29 min/day (95% CI − 47.85, − 4.72) and 0.41 times/day (95% CI − 0.72, − 0.10) lower for those who owned a dog compared to those not owning a dog, respectively. Compared with non-owners, dog-owners had significantly higher means of the number of sedentary breaks (95% CI 0.14, 1.22), and light-intensity physical activity (95% CI 1.31, 37.51). No significant differences in duration of long (≥ 30 min) sedentary bouts, moderate, vigorous, and moderate-to-vigorous-intensity physical activity were observed between dog-owners and non-owners. A novel finding of this study is that owning a dog was associated with several types of adults’ sedentary behaviours but not medium-to-high-intensity physical activities. These findings provide new insights for dog-based behavioural health interventions on the benefits of dog ownership for reducing sedentary behaviour.

    DOI: 10.1038/s41598-020-74365-6

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  168. Light Yield and Timing Characteristics of Lu.Gd.(Al5-xGax)O:Ce,Mg Single Crystals

    Sakthong O., Chewpraditkul W., Pattanaboonmee N., Chewpraditkul W., Yamaji A., Kamada K., Kurosawa S., Yoshikawa A., Witkowski M., Drozdowski W., Szczesniak T., Moszynski M., Babin V., Nikl M.

    IEEE Transactions on Nuclear Science   Vol. 67 ( 10 ) page: 2295 - 2299   2020.10

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    The scintillation characteristics of Lu0.8Gd2.2 (Al5-xGax)O12:Ce,Mg ( $x = 2.6$ and 3) single crystals grown by the micropulling down method are investigated. The light yield of 27600 photons/MeV obtained for Lu0.8Gd2.2Al2Ga3O12:Ce,Mg is higher than that of 25 400 photons/MeV obtained for Lu0.8Gd2.2Al2.4Ga2.6O12:Ce,Mg. The photoluminescence and scintillation decays measured at room temperature (RT) for Lu0.8Gd2.2Al2Ga3O12:Ce,Mg are faster than those for Lu0.8Gd2.2Al2.4Ga2.6O12:Ce,Mg. Temperature dependence of radioluminescence (RL) intensity indicates a lower quenching temperature for Lu0.8Gd2.2Al2Ga3O12:Ce,Mg. Coincidence time resolution of a Lu0.8Gd2.2Al2Ga3O12:Ce,Mg detector in coincidence experiment with a BaF2 detector was measured to be 410 ps. The afterglow and thermally stimulated luminescence (TSL) characteristics below RT are also measured.

    DOI: 10.1109/TNS.2020.3005410

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  169. Effect of thickness ratio of double layered thickness-shear resonator on temperature characteristics of resonance frequency

    Owada Y., Ohashi Y., Omote M., Yokota Y., Kurosawa S., Kamada K., Sato H., Toyoda S., Yamaji A., Yoshino M., Hanada T., Yoshikawa A.

    IEEE International Ultrasonics Symposium Ius   Vol. 2020-September   2020.9

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    The factor dictating the temperature characteristic of the double layered thickness-shear resonator was investigated by evaluating the resonators with different thickness ratios. Using Ca3TaGa3Si2O14[CTGS], one of the Langasite-type piezoelectric single crystal, double layered resonators with thickness ratios x = 0.25 and 0.5 were fabricated and the temperature dependence of their resonance frequency were measured at -30 to 80°C. As a result, the temperature characteristics for the resonator with x = 0.25 exhibited different profiles depending on the order of resonance mode, on the other hand, those for the resonator with x = 0.5 exhibited no difference among all of the order. Comparing these results with the wave propagation model in the resonator, it was found that the thickness ratio of two layers at the region effectively contributing to the electric field output was deeply related to the deviation of the temperature characteristics.

    DOI: 10.1109/IUS46767.2020.9251706

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  170. Fast Scanning Method for Measuring Material Homogeneity using the Line-Focus-Beam Ultrasonic-Material-Characterization System

    Ohashi Y., Yokota Y., Yamaji A., Yoshino M., Kurosawa S., Kamada K., Sato H., Toyoda S., Yoshikawa A.

    IEEE International Ultrasonics Symposium Ius   Vol. 2020-September   2020.9

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    A new method for measuring material homogeneity using fast scanning technique was proposed and demonstrated with the line-focus-beam ultrasonic-material-characterization (LFB-UMC) system. Similar velocity profiles of leaky surface acoustic wave (LSAW) for a Ca3Ta(Ga0.75Al0.25)3Si2O14[CTGAS] single crystal specimen were successfully obtained by both of the new V(x) and the conventional V(z) methods. We have verified the new V(x) method was 56 times faster than the conventional V(z) method. Although the V(z) method is superior to the V(x) method in a viewpoint of measurement accuracy, the V(x) method has great advantage enabling us to quickly evaluate material homogeneity over the wide area of specimen.

    DOI: 10.1109/IUS46767.2020.9251779

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  171. Outcome of Allogeneic Hematopoietic Stem Cell Transplantation in Patients with Myelodysplastic/Myeloproliferative Neoplasms-Unclassifiable: A Retrospective Nationwide Study of the Japan Society for Hematopoietic Cell Transplantation Open Access

    Kurosawa, S; Shimomura, Y; Tachibana, T; Ishiyama, K; Ota, S; Kobayashi, T; Uchida, N; Fukushima, K; Ashida, T; Matsuoka, K; Kanda, J; Ichinohe, T; Atsuta, Y; Murata, M; Aoki, J

    BIOLOGY OF BLOOD AND MARROW TRANSPLANTATION   Vol. 26 ( 9 ) page: 1607 - 1611   2020.9

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    To date, there are no data focusing on outcomes of allogeneic hematopoietic stem cell transplantation (allo-HSCT) in patients with myelodysplastic/myeloproliferative neoplasms, unclassifiable (MDS/MPN-U). This study aimed to evaluate outcomes and prognostic factors in patients with MDS/MPN-U after allo-HSCT using Japanese nationwide registry data. The primary endpoint was 3-year overall survival (OS); secondary endpoints included the cumulative incidence of relapse and nonrelapse mortality (NRM). We evaluated the prognostic factors for 3-year OS by univariate analysis using the log-rank test. In our cohort of 86 patients with MDS/MPN-U, we found a 3-year OS of 48.5%, cumulative incidence of relapse of 23.7%, and NRM of 26.3%. The 3-year OS was significantly worse in patients age ≥50 years compared with those age <50 years (38.1% versus 65.0%; P = .049) and in patients with disease progression compared with those without disease progression (28.4% versus 57.2%; P = .042). Our results suggest that allo-HSCT may offer a curative option for patients with MDS/MPN-U, and that age and disease status could be important indicators in helping clinicians determine treatment options for these patients.

    DOI: 10.1016/j.bbmt.2020.05.013

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  172. Optical Evaluation of Divalent and Trivalent Eu Ions Doped in CaF<sub>2</sub>Crystals Using Multiphoton Luminescence 3D Distribution Measurements

    Ito, H; Tanaka, M; Ono, S; Yamaji, A; Kurosawa, S; Yoshikawa, A

    PHYSICA STATUS SOLIDI B-BASIC SOLID STATE PHYSICS   Vol. 257 ( 8 )   2020.8

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    Eu-doped CaF<inf>2</inf> is studied for use as a scintillator. Herein, the 3D spatial distribution of Eu ions doped in CaF<inf>2</inf> crystal is evaluated. It is confirmed that both divalent and trivalent Eu ions are doped in CaF<inf>2</inf> crystals from the luminescence spectra of the Eu-doped CaF<inf>2</inf> crystals. Using bandpass filter, the 3D spatial distribution of divalent and trivalent Eu ions is measured, respectively. The 3D spatial distribution of divalent Eu ions with ionic radius larger than that of Ca site is nonuniform with mesh-like pattern. In contrast, the 3D spatial distribution of trivalent Eu ions with ionic radius smaller than that of Ca site is uniform. In Eu-doped CaF<inf>2</inf> crystals grown by micropulling down method, strain caused by the difference in lattice constants between CaF<inf>2</inf> and a seed crystal is confirmed.

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  173. Relationship Between Li/Ce Concentration and the Luminescence Properties of Codoped Gd<sub>3</sub>(Ga, Al)<sub>5</sub>O<sub>12</sub>:Ce

    Yoshino, M; Bartosiewicz, K; Horiai, T; Kamada, K; Yamaji, A; Shoji, Y; Yokota, Y; Kurosawa, S; Ohashi, Y; Sato, H; Toyoda, S; Kucerkova, R; Jary, V; Nikl, M; Yoshikawa, A

    PHYSICA STATUS SOLIDI B-BASIC SOLID STATE PHYSICS   Vol. 257 ( 8 )   2020.8

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    Li<sup>+</sup> codoping of Gd<inf>3</inf>(Ga, Al)<inf>5</inf>O<inf>12</inf>:Ce (GGAG:Ce) single crystals induces the acceleration of scintillation decay time. However, its effect on the scintillation properties of GGAG:Ce remains poorly understood. Herein, the relationship between Ce/Li concentration and scintillation properties is investigated. GGAG crystals with a range of Ce and Li concentrations are grown by the Czochralski method and the scintillation decay and light output of GGAG:Ce, Li are measured. The results show comparable or improved performance compared with conventional scintillators. In optical absorption and photoluminescence (PL) measurements, the conversion of the stable Ce<sup>3+</sup> to Ce<sup>4+</sup> is not observed in a clear manner in GGAG:Ce samples with variable Li concentration. Instead, some defect-related absorption seems to appear. Temperature dependence of PL decay for samples with variable Ce concentration is also evaluated. A shift of the luminescence quenching temperature is observed for GGAG samples with >0.2% Ce.

    DOI: 10.1002/pssb.201900504

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  174. Research on Efficient Fast Scintillators: Evidence and X-Ray Absorption Near Edge Spectroscopy Characterization of Ce<SUP>4+</SUP> in Ce<SUP>3+</SUP>, Mg<SUP>2+</SUP>-Co-Doped Gd<sub>3</sub>Al<sub>2</sub>Ga<sub>3</sub>O<sub>12</sub> Garnet Crystal Open Access

    Dantelle, G; Boulon, G; Guyot, Y; Testemale, D; Guzik, M; Kurosawa, S; Kamada, K; Yoshikawa, A

    PHYSICA STATUS SOLIDI B-BASIC SOLID STATE PHYSICS   Vol. 257 ( 8 )   2020.8

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    Herein, the most advanced oxide scintillator Ce<sup>3+</sup>, Mg<sup>2+</sup>-co-doped Gd<inf>3</inf>Al<inf>2</inf>Ga<inf>3</inf>O<inf>12</inf> (GAGG) garnet host, grown using the Czochralski method is reported. The charge transfer absorption band in UV, such as in other Ce<sup>3+</sup>, Mg<sup>2+</sup>-co-doped oxides, reveals the creation of stable Ce<sup>4+</sup> oxidation state, in addition to the usual Ce<sup>3+</sup> one, admitted as responsible of the scintillation mechanism improvement displayed by this garnet. Strangely, the confirmation of quantitative values of Ce<sup>4+</sup> concentration has never been done, and the goal is mainly focused on the presence of Ce<sup>4+</sup> and the evaluation of the Ce<sup>3+</sup>/Ce<sup>4+</sup> ratio measured by X-ray absorption near edge spectroscopy (XANES) spectroscopy at the Ce L<inf>III</inf> threshold of the European Synchrotron Radiation Facility (ESRF). This result is compared with those obtained for Ce<sup>3+</sup>, Mg<sup>2+</sup>-co-doped Lu<inf>3</inf>Al<inf>5</inf>O<inf>12</inf> (LuAG) and, also, in garnets without any Mg<sup>2+</sup> ions such as Ce<sup>3+</sup>-doped GAGG, Ce<sup>3+</sup>-doped LuAG, and Ce<sup>3+</sup>-doped YAG. The role of Li<sup>+</sup> ion in place of Mg<sup>2+</sup> one is also considered in Ce<sup>3+</sup>, Li<sup>+</sup>-co-doped LuAG single crystal.

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  175. Single-crystal growth, structure and luminescence properties of Cs<sub>2</sub>HfCl<sub>3</sub>Br<sub>3</sub>

    Kodama, S; Kurosawa, S; Fujii, K; Murakami, T; Yashima, M; Pejchal, J; Král, R; Nikl, M; Yamaji, A; Yoshino, M; Toyoda, S; Sato, H; Ohashi, Y; Kamada, K; Yokota, Y; Yoshikawa, A

    OPTICAL MATERIALS   Vol. 106   2020.8

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    Single crystal of the mixed-halogen compound Cs<inf>2</inf>HfCl<inf>3</inf>Br<inf>3</inf> was grown by the vertical Bridgman method, and we investigated its crystal structure and optical properties. Single-crystal X-ray diffraction and energy dispersive X-ray spectroscopy analyses indicated the chemical composition to be Cs<inf>2</inf>Hf(Cl<inf>0.578(6)</inf>Br<inf>0.422(6)</inf>)<inf>6</inf> (= Cs<inf>2</inf>HfCl<inf>3.47(4)</inf>Br<inf>2.53(4)</inf>, approximately Cs<inf>2</inf>Hf(Cl<inf>0</inf> <inf>58</inf>Br<inf>0.42</inf>)<inf>6</inf>) where the number in the parentheses denotes the estimated standard deviation in the last digit. Cs<inf>2</inf>Hf(Cl<inf>0.58</inf>Br<inf>0.42</inf>)<inf>6</inf> was found to have a cubic Fm3‾m potassium hexachloroplatinate structure consisting of Cs<sup>+</sup> cations and Hf(Cl<inf>0</inf> <inf>.</inf> <inf>58</inf>Br<inf>0.42</inf>)<inf>6</inf> <sup>2−</sup> anions. The emission peak of Cs<inf>2</inf>HfCl<inf>3</inf>Br<inf>3</inf> was red-shifted by Br substitution, and the photoluminescence decays of Cs<inf>2</inf>HfCl<inf>3</inf>Br<inf>3</inf> were accelerated when compared to those of Cs<inf>2</inf>HfCl<inf>6</inf>. Cs<inf>2</inf>HfCl<inf>3</inf>Br<inf>3</inf> had an emission peak at 450 nm under X-ray irradiation, while under UV-excitation, two photoluminescence emission peaks at 420 and 525 nm were observed. The decay profile of the 420-nm emission band had a single-exponential component with a decay time of 1.95 ± 0.01 μs under the 280-nm-excitation. On the other hand, 525-nm-emisison had two decay components of 0.28 ± 0.03 μs (11%) and 6.54 ± 0.03 μs (89%) under 305-nm-photons excitation.

    DOI: 10.1016/j.optmat.2020.109942

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  176. Thermal analysis of cesium hafnium chloride using DSC-TG under vacuum, nitrogen atmosphere, and in enclosed system

    Král, R; Zemenová, P; Vanecek, V; Bystricky, A; Kohoutková, M; Jary, V; Kodama, S; Kurosawa, S; Yokota, Y; Yoshikawa, A; Nikl, M

    JOURNAL OF THERMAL ANALYSIS AND CALORIMETRY   Vol. 141 ( 3 ) page: 1101 - 1107   2020.8

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    This paper reports on the preparation of undoped cesium hafnium chloride (Cs<inf>2</inf>HfCl<inf>6</inf>) and study of its thermal properties. The Cs<inf>2</inf>HfCl<inf>6</inf> is considered, due to its excellent scintillation properties, as a promising candidate for cost-effective radiation detectors with potential to replace traditional halide scintillators, e.g., NaI:Tl and CsI:Tl. The Cs<inf>2</inf>HfCl<inf>6</inf> material was successfully synthesized from a cesium chloride and a hafnium chloride mixed together in stoichiometric ratio. The presence of only one crystalline phase of the Cs<inf>2</inf>HfCl<inf>6</inf> in the material was confirmed by the X-ray diffraction analysis. The simultaneous non-isothermal differential scanning calorimetry and thermogravimetry (DSC–TG) of the synthesized material under nitrogen atmosphere, vacuum, and in enclosed system was performed. The Cs<inf>2</inf>HfCl<inf>6</inf> decomposition and melting of CsCl–Cs<inf>2</inf>HfCl<inf>6</inf> mixture under nitrogen and vacuum were observed. On the contrary, the DSC measurement of the cesium hafnium chloride in enclosed system showed only one endothermic peak related to the congruent melting point. Furthermore, the repeated DSC–TG measurements to investigate the materials’ stability in enclosed system were carried out as well.

    DOI: 10.1007/s10973-019-09087-7

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  177. The prognostic impact of <i>FLT3</i>-ITD, <i>NPM1</i> and <i>CEBPa</i> in cytogenetically intermediate-risk AML after first relapse

    Kurosawa, S; Yamaguchi, H; Yamaguchi, T; Fukunaga, K; Yui, S; Kanamori, H; Usuki, K; Uoshima, N; Yanada, M; Takeuchi, J; Mizuno, I; Kanda, J; Okamura, H; Yano, S; Tashiro, H; Shindo, T; Chiba, S; Tomiyama, J; Inokuchi, K; Fukuda, T

    INTERNATIONAL JOURNAL OF HEMATOLOGY   Vol. 112 ( 2 ) page: 200 - 209   2020.8

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    We evaluated the impact of FLT3-ITD, NPM1 mutations, and double mutant CEBPa (dmCEBPa) on overall survival (OS) after relapse in patients with cytogenetically intermediate-risk acute myeloid leukemia (AML) who were treated with chemotherapy alone in the first remission (CR1). Patients aged 16–65 years diagnosed with cytogenetically intermediate-risk AML, and who achieved CR1 were included. We retrospectively analyzed FLT3-ITD, NPM1 mutations and CEBPa using samples obtained at diagnosis, which therefore did not affect the therapeutic decisions. Among 235 patients who had achieved CR1, 152 relapsed, and 52% of them achieved second CR. The rate of achieving second CR was significantly higher (85%) in those with dmCEBPa. Patients with FLT3-ITD had significantly worse OS after relapse than those without (19% vs 41%, p = 0.002), while OS was comparable between patients with and without NPM1 mutations (37% vs 34%, p = 0.309). Patients with dmCEBPa had improved OS than those without (61% vs 32%, p = 0.006). By multivariate analysis, FLT3-ITD was independently associated with worse OS after relapse [hazard ratio (HR) 1.99, 95% CI 1.27–3.12, p = 0.003], and dmCEBPa with improved OS (HR 0.40, 95% CI 0.17–0.93, p = 0.033). Our data show that screening for these mutations at diagnosis is useful for facilitating effective therapeutic decision-making even after relapse.

    DOI: 10.1007/s12185-020-02894-x

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  178. Guanidyl modification of the 1-azabicyclo[3.1.0]hexane ring in ficellomycin essential for its biological activity.

    Kurosawa S, Matsuda K, Hasebe F, Shiraishi T, Shin-Ya K, Kuzuyama T, Nishiyama M

    Organic & biomolecular chemistry   Vol. 18 ( 27 ) page: 5137 - 5144   2020.7

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    DOI: 10.1039/d0ob00339e

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  179. Development of double layered thickness-shear resonator using langasite-type piezoelectric single crystal

    Owada, Y; Ohashi, Y; Omote, M; Yokota, Y; Kurosawa, S; Kamada, K; Sato, H; Toyoda, S; Yoshino, M; Yamaji, A; Yoshikawa, A

    JAPANESE JOURNAL OF APPLIED PHYSICS   Vol. 59 ( SK )   2020.7

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    A novel device structure "double layered thickness-shear resonator" was proposed to improve the temperature characteristics of a bulk acoustic wave resonator. In order to design the double layered resonator, optimal combination of cut angles and thickness ratio of the substrates were determined from calculations using material constants and their temperature coefficients measured for a Ca<inf>3</inf>TaGa<inf>3</inf>Si<inf>2</inf>O<inf>14</inf> (CTGS) single crystal. Based on the results, a double layered resonator was fabricated by directly bonding two CTGS substrates with cut angles of 122°Y and 171°Y under the thickness ratio of 0.248. As a result, the double layered resonator operated successfully at a fundamental mode of around 7.5 MHz like a normal resonator exhibiting temperature compensation effect. The mechanism of the deviation from the expected value observed in the measured temperature dependence of the frequency changes was discussed using the model of the wave propagation and the electric field generated in the double layer structure.

    DOI: 10.35848/1347-4065/ab80da

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  180. Growth and Scintillation Properties of Directionally Solidified Ce:LaBr<sub>3</sub>/AEBr<sub>2</sub>(AE = Mg, Ca, Sr, Ba) Eutectic System Open Access

    Kim, KJ; Furuya, Y; Kamada, K; Murakami, R; Kochurikhin, VV; Yoshino, M; Chiba, H; Kurosawa, S; Yamaji, A; Shoji, Y; Toyoda, S; Sato, H; Yokota, Y; Ohashi, Y; Yoshikawa, A

    CRYSTALS   Vol. 10 ( 7 ) page: 1 - 9   2020.7

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    Publisher:Crystals  

    Ce-doped LaBr<inf>3</inf> /AEBr<inf>2</inf> (AE = Mg, Ca, Sr, Ba) eutectics were grown using the Bridgman–Stockbarger (BS) method in quartz ampoules. The eutectics (AE = Mg and Ca) showed optical transparency like optical fiber bundles. A grown Ce-doped LaBr<inf>3</inf> /MgBr<inf>2</inf> eutectic shows a 355 nm emission ascribed to Ce<sup>3+</sup> 4f-5d transition under X-ray excitation. The smaller the ionic size of AE, the higher the light yield of the sample was. The light yield of Ce:LaBr<inf>3</inf> /MgBr<inf>2</inf> was 34,300 photon/MeV, which is higher than Ce:LYSO standard. Scintillation decay time under 662 keV gamma-ray excitation was 18.8 ns.

    DOI: 10.3390/cryst10070584

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  181. Growth of Lu<sub>2</sub>O<sub>3</sub>and HfO<sub>2</sub>Based High Melting Temperature Single Crystals by Indirect Heating Method Using Arc Plasma Open Access

    Kim, KJ; Kamada, K; Murakami, R; Horiai, T; Ishikawa, S; Kochurikhin, VV; Yoshino, M; Yamaji, A; Shoji, Y; Kurosawa, S; Toyoda, S; Sato, H; Yokota, Y; Ohashi, Y; Yoshikawa, A

    CRYSTALS   Vol. 10 ( 7 ) page: 1 - 8   2020.7

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    A novel single-crystal growth method was developed, using arc plasma and metal melt, for a quick survey of high melting point materials. Single crystals of Yb-doped Lu<inf>2</inf>O<inf>3</inf>, Lu<inf>0.388</inf>Hf<inf>0.612</inf>O<inf>1.806</inf>, and Lu<inf>0.18</inf>Hf<inf>0.82</inf>O<inf>1.91</inf>, with melting points of 2460, 2900, and 2840<sup>◦</sup>C, respectively, were grown by an indirect heating method using arc plasma. We refer to this indirect heating growth method as the core heating (CH) method. The CH-grown Yb1%-doped Lu<inf>2</inf>O<inf>3</inf> sample showed a full width at half maximum of 286 arcsec in the X-ray rocking curve. This value is better than the 393 arcsec obtained for the crystal grown by the micro-pulling-down (µ-PD) method. The Yb charge transfer state (CTS) emission was observed at 350 nm in the Yb1%-doped Lu<inf>2</inf>O<inf>3</inf> and Lu<inf>0.18</inf>Hf<inf>0.82</inf>O<inf>1.91</inf>. In the case of the µ-PD method, using a rhenium (Re) crucible, absorption due to Re contamination and a resulting reduction in the Yb CTS emission were confirmed. However, contamination did not influence the properties observed in the crystals grown by the CH method.

    DOI: 10.3390/cryst10070619

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  182. Vascular resistance of carotid and vertebral arteries is associated with retinal microcirculation measured by laser speckle flowgraphy in patients with type 2 diabetes mellitus

    Sawada, S; Tsuchiya, S; Kodama, S; Kurosawa, S; Endo, A; Sugawara, H; Hosaka, S; Kawana, Y; Asai, Y; Yamamoto, J; Munakata, Y; Izumi, T; Takahashi, K; Kaneko, K; Imai, J; Ito, A; Yasuda, M; Kunikata, H; Nakazawa, T; Katagiri, H

    DIABETES RESEARCH AND CLINICAL PRACTICE   Vol. 165   page: 108240   2020.7

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    Aims: Evaluation of the retinal microcirculation is key to understanding retinal vasculopathies, such as diabetic retinopathy. Laser speckle flowgraphy (LSFG) has recently enabled us to directly evaluate the vascular resistance in both retinal vessels and capillaries, non-invasively. We therefore assessed whether retinal vessel blood flow and/or the capillary microcirculation are associated with blood flow in the cervical arteries in diabetic patients without severe retinopathy. Methods: We enrolled 110 type 2 diabetes patients, with no or mild non-proliferative diabetic retinopathy, in this prospective cross-sectional study. We measured the resistivity indices (RIs) of the retinal vessel and capillaries by LSFG and those of cervical arteries by Doppler ultrasonography, followed by analyzing associations. Results: The RIs of not only the carotid but also vertebral arteries were associated with those of retinal vessel blood flow and the retinal capillary microcirculation. Multiple regression analyses revealed these associations to be independent of other explanatory variables including age and diabetes duration. Conclusions: We obtained novel and direct evidence demonstrating a close association between the retinal microcirculation and cervical artery hemodynamics in diabetic patients. These findings suggest shared mechanisms to underlie micro- and macro-angiopathies. Thus, high vascular resistance of cervical arteries may be a risk of developing retinopathy.

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  183. Tungsten co -doping effects on Ce:Gd 3 Ga 3 Al 2 O 12 scintillator grown by the micro -pulling down method

    Ueno, M; Kim, KJ; Kamada, K; Nihei, T; Yoshino, M; Yamaji, A; Toyoda, S; Sato, H; Yokota, Y; Kurosawa, S; Ohashi, Y; Nikl, M; Kochurikhin, V; Yoshikawa, A

    JOURNAL OF CRYSTAL GROWTH   Vol. 539   2020.6

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  184. Tungsten co-doping effects on Ce:Gd3Ga3Al2O12 scintillator grown by the micro-pulling down method

    Ueno M., Kim K.J., Kamada K., Nihei T., Yoshino M., Yamaji A., Toyoda S., Sato H., Yokota Y., Kurosawa S., Ohashi Y., Nikl M., Kochurikhin V., Yoshikawa A.

    Journal of Crystal Growth   Vol. 539   2020.6

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    Single crystal scintillators are extensively used in various radiation detection applications and their scintillation performances can be improved via co-doping. Therefore, in this study, tungsten-ion co-doped Ce:Gd<inf>3</inf>(Ga,Al)<inf>5</inf>O<inf>12</inf> (Ce:GGAG) crystals were grown using the micro-pulling-down (μ-PD) method to investigate the effects of co-doping on their scintillation properties. The relationships between the W concentration, optical and luminescence properties, and radiation response of the W-co-doped Ce:GGAG crystals were evaluated. The W-co-doped Ce 0.5%:Gd<inf>3</inf>Ga<inf>3</inf>Al<inf>2</inf>O<inf>12</inf> single crystals of diameter 3 mm and length 30–60 mm were grown by the μ-PD method. The light yield increased at W concentrations of 200 and 500 ppm and decreased at W concentrations above 1000 ppm. There was no significant change in the fast decay component of scintillation.

    DOI: 10.1016/j.jcrysgro.2020.125513

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  185. Bulk Single Crystal Growth of W Co-Doped Ce:Gd<sub>3</sub>Ga<sub>3</sub>Al<sub>2</sub>;O<sub>12</sub> by Czochralski Method

    Ueno, M; Kim, KJ; Kamada, K; Babin, V; Nikl, M; Nihei, T; Yoshino, M; Yamaji, A; Toyoda, S; Sato, H; Yokota, Y; Kurosawa, S; Ohashi, Y; Kochurikhin, VV; Yoshikawa, A

    IEEE TRANSACTIONS ON NUCLEAR SCIENCE   Vol. 67 ( 6 ) page: 1045 - 1048   2020.6

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    Publisher:IEEE Transactions on Nuclear Science  

    Effects of the tungsten (W) ions co-doping on the crystal growth, optical and scintillation properties for the Czochralski (Cz) grown Ce:Gd3Ga3Al2O12(GGAG) single crystals were investigated. The W 0%, 0.1%, 0.3%, 1%, and 5% co-doped Ce 1%:GGAG single crystals with a diameter of 1 in and length of 60-80 mm were grown by the Cz method. The effective segregation coefficient of the W ions was found as 0.002, 0.001, and 0.005 for W 0.1%, 0.3%, and 1%, Ce:GGAG, respectively. The segregation of W ions in GGAG host, light yield, and scintillation decay of the W co-doped Ce:GGAG were evaluated. The light yield decreased as the concentration of W co-dopant increased and toward the tail of the crystal. Furthermore, the defect role and related charge trapping in the W co-doped crystals were monitored by the thermo-stimulated luminescence.

    DOI: 10.1109/TNS.2020.2968088

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  186. Crystal Growth and Scintillation Properties of Carbazole for Neutron Detection

    Yamaji, A; Yamato, S; Kurosawa, S; Yoshino, M; Toyoda, S; Kamada, K; Yokota, Y; Sato, H; Ohashi, Y; Yoshikawa, A

    IEEE TRANSACTIONS ON NUCLEAR SCIENCE   Vol. 67 ( 6 ) page: 1027 - 1031   2020.6

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    Carbazole crystals were grown using self-seeding vertical Bridgman technique, and the scintillation properties for neutron detection were investigated. Results of powder X-ray diffraction (XRD) and Fourier transform infrared spectroscopy (FTIR) analyses indicated the single phase of the grown carbazole crystal with orthorhombic structure. Photo-and radio-luminescence measurements were carried out, and maxima of both emission peaks were at 420 nm. The light yield under 5.5-MeV alpha-ray irradiation was estimated to be 1.87 times higher than that of lithium glass GS-20. The scintillation decay time under neutron irradiation was estimated to be 11.4 ± 0.3 ns. It follows from the temperature dependence measurements that the light output under 662-keV gamma-ray excitation decreases with increasing temperature.

    DOI: 10.1109/TNS.2020.2996276

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  187. Conference Comments by the Editors Open Access

    Yoshikawa A., Nikl M., Williams R.T., Bizarri G., Fasoli M., Gundacker S., Jary V., Korzhik M., Kurosawa S., Wu Y.

    IEEE Transactions on Nuclear Science   Vol. 67 ( 6 )   2020.6

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    DOI: 10.1109/TNS.2020.2998652

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  188. Composite Scintillators Based on the Films and Crystals of (Lu,Gd,La)<sub>2</sub>Si<sub>2</sub>O<sub>7</sub> Pyrosilicates

    Kurosawa, S; Yoshikawa, A; Gorbenko, V; Zorenko, T; Witkiewicz-Lukaszek, S; Fedorov, A; Zorenko, Y

    IEEE TRANSACTIONS ON NUCLEAR SCIENCE   Vol. 67 ( 6 ) page: 994 - 998   2020.6

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    This article is directed on the creation of composite scintillators which are based on the films and crystals of R2Si2O7:Ce (R = Lu, Gd, La) pyrosilicates using the liquid phase epitaxy (LPE) growth method for application in the radiation monitoring of different components of mixed ionization fluxes. Such types of composite scintillators are epitaxial structures containing film scintillators grown by the LPE method onto the substrates of crystal scintillators. In this article, the film and crystal parts of the composite scintillators were fabricated from effective scintillation materials on the base of Ce3+ doped Gd2-xLuxSi2O7 and Gd2-xLaxSi2O7, and x = {0} and 0.25 mixed pyrosilicates with various scintillation decay kinetics due to the different Lu/Gd/La cation content. We briefly report on the results of the LPE growth of the composite scintillators based on the Ce3+ doped (Lu,Gd)2Si2O7 films and (Gd,La)2Si2O7:Ce crystal substrates, as well as the results of investigation of their luminescent and scintillation properties.

    DOI: 10.1109/TNS.2020.2983657

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  189. Development of Gamma-Ray Detector Arrays Consisting of Diced Eu-Doped SrI<sub>2</sub> Scintillator Arrays and TSV-MPPC Arrays

    Yoshino, M; Kamada, K; Shoji, Y; Yokota, Y; Kurosawa, S; Yamaji, A; Ohashi, Y; Sato, H; Fujieda, K; Kataoka, J; Yoshikawa, A

    IEEE TRANSACTIONS ON NUCLEAR SCIENCE   Vol. 67 ( 6 ) page: 999 - 1002   2020.6

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    This article presents the development of diced SrI2:Eu arrays and their scintillation properties when coupled with a multipixel photon counter (MPPC) array. Using a dicing technique specific to halide scintillators, a high-energy resolution scintillator array is developed that is cost-effective and widely applicable. The developed SrI2:Eu arrays are of 3 × 3 × 3 mm3/pixel 4 × 4 matrix (TYPE1) and 1 × 1 × 1 mm3/pixel 9 × 9 matrix (TYPE2) structures. We fabricated test gamma-ray detector modules consisting of the TYPE1 and TYPE2 arrays coupled with an MPPC array. The mean peak to valleys ratio is 85.3 ± 14.9 for the TYPE1 array and 38.5 ± 16.6 for the TYPE2 array detector. The average energy resolutions obtained for the TYPE1 and TYPE2 gamma-ray detectors were 5.4 ± 0.4% full-width at half-maximum (FWHM) and 5.2 ± 0.6% FWHM, respectively, for 662-keV gamma-rays. The variation in the signal pulse height of the TYPE1 and TYPE2 detectors was only 10.6% and 10.4% in FWHM, respectively. These results demonstrated that the dicing technique proposed in this article could be applied to hygroscopic halide scintillators.

    DOI: 10.1109/TNS.2020.2986460

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  190. Growth and Scintillation Properties of a New Red-Emitting Scintillator Rb<sub>2</sub>HfI<sub>6</sub> for the Fiber-Reading Radiation Monitor

    Kodama, S; Kurosawa, S; Morishita, Y; Usami, H; Torii, T; Hayashi, M; Sasano, M; Azuma, T; Tanaka, H; Kochurikhin, V; Pejchal, J; Král, R; Yoshino, M; Yamaji, A; Toyoda, S; Sato, H; Ohashi, Y; Yokota, Y; Kamada, K; Nikl, M; Yoshikawa, A

    IEEE TRANSACTIONS ON NUCLEAR SCIENCE   Vol. 67 ( 6 ) page: 1055 - 1062   2020.6

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    A new red-emitting halide scintillator Rb2HfI6 was developed using the vertical Bridgman furnace and quartz ampoule. Under X-ray irradiation, Rb2HfI6 had a broad emission band of around 725 nm. The light output and energy resolution were determined to be 40000 photons/MeV and 7.4% (full-width at half-maximum at 662 keV), respectively. Since red photons are transmitted with smaller losses than blue or yellow photons inside an optical fiber, a long-fiber-reading radiation detection system using the high light-output red scintillator can be established for severe or hazardous environments. We fabricated the Rb2HfI6 scintillation crystal and performed the gamma-ray detection test under high-dose irradiation condition from a 60Co source with an activity of 100 TBq. The dynamic range of the Rb2HfI6 gamma-ray detection with a 20-m optical fiber was evaluated and compared with the previously developed Cs2HfI6 crystal and the conventional deep-red Cr: α-Al2O3 (ruby) scintillator. The gamma-ray doses from 0.4 to 1 kSv/h were successfully measured using Rb2HfI6 through the 20-m fiber.

    DOI: 10.1109/TNS.2020.2976695

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  191. Luminescence and Scintillation Properties of Mg<SUP>2+</SUP>-Codoped Lu<sub>0.6</sub>Gd<sub>2.4</sub>Al<sub>2</sub>Ga<sub>3</sub>O<sub>12</sub>:Ce Single Crystal

    Chewpraditkul, W; Pattanaboonmee, N; Sakthong, O; Chewpraditkul, W; Yoshino, M; Horiai, T; Yoshikawa, A; Gushchina, L; Kamada, K; Kurosawa, S; Drozdowski, W; Witkowski, ME; Szczesniak, T; Moszynski, M; Nikl, M

    IEEE TRANSACTIONS ON NUCLEAR SCIENCE   Vol. 67 ( 6 ) page: 904 - 909   2020.6

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    The scintillation properties of Mg2+-codoped Lu0.6Gd2.4Al2Ga3O12:Ce (LGAGG:Ce,Mg) single crystal grown by Czochralski's method are investigated. The light yield (LY), scintillation decay time, and coincidence time resolution are presented in comparison with a GAGG:Ce,Mg reference crystal. The LY of 26 200 photons/MeV obtained for LGAGG:Ce,Mg is lower than that of 39 600 photons/MeV for GAGG:Ce,Mg. Despite a lower LY value, the time resolution of LGAGG:Ce,Mg is comparable to that of GAGG:Ce,Mg due to its faster scintillation decay time. LGAGG:Ce,Mg exhibits a much faster afterglow decay and a lower thermally stimulated luminescence intensity with respect to GAGG:Ce,Mg.

    DOI: 10.1109/TNS.2020.2984518

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  192. Measurement of the Anisotropic Response of the ZnWO<sub>4</sub> Crystal for Developing the Direction-Sensitive Dark Matter Detector Open Access

    Ichimura, K; Sekiya, H; Pedersen, JW; Yamaji, A; Kurosawa, S

    IEEE TRANSACTIONS ON NUCLEAR SCIENCE   Vol. 67 ( 6 ) page: 894 - 897   2020.6

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    We measured the scintillation light yield of ZnWO4 crystals using a quasi-monochromatic neutron beam energy of 865 keV. Irradiating the neutron beam on two surfaces, which are almost perpendicular to the crystal axis, the light yield of oxygen recoil was measured. The obtained light yield ratio of a neutron recoil to gamma-ray-induced electron recoil for two surfaces was 0.235 ± 0.026 and 0.199 ± 0.020, respectively, which corresponds to 15.3% of anisotropy for 200-keV nuclear recoils of this crystal. This property can be applied to a direction-sensitive dark matter (DM) detector.

    DOI: 10.1109/TNS.2020.2985027

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  193. Scintillation Characteristics of Mg<SUP>2+</SUP>-Codoped Y<sub>0.8</sub>Gd<sub>2.2</sub>(Al<sub>5-<i>x</i></sub>Ga<i><sub>x</sub></i>)O<sub>12</sub>:Ce Single Crystals

    Chewpraditkul, W; Pattanaboonmee, N; Chewpraditkul, W; Sakthong, O; Yamaji, A; Kamada, K; Kurosawa, S; Yoshikawa, A; Drozdowski, W; Witkowski, ME; Szczesniak, T; Grodzicka, M; Moszynski, M

    IEEE TRANSACTIONS ON NUCLEAR SCIENCE   Vol. 67 ( 6 ) page: 910 - 914   2020.6

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    Scintillation characteristics of Y<inf>0.8</inf>Gd<inf>2.2</inf> (Al<inf>5-x</inf>Ga<inf>x</inf>)O<inf>12</inf>:Ce,Mg ($x = 2.6$ and 3) single crystals are presented. At 662-keV $\gamma $-rays, the light yield of 35 600 photons/MeV obtained for Y<inf>0.8</inf>Gd<inf>2.2</inf>Al<inf>2</inf>Ga<inf>3</inf>O<inf>12</inf>:Ce,Mg is higher than that of 32 600 photons/MeV for Y<inf>0.8</inf>Gd<inf>2.2</inf>Al<inf>2.4</inf>Ga<inf>2</inf><inf>6</inf>O<inf>12</inf>:Ce,Mg. Scintillation decay components of 32.3 ns (52.4%) + 104 ns (47.6%) obtained for Y<inf>0.8</inf>Gd<inf>2.2</inf>Al<inf>2</inf>Ga<inf>3</inf>O<inf>12</inf>:Ce,Mg are faster than those of 11.5 ns (5%) + 51.2 ns (69%) + 302 ns (26%) obtained for Y<inf>0.8</inf>Gd<inf>2.2</inf>Al<inf>2.4</inf>Ga<inf>2</inf><inf>6</inf>O<inf>12</inf>:Ce,Mg. The coincidence time resolution of 336 and 389 ps was obtained, respectively, for Y<inf>0.8</inf>Gd<inf>2.2</inf>Al<inf>2</inf>Ga<inf>3</inf>O<inf>12</inf>:Ce,Mg-photomultiplier (PMT) and Y<inf>0.8</inf>Gd<inf>2.2</inf>Al<inf>2.4</inf>Ga<inf>2</inf><inf>6</inf>O<inf>12</inf>:Ce,Mg-PMT, in coincidence experiment with a BaF<inf>2</inf>-PMT detector. The radioluminescence yield at room temperature (RT) is comparable for both crystals while the yield below 130 K is about 20% higher for Y<inf>0.8</inf>Gd<inf>2.2</inf>Al<inf>2</inf>Ga<inf>3</inf>O<inf>12</inf>:Ce,Mg. Afterglow and thermally stimulated luminescence (TSL) below RT are also measured.

    DOI: 10.1109/TNS.2020.2975734

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  194. Current Status and Needs of Long-Term Follow-Up Clinics for Hematopoietic Cell Transplantation Survivors: Results of a Nationwide Survey in Japan Open Access

    Kurosawa, S; Mori, A; Tsukagoshi, M; Onishi, Y; Ohwada, C; Mori, T; Goto, H; Asano-Mori, Y; Nawa, Y; Hino, M; Fukuchi, T; Mori, Y; Yamahana, R; Inamoto, Y; Fukuda, T

    BIOLOGY OF BLOOD AND MARROW TRANSPLANTATION   Vol. 26 ( 5 ) page: 949 - 955   2020.5

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    With increasing focus on the importance of long-term survivorship care after allogeneic hematopoietic cell transplantation (allo-HCT), more institutions have been establishing long-term follow-up (LTFU) clinics. Currently, however, with varying volumes of HCT procedures and resources, there is no standardized operation of these clinics in HCT centers. We conducted a nationwide questionnaire survey to characterize the current operation of LTFU clinics in Japan. We targeted 271 HCT centers (189 adult and 82 pediatric) that registered allo-HCT cases to the national transplant registry database. The response rate was 69%, and 117 of the 188 participating centers (62%) had an established LTFU clinic. The most frequent reason cited for not operating an LTFU clinic was a “lack of human resources,” especially nurses. Most centers with an LTFU clinic targeted allo-HCT recipients, although autologous HCT survivors were followed up at 18% of adult centers and 48% of pediatric centers. Ninety-two percent of centers did not terminate LTFU at a specific time point, and 56% recommended that patients visit the LTFU clinic beyond 5 years after HCT. Fifteen of 20 pediatric centers indicated that they did not routinely refer survivors who underwent HCT at a young age to an adult HCT center for their adulthood LTFU. We found that staffing and standard practices varied widely among centers, and that most centers continued to see long-term HCT survivors at their own outpatient clinics. The development of common LTFU tools may help standardize LTFU practices and facilitate efficient transitions.

    DOI: 10.1016/j.bbmt.2020.01.008

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  195. Shaped Crystal Growth of Fe-Al Alloy Plates by Micro Pulling down Method Open Access

    Kamada, K; Murakami, R; Arakawa, M; Minamitani, T; Ueno, T; Shoji, Y; Yamaji, A; Yoshino, M; Kurosawa, S; Yokota, Y; Ohashi, Y; Kochurikhin, VV; Yoshikawa, A

    ACTA PHYSICA POLONICA A   Vol. 137 ( 5 ) page: 1009 - 1012   2020.5

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    Plate shaped Fe–Al alloy crystals were successfully grown using the µ-PD method. The orientation and grain size could be controlled by using the well oriented Fe0.95Al0.05 seed crystal. The as-grown Fe0.82Al0.18 and Fe0.80Al0.20 showed the magnetostriction 3/2λ = 121 and 149 ppm, respectively, which is comparable to the values for single crystal samples grown by the Bridgman-Stockbarger method. Distributions of Fe and Al were homogenous along the growth direction within standard deviations of 0.35% and 1.3%, respectively. A prototype vibration energy harvester was demonstrated using the grown Fe–Al alloys.

    DOI: 10.12693/APhysPolA.137.1009

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  196. Phase diagram of BaI<sub>2</sub>-LuI<sub>3</sub> system and growth of BaI<sub>2</sub>/LuI<sub>3</sub> eutectic scintillator

    Origuchi, K; Yokota, Y; Kral, R; Yoshino, M; Yamaji, A; Toyoda, S; Sato, H; Ohashi, Y; Kurosawa, S; Kamada, K; Yoshikawa, A

    JOURNAL OF CRYSTAL GROWTH   Vol. 536   2020.4

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    Publisher:Journal of Crystal Growth  

    The phase diagram of the BaI<inf>2</inf>-LuI<inf>3</inf> system was created using powder X-ray diffraction (XRD) and differential scanning calorimetry (DSC) analysis, and a eutectic scintillator crystal was grown by the halide-vertical bridgman (H-VB) method. The results of XRD patterns and DSC curves showed that the phase diagram of the BaI<inf>2</inf>-LuI<inf>3</inf> system had a eutectic point around 77.5 mol% BaI<inf>2</inf>/22.5 mol% LuI<inf>3</inf>, and no new compound was generated from BaI<inf>2</inf> and LuI<inf>3</inf>. The 77.5 mol% BaI<inf>2</inf>/22.5 mol% LuI<inf>3</inf> eutectic crystal was composed of BaI<inf>2</inf> in rod phase and LuI<inf>3</inf> in matrix phase. In addition, the Ce-doped 77.5 mol% BaI<inf>2</inf>/22.5 mol% LuI<inf>3</inf> specimen showed emission peaks originating from 5d–4f transition of Ce<sup>3+</sup> ion in the X-ray radioluminescence (XRL) spectrum and the decay time under γ-ray irradiation was approximately 38 ns.

    DOI: 10.1016/j.jcrysgro.2020.125573

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  197. Fiber-read radiation monitoring system using an optical fiber and red-emitting scintillator for ultra-high-dose conditions

    Kodama, S; Kurosawa, S; Ohno, M; Morishita, Y; Usami, H; Hayashi, M; Sasano, M; Azuma, T; Tanaka, H; Kochurikhin, V; Yamaji, A; Yoshino, M; Toyoda, S; Sato, H; Ohashi, Y; Kamada, K; Yokota, Y; Yoshikawa, A; Torii, T

    APPLIED PHYSICS EXPRESS   Vol. 13 ( 4 )   2020.4

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    We have developed a remote scintillation detector using a CCD spectrometer and a red-emitting scintillator coupled with a 20 m optical fiber for ultra-high-dose conditions. Gamma rays were detected with a conventional deep-red-emitting ruby scintillator and Cs<inf>2</inf>HfI<inf>6</inf>, which is a novel material with 700 nm red emission and a high light output. The scintillators were irradiated with gamma rays from a <sup>60</sup>Co source under an effective dose rate from ∼0.002 to ∼1 kSv h<sup>-1</sup>. The integrated area of the Cs<inf>2</inf>HfI<inf>6</inf> emission spectra was larger than that of the ruby, and good linearity of the Cs<inf>2</inf>HfI<inf>6</inf> signal as a function of dose rate was confirmed.

    DOI: 10.35848/1882-0786/ab77f7

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  198. Multiple shaped-crystal growth of oxide scintillators using Mo crucible and die by the edge defined film fed growth method

    Kamada, K; Nikl, M; Kotaki, T; Saito, H; Horikoshi, F; Miyazaki, M; Kim, KJ; Murakami, R; Yoshino, M; Yamaji, A; Shoji, Y; Kurosawa, S; Toyoda, S; Sato, H; Yokota, Y; Ohashi, Y; Kochurikhin, V; Yoshikawa, A

    JOURNAL OF CRYSTAL GROWTH   Vol. 535   2020.4

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    Edge defined Film Fed Growth (EFG) method with molybdenum (Mo) crucible and die was studied for the growth of several oxide-based single crystals. At first, reactivity between the molybdenum (Mo) metal and oxide melts of Ce:(Lu,Y)<inf>2</inf>SiO<inf>5</inf> (LYSO) Ce:Y<inf>2</inf>SiO<inf>5</inf> (YSO), Ce:Gd<inf>3</inf>(Al,Ga)<inf>5</inf>O<inf>12</inf> (GAGG), Ce:Lu<inf>3</inf>Al<inf>5</inf>O<inf>12</inf> (LuAG), Ce:Y<inf>3</inf>Al<inf>5</inf>O<inf>12</inf> (YAG) was investigated. The experimental and calculation results on the reactivity with Mo show that the aluminum garnets (LuAG, YAG) had the smallest reactivity with Mo metal. On the contrary, GAGG showed the strongest reaction with Mo. Then, the multiple-die grown shaped single crystal growth of Ce:LuAG was demonstrated by EFG method. Single crystal plates up to 320 mm in length were grown successfully. The homogeneity of dopant distribution, Mo contamination, luminescence and scintillation responses of the grown crystals were evaluated.

    DOI: 10.1016/j.jcrysgro.2020.125510

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  199. Modified vertical Bridgman method: Time and cost effective tool for preparation of Cs<sub>2</sub>HfCl<sub>6</sub> single crystals

    Vanecek, V; Kral, R; Paterek, J; Babin, ; Jary, ; Hybler, J; Kodama, S; Kurosawa, S; Yokota, Y; Yoshikawa, A; Nikl, M

    JOURNAL OF CRYSTAL GROWTH   Vol. 533   2020.3

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    Time and cost effective methods are highly desirable in research and development of new scintillators. Modern techniques like micro-pulling down (μ-PD) are suitable for material screening but are unfit for the growth of some crystals. These crystals must be grown by different methods that are usually very time demanding. Modification of halide μ-PD apparatus by custom made elements allowed us to grow cesium hafnium chloride (Cs<inf>2</inf>HfCl<inf>6</inf>) by vertical Bridgman method (VB) with significantly reduced growth time. Structural and optical properties of samples prepared from as-grown crystals were studied and compared to crystals grown by standard VB method. The X-ray diffraction confirmed the formation of cesium hafnium chloride single-phase and natural cleavage of the crystals along the (1 1 1) crystallographic plane. Photoluminescence emission, excitation, absorption, and radioluminescence spectroscopy revealed that the optical quality of the crystals grown by modified VB method was comparable to the quality of the crystals grown by standard VB method. Therefore we can use samples prepared by modified VB to estimate and optimize the performance of Cs<inf>2</inf>HfCl<inf>6</inf> based crystals in scintillation detectors. This setup allows the time and cost-effective material screening and it is a powerful tool for the development of new halide based single crystal scintillators.

    DOI: 10.1016/j.jcrysgro.2020.125479

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  200. A decision analysis comparing unrelated bone marrow transplantation and cord blood transplantation in patients with aggressive adult T-cell leukemia-lymphoma

    Fuji, S; Kurosawa, S; Inamoto, Y; Murata, T; Utsunomiya, A; Uchimaru, K; Yamasaki, S; Inoue, Y; Moriuchi, Y; Choi, I; Ogata, M; Hidaka, M; Yamaguchi, T; Fukuda, T

    INTERNATIONAL JOURNAL OF HEMATOLOGY   Vol. 111 ( 3 ) page: 427 - 433   2020.3

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    Language:English   Publisher:International Journal of Hematology  

    Patients with aggressive adult T-cell leukemia-lymphoma (ATL) have dismal outcomes with intensive chemotherapy. Early up-front allogeneic hematopoietic stem cell transplantation (allo-HSCT) is generally recommended. However, the choice of stem cell source, i.e., unrelated bone marrow transplant (UBMT) or cord blood transplantation (CBT), when an HLA-matched related donor is unavailable remains controversial. Thus, we undertook a decision analysis to compare the outcomes of two therapeutic strategies: chemotherapy followed by up-front UBMT at 6 months, and chemotherapy followed by up-front CBT at 3 months. Patients were stratified into low-, intermediate-, and high-risk groups according to the modified ATL-prognostic index. The model simulated life expectancy (LE) and quality-adjusted LE (QALE). LE following up-front UBMT was higher than that following up-front CBT in the low-risk group (2.63 vs. 2.28 years), but was comparable in the intermediate- (2.06 vs. 2.01 years) and high-risk groups (1.25 vs. 1.30 years). The Monte Carlo simulation for LE and QALE in each risk group showed that there was significant uncertainty in all categories. In conclusion, up-front UBMT was superior to up-front CBT in the low-risk group, but the strategies were comparable in the intermediate- and high-risk groups.

    DOI: 10.1007/s12185-019-02777-w

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  201. Epitaxial growth of Ce-doped (Pb,Gd)<sub>3</sub>(Al,Ga)<sub>5</sub>O<sub>12</sub> films and their optical and scintillation properties Open Access

    Vasil'ev, DA; Spassky, DA; Kurosawa, S; Omelkov, S; Vasil'eva, NV; Plotnichenko, VG; Khakhalin, A; Voronov, VV; Kochurikhin, VV

    JOURNAL OF SCIENCE-ADVANCED MATERIALS AND DEVICES   Vol. 5 ( 1 ) page: 95 - 103   2020.3

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    Publisher:Journal of Science Advanced Materials and Devices  

    Се-doped (Pb,Gd)<inf>3</inf>(Al,Ga)<inf>5</inf>O<inf>12</inf> single crystalline garnet films were grown using liquid-phase epitaxy from four series of supercooled PbO–B<inf>2</inf>O<inf>3</inf>-based melt solutions on Gd<inf>3</inf>Ga<inf>5</inf>O<inf>12</inf> and Gd<inf>3</inf>Al<inf>2.26</inf>Ga<inf>2.74</inf>O<inf>12</inf> single crystal substrates. The optical and scintillation properties of the epitaxial garnet films were studied. The 5d-4f emission of Ce<sup>3+</sup> ions within 450–650 nm was observed. The highest pulsed cathodoluminescence yield and scintillation yield values under <sup>133</sup>Ba excitation for the Pb<inf>0.01</inf>Ce<inf>0.02</inf>Gd<inf>2.97</inf>Al<inf>3.13</inf>Ga<inf>1.87</inf>O<inf>12</inf> film were 43,100 photons/MeV and 20,000 photons/MeV, respectively. The pulsed cathodoluminescence decay times of the film were 1.8 (1%), 24 (25%), and 60 ns (74%), and the scintillation decay times were 3.9 (7%) and 43.6 ns (93%). Because of the rapid decay and high light yield, Се-doped (Pb,Gd)<inf>3</inf>(Al,Ga)<inf>5</inf>O<inf>12</inf> garnet films can be used in X-ray scintillators for different applications, such as homeland security.

    DOI: 10.1016/j.jsamd.2020.01.005

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  202. Luminescence properties of scintillators in soft X-ray region Open Access

    Ejima, T; Kurosawa, S; Yamaji, A; Hatano, T; Wakayama, T; Higashiguchi, T; Kitaura, M

    JOURNAL OF LUMINESCENCE   Vol. 219   2020.3

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    Publisher:Journal of Luminescence  

    Both the total luminescence yield (TLY) and the luminescence spectra of scintillators were measured to identify which scintillator exhibited high luminosity in the soft X-ray (SX) region from 300 eV to 1.3 keV. The TLY intensities and the peak intensities of the luminescence spectra were compared to identify the scintillators that have high luminosity for reducing the pixel size of a two-dimensional detector by applying the stimulated emission depletion phenomenon. The obtained TLY intensities were Tl:CsI, Eu:GGG, Ce:LYSO, Tb:LSO, Eu:YAP and Ce:YAP (in descending order of strength), which differs from the known luminosities in the hard X-ray region. The order of the measured TLY intensity and the change of order between the present and the previous values of luminosities can be explained by the number of secondary electrons generated in the base material of the scintillator in the SX region.

    DOI: 10.1016/j.jlumin.2019.116850

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  203. Microstructure and Mechanical Properties of Platinum Fiber Fabricated by Unidirectional Solidification Open Access

    Yokota, Y; Nihei, T; Yoshino, M; Yamaji, A; Toyoda, S; Sato, H; Ohashi, Y; Kurosawa, S; Kamada, K; Yoshikawa, A

    CRYSTALS   Vol. 10 ( 3 )   2020.3

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    Publisher:Crystals  

    The microstructure and mechanical properties of platinum (Pt) fibers fabricated by unidirectional solidification using the alloy-micro-pulling-down (A-μ-PD) method were investigated using a Universal Testing Machine and Electron Backscattered Diffraction (EBSD). The Pt fiber fabricated at a growth rate of 10 mm/min was composed of relatively large grains with <100> crystal orientation along the growth direction. The crystal orientation was consistent with the easy axis of the crystal growth on the face-centered-cubic (f.c.c.) structure. On the other hand, the adjacent grains of the Pt fiber fabricated at 50 mm/min were randomly oriented owing to a faster growth rate. In tensile tests, the Pt fibers fabricated by the A-μ-PD method indicated extremely different stress–strain curves compared to the commercial Pt wire. The maximum tensile stress of the Pt fiber reached ~100 MPa, and the Pt fiber ruptured after 58% nominal strain.

    DOI: 10.3390/cryst10030216

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  204. Control of Microstructure for Co-Cr-Mo Fibers Fabricated by Unidirectional Solidification Open Access

    Abe, S; Yokota, Y; Nihei, T; Yoshino, M; Yamaji, A; Toyoda, S; Sato, H; Ohashi, Y; Kurosawa, S; Kamada, K; Yoshikawa, A

    CRYSTALS   Vol. 10 ( 1 )   2020.1

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    Publisher:Crystals  

    Co-Cr-Mo alloy fibers of 2 mm in diameter were fabricated from the melt at 1, 2, and 5 mm/min growth rates by unidirectional solidification using an alloy-micro-pulling-down (A-µ-PD) method to control the microstructure. All elements, Co, Cr, and Mo, were distributed in stripes elongated along the growth direction due to constitutional undercooling. Both Co-Cr-Mo fibers fabricated at 2 and 5 mm/min growth rates were composed of the γ phase with a face-centered cubic structure (fcc-γ phase) and ε-phase with a hexagonal close-packed structure (hcp-ε phase), and the ratio of the fcc-γ phase in the fiber fabricated at 5 mm/min growth rate was higher than that in the fiber fabricated at 2 mm/min. The results suggest that a faster growth rate increases the ratio of the fcc-γ phase in the Co-Cr-Mo fiber fabricated by unidirectional solidification.

    DOI: 10.3390/cryst10010011

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  205. Growth and scintillation properties of Tl-doped CsI/CsCl/NaCl ternary eutectic scintillators

    Takizawa Y., Kamada K., Yoshino M., Yamaji A., Kurosawa S., Yokota Y., Sato H., Toyoda S., Ohashi Y., Hanada T., Kochurikhin V.V., Yoshikawa A.

    Japanese Journal of Applied Physics   Vol. 60 ( SB )   2020

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    Publisher:Japanese Journal of Applied Physics  

    Tl:CsI/CsCl/NaCl eutectic scintillators were grown by the Bridgman-Stockbarger method. The eutectic phases were uniformly distributed in the transverse direction and slightly aligned along the growth direction. Then, the CsI phase can be designed as columnar. The expected emission peak observed at 550 nm was observed under X-ray excitation and cathodoluminescence and was ascribed to the self-trapped exciton perturbed by TI+ in Tl:CsI. The mapping of optically waveguided light emission was observed by confocal laser microscopy, consequently optical waveguiding of Tl+ emission in the CsI phase was demonstrated.

    DOI: 10.35848/1347-4065/abcdab

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  206. High-redshift gamma-ray burst for unraveling the Dark Ages Mission - HiZ-GUNDAM -

    Yonetoku D., Mihara T., Doi A., Sakamoto T., Tsumura K., Ioka K., Amaya Y., Arimoto M., Enoto T., Fujii T., Goto H., Gunji S., Hiraga J., Ikeda H., Kawai N., Kurosawa S., Li J., Maeda Y., Mitsuishi I., Murakami T., Nakagawa Y., Ogino N., Ohno M., Sawano T., Sei K., Serino M., Sugita S., Tamagawa T., Tamura K., Tanaka T., Tanimori T., Tashiro M.S., Tomida H., Wang H., Yamaguchi T., Yamamoto A., Yamaoka K., Yamauchi M., Yatsu Y., Yoshida A., Yuhi D., Akitaya H., Fukui A., Ita Y., Kaneda H., Kawabata K., Kawata Y., Kurimata M., Matsumoto T., Matsuura S., Miyasaka A., Motohara K., Narita N., Noda H., Ohashi A., Okita H., Sano K., Tanaka M., Urata Y., Wada T., Yamaguchi H., Yanagisawa K., Yoshida M., Asano K., Inayoshi K., Inoue S., Ito H., Izumiura H., Kawanaka N., Kinugawa T., Kisaka S., Kiuchi K., Kyutoku K., Matsumoto J., Mizuta A., Murase K., Nagakura H., Nagataki S., Nakada Y., Nakamura T., Niino Y., Suwa Y., Takahashi K., Tanaka T., Toma K., Totani T., Yamazaki R., Yokoyama J.

    Proceedings of SPIE the International Society for Optical Engineering   Vol. 11444   2020

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    Publisher:Proceedings of SPIE the International Society for Optical Engineering  

    HiZ-GUNDAM is a future satellite mission which will lead the time-domain astronomy and the multi-messenger astronomy through observations of high-energy transient phenomena. A mission concept of HiZ-GUNDAM was approved by ISAS/JAXA, and it is one of the future satellite candidates of JAXA's medium-class mission. We are in pre-phase A (before pre-project) and elaborating the mission concept, mission/system requirements for the launch in the late 2020s. The main themes of HiZ-GUNDAM mission are (1) exploration of the early universe with high-redshift gamma-ray bursts, and (2) contribution to the multi-messenger astronomy. HiZ-GUNDAM has two kinds of mission payload. The wide field X-ray monitors consist of Lobster Eye optics array and focal imaging sensor, and monitor ~1 steradian field of view in 0.5 - 4 keV energy range. The near infrared telescope has an aperture size 30 cm in diameter, and simultaneously observes four wavelength bands between 0.5 - 2.5 µm. In this paper, we introduce the mission overview of HiZ-GUNDAM.

    DOI: 10.1117/12.2560603

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  207. SMILE-3: Sky survey in MeV gamma-ray using an electron-tracking Compton telescope loaded on balloons

    Takada A., Tanimori T., Mizumura Y., Takemura T., Yoshikawa K., Nakamura Y., Abe M., Kubo H., Kurosawa S., Miuchi K., Sawano T., Hamaguchi H.

    Proceedings of SPIE the International Society for Optical Engineering   Vol. 11444   2020

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    Publisher:Proceedings of SPIE the International Society for Optical Engineering  

    MeV gamma-ray astronomy in an energy range of hundreds of keV to tens of MeV is a unique window for observing nucleosynthesis, however this field has not opened up until recently because of imaging difficulties. Thus, we are developing an electron-tracking Compton camera (ETCC), which consists of a gaseous electron tracker and pixel scintillator arrays, as a next generation MeV gamma-ray telescope. Because the ETCC detects all parameters after Compton scattering, we can determine the momentum of incident gamma-rays with powerful background rejection. This ETCC has confirmed low-noise and high-sensitivity observations at high altitude through Sub-MeV gamma-ray Imaging Loaded-on-balloon Experiment I (SMILE-I) in 2006 and SMILE-2+ in 2018. Therefore, we are planning scientific observations using an ETCC with an effective area of ∼10 cm<sup>2</sup> for 0.3 MeV, a spatial resolution of ≤10 degrees for 0.5 MeV, and a field of view of 3 sr as the next step (SMILE-3). In this paper, we present the design of the SMILE-3 ETCC and its expected observations.

    DOI: 10.1117/12.2560886

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  208. Ga for Al substitution effects on the garnet phase stability and luminescence properties of Gd<sub>3</sub>Ga<sub>x</sub>Al<sub>5-x</sub>O<sub>12</sub>:Ce single crystals

    Bartosiewicz, K; Babin, V; Kamada, K; Yoshikawa, A; Kurosawa, S; Beitlerova, A; Kucerkova, R; Nikl, M; Zorenko, Y

    JOURNAL OF LUMINESCENCE   Vol. 216   2019.12

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    Publisher:Journal of Luminescence  

    This research deals with the luminescence and physical properties of Gd<inf>3</inf>(Ga,Al)<inf>5</inf>O<inf>12</inf>:Ce single crystal set and it is a complementary study to analogous (Y,Gd)<inf>3</inf>Al<inf>5</inf>O<inf>12</inf>:Ce and (Gd,Lu)<inf>3</inf>Al<inf>5</inf>O<inf>12</inf>:Ce single crystal sets. Those three groups of materials show similar luminescence and physical properties. In this research, the influence of substitution Ga for Al in Gd<inf>3</inf>(Ga,Al)<inf>5</inf>O<inf>12</inf>:Ce single crystals on the luminescence and scintillation characteristics as well as thermodynamical stability of the garnet phase is studied, and it is compared to (Y,Gd)<inf>3</inf>Al<inf>5</inf>O<inf>12</inf>:Ce and (Gd,Lu)<inf>3</inf>Al<inf>5</inf>O<inf>12</inf>:Ce single crystal sets. The unbalanced substitution Ga for Al makes garnet phase thermodynamically unstable and leads to the formation of the multiphase system with luminescence centers in UV and visible spectral ranges. The wavelength-dispersive X-ray spectroscopy, X-ray powder diffraction analysis, photoluminescence and decay kinetic measurements reviled all phase types within multiphase crystals. Temperature dependent measurements were applied to determine the quenching mechanism for Ce<sup>3+</sup> luminescence. The timing characteristics are studied as the function of Ga content.

    DOI: 10.1016/j.jlumin.2019.116724

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  209. The Presence of Minimal Residual Disease, As Determined By Highly Sensitive Quantitation of <i>NPM1</i>-Mutatation, Provided Powerful Prognostic Information in Acute Myeloid Leukemia

    Marumo, A; Yamaguchi, H; Najima, Y; Usuki, K; Kako, S; Uchiyama, H; Nagao, Y; Shono, K; Kurosawa, S; Hagihara, M; Kanda, J; Kubota, Y; Ando, J; Date, K; Kuboyama, M; Sakaguchi, M; Yui, S; Wakita, S; Arai, K; Kitano, T; Kakihana, K; Fukuda, T; Doki, N; Ohashi, K; Inokuchi, K

    BLOOD   Vol. 134   2019.11

  210. Significance of <i>FLT3</i>-tyrosine kinase domain mutation as a prognostic factor for acute myeloid leukemia

    Sakaguchi, M; Yamaguchi, H; Kuboyama, M; Najima, Y; Usuki, K; Ueki, T; Oh, I; Mori, S; Kawata, E; Uoshima, N; Kobayashi, Y; Kako, S; Tajika, K; Shono, K; Kayamori, K; Hagihara, M; Kanda, J; Uchiyama, H; Kuroda, J; Uchida, N; Kubota, Y; Kimura, S; Kurosawa, S; Date, K; Nakajima, N; Marumo, A; Omori, I; Fujiwara, Y; Terada, K; Yui, S; Wakita, S; Arai, K; Kitano, T; Kakihana, K; Kanda, Y; Ohashi, K; Fukuda, T; Inokuchi, K

    INTERNATIONAL JOURNAL OF HEMATOLOGY   Vol. 110 ( 5 ) page: 566 - 574   2019.11

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    The prognostic significance of FLT3-tyrosine kinase domain (TKD) mutations remains unknown. To investigate the prognostic impact of FLT3-TKD, 676 de novo acute myeloid leukemia (AML), we retrospectively analyzed cases and conducted a review of the literature. Of the 676 de novo AML cases, 34 (5.0%) were FLT3-TKD-positive; both FLT3-TKD and FLT3-ITD were noted in only two cases (0.3%). Although no significant differences in relapse-free survival (RFS) were noted, FLT3-TKD-positive cases showed better prognoses than FLT3-ITD-positive cases (FLT3-TKD versus FLT3-ITD, p = 0.152). For overall survival (OS), although FLT3-TKD-positive cases showed prognoses similar to those for FLT3-WT cases, their prognoses were significantly better than those of FLT3-ITD-positive cases (FLT3-TKD versus FLT3-ITD, p = 0.032). Moreover, the 5-year OS for FLT3-TKD-positive cases was 46.1%, indicating that this as an intermediate prognosis group. Although no reports from Asia have indicated a frequency of FLT3-TKD-positive cases > 10%, several reports from Europe and the United States have indicated frequencies > 10%. This suggests the possibility that FLT3-TKD-positive cases are less common in Asia than in Europe and the United States. We anticipate that in the future, the appearance of targeting agents, such as FLT3 inhibitors, will improve the prognosis of FLT3-TKD-positive AML relative to that of FLT3-WT AML.

    DOI: 10.1007/s12185-019-02720-z

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  211. Association between psychological factors, and emotional distress and quality of life after allogeneic hematopoietic cell transplantation

    Nakahara, R; Kurosawa, S; Yamaguchi, T; Inoguch, H; Kusaka, K; Tanaka, M; Sugita, J; Umemoto, Y; Kondo, T; Yoshida, H; Ohwada, C; Murayama, T; Ota, S; Yano, S; Takahashi, S; Fujisawa, S; Hagihara, M; Yokoyama, H; Fukuda, T; Shimizu, K

    QUALITY OF LIFE RESEARCH   Vol. 28   page: S85 - S86   2019.10

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  212. RD of new high-performance scintillator including double beta decay nuclei

    Iida T., Kamada K., Yoshino M., Kim K.J., Kurosawa S., Yoshikawa A.

    2019 IEEE Nuclear Science Symposium and Medical Imaging Conference NSS Mic 2019     2019.10

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    Publisher:2019 IEEE Nuclear Science Symposium and Medical Imaging Conference NSS Mic 2019  

    Inorganic scintillators have been used for underground astroparticle physics experiment, such as dark matter search and double beta decay search. We have developed CaI<inf>2</inf> which has a large amount of luminescence and contains <sup>48</sup>Ca from double beta decay nuclei. Half-inch CaI<inf>2</inf> crystals were prepared by the Bridgman method in Institute for Materia Research, cut into several mm squares, and the scintillation characteristics were measured. The light emission amount was 107,000 ph. / MeV, 2.7 times NaI (Tl) and 10 times undoped CaF<inf>2</inf>. The light emission wavelength was 410 nm, which was in agreement with sensitive wavelength of photomultiplier tubes. When the waveform discrimination characteristics were measured using alpha rays of <sup>241</sup>Am and gamma rays of <sup>137</sup>Cs, it was found that there was a large difference in the first 300 ns between the waveforms. Our pulse shape discrimination analysis using fast/total ratio method gives 4.2 for CaI<inf>2</inf> in figure of merit, and it was 2.0 for CaF2(Eu). CaI<inf>2</inf> showed high potential for pulse shape discrimination. Low temperature dependence of light yield was also investigated, and we confirm that light yield of CaI<inf>2</inf> increase at low temperature. At present, the growth and processing of large crystals is difficult due to the strong deliquescence and cleavage of CaI<inf>2</inf>. Work is underway to develop better growth and processing method for CaI<inf>2</inf> crystal.

    DOI: 10.1109/NSS/MIC42101.2019.9059845

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  213. Al concentration dependence of crystal structure for Ca<sub>3</sub>Ta(Ga,Al)<sub>3</sub>Si<sub>2</sub>O<sub>14</sub> piezoelectric single crystals

    Yokota, Y; Kudo, T; Ohashi, Y; Inoue, K; Yoshino, M; Yamaji, A; Kurosawa, S; Kamada, K; Yoshikawa, A

    JOURNAL OF SOLID STATE CHEMISTRY   Vol. 277   page: 195 - 200   2019.9

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    Al concentration dependence of the crystal structure on Ca<inf>3</inf>Ta(Ga<inf>1-x</inf>Al<inf>x</inf>)Si<inf>2</inf>O<inf>14</inf> (CTGAS) piezoelectric single crystals were investigated by X-ray crystal structure analysis. O(2)-Si-O(2) and Si-O(2)-(Ga,Al) bond angles systematically increased with increasing Al concentration, and the result suggests that the increase of structural anisotropy by the Al substitution is attributable to the planarization of the O(2)-Si-O(2)-(Ga,Al). In addition, (Ga,Al)-O(2), (Ga,Al)-O(3) and Ca-O(1) bond lengths systematically decreased with increasing the Al substitution. The cation shift of the Si and (Ga,Al) ions out of center from the barycenter of the oxygen coordination environment decreased with increasing Al concentration.

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  214. Resolved versus Active Chronic Graft-versus-Host Disease: Impact on Post-Transplantation Quality of Life Open Access

    Kurosawa, S; Yamaguchi, T; Oshima, K; Yanagisawa, A; Fukuda, T; Kanamori, H; Mori, T; Takahashi, S; Kondos, T; Kohno, A; Miyamura, K; Umemoto, Y; Teshima, T; Taniguchi, S; Yamashita, T; Inamoto, Y; Kanda, Y; Okamoto, S; Atsuta, Y

    BIOLOGY OF BLOOD AND MARROW TRANSPLANTATION   Vol. 25 ( 9 ) page: 1851 - 1858   2019.9

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    The aim of this study was to determine whether impaired quality of life (QOL) persisted among patients who experienced resolved chronic graft-versus-host disease (GVHD) after allogeneic hematopoietic cell transplantation (allo-HCT). Eligible participants were patients who were relapse-free for 3 years after allo-HCT who were age ≥16 years at the time of transplantation and age ≥20 years without relapse at the time of the survey. The Medical Outcomes Study's 36-Item Short-Form Survey (SF-36), the Functional Assessment of Cancer Therapy-Bone Marrow Transplant (FACT-BMT), and a visual analog scale (VAS) were administered to assess QOL. Physicians evaluated the current status of chronic GVHD at survey using National Institutes of Health (NIH) criteria, and pretransplantation characteristics and history of GVHD were extracted from the national transplant registry database. Patients without currently active GVHD but with a history of chronic GVHD were categorized as having “resolved GVHD.” Of 1250 patients informed of the study, 1216 provided consent and 1130 were included in the final analysis. A total of 745 patients (66%) had currently active chronic GVHD, 149 (13%) had resolved chronic GVHD, and 236 (21%) never had chronic GVHD after allo-HCT. Multivariable analyses showed that compared with patients with resolved or no chronic GVHD, those with active chronic GVHD reported significantly poorer QOL. The QOL scores were similar in patients with resolved chronic GVHD and those without chronic GVHD. Greater between-group differences were observed in SF-36 Physical component and VAS scores in patients age ≥50 years, but the differences were not statistically significant. Our data indicate that only currently active chronic GVHD has a significant impact on physical, mental, and social QOL in allo-HCT survivors, whereas previous chronic GVHD does not impair QOL if it has been resolved.

    DOI: 10.1016/j.bbmt.2019.05.016

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  215. SAPPHIRE: a randomised phase II study of planned discontinuation or continuous treatment of oxaliplatin after six cycles of modified FOLFOX6 plus panitumumab in patients with colorectal cancer Open Access

    Munemoto Y., Nakamura M., Takahashi M., Kotaka M., Kuroda H., Kato T., Minagawa N., Noura S., Fukunaga M., Kuramochi H., Touyama T., Takahashi T., Miwa K., Satake H., Kurosawa S., Miura T., Mishima H., Sakamoto J., Oba K., Nagata N.

    European Journal of Cancer   Vol. 119   page: 158 - 167   2019.9

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    Background: Fluorouracil (5-FU), leucovorin (LV) and oxaliplatin (FOLFOX) plus panitumumab therapy is a commonly used first-line chemotherapy for metastatic colorectal cancer (mCRC). However, the long-term administration of oxaliplatin is associated with peripheral neuropathy (PN). We investigated whether the planned discontinuation of oxaliplatin after FOLFOX plus panitumumab therapy can maintain efficacy and reduce PN incidence. Patients and methods: Chemotherapy-naive patients with RAS wild-type mCRC, aged ≥20 years, were enrolled and received six cycles of modified FOLFOX6 (mFOLFOX6) plus panitumumab as induction therapy. Patients who completed induction therapy without progression were randomised to mFOLFOX6 plus panitumumab (group A) or to 5-FU/LV plus panitumumab (group B). The primary end-point was the progression-free survival (PFS) rate at 9 months after randomisation. The secondary end-points were PFS, overall survival (OS), time to treatment failure (TTF), response rate (RR) and safety. Results: In total, 164 patients were enrolled; of whom, 113 patients were then randomised (group A, n = 56; group B, n = 57). The median follow-up after randomisation was 19.6 months. The PFS rates at 9 months and median PFS were 46.4% (80% confidence interval [CI], 38.1–54.9) and 9.1 months (95% CI, 8.6–11.1) in group A, compared with 47.4% (80% CI, 39.1–55.8) and 9.3 months (95% CI, 6.0–13.0) in group B, respectively. RR, OS and TTF were also similar in both groups. Grade ≥2 PN incidence was lower in group B (9.3%) than in group A (35.7%). Conclusion: Planned discontinuation of oxaliplatin after six cycles of mFOLFOX6 plus panitumumab is a potential treatment option in patients with mCRC, achieving similar efficacy while reducing oxaliplatin-associated PN compared with mFOLFOX6 plus panitumumab. Trial registration number: NCT02337946

    DOI: 10.1016/j.ejca.2019.07.006

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  216. Development of a laser driven neutron source using repetitive irradiation of ultra-intense laser

    Nagatomo Hideo, Mima Kunioki, Hatanaka Takeru, Sunahara Atsushi, Kato Yoshiaki, Tanaka Hiroki, Hanayama Ryohei, Kurosawa Shunsuke

    Proceedings of JSPE Semestrial Meeting   Vol. 2019A ( 0 ) page: 530 - 530   2019.8

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    DOI: 10.11522/pscjspe.2019a.0_530

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  217. Crystal growth and luminescence properties of organic crystal scintillators for α-rays detection

    Yamato, S; Yamaji, A; Kurosawa, S; Yoshino, M; Ohashi, Y; Kamada, K; Yokota, Y; Yoshikawa, A

    OPTICAL MATERIALS   Vol. 94   page: 58 - 63   2019.8

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    Scintillation and luminescence properties of a novel organic crystal scintillator, 1,4-bis(2-methylstyryl)benzene (bis-MSB), were measured and compared with those of the conventional trans-stilbene organic crystal scintillator. Although trans-stilbene has been used for beta or neutron detection, trans-stilbene cannot be applied at high temperature conditions due to a lower melting point (124 °C). Liquid scintillators or plastic scintillators also cannot be used at high temperature. Usually, bis-MSB has been used as dopant in liquid scintillators to obtain fast scintillation decay and high luminescence quantum yield, and its melting point is 181 °C higher than that of trans-stilbene. In this paper, we focused on bis-MSB in solid state. The bis-MSB and trans-stilbene crystals were grown by the self-seeding vertical Bridgman method using double quartz ampoules. The bis-MSB crystal had the fast decay time of ∼4.2 ns and the increased light yield of ∼12,000 ph/5.5 MeV(α), while trans-stilbene had the decay time of ∼8.5 ns and the light yield of ∼8500 ph/5.5 MeV(α). The photoluminescence quantum yield was almost constant up to 125 °C for bis-MSB and only up to 50 °C for trans-stilbene. We succeeded in obtaining the novel organic crystal scintillator which can operate even at higher temperature up to 125 °C.

    DOI: 10.1016/j.optmat.2019.04.051

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  218. Crystal growth and scintillation properties of Eu-doped Ca(Br<sub>x</sub>I<sub>1-x</sub>)<sub>2</sub> crystals

    Kamada, K; Iida, T; Furuya, Y; Kim, KJ; Yoshino, M; Murakami, R; Shoji, Y; Kochurikhin, VV; Yamaj, A; Kurosawa, S; Ohashi, Y; Yokota, Y; Yoshikawa, A

    RADIATION MEASUREMENTS   Vol. 127   2019.8

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    In this study, solid solutions of Ca(Br,I)<inf>2</inf> were prepared to mitigate the cleavage feature of CaI<inf>2</inf>. Samples were grown using the Bridgman–Stockbarger (BS) method in a quartz ampoule. Eu<sup>2+</sup> 4f–5d emissions were observed, peaking at 462–464 nm with a scintillation decay time of around 1000–1500 ns. Eu2%:CaBr<inf>0.5</inf>I<inf>1.5</inf> showed the best light output of 109,000 photons/MeV, and Eu2%:CaBrI showed the best energy resolution (7.9%@662 keV) among the crystals grown. Eu2%:CaBr<inf>0.5</inf>I<inf>1.5</inf> showed the same crystal phase as CaI<inf>2</inf> and a strong cleavage feature. In contrast, Eu2%:CaBrI did not exhibit the cleavage feature and was more feasible for mass production as a detector material. Eu-doped CaBrI was the most promising material, not only for applications in the observation of neutrinoless double beta decay, but also other high-energy physics, gamma ray surveys, and gamma camera applications, owing to the optimization of light yield and energy resolution without cleavage.

    DOI: 10.1016/j.radmeas.2019.106139

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  219. Scintillation properties of Y-Admixed Gd<sub>2</sub>Si<sub>2</sub>O<sub>7</sub> scintillator

    Kurosawa, S; Shishido, T; Sugawara, T; Yubuta, K; Horiai, T; Jary, V; Yamaji, A; Yoshino, M; Yokota, Y; Shoji, Y; Kamada, K; Yoshikawa, A; Pejchal, J; Nikl, M

    RADIATION MEASUREMENTS   Vol. 126   2019.7

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    Pyrosilicate scintillation crystals are expected to be the next generation scintillators, because they have good light output and no hygroscopic nature. In this work, (Ce<inf>0.01</inf> Gd<inf>0.90</inf> Y<inf>0.09</inf>)<inf>2</inf>Si<inf>2</inf>O<inf>7</inf> (Ce:Y-GPS)crystal was grown by the floating zone method. Emission wavelengths of this material were at 360 and 380 nm originated from Ce<sup>3+</sup> 5d-4f transition, and these emission peaks were located at shorter wavelength side compared with Ce-doped (Gd, La)<inf>2</inf>Si<inf>2</inf>O<inf>7</inf> due to the change of the crystal field. Gamma-ray-excited pulse height and scintillation decay measurements showed that Ce:Y-GPS had a light output of 48,000 ± 3000 photons/MeV, FWHM energy resolution of 11.8 ± 0.5% at 662 keV and the decay time components of 42 ± 1 ns (58 ± 2%)and 180 ± 10 ns (42 ± 2%).

    DOI: 10.1016/j.radmeas.2019.106123

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  220. Immunosuppressive effect of a non-proteinogenic amino acid from Streptomyces through inhibiting allogeneic T cell proliferation.

    Yashiro T, Sakata F, Sekimoto T, Shirai T, Hasebe F, Matsuda K, Kurosawa S, Suzuki S, Nagata K, Kasakura K, Nishiyama M, Nishiyama C

    Bioscience, biotechnology, and biochemistry   Vol. 83 ( 6 ) page: 1111 - 1116   2019.6

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    DOI: 10.1080/09168451.2019.1591262

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  221. Pulse-shape discrimination potential of new scintillator material: La-GPS:Ce Open Access

    Mizukoshi, K; Iida, T; Ogawa, I; Shimizu, K; Kurosawa, S; Karnada, K; Yoshino, M; Yoshikawa, A

    JOURNAL OF INSTRUMENTATION   Vol. 14 ( 6 )   2019.6

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    (Gd,La)<inf>2</inf>Si<inf>2</inf>O<inf>7</inf>:Ce (La-GPS:Ce) is a new scintillator material with high light output, high energy resolution, and fast decay time. Moreover, the scintillator has a good light output even at high temperature (up to 150<sup>◦</sup>C) and is non-hygroscopic in nature; thus, it is especially suitable for underground resource exploration. Particle identification greatly expands the possible applications of scintillator. For resource exploration, the particle identification should be completed in a single pulse only. The pulse-shape discrimination of the scintillator was confirmed. We compared two methods: a double gate method and a digital filter method. Using digital filter method (shape indicator), F-measure to evaluate these separation between α and γ particles was obtained to be 0.92 at 0.66 MeVee.

    DOI: 10.1088/1748-0221/14/06/P06037

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  222. Scintillation properties of Gd<sub>3</sub>Al<sub>2</sub>Ga<sub>3</sub>O<sub>12</sub>:Ce, Li and Gd<sub>3</sub>Al<sub>2</sub>Ga<sub>3</sub>O<sub>12</sub>:Ce, Mg single crystal scintillators: A comparative study

    Chewpraditkul, W; Pattanaboonmee, N; Sakthong, O; Wantong, K; Chewpraditkul, W; Yoshikawa, A; Kamada, K; Kurosawa, S; Szczesniak, T; Moszynski, M; Babin, V; Nikl, M

    OPTICAL MATERIALS   Vol. 92   page: 181 - 186   2019.6

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    The scintillation characteristics of Gd<inf>3</inf>Al<inf>2</inf>Ga<inf>3</inf>O<inf>12</inf>:Ce, Li (GAGG:Ce,Li) and Gd<inf>3</inf>Al<inf>2</inf>Ga<inf>3</inf>O<inf>12</inf>:Ce, Mg (GAGG:Ce,Mg) single crystals were compared. Radioluminescence spectra and photoluminescence decay curves were measured at various temperatures between 77 and 500 K to investigate the thermal luminescence quenching. At 662 keV γ rays, the LY value of 35,400 photons/MeV and energy resolution of 6.9% obtained for GAGG:Ce, Li are superior to those of 24,200 photons/MeV and 9.5% for GAGG:Ce,Mg. Scintillation decays are approximated by a double exponentials with a fast principal decay component of 47 ns (83%) for GAGG:Ce, Mg and 90 ns (86%) for GAGG:Ce,Li. Coincidence time resolution of 282 ps obtained for GAGG:Ce, Mg is better than that of 389 ps for GAGG:Ce,Li. GAGG:Ce, Mg shows a much lower afterglow and thermally stimulated luminescence intensity with respect to GAGG:Ce,Li.

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  223. Development of a novel red-emitting cesium hafnium iodide scintillator

    Kodama, S; Kurosawa, S; Ohno, M; Yamaji, A; Yoshino, M; Pejchal, J; Král, R; Ohashi, Y; Kamada, K; Yokota, Y; Nikl, M; Yoshikawa, A

    RADIATION MEASUREMENTS   Vol. 124   page: 54 - 58   2019.5

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    Cesium hafnium iodide (CHI) was reported as a novel red-emitting scintillator in our previous article, while optimization of the crystal quality and evaluation of the scintillation performance were insufficient. In this study, a large and transparent CHI single crystalline specimen was obtained using slow crystal growth speed. Coupled with a Si avalanche photo-diode, the full width at half maximum energy resolution was evaluated to be 4.2 ± 0.2% at 662 keV which was the best value among conventional red-emitting scintillators. The scintillation light output, non-proportional response of light output and scintillation decay were also evaluated with a photomultiplier tube.

    DOI: 10.1016/j.radmeas.2019.03.005

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  224. Development of a high resolution LaGPS imaging detector with pulse shape discrimination capability of different types of radiations

    Yamamoto, S; Kamada, K; Kurosawa, S; Yoshikawa, A

    NUCLEAR INSTRUMENTS & METHODS IN PHYSICS RESEARCH SECTION A-ACCELERATORS SPECTROMETERS DETECTORS AND ASSOCIATED EQUIPMENT   Vol. 922   page: 8 - 18   2019.4

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    Publisher:Nuclear Instruments and Methods in Physics Research Section A Accelerators Spectrometers Detectors and Associated Equipment  

    Ce doped (GdLa) <inf>2</inf> Si <inf>2</inf> O <inf>7</inf> (LaGPS) is a new scintillator which has high light output and is a promising candidate for high resolution radiation imaging detectors. Thus we developed a radiation imaging detector using a LaGPS plate combined with a position sensitive photomultiplier tube (PSPMT) and evaluated the performance. We found that the decay times of LaGPS were different with the types of radiations and the separations of the images of the different types of radiations were possible using pulse shape discrimination. The spatial resolution for Am-241 alpha particles (5.5 MeV) was better than 0.31 mm FWHM and the energy resolution was 11 % FWHM. The spatial resolution for Sr–Y-90 beta particles was ∼0.6 mm FWHM and those for Co-57 gamma photons (122 keV) and Cs-137 X-ray (∼35 keV) were better than 0.6 mm FWHM and ∼0.8 mm FWHM, respectively. The decay times for alpha particles, beta particles, and gamma photons were 143 ns, 124 ns, and 119 ns, respectively. With these different decay times, the separation of alpha particles and gamma photons or beta particles was possible using the pulse shape discrimination. We conclude that the developed LaGPS imaging detector has high resolution for all types of radiations and is also capable of the simultaneous imaging and separating the different types of radiations.

    DOI: 10.1016/j.nima.2018.11.056

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  225. Employment status was highly associated with quality of life after allogeneic hematopoietic cell transplantation, and the association may differ according to patient age and graft-versus-host disease status: analysis of a nationwide QOL survey

    Kurosawa, S; Yamaguchi, T; Oshima, K; Yanagisawa, A; Fukuda, T; Kanamori, H; Mori, T; Takahashi, S; Kondo, T; Fujisawa, S; Onishi, Y; Yano, S; Onizuka, M; Kanda, Y; Mizuno, I; Taniguchi, S; Yamashita, T; Inamoto, Y; Okamoto, S; Atsuta, Y

    BONE MARROW TRANSPLANTATION   Vol. 54 ( 4 ) page: 611 - 615   2019.4

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    DOI: 10.1038/s41409-018-0343-x

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  226. Thermoelectric Properties of Nb-Doped SrTiO<sub>3</sub>/TiO<sub>2</sub> Eutectic Solids Fabricated by Unidirectional Solidification

    Yokota, Y; Horii, S; Ogino, H; Yoshino, M; Yamaji, A; Ohashi, Y; Kurosawa, S; Kamada, K; Yoshikawa, A

    JOURNAL OF ELECTRONIC MATERIALS   Vol. 48 ( 4 ) page: 1827 - 1832   2019.4

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    Undoped and Nb-doped SrTiO <inf>3</inf> /TiO <inf>2</inf> (STO/TO) eutectic solids were fabricated from the melt at a eutectic point of STO and TO by unidirectional solidification. Fabricated undoped and Nb:STO/TO eutectic solids were composed of the TiO <inf>2</inf> rod-like and the SrTiO <inf>3</inf> matrix phases, and the periodic and uniform eutectic morphology could be achieved in the Nb:STO/TO eutectic solids by stable control of the liquid–solid interface during the fabrication. The thermal conductivity of the Nb:STO/TO eutectic solid was less than half of that of the Nb:STO single crystal owing to the decrease of the lattice thermal conductivity by phonon scattering at the grain boundaries. The figures of merit ZT’s of the Nb:STO/TO eutectic solid, parallel and perpendicular to the growth direction, were ∼ 0.007 and ∼ 0.0004, respectively. The small ZT’s are attributable to the higher electrical resistivity originating from the insufficient carrier doping and high electrical resistivity of the TO phase.

    DOI: 10.1007/s11664-018-06880-2

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  227. The Lu for La substitution effects on the single crystal growth and luminescence properties in Lu<sub>3-x</sub>La<sub>x</sub>Ga<sub>3</sub>Al<sub>2</sub>O<sub>12</sub>:Ce<sup>3+</sup> scintillators

    Yoshikawa Akira, Bartosiewicz Karol, Kurosawa Shunsuke, Yamaji Akihiro, Nikl Martin, Zorenko Yuriy

    JSAP Annual Meetings Extended Abstracts   Vol. 2019.1 ( 0 ) page: 493 - 493   2019.2

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    DOI: 10.11470/jsapmeeting.2019.1.0_493

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  228. Feasibility Study on a red-emitting-scintillation probe with an optical fiber for a high-rate dose-monitor

    Kodama Shohei, Kurosawa Shunsuke, Morishita Yuki, Usami Hiroshi, Hayashi Masateru, Tanaka Hiroki, Yamaji Akihiro, Yoshino Masao, ohashi Yuji, Kamada Kei, Yokota Yuui, Yoshikawa Akira, Torii Tatsuo

    JSAP Annual Meetings Extended Abstracts   Vol. 2019.1 ( 0 ) page: 525 - 525   2019.2

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    DOI: 10.11470/jsapmeeting.2019.1.0_525

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  229. Al-doping effects on mechanical, optical and scintillation properties of Ce:(La,Gd)<sub>2</sub>Si<sub>2</sub>O<sub>7</sub> single crystals

    Takasugi, T; Yokota, Y; Horiai, T; Yoshino, M; Yamaji, A; Ohashi, Y; Kurosawa, S; Kamada, K; Babin, V; Nikl, M; Yoshikawa, A

    OPTICAL MATERIALS   Vol. 87   page: 11 - 15   2019.1

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    Ce:(Gd,La)<inf>2</inf>Si<inf>2</inf>O<inf>7</inf> (Ce:La-GPS) and Al co-doped Ce:(Gd,La)<inf>2</inf>Si<inf>2</inf>O<inf>7</inf> (Al,Ce:La-GPS) single crystals were grown by the micro-pulling-down method to improve the mechanical, optical and scintillation properties. In a tensile test, the maximum strain and stress values in the stress-strain curve of the Al,Ce:La-GPS single crystal compared to the Ce:La-GPS single crystal and the result suggests that there is a possibility of the improvement on the mechanical property by Al co-doping. In addition, the light yield of the La-GPS single crystal under γ-ray irradiation was slightly increased and the decay time was accelerated by the Al co-doping.

    DOI: 10.1016/j.optmat.2018.07.067

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  230. Single crystal growth and luminescent properties of Tb doped GdTaO<sub>4</sub> by the μ-pulling down method

    Murakami, R; Kamada, K; Hatakeyama, S; Ueno, K; Ueno, Y; Tadokoro, T; Shoji, Y; Kurosawa, S; Yamaji, A; Ohashi, Y; Yoshino, M; Yokota, Y; Yoshikawa, A

    OPTICAL MATERIALS   Vol. 87   page: 94 - 97   2019.1

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    GdTaO<inf>4</inf> and (Gd<inf>1-x</inf>Tb<inf>x</inf>)TaO<inf>4</inf> (x = 0, 0.001, 0.02, 0.04, 0.10, and 0.16) single crystals were grown by the micro-pulling down method. The crystallographic system of the grown crystals was identified to be monoclinic (I2/a), which is the stable low-temperature phase of GdTaO<inf>4</inf>. In the photoluminescence (PL) spectra, intense emission was observed at 549 nm (<sup>5</sup>D<inf>3</inf>→<sup>7</sup>F<inf>4</inf> transition of Tb<sup>3+</sup>) for every Tb doped GdTaO<inf>4</inf>. In the excitation spectra for the 549 nm emission, several excitation paths to the Tb<sup>3+</sup> were attributed: 4f-4f transitions of Gd<sup>3+</sup>, 4f<sup>8</sup>-4f<sup>7</sup>5d transitions of Tb<sup>3+</sup> and charge transfer of TaO<inf>4</inf> <sup>3−</sup> group. Radiolumincece spectra under X-ray irradiation were taken, and the highest emission peak was observed at 544 nm, which was ascribed to the <sup>5</sup>D<inf>4</inf>→<sup>7</sup>F<inf>5</inf> transition of Tb<sup>3+</sup>. The Tb 2% doped GdTaO<inf>4</inf> showed the highest emission intensity at the 544 nm, and as increasing dopant concentration, the intensity decreased due to the cross-relaxation of Tb<sup>3+</sup>.

    DOI: 10.1016/j.optmat.2018.05.031

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  231. Eruptive xanthomas in a patient h soft-drink diabetic ketosis and apolipoprotein E4/2 Open Access

    Tsuchiya, S; Sawada, S; Takeda, K; Takahashi, K; Nakajima, T; Kohata, M; Kurosawa, S; Satake, C; Imai, J; Kikuchi, K; Aiba, S; Katagiri, H

    ENDOCRINE JOURNAL   Vol. 66 ( 1 ) page: 107 - 114   2019

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    Soft-drink diabetic ketosis, characterized by acute onset ketosis induced by excessive ingestion of sugar-containing drinks, is often seen in obese, young patients, even with undiagnosed type 2 diabetes. We herein report a 15-year-old obese patient with the apolipoprotein E4/2 phenotype, in whom eruptive xanthomas lead to a diagnosis of soft-drink diabetic ketosis. He developed multiple asymptomatic yellowish papules on the auricles, back, buttocks and the extensor surfaces of the elbows and knees. He initially visited a dermatology clinic and his blood triglyceride and HbA1c levels were found to be 6,490 mg/dL and 16.5%, respectively. He was referred to our hospital for treatment of hyperglycemia and hypertyriglyceridemia. On admission, he had ketonuria and increased blood levels of 3-hydroxybutylate and acetoacetate. He habitually drank 1–3 litters of sweet beverages daily to quench his thirst. Therefore, “soft-drink diabetic ketosis” was diagnosed. Severe hypertriglyceridemia was considered to have been a consequence of impaired insulin action and his apolipoprotein E4/2 phenotype. We treated the diabetic ketosis and hypertriglyceridemia with intensive insulin therapy and a fat-restricted diet. At discharge, he no longer required insulin therapy and his blood glucose levels were controlled with metformin and voglibose. Along with amelioration of the hyperglycemia, triglyceride levels decreased to 247 mg/dL without administration of anti-hyperlipidemia agents. The eruptive xanthoma lesions gradually diminished in size and number and eventually disappeared by 12 months. This case provides an instructive example of eruptive xanthomas serving as a sign of severe dysregulation, not only of lipid, but also glucose, metabolism.

    DOI: 10.1507/endocrj.EJ18-0356

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  232. Evaluation of neutron pulse width in laser-driven neutron source using organic scintillator

    Tanaka, H; Kurosawa, S; Yamaji, A; Yamato, S; Hanayama, R; Sunahara, A; Asahina, T; Nagatomo, H; Mima, K; Kato, Y

    2019 IEEE NUCLEAR SCIENCE SYMPOSIUM AND MEDICAL IMAGING CONFERENCE (NSS/MIC)     2019

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    Laser-driven neutron source is possible to obtain data with higher energy resolution than accelerator based neutron source. The purpose of this study is to evaluate the neutron pulse width for the energy spectrum emitted by the reaction between charged particles experimentally obtained by LFEX laser and a beryllium neutron production target. Monte Carlo simulation code of PHITS 3.02 was used for neutron pulse width evaluation.Furthermore, we investigate the candidate of scintillator for the detection of neutrons in laser-driven neutron source. It was confirmed that the neutron pulse width of a laser-driven neutron source was shorter than that of the accelerator based neutron source in the keV to MeV region. We also experimentally confirmed that organic scintillator such as p-terphenyl was the candidate for the detection of keV to MeV energy region neutron because of high light output and fast decay.

    DOI: 10.1109/nss/mic42101.2019.9059945

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  233. R&D of new high-performance scintillator including double beta decay nuclei

    Iida, T; Kamada, K; Yoshino, M; Kim, KJ; Kurosawa, S; Yoshikawa, A

    2019 IEEE NUCLEAR SCIENCE SYMPOSIUM AND MEDICAL IMAGING CONFERENCE (NSS/MIC)     2019

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  234. ZICOS - Neutrinoless double beta decay experiment using Zr-96 with an organic liquid scintillator -

    Fukuda Y., Moriyama S., Hiraide K., Ogawa I., Gunji T., Hayami R., Tsukada S., Kurosawa S.

    Proceedings of Science   Vol. 364   2019

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    A liquid scintillator containing a tetrakis (isopropyl acetoacetato) zirconium has been developed for ZICOS experiment. In order to reach the sensitivity T<inf>1</inf><sup>0</sup><inf>/</inf><sup>ν</sup><inf>2</inf> ≥ 10<sup>27</sup> years, we have to use tone scale of <sup>96</sup>Zr and have to reduce 95 % of <sup>208</sup>Tl decay background. Using Monte Carlo simulation, we could demonstrate new method using the topological information of Cherenkov light, and could reduce 93 % of <sup>208</sup>Tl background with 78 % efficiency for 0νββ signal. For the discrimination of Cherenkov light, the precise spectral pulse shape from Cherenkov lights was directly measured by using sub-MeV electrons from <sup>90</sup>Sr/<sup>90</sup>Y beta source. The observed shape was clearly different from the shape of scintillation light. The pulse rise and fall (decay) time for Cherenkov light were 0.8 ns and 2.5 ns, respectively. They were actually shorter than those times of scintillation light which were also measured by 1.6 ns and 6.5 ns, respectively. This clear difference of rise time will be used for the pulse shape discrimination in order to select PMT which receive Cherenkov lights, and the topological information due to Cherenkov light will be used for the reduction of backgrounds from <sup>208</sup>Tl decay which should be major backgrounds observed around Q-value (3.35MeV) of <sup>96</sup>Zr neutrinoless double beta decay.

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  235. Development of Novel Scintillation Materials as Transparent Ceramics Open Access

    HARATA Koichi, SONE Hiroshi, KUROSAWA Shunsuke, UJIIE Hiroki

    The Review of Laser Engineering   Vol. 47 ( 8 ) page: 433   2019

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    Scintillators are group of materials applied for radiation detection. Among them, heavy inorganic single
    crystals are used for detection of gamma rays. In order to avoid doping ion segregation or issues related
    to high melting point (more than 2,500 °C), some researchers have focused on transparent ceramics. In
    this paper, we review the transparent ceramics scintillators, especially those prepared by spark plasma
    sintering method.

    DOI: 10.2184/lsj.47.8_433

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  236. New readout and data-acquisition system for reducing dead time in the Gamma Ray Compton Telescope

    Yoshikawa K., Tanimori T., Takada A., Mizumoto T., Mizumura Y., Komura S., Kishimoto T., Takemura T., Nakamasu Y., Taniguchi T., Nakamura Y., Kubo H., Sawano T., Nakamura K., Sonoda S., Miuchi K., Kurosawa S., Parker J.D.

    2017 IEEE Nuclear Science Symposium and Medical Imaging Conference NSS Mic 2017 Conference Proceedings     2018.11

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    Publisher:2017 IEEE Nuclear Science Symposium and Medical Imaging Conference NSS Mic 2017 Conference Proceedings  

    For MeV gamma-ray astronomy, We have developed an electron-tracking Compton camera (ETCC) as a next generation satellite telescope. Our detector consists of a Comptonscattering target and a scattered gamma-ray absorber. The target is a gaseous Time Projection Chamber (TPC), which uses \mu PIC as the 2-dimensional readout detector, and the absorber is position sensitive scintillation arrays (PSAs). We developed a prototype ETCC and certificated its performance in a groundbased experiment. The prototype ETCC had a sharp PSF of 15° included 50%, 662 keV) at the ARM of 5° and the SPD of 100°. We plan to update the prototype ETCC and observe the electronpositron annihilation line of the galactic center in Australia in early 2018 (SMILE-II +). In the data acquisition (DAQ) system of the prototype ETCC, the dead time is estimated to be \sim 20 % at the trigger rate of \sim 100 Hz in a balloon observation, and the prototype ETCC can work. The SMILE-II + ETCC can also work at the balloon altitude. On the other hand, in the future observation with the ETCC, that has a larger effective area than the effective area of SMILE-II + ETCC, the DAQ rate is expected to be \sim~1 kHz. The dead time gets saturation due to sending data via VME bus and common start system in PSA. To overcome the two problem, we develop a new TPC readout board and a PSA readout unit. We create a test model ETCC which have the new TPC readout boards and the new PSA readout units. Although the dead time is \sim 20 % at 30 Hz with a small ETCC in the prototype DAQ system, the dead time is \sim 20 % at 2 kHz in the new system.

    DOI: 10.1109/NSSMIC.2017.8532606

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  237. Phase formation and crystal growth of Ca<sub>3</sub>TaAl<sub>3</sub>Si<sub>2</sub>O<sub>14</sub> piezoelectric single crystal

    Yokota, Y; Ohashi, Y; Yoshino, M; Yamaji, A; Kurosawa, S; Kamada, K; Yoshikawa, A

    JAPANESE JOURNAL OF APPLIED PHYSICS   Vol. 57 ( 11 )   2018.11

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    Publisher:Japanese Journal of Applied Physics  

    Ca<inf>3</inf>TaAl<inf>3</inf>Si<inf>2</inf>O<inf>14</inf> (CTAS) piezoelectric powders were sintered at various temperatures to investigate phase formation. The CTAS powder sintered at 1350 °C was composed of a main phase with a langasite-type structure in addition to two secondary phases, whereas the main phases of the CTAS powders sintered at 1200 and 1300 °C were the secondary phases in X-ray diffraction patterns. CTAS single crystals with a diameter of 1 in. were grown by a Czochralski method using the sintered powders, and CTAS single crystals without impurity phases could be grown using the powder sintered at 1350 °C. A higher sintering temperature of starting materials contributes to the creation of CTAS single crystals without impurity phases.

    DOI: 10.7567/JJAP.57.11UD11

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  238. Prognostic impact of low allelic ratio <i>FLT3</i>-ITD and <i>NPM1</i> mutation in acute myeloid leukemia Open Access

    Sakaguchi, M; Yamaguchi, H; Najima, Y; Usuki, K; Ueki, T; Oh, I; Mori, S; Kawata, E; Uoshima, N; Kobayashi, Y; Kako, S; Tajika, K; Gomi, S; Shono, K; Kayamori, K; Hagihara, M; Kanda, J; Uchiyama, H; Kuroda, J; Uchida, N; Kubota, Y; Kimura, S; Kurosawa, S; Nakajima, N; Marumo, A; Omori, I; Fujiwara, Y; Yui, S; Wakita, S; Arai, K; Kitano, T; Kakihana, K; Kanda, Y; Ohashi, K; Fukuda, T; Inokuchi, K

    BLOOD ADVANCES   Vol. 2 ( 20 ) page: 2744 - 2754   2018.10

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    In the opinion of the European LeukemiaNet (ELN), nucleophosmin member 1 gene mutation (NPM1 mut)-positive acute myeloid leukemia (AML) with an fms-like kinase 3-internal tandem duplication (FLT3-ITD) allele ratio (AR)<0.5 (low AR) has a favorable prognosis, and allogeneic hematopoietic stem cell transplant (allo-HSCT) in the first complete remission (CR1) period is not actively recommended. We studied 147 patients with FLT3-ITD gene mutation-positive AML, dividing them into those with low AR and those with AR of ≥0.5 (high AR), and examined the prognostic impact according to allo-HSCT in CR1. Although FLT3-ITD AR and NPM1 mut are used in the prognostic stratification, we found that NPM1 mut-positive AML with FLT3-ITD low AR was not associated with favorable outcome (overall survival [OS], 41.3%). Moreover, patients in this group who underwent allo-HSCT in CR1 had a significantly more favorable outcome than those who did not (relapse-free survival [RFS] P = .013; OS P = .003). Multivariate analysis identified allo-HSCT in CR1 as the sole favorable prognostic factor (RFS P< .001; OS P < .001). The present study found that prognosis was unfavorable in NPM1 mut-positive AML with FLT3-ITD low AR when allo-HSCT was not carried out in CR1.

    DOI: 10.1182/bloodadvances.2018020305

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  239. A multi-center prospective study randomizing the use of fat emulsion in intensive glucose control after allogeneic hematopoietic stem cell transplantation using a myeloablative conditioning regimen

    Fuji, S; Kim, SW; Kamiya, S; Nakane, T; Matsumoto, K; Onishi, Y; Yakushijin, K; Yamazaki, E; Hino, M; Kurosawa, S; Yoshimura, K; Fukuda, T

    CLINICAL NUTRITION   Vol. 37 ( 5 ) page: 1534 - 1540   2018.10

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    Background & aims: Although parenteral nutrition (PN) is often used after allogeneic hematopoietic stem cell transplantation (allo-HSCT), there is controversy regarding PN management, for instance in the use of fat emulsion and glucose control (GC). To clarify these issues, we conducted a multi-center prospective study with intensive GC, randomizing the use of fat emulsion after allo-HSCT using a myeloablative conditioning regimen. Methods: The primary endpoint was the cumulative incidence of documented infectious disease, namely bacterial and fungal infection, at day 100 after allo-HSCT. Between August 2007 and March 2012, we enrolled 81 patients at 5 centers. Excluding 5 ineligible patients, 76 patients received the protocol treatment. The target fasting glucose level was 80–110 mg/dL. Results: The median follow-up of surviving patients was 1796 days. The cumulative incidences of documented infectious disease at day 100 were 16% (95% confidence interval [CI] 6–29%) in the no-fat group and 19% (95% CI 8–32%) in the fat group, indicating no significant difference. The mean glucose level at 28 days after allo-HSCT was 107 mg/dL in the no-fat group and 111 mg/dL in the fat group. Grade 3 hyperglycemia (>250 mg/dL) and grade 3 hypoglycemia (<40 mg/dL) occurred in 4 patients each (5.3%). Overall survival and non-relapse mortality rates at 4 years were 75% and 11% in the no-fat group and 69% and 8% in the fat group, respectively. Conclusions: Irrespective of the use of fat emulsion, the long-term clinical outcomes of the enrolled patients were favorable under intensive GC. To further clarify the benefits of GC after allo-HSCT, a prospective study randomizing the level of GC is warranted.

    DOI: 10.1016/j.clnu.2017.08.022

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  240. Impact of past and present chronic graft-versus-host disease on quality of life in hematopoietic cell transplantation survivors

    Kurosawa, S; Yamaguchi, T; Oshima, K; Yanagisawa, A; Fukuda, T; Kanamori, H; Mori, T; Takahashi, S; Kondo, T; Megumi, I; Miyamura, K; Umemoto, Y; Teshima, T; Taniguchi, S; Yamashita, T; Inamoto, Y; Kanda, Y; Okamoto, S; Atsuta, Y

    QUALITY OF LIFE RESEARCH   Vol. 27   page: S139 - S139   2018.10

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  241. Growth and characterization of directionally solidified eutectic systems for scintillator applications

    Yoshikawa, A; Kamada, K; Kurosawa, S; Yokota, Y; Yamaji, A; Chani, VI; Ohashi, Y; Yoshino, M

    JOURNAL OF CRYSTAL GROWTH   Vol. 498   page: 170 - 178   2018.9

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    Publisher:Journal of Crystal Growth  

    Fabrication of scintillating eutectic composites by various directional solidification techniques is introduced and discussed in some details. Number of methods widely practiced for the single crystal growth including Czochralski, Bridgman or vertical zone melting, and micro-pulling-down are also acceptable for the production of eutectic materials. Two types of such materials are considered here. These are (1) composites used for neutron scintillators; eutectic materials that consist of high neutron cross section material and efficient scintillator (they do not require regular micro-structure) and (2) high resolution scintillators; eutectic materials that have well ordered rod/fiber structure of one of the phases immersed into matrix of second phase (one of them should be efficient scintillator). In later one, the wave guiding can be established in one of the phases (either matrix or fibers). The composites with fiber structure are supposed to be very promising substances for detecting initial irradiation with high spatial resolution. LiF/LiYF<inf>4</inf> and LiF/CaF<inf>2</inf>:Eu eutectic composites represent first group of the scintillators, but CsI/NaCl and GdAlO<inf>3</inf>/α-Al<inf>2</inf>O<inf>3</inf> correspond to the second one.

    DOI: 10.1016/j.jcrysgro.2018.02.032

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  242. The effect of Li and Mg codoping strategy on the properties of Gd<sub>3</sub>Ga<sub>3</sub>Al<sub>2</sub>O<sub>12</sub> single Crystal scintillators

    Bartosiewicz Karol, Yoshikawa Akira, Kurosawa Shunsuke, Yamaji Akihiro, Nikl Martin

    JSAP Annual Meetings Extended Abstracts   Vol. 2018.2 ( 0 ) page: 435 - 435   2018.9

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    DOI: 10.11470/jsapmeeting.2018.2.0_435

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  243. Luminescence processes in Ti-doped LiAlO<sub>2</sub> single crystals for neutron scintillators

    Pejchal, J; Babin, V; Kucerkova, R; Mihokova, E; Beitlerova, A; Kurosawa, S; Nikl, M; Yoshikawa, A

    JOURNAL OF LUMINESCENCE   Vol. 201   page: 231 - 244   2018.9

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    Publisher:Journal of Luminescence  

    LiAlO<inf>2</inf> can be considered as a good candidate for neutron scintillator host matrix due to the high Li content and high energy deposit of reaction of <sup>6</sup>Li isotope with neutron. Low density (2.75 g/cm<sup>3</sup>) is of advantage to achieve low sensitivity of background gamma radiation in mixed radiation fields. Ti-doped LiAlO<inf>2</inf> shows relatively high neutron light yield comparable to that of the Li-glass standard neutron scintillator. At room temperature the Ti<sup>4+</sup> charge transfer (CT) luminescence at 375 nm with the 2.5 µs decay time is the leading emission process. Besides the CT luminescence host emission at shorter wavelengths (350 nm), defect-related emission at 440 nm and impurity Fe<sup>3+</sup> luminescence at 740 nm are observed. Their emission spectra, excitation spectra and decay kinetics including temperature dependences were studied. Luminescence mechanism in the material and interplay between the luminescence processes are discussed together with possible role of nonstoichiometry and Mg codoping.

    DOI: 10.1016/j.jlumin.2018.04.047

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  244. Relationship between employment status and quality of life after allogeneic hematopoietic cell transplantation according to patient age and GVHD status

    Kurosawa, S; Yamaguchi, T; Oshima, K; Yanagisawa, A; Fukuda, T; Kanamori, H; Mori, T; Takahashi, S; Kondo, T; Fujisawa, S; Onishi, Y; Yano, S; Onizuka, M; Kanda, Y; Mizuno, I; Taniguchi, S; Yamashita, T; Inamoto, Y; Okamoto, S; Atsuta, Y

    BONE MARROW TRANSPLANTATION   Vol. 53   page: 365 - 367   2018.9

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  245. Outcomes of patients who developed subsequent solid cancer after hematopoietic cell transplantation. Open Access

    Inamoto Y, Matsuda T, Tabuchi K, Kurosawa S, Nakasone H, Nishimori H, Yamasaki S, Doki N, Iwato K, Mori T, Takahashi S, Yabe H, Kohno A, Nakamae H, Sakura T, Hashimoto H, Sugita J, Ago H, Fukuda T, Ichinohe T, Atsuta Y, Yamashita T, Japan Society for Hematopoietic Cell Transplantation Late Effects and Quality of Life Working Group

    Blood advances   Vol. 2 ( 15 ) page: 1901 - 1913   2018.8

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    DOI: 10.1182/bloodadvances.2018020966

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  246. The putative anti-leukemic effects of anti-thymocyte globulins in patients with CD7-positive acute myeloid leukemia

    Ochi K., Fuji S., Takano K., Tajima K., Ito A., Tanaka T., Inamoto Y., Kurosawa S., Kim S.W., Tojo A., Fukuda T.

    Bone Marrow Transplantation   Vol. 53 ( 8 ) page: 1019 - 1029   2018.8

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    Polyclonal anti-thymocyte globulins (ATGs) are widely used in allogeneic stem cell transplantation (allo-SCT) for GvHD prophylaxis. ATGs exerted anti-tumor effects in in vitro experiments, but in vivo studies are lacking. We experienced a case of relapsed AML with cells positive for CD7 who underwent haploidentical SCT and unexpectedly achieved a significant reduction of AML cells in the peripheral blood after receiving ATGs before the administration of other drugs in the conditioning regimen. This patient achieved long-term survival after haploidentical SCT. To assess the impact of ATGs on clinical outcomes in patients with AML, we performed a retrospective analysis of allo-SCT for relapsed/refractory AML and divided 132 patients into four groups according to the expression of CD7 in AML cells and use of ATGs as part of the conditioning regimen, as follows: CD7-positive ATG group (n = 15), CD7-positive no-ATG group (n = 32), CD7-negative ATG group (n = 19), and CD7-negative no-ATG group (n = 66). The overall survival rates in the CD7-positive ATG group were significantly higher than those in the CD7-positive no-ATG group, whereas these rates did not differ statistically between the CD7-negative ATG and CD7-negative no-ATG groups. Our results indicate a possible anti-leukemic effect of ATGs against CD7-positive AML in humans.

    DOI: 10.1038/s41409-018-0115-7

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  247. Comprehensive Study on Ce-Doped (Gd,La)<sub>2</sub>Si<sub>2</sub>O<sub>7</sub> Scintillator

    Kurosawa, S; Horiai, T; Murakami, R; Shoji, Y; Pejchal, J; Yamaji, A; Kodama, S; Ohashi, Y; Yokota, Y; Kamada, K; Yoshikawa, A; Ohnishi, A; Kitaura, M

    IEEE TRANSACTIONS ON NUCLEAR SCIENCE   Vol. 65 ( 8 ) page: 2136 - 2139   2018.8

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    Publisher:IEEE Transactions on Nuclear Science  

    Ce-doped (Gd, La) <inf>2</inf> Si <inf>2</inf> O <inf>7</inf> (Ce:La-GPS) scintillator was found to have a good light output of around 40 000 photons/MeV, while some other parameters have not been determined so far. In order to clarify the cause for such a high light yield, some physical parameters have been estimated in this paper. The bandgap energy of Ce:La-GPS was evaluated to be over 7.13 ± 0.03 eV for (Gd <inf>0.75</inf> , La <inf>0.25</inf> ) <inf>2</inf> Si <inf>2</inf> O <inf>7</inf> . Although Ce:La-GPS had wider bandgap compared with the other oxide scintillators, its light output was larger than values for some other scintillators. Since quantum yield of Ce:La-GPS was as high as around 0.8, the product of transfer efficiency and electron-hole pair generation efficiency was estimated to be around 0.9, which was higher than for the other scintillators. Thus, Ce:La-GPS was suggested to have high the product of transfer efficiency and/or electron-hole pair generation efficiency.

    DOI: 10.1109/TNS.2018.2841917

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  248. Growth and Luminescent Properties of Cs<sub>2</sub>HfCl<sub>6</sub> Scintillators Doped With Alkaline Earth Metals

    Kodama, S; Kurosawa, S; Pejchal, J; Král, R; Yamaji, A; Ohashi, Y; Yokota, Y; Kamada, K; Nikl, M; Yoshikawa, A

    IEEE TRANSACTIONS ON NUCLEAR SCIENCE   Vol. 65 ( 8 ) page: 2169 - 2173   2018.8

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    Publisher:IEEE Transactions on Nuclear Science  

    Nondoped Cs<inf>2</inf>HfCl<inf>6</inf> (CHC) and alkaline earth metal-doped CHC (AE:CHC) crystals were grown by the vertical Bridgman-Stockbarger method. The spectra of the AE:CHC under X-ray excitation were similar to those for the AE-free crystal; thus, AE doping did not change emission wavelength of CHC. We determined the light outputs and energy resolutions of nondoped CHC and AE:CHC by measuring pulse-height spectra under 662-keV gamma-ray excitation of a <sup>137</sup>Cs source. Both light output and energy resolution were deteriorated with AE doping. For example, nondoped CHC had a light output of 44 000 photons/MeV and energy resolution of 5.2%; on the other hand, Sr 0.5 at.%-doped CHC had a light output of only 28 000 photons/MeV and energy resolution of 10%. Scintillation decay also did not change. The nonproportional response values of light output versus gamma-ray energy did not improve in AE:CHC either. Therefore, doped AEs can be responsible for creation of defect trap levels which would hamper the carrier transport in CHC structure.

    DOI: 10.1109/TNS.2018.2848474

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  249. Optimization of Dopants and Scintillation Fibers' Diameter of GdAlO<sub>3</sub>/α-Al<sub>2</sub>O<sub>3</sub> Eutectic for High-Resolution X-Ray Imaging

    Kamada, K; Yasui, N; Ohashi, Y; Den, T; Yamaguchi, H; Yamaji, A; Shoji, Y; Yoshisno, M; JinKim, K; Kurosawa, S; Ohashi, Y; Yokota, Y; Yoshikawa, A

    IEEE TRANSACTIONS ON NUCLEAR SCIENCE   Vol. 65 ( 8 ) page: 2036 - 2040   2018.8

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    Submicrometer diameter phase-separated scintillator fibers (PSSFs) were reported and they possessed both the properties of an optical fiber and radiation-to-light conversion. The PSSFs were fabricated using a directionally solidified eutectic system. High-resolution X-ray imaging can be developed using the PSSFs. In this paper, Tb- and Eu-doped GdAlO<inf>3</inf> (GAP)/ α-Al<inf>2</inf>O<inf>3</inf> eutectic scintillator was grown by the micro pulling down method with various growth rates in order to achieve the high light output and the high light-guiding efficiency. Relationship between radioluminescence intensity and dopant concentration of Eu and Tb was investigated. At the optimized dopant concentration, relationship between growth rate, eutectic period structure, diameter of PSSFs, and contrast transfer function was investigated to achieve high-resolution X-ray imaging.

    DOI: 10.1109/TNS.2018.2841026

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  250. Shallow electron traps formed by Gd<SUP>2+</SUP> ions adjacent to oxygen vacancies in cerium-doped Gd<sub>3</sub>Al<sub>2</sub>Ga<sub>3</sub>O<sub>12</sub> crystals

    Kitaura, M; Watanabe, S; Kamada, K; Kim, KJ; Yoshino, M; Kurosawa, S; Yagihashi, T; Ohnishi, A; Hara, K

    APPLIED PHYSICS LETTERS   Vol. 113 ( 4 )   2018.7

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    To clarify the origin of shallow electron traps in cerium-doped Gd<inf>3</inf>Al<inf>2</inf>Ga<inf>3</inf>O<inf>12</inf> (Ce:GAGG), the optical properties of cerium-doped Lu<inf>3-</inf> <inf>x</inf>Gd<inf>x</inf>Al<inf>2</inf>Ga<inf>3</inf>O<inf>12</inf> crystals were investigated. Absorption spectra for x = 3 exhibited a prominent band at 12 000 cm<sup>-1</sup> when excited by 3.31-eV ultraviolet light. This band has been previously attributed to shallow electron traps at defect complexes associated with oxygen vacancies. When Gd<sup>3+</sup> ions were replaced with Lu<sup>3+</sup> ions, the 12 000 cm<sup>-1</sup> band weakened and disappeared completely for Ce:Lu<inf>3</inf>Al<inf>2</inf>Ga<inf>3</inf>O<inf>12</inf>. In addition, thermally stimulated luminescence glow curves were observed. Optically stimulated luminescence indicated that the energy of the conduction band minimum did not change by the presence of Lu<sup>3+</sup> ions. Thus, the Gd<sup>3+</sup> ions were important for the formation of shallow electron traps in Ce:GAGG. First-principles calculations implied that Gd<sup>3+</sup> ions responsible for shallow electron traps formed antisite defects at GAGG octahedral sites. Hence, defect complexes of antisite Gd<sup>2+</sup> ions adjacent to oxygen vacancies were the most plausible candidates for shallow electron traps in Ce:GAGG.

    DOI: 10.1063/1.5043218

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  251. Fabrication and Evaluation of Ce3+ Ion Doped CaF2 Thin Film Phosphor

    Hishiki M., Inoue Y., Ono S., Kurosawa S., Yoshikawa A.

    2018 Conference on Lasers and Electro Optics Pacific Rim CLEO PR 2018     2018.7

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    We fabricated Ce<sup>3+</sup>: CaF2 thin films with different doping concentration in anticipation of use as a phosphor. We calculated practical doping concentration from lattice distortion and evaluated the optimized doping concentration for high efficiency light emission.

    DOI: 10.1364/cleopr.2018.w3a.92

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  252. Crystal growth, optical properties, and scintillation responses of Pr-doped CeBr<sub>3</sub> single crystals

    Yokota, Y; Ito, T; Yoshino, M; Yamaji, A; Ohashi, Y; Kurosawa, S; Kamada, K; Yoshikawa, A

    JAPANESE JOURNAL OF APPLIED PHYSICS   Vol. 57 ( 7 )   2018.7

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    Publisher:Japanese Journal of Applied Physics  

    CeBr<inf>3</inf> and Pr-doped CeBr<inf>3</inf> (Pr:CeBr<inf>3</inf>) single crystals were grown by the halide-micro-pulling-down method, and the effects of Pr doping on the optical and scintillation properties of the CeBr<inf>3</inf> single crystal were investigated. The emission peaks originating from the 4f-4f transition of Pr<sup>3+</sup>ions were observed in the photoluminescence spectrum of the Pr:CeBr<inf>3</inf> single crystal in addition to the emission peaks related to the 5d-4f transition of Ce<sup>3+</sup> ions. The decay of fast and slow components under gamma-ray irradiation systematically accelerated with increasing Pr concentration while the light yield decreased.

    DOI: 10.7567/JJAP.57.070312

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  253. Growth and Scintillation Properties of Two-Inch-Diameter SrI<sub>2</sub>(Eu) Single Crystals

    Shoji, Y; Kurosawa, S; Yokota, Y; Hayasaka, S; Kamada, K; Yoshino, M; Yamaji, A; Chani, V; Ohashi, Y; Sakuragi, S; Yoshikawa, A

    CRYSTAL GROWTH & DESIGN   Vol. 18 ( 7 ) page: 3747 - 3752   2018.7

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    Publisher:Crystal Growth and Design  

    The sealed vertical Bridgman (VB) method is the main technique used to grow SrI<inf>2</inf>(Eu) crystals because SrI<inf>2</inf>(Eu) is very hygroscopic. In this study, we grew SrI<inf>2</inf>(Eu) single crystals with two-inch diameters and four-inch lengths using the VB method equipped with a removable chamber. The SrI<inf>2</inf>(Eu) single crystals were produced by the Liquinert process, which requires careful consideration of the crucible material and growth atmosphere. After a review of available materials, carbon crucibles were selected due to their several advantages over traditional quartz ampules: (1) they are suitable for large size crystal growth due to which they do not require any process for sealing of quartz ampule before the growth; (2) ease in controlling the temperature gradient because carbon crucibles can be heated directly via a high frequency induction heating system; and (3) carbon crucibles can assist in removing oxygen and moisture from the melt. The starting material, seed, and hot zone were prepared inside the glovebox in the removable growth chamber, which was used as the growth unit. This unit was installed in the growth system and heated to the melting point of SrI<inf>2</inf>(Eu) in a high-purity Ar atmosphere. The crucible in the growth chamber was then displaced in the downward direction for crystal growth. Crack-free SrI<inf>2</inf>(Eu) bulk single crystals with two-inch diameters were produced. The crystals were cut into cylindrical specimens (diameter = length = 2 in.), polished, and sealed in an aluminum case with a quartz glass window for evaluation. Negligible self-absorption was observed because of the large length of the crystal. The light output of the SrI<inf>2</inf>(Eu) examined in this study was estimated to be 70 000 photons/MeV, and the calculated energy resolution was 3.4% (662 keV, full width at half-maximum) at room temperature.

    DOI: 10.1021/acs.cgd.7b01044

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  254. Refractory Graft-Versus-Host Disease-Free, Relapse-Free Survival as an Accurate and Easy-to-Calculate Endpoint to Assess the Long-Term Transplant Success

    Kawamura, K; Nakasone, H; Kurosawa, S; Yoshimura, K; Misaki, Y; Gomyo, A; Hayakawa, J; Tamaki, M; Akahoshi, Y; Kusuda, M; Kameda, K; Wada, H; Ishihara, Y; Sato, M; Terasako-Saito, K; Kikuchi, M; Kimura, SI; Tanihara, A; Kako, S; Kanamori, H; Mori, T; Takahashi, S; Taniguchi, S; Atsuta, Y; Kanda, Y

    BIOLOGY OF BLOOD AND MARROW TRANSPLANTATION   Vol. 24 ( 7 ) page: 1521 - 1526   2018.7

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    The aim of this study was to develop a new composite endpoint that accurately reflects the long-term success of allogeneic hematopoietic stem cell transplantation (allo-HSCT), as the conventional graft-versus-host disease (GVHD)–free, relapse-free survival (GRFS) overestimates the impact of GVHD. First, we validated current GRFS (cGRFS), which recently was proposed as a more accurate endpoint of long-term transplant success. cGRFS was defined as survival without disease relapse/progression or active chronic GVHD at a given time after allo-HSCT, calculated using 2 distinct methods: a linear combination of a Kaplan-Meier estimates approach and a multistate modelling approach. Next, we developed a new composite endpoint, refractory GRFS (rGRFS). rGRFS was calculated similarly to conventional GRFS treating grade III to IV acute GVHD, chronic GVHD requiring systemic treatment, and disease relapse/progression as events, except that GVHD that resolved and did not require systemic treatment at the last evaluation was excluded as an event in rGRFS. The 2 cGRFS curves obtained using 2 different approaches were superimposed and both were superior to that of conventional GRFS, reflecting the proportion of patients with resolved chronic GVHD. Finally, the curves of cGRFS and rGRFS overlapped after the first 2 years of post-transplant follow-up. These results suggest that cGRFS and rGRFS more accurately reflect transplant success than conventional GRFS. Especially, rGRFS can be more easily calculated than cGRFS and analyzed with widely used statistical approaches, whereas cGRFS more accurately represents the burden of GVHD-related morbidity in the first 2 years after transplantation.

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  255. Scintillation properties of Gd<sub>3</sub>(Al<sub>5-x</sub>Ga<sub>x</sub>)O<sub>12</sub>:Ce (x=2.3, 2.6, 3.0) single crystals

    Chewpraditkul, W; Pattanaboonmee, N; Sakthong, O; Chewpraditkul, W; Szczesniak, T; Moszynski, M; Kamada, K; Kurosawa, S; Yoshikawa, A; Nikl, M

    OPTICAL MATERIALS   Vol. 81   page: 23 - 29   2018.7

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    Scintillation properties of Czochralski-grown Gd<inf>3</inf>(Al<inf>5-x</inf>Ga<inf>x</inf>)O<inf>12</inf>:Ce (x = 2.3, 2.6, 3.0) single crystals were investigated. With increasing Ga content in garnet host, the radioluminescence band due to 5d<inf>1</inf> → 4f emission transition was blue-shifted due to a decrease in the crystal field splitting of the 5 d levels. At 662 keV γ rays, the LY value of 47,000, 55,100 and 51,900 ph/MeV was obtained for Gd<inf>3</inf>Al<inf>2.7</inf>Ga<inf>2.3</inf>O<inf>12</inf>:Ce, Gd<inf>3</inf>Al<inf>2.4</inf>Ga<inf>2.6</inf>O<inf>12</inf>:Ce and Gd<inf>3</inf>Al<inf>2</inf>Ga<inf>3</inf>O<inf>12</inf>:Ce, respectively. In spite of a lower LY value, Gd<inf>3</inf>Al<inf>2.7</inf>Ga<inf>2.3</inf>O<inf>12</inf>:Ce shows good energy resolution of 4.1% due to its proportionality of LY. The ratio of LY values under excitation with α- and γ-rays (α/γ ratio) was also determined. The fast component decay time with relative intensity of 146 ns (66%), 142 ns (76%) and 112 ns (76%) was measured in the scintillation decay of Gd<inf>3</inf>Al<inf>2.7</inf>Ga<inf>2.3</inf>O<inf>12</inf>:Ce, Gd<inf>3</inf>Al<inf>2.4</inf>Ga<inf>2.6</inf>O<inf>12</inf>:Ce and Gd<inf>3</inf>Al<inf>2</inf>Ga<inf>3</inf>O<inf>12</inf>:Ce, respectively. Good coincidence time resolution of Gd<inf>3</inf>Al<inf>2</inf>Ga<inf>3</inf>O<inf>12</inf>:Ce is due to a high initial photon emission rate.

    DOI: 10.1016/j.optmat.2018.05.015

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  256. Role of up-front allogeneic hematopoietic stem cell transplantation for patients with aggressive adult T-cell leukemia-lymphoma: a decision analysis Open Access

    Fuji, S; Kurosawa, S; Inamoto, Y; Murata, T; Utsunomiya, A; Uchimaru, K; Yamasaki, S; Inoue, Y; Moriuchi, Y; Choi, I; Ogata, M; Hidaka, M; Yamaguchi, T; Fukuda, T

    BONE MARROW TRANSPLANTATION   Vol. 53 ( 7 ) page: 905 - 908   2018.7

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    DOI: 10.1038/s41409-017-0082-4

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  257. Growth and luminescent properties of Ce and Eu doped Cesium Hafnium Iodide single crystalline scintillators

    Kodama, S; Kurosawa, S; Yamaji, A; Pejchal, J; Král, R; Ohashi, Y; Kamada, K; Yokota, Y; Nikl, M; Yoshikawa, A

    JOURNAL OF CRYSTAL GROWTH   Vol. 492   page: 1 - 5   2018.6

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    In order to obtain new scintillators with high light output and high effective atomic number (Z<inf>eff</inf>), we performed anion-substitution for Cs<inf>2</inf>HfCl<inf>6</inf> (CHC) scintillator, and then, we succeeded in growing Cs<inf>2</inf>HfI<inf>6</inf> (CHI) single crystalline scintillator. It had Z<inf>eff</inf> of 58, which is the same as that of CHC, and had high light output of ∼70,000 photons/MeV with 700 nm emission. However, its scintillation decay time of ∼2.5 µs was slow for practical use as gamma-ray monitor. In this study, we performed Ce<sup>3+</sup>/Eu<sup>2+</sup> doping to Hf<sup>4+</sup> site to improve decay time of CHI, introducing the fast 5d-4f luminescence. Ce:CHI and Eu:CHI single crystals were finally obtained by the vertical Bridgman-Stockbarger method. The luminescence spectra of the Ce:CHI and Eu:CHI were very similar to that of the non-doped CHI, which would mean that no 5d-4f luminescence of Ce<sup>3+</sup>/Eu<sup>2+</sup> was observed. The measured light output and decay time of Ce:CHI were ∼48,000 photon/MeV and 2.3 ± 0.1 µs, respectively. As for Eu:CHI, light output and decay time were ∼69,000 photon/MeV and 2.8 ± 0.1 µs, respectively.

    DOI: 10.1016/j.jcrysgro.2018.03.033

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  258. Melt growth of zinc aluminate spinel single crystal by the micro-pulling down method under atmospheric pressure

    Kamada, K; Shoji, Y; Yamaji, A; Kurosawa, S; Yokota, Y; Ohashi, Y; Kim, KJ; Ivanov, M; Kochurikhin, VV; Yoshikawa, A

    JOURNAL OF CRYSTAL GROWTH   Vol. 492   page: 67 - 70   2018.6

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    ZnAl<inf>2</inf>O<inf>4</inf> crystals were grown using few starting compositions with various ZnO:AlO<inf>3/2</inf> ratio using an Ir wire seed and Ir + Re crucible under ordinary pressure with Ar + 2%O<inf>2</inf> atmosphere by the radiofrequency heating µ-PD furnace. The ZnAl<inf>2</inf>O<inf>4</inf> spinel single crystal with 4 mm diameter could be successfully grown by the µ-PD method by optimization of starting melt composition considering with Zinc oxide evaporation. During 10 min of growth under normal pressure the formation of ZnAl<inf>2</inf>O<inf>4</inf> single phase observed even at high vapor pressure of ZnO. The transmittance spectra and X-ray locking curve were measured for evaluating of grown ZnAl<inf>2</inf>O<inf>4</inf> crystals quality.

    DOI: 10.1016/j.jcrysgro.2018.03.009

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  259. Single crystal growth of submillimeter diameter sapphire tube by the micro-pulling down method

    Kamada, K; Murakami, R; Kochurikhin, VV; Luidmila, G; Kim, KJ; Shoji, Y; Yamaji, A; Kurosawa, S; Ohashi, Y; Yokota, Y; Yoshikawa, A

    JOURNAL OF CRYSTAL GROWTH   Vol. 492   page: 45 - 49   2018.6

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    This paper addresses several aspects of the µ-PD growth technology as applied to submillimeter diameter sapphire tubes for UFD application. The μ-PD method has been successfully adapted for single crystal sapphire tube growth. A compound crucible made possible the growth of single crystal sapphire tube as small as around 0.70–0.72 mm in outer diameter and 0.28–0.29 in inner diameter over 160 mm in length at growth rate of 2–4 mm/min along 〈0 0 1〉 direction. An Ir crucible with a die composed of an equivalent hole and Ir wire was heated by RF coil in N<inf>2</inf> atmosphere. The μ-PD method has been successfully adapted for single crystal sapphire tube growth. Grown crystal tube showed good XRC value of 30.2 arcsec.

    DOI: 10.1016/j.jcrysgro.2018.03.023

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  260. Crystal structure of Ce-doped (La,Gd)<sub>2</sub>Si<sub>2</sub>O<sub>7</sub> grown by the Czochralski process

    Murakami, R; Kurosawa, S; Yamane, H; Horiai, T; Shoji, Y; Yokota, Y; Yamaji, A; Ohashi, Y; Kamada, K; Yoshikawa, A

    JOURNAL OF ALLOYS AND COMPOUNDS   Vol. 748   page: 404 - 410   2018.6

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    Single crystals of (La<inf>0.25</inf>Gd<inf>0.75</inf>)<inf>2</inf>Si<inf>2</inf>O<inf>7</inf> and (La<inf>0.235</inf>Ce<inf>0.015</inf>Gd<inf>0.75</inf>)<inf>2</inf>Si<inf>2</inf>O<inf>7</inf> were grown by the Czochralski method. Structure analysis of the single crystals by X-ray diffraction (XRD) revealed that (La<inf>0.25</inf>Gd<inf>0.75</inf>)<inf>2</inf>Si<inf>2</inf>O<inf>7</inf> and (La<inf>0.235</inf>Ce<inf>0.015</inf>Gd<inf>0.75</inf>)<inf>2</inf>Si<inf>2</inf>O<inf>7</inf> crystalize in monoclinic cells (space group P2<inf>1</inf>/c), a = 5.3905(8) Å, b = 8.5605(11) Å, c = 13.957(2) Å, β = 112.223(6)º, and a = 5.3921(7) Å, b = 8.5688(10) Å, c = 13.9172(14) Å, β = 111.980(5)º, respectively. One of the two different rare-earth sites is preferentially occupied by La and Gd atoms or by La, Ce and Gd atoms, and the other is occupied by Gd atoms only. Peaks attributed to the 4f-4f transitions (<sup>8</sup>S<inf>7/2</inf>–<sup>6</sup>G<inf>7/2</inf> and <sup>8</sup>S<inf>7/2</inf>–<sup>6</sup>I<inf>x</inf>) of Gd<sup>3+</sup> and 4f-5d transitions of Ce<sup>3+</sup> were observed in the absorption spectra of (La<inf>0.25</inf>Gd<inf>0.75</inf>)<inf>2</inf>Si<inf>2</inf>O<inf>7</inf> and (La<inf>0.235</inf>Ce<inf>0.015</inf>Gd<inf>0.75</inf>)<inf>2</inf>Si<inf>2</inf>O<inf>7</inf> single crystals.

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  261. Li<SUP>+</SUP>, Na<SUP>+</SUP> and K<SUP>+</SUP> co-doping effects on scintillation properties of Ce: Gd<sub>3</sub>Ga<sub>3</sub>Al<sub>2</sub>O<sub>12</sub> single crystals

    Yoshino, M; Kamada, K; Kochurikhin, VV; Ivanov, M; Nikl, M; Okumura, S; Yamamoto, S; Yeom, JY; Shoji, Y; Kurosawa, S; Yokota, Y; Ohashi, Y; Yoshikawa, A

    JOURNAL OF CRYSTAL GROWTH   Vol. 491   page: 1 - 5   2018.6

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    Ce0.5%: Ce:Gd<inf>3</inf>Ga<inf>3</inf>Al<inf>2</inf>O<inf>12</inf>(GGAG) single crystals co-doped with 500at.ppm Li<sup>+</sup>, Na<sup>+</sup> and K<sup>+</sup> were grown by using the micro-pulling down method. The smooth Ce<sup>4+</sup> charge transfer absorption below 350 nm and decay time acceleration were observed in Li co-doped sample. Na<sup>+</sup> and K<sup>+</sup> co-doping did not show a large effect on the acceleration of decay time compared with Li co-doping. Ce0.5%:GGAG single crystals co-doped with 500 at.ppm Li<sup>+</sup> were also grown by the Czochralski method. Optical, scintillation properties and timing performance were evaluated to investigate the effect of univalent alkali metal ions co-doping on Ce:GGAG scintillators. The scintillation decay curves were accelerated by Li co-doping: the decay time was significantly accelerated to 54.8 ns (47%) for the faster component and 158 ns (53%) for the slower component. The light output was 94% of the non co-doped Ce:GGAG standard. The coincidence time resolution was improved to 258 ps by Li co-doping.

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  262. Effects of Ca/Sr ratio control on optical and scintillation properties of Eu-doped Li(Ca,Sr)AlF<sub>6</sub> single crystals

    Yokota, Y; Tanaka, C; Kurosawa, S; Yamaji, A; Ohashi, Y; Kamada, K; Nikl, M; Yoshikawa, A

    JOURNAL OF CRYSTAL GROWTH   Vol. 490   page: 71 - 76   2018.5

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    Eu-doped Li(Ca,Sr)AlF<inf>6</inf> [Eu:LiCSAF] single crystals with various Ca/Sr ratios were grown by the micro-pulling-down method, and their optical and scintillation properties were investigated to reveal the effects of Ca/Sr ratio on optical and scintillation properties of the Eu:LiCSAF single crystals. The Li(Ca<inf>1−</inf> <inf>x</inf> <inf>−</inf> <inf>y</inf>Sr<inf>x</inf>Eu<inf>y</inf>)AlF<inf>6</inf> single crystals could be grown in 0 ≤ x ≤ 0.1, 0.5 ≤ x ≤ 1.0 and y = 0.02 while the Eu:LiCSAF crystals with x = 0.2, 0.25 and 0.4 included two colquiriite-type phases with different lattice parameters. The Li(Ca<inf>1−</inf> <inf>x−y</inf>Sr<inf>x</inf>Eu<inf>y</inf>)AlF<inf>6</inf> single crystal with x = 0.25 and y = 0.02 showed the highest light yield under neutron irradiation.

    DOI: 10.1016/j.jcrysgro.2018.03.022

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  263. Crystal growth and scintillation properties of Pr-doped SrI<sub>2</sub> single crystals

    Yokota, Y; Ito, T; Yoshino, M; Yamaji, A; Ohashi, Y; Kurosawa, S; Kamada, K; Yoshikawa, A

    JOURNAL OF CRYSTAL GROWTH   Vol. 487   page: 126 - 130   2018.4

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    Pr-doped SrI<inf>2</inf> (Pr:SrI<inf>2</inf>) single crystals with various Pr concentrations were grown by the halide-micro-pulling-down (H-μ-PD) method, and the scintillation properties were investigated. Pr1%:SrI<inf>2</inf> single crystal with high transparency could be grown by the H-μ-PD method while Pr2, 3 and 5%:SrI<inf>2</inf> single crystals included some cracks and opaque parts. In the photoluminescence spectrum of the Pr1%:SrI<inf>2</inf> single crystal, an emission peak originated from the Pr<sup>3+</sup> ion was observed around 435 nm while the radioluminescence spectra showed an emission peak around 535 nm for the undoped SrI<inf>2</inf> and Pr:SrI<inf>2</inf> single crystals. Light yields of Pr1, 2, 3 and 5%:SrI<inf>2</inf> single crystals under γ-ray irradiation were 7700, 8700, 7200 and 6700 photons/MeV, respectively. Decay times of Pr1 and 2%:SrI<inf>2</inf> single crystals under γ-ray irradiation were 55.9 and 35.0 ns of the fast decay component, and 435 and 408 ns of the slow decay component, respectively.

    DOI: 10.1016/j.jcrysgro.2018.02.025

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  264. Fabrication of flexible Ir and Ir-Rh wires and application for thermocouple

    Murakami, R; Kamada, K; Shoji, Y; Yokota, Y; Yoshino, M; Kurosawa, S; Ohashi, Y; Yamaji, A; Yoshikawa, A

    JOURNAL OF CRYSTAL GROWTH   Vol. 487   page: 72 - 77   2018.4

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    The fabrication and thermal electromotive force characteristics of Ir/Ir-Rh thermocouples capable of repeated bending deformation are described. Ir and Ir-Rh wires with a diameter of 0.5 mm were fabricated using the alloy-micro-pulling-down method. Scanning electron microscopy and electron backscattering diffraction of the radial cross section of the grown wires were performed to investigate the microstructure and orientation of the crystal grains. At the start of growth, the microstructure was polycrystalline with diameters of several hundred micrometers, while at the 8-m growth point it was found to be monocrystalline. The observed single crystals of pure Ir and Ir-Rh alloy were oriented in the 〈1 1 3〉 and 〈1 1 2〉 directions, respectively, whereas the polycrystalline Ir-Rh samples showed preferential growth in the 〈1 0 0〉 direction. The thermal electromotive force of the fabricated Ir/Ir-Rh thermocouple was measured by the comparison technique and the fixed-point technique, and the thermoelectric power was estimated to be 5.9 μV/°C in the range from 600°C to 1100°C.

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  265. Mg, Ce co-doped Lu<sub>2</sub>Gd<sub>1</sub>(Ga,Al)<sub>5</sub>O<sub>12</sub> by micro-pulling down method and their luminescence properties

    Kamada, K; Yamaguchi, H; Yoshino, M; Kurosawa, S; Shoji, Y; Yokota, Y; Ohashi, Y; Pejchal, J; Nikl, M; Yoshikawa, A

    JAPANESE JOURNAL OF APPLIED PHYSICS   Vol. 57 ( 4 )   2018.4

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    Publisher:Japanese Journal of Applied Physics  

    The effects of Mg co-doping on the scintillation properties of Ce:Lu<inf>2</inf>Gd<inf>1</inf>(Ga,Al)<inf>5</inf>O<inf>12</inf> (LGGAG) single crystals with different Ga/Al ratios were investigated. Mg co-doped and non co-doped Ce:LGGAG single crystals were grown by the micro-pulling down (μ-PD) method and then cut, polished and annealed for each measurement. Absorption spectra, radioluminescence (RL) spectra, pulse height spectra, and scintillation decay were measured to reveal the effect of Mg co-doping. Ce<sup>4+</sup> charge transfer (CT) absorption band peaking at ∼260nm was observed in Mg co-doped samples, which is in good agreement with previous reports for the Ce<sup>4+</sup> CT absorption band in other garnet-based crystals. The scintillation decay time tended to be accelerated and the light yield tended to be decreased by Mg co-doping at higher Ga concentrations.

    DOI: 10.7567/JJAP.57.04FJ06

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  266. Crystal growth and temperature dependence of light output of Ce-doped (Gd, La, Y)<sub>2</sub>Si<sub>2</sub>O<sub>7</sub> single crystals

    Horiai, T; Kurosawa, S; Murakami, R; Shoji, Y; Pejchal, J; Yamaji, A; Ohashi, Y; Kamada, K; Yokota, Y; Ishizu, T; Ohishi, Y; Nakaya, T; Yoshikawa, A

    JOURNAL OF CRYSTAL GROWTH   Vol. 486   page: 173 - 177   2018.3

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    Ce-doped (Gd, La)<inf>2</inf>Si<inf>2</inf>O<inf>7</inf> scintillation crystals are expected to be used as gamma-ray detectors for high temperature measurement. To realize scintillators for high temperature environment, we investigated (Ce<inf>0.01</inf> Gd<inf>0.59−x</inf> La<inf>0.40</inf> Y<inf>x</inf>)<inf>2</inf>Si<inf>2</inf>O<inf>7</inf> (x = 0.00, 0.05, 0.10, 0.15) single crystals grown by the micro-pulling-down method. The results showed that a 5% Y-admixed Ce-doped (Gd, La)<inf>2</inf>Si<inf>2</inf>O<inf>7</inf> scintillator can yield higher light output when compared with Y-free Ce-doped (Gd, La)<inf>2</inf>Si<inf>2</inf>O<inf>7</inf> scintillator. The light outputs at 25°C and 175°C were determined to be ∼43,000 and ∼40,000 photons/MeV, respectively. Moreover, 1 inch size 5% Y-admixed Ce-doped (Gd, La)<inf>2</inf>Si<inf>2</inf>O<inf>7</inf> scintillator was grown by the Czochralski technique, and its light output at 175°C kept the value of around 95% of the value at 25°C.

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  267. Crystal growth and piezoelectric properties of Ca<sub>3</sub>Ta(Ga<sub>0.9</sub>Sc<sub>0.1</sub>)<sub>3</sub>Si<sub>2</sub>O<sub>14</sub> bulk single crystal

    Igarashi, Y; Yokota, Y; Ohashi, Y; Inoue, K; Yamaji, A; Shoji, Y; Kamada, K; Kurosawa, S; Yoshikawa, A

    JOURNAL OF CRYSTAL GROWTH   Vol. 485   page: 69 - 72   2018.3

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    Ca<inf>3</inf>Ta(Ga<inf>0.9</inf>Sc<inf>0.1</inf>)<inf>3</inf>Si<inf>2</inf>O<inf>14</inf> langasite-type single crystal with a diameter of 1 in. was grown by Czochralski (Cz) method. Obtained crystal had good crystallinity and its lattice constants exceeded those of Ca<inf>3</inf>TaGa<inf>3</inf>Si<inf>2</inf>O<inf>14</inf> (CTGS) according to the X-ray analysis. A crack-free specimen cut from the grown crystal was used for the measurements of dielectric constant ε<inf>11</inf><sup>T</sup>/ε<inf>0</inf>, electromechanical coupling factor k<inf>12</inf>, and piezoelectric constant d<inf>11</inf>. The accuracies of these measurements were better than those for the crystal grown by micro-pulling-down (μ-PD) method. Substitution of Ga with Sc resulted modification of these constants in the directions opposite to those observed after partial substitution of Ga (of CTGS) with Al. This suggests that increase of |d<inf>14</inf>| was most probably associated with enlargement of average size of the Ga sites. The crystal reported here had greater dimensions as compared to analogous crystals grown by the μ-PD method. As a result, accuracy of determination of acoustic constants of this material may be improved.

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  268. Fabrication of Metallic Fibers with High Melting Point and Poor Workability by Unidirectional Solidification

    Yokota, Y; Nihei, T; Tanaka, K; Sakairi, K; Chani, V; Ohashi, Y; Kurosawa, S; Kamada, K; Yoshikawa, A

    ADVANCED ENGINEERING MATERIALS   Vol. 20 ( 3 )   2018.3

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    Innovative method acceptable for production of Iridium (Ir) and Ruthenium (Ru) metal fibers with high melting point and poor workability is developed using an alloy-micro-pulling-down (A-μ-PD) method and ceramic crucibles with sufficient mechanical and thermal shock resistance. As-grown (as-solidified) Ir and Ru fibers are approximately 1 mm in diameter and their lengths exceed 15 and 0.3 m, respectively. Both Ir and Ru fibers are composed of number of elongated grains oriented along a growth direction, which is attributable to the unidirectional solidification. The flexibility and oxidation resistance of the Ir fiber grown by the A-μ-PD method is considerably improved as compared to a commercial Ir wire made by wire-drawing process.

    DOI: 10.1002/adem.201700506

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  269. Scintillating ceramics based on non-stoichiometric strontium hafnate

    Jary, V; Bohácek, P; Pejchal, J; Beitlerová, A; Trunda, B; Pánek, D; Bruza, P; Kurosawa, S; Yoshikawa, A; Nikl, M

    OPTICAL MATERIALS   Vol. 77   page: 246 - 252   2018.3

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    A set of non-stoichiometric strontium-hafnate ceramic samples was synthesized by the spark plasma sintering technique from powder precursors of optimized composition. The scintillation and optical properties of ceramic samples were investigated by means of time-resolved luminescence spectroscopy. We measured radioluminescence, photoluminescence excitation and emission spectra as well as luminescence decays excited by UV and soft X-rays, respectively. Multiple annealing was employed to optimize ceramic performance. Furthermore, optical properties of powder and ceramic sample of the same composition were compared. Application potential of studied ceramics in superfast imaging applications is discussed as well.

    DOI: 10.1016/j.optmat.2018.01.042

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  270. The impact of gender on medical visit communication and patient satisfaction within the Japanese primary care context

    Noro, I; Roter, DL; Kurosawa, S; Miura, Y; Ishizaki, M

    PATIENT EDUCATION AND COUNSELING   Vol. 101 ( 2 ) page: 227 - 232   2018.2

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    Objective: This study was designed to address significant gaps in the predominantly western-centric research literature by examining the influence of gender concordance in medical communication and patient satisfaction within the Japanese context. Methods: New primary care patients (54 male and 49 female) were randomly assigned to study internists (6 males and 5 females). Recorded visits were coded with the Roter Interaction Analysis System (RIAS). Post-visit, patients completed a Japanese version of the Medical Interview Satisfaction Scale (MISS). Results: Female concordant visits showed higher levels of patient-centeredness than all other gender combinations. Female physicians substantially modified their communication based on patient gender while male physicians did not. Gender concordance was associated with higher female, but lower male patient satisfaction relative to gender discordant visits. Conclusion: Contrary to normative experience of medicine as a male dominated profession in Japan, and gender-based power differentials, male-gendered clinical communication is less likely to satisfy male than female patients, while female-gendered communication is positively associated with female patient satisfaction. Practice implications: Patient satisfaction ratings reflect greater gender flexibility in terms of acceptable physician behavior than Japanese norms would suggest.

    DOI: 10.1016/j.pec.2017.08.001

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  271. Visualizing hidden electron trap levels in Gd<sub>3</sub>Al<sub>2</sub>Ga<sub>3</sub>O<sub>12</sub>:Ce crystals using a mid-infrared free-electron laser

    Kitaura, M; Zen, H; Kamada, K; Kurosawa, S; Watanabe, S; Ohnishi, A; Hara, K

    APPLIED PHYSICS LETTERS   Vol. 112 ( 3 )   2018.1

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    Publisher:Applied Physics Letters  

    The energy levels of electron traps (namely, defect complexes associated with oxygen vacancies) in Gd<inf>3</inf>Al<inf>2</inf>Ga<inf>3</inf>O<inf>12</inf>:Ce (GAGG:Ce) were studied at 12 K using mid-infrared (MIR) light pulses from a free-electron laser (FEL) as the probe light. Ce<sup>3+</sup> 5d-4f luminescence was stimulated by the MIR light pulse following an ultraviolet light pulse. Stimulation of Ce<sup>3+</sup> 5d-4f luminescence by MIR light pulses was pronounced above 0.31 eV. This result is consistent with that of previous work based on a trap-mediated luminescence model. It is concluded that the electron trap levels are located 0.31 eV below the bottom of the conduction band. This study demonstrates that MIR-FEL is applicable for the determination of hidden electron trap levels.

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  272. Application of Silicon Photomultipliers to Compton-scattering-type Polarimeters for Gamma Ray Bursts

    Saito, Y; Gunji, S; Nakamori, T; Mihara, T; Yonetoku, D; Sawano, T; Kurosawa, S; Kodaira, S; Gaskin, J

    2018 IEEE NUCLEAR SCIENCE SYMPOSIUM AND MEDICAL IMAGING CONFERENCE PROCEEDINGS (NSS/MIC)     2018

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  273. Crystal Growth and Optical Properties of Organic Crystals for Neutron Scintillators Open Access

    YAMAJI Akihiro, KUROSAWA Shunsuke, OHASHI Yuji, YOKOTA Yuui, KAMADA Kei, YOSHIKAWA Akira

    Plasma and Fusion Research   Vol. 13 ( 0 ) page: 2405011 - 2405011   2018

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    <p>This paper presents the study of prospective organic-based materials, trans-stilbene and p-terphenyl, as their potential application for new neutron scintillators. Growth of their single crystals by the self-seeding vertical Bridgman method is reported. And evaluation of grown crystals concerning the composition, optical and luminescence properties, and scintillation performance at room temperature is discussed. Their photo- and radio-luminesce spectra were peaking at 388 and 408 nm, their quantum yield was of 52.4% and 79.7%, and the light yield were of 0.89 and 1.80 times higher than that of GS-20 standard, respectively. The scintillation decay times of 8.2 ns (trans-stilbene) and 5.8 ns (p-terphenyl) were observed as well.</p>

    DOI: 10.1585/pfr.13.2405011

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  274. Effect of cytogenetic risk status on outcomes for patients with acute myeloid leukemia undergoing various types of allogeneic hematopoietic cell transplantation: an analysis of 7812 patients

    Yanada, M; Mori, J; Aoki, J; Harada, K; Mizuno, S; Uchida, N; Kurosawa, S; Toya, T; Kanamori, H; Ozawa, Y; Ogawa, H; Henzan, H; Iwato, K; Sakura, T; Ota, S; Fukuda, T; Ichinohe, T; Atsuta, Y; Yano, S

    LEUKEMIA & LYMPHOMA   Vol. 59 ( 3 ) page: 601 - 609   2018

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    This study aimed at determining how cytogenetic risk status affects outcomes for patients with acute myeloid leukemia (AML) after undergoing various types of allogeneic hematopoietic cell transplantation (HCT). Of 7812 patients eligible for analysis, cytogenetic risk was classified as favorable for 1088, intermediate for 5025, and poor for 1699. Overall, multivariate analysis showed significant intergroup differences in terms of relapse and survival, with the difference between poor- and intermediate-risk groups being greater than that between favorable- and intermediate-risk groups. Non-relapse mortality was identical for the three groups. Significant effects of cytogenetic risk status on survival were documented irrespective of donor type (related, unrelated, and umbilical cord blood), disease status at the time of transplantation (first or second complete remission, and more advanced disease status), and conditioning intensity (myeloablative and reduced-intensity). Our findings demonstrate robust and constant effects of cytogenetic risk status on survival after allogeneic HCT for patients with AML.

    DOI: 10.1080/10428194.2017.1357173

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  275. Fabrication and evaluation of Ce3+ ion doped CaF2 thin film phosphor

    Hishiki M., Inoue Y., Ono S., Kurosawa S., Yoshikawa A.

    Optics Infobase Conference Papers   Vol. Part F113-CLEOPR 2018   2018

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    We fabricated Ce<sup>3+</sup>:CaF2 thin films with different doping concentration in anticipation of use as a phosphor. We calculated practical doping concentration from lattice distortion and evaluated the optimized doping concentration for high efficiency light emission.

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  276. Feasibility Study on an Application of Scintillation Fiber Imager to Realtime Range Monitoring System for Carbon Ion Therapy Open Access

    Iwai T., Morimoto K., Kurosawa S., Tokanai F., Umebayashi T., Ohashi Y., Moriya T., Ishizawa S., Murata M.

    Proceedings of the 2nd International Symposium on Radiation Detectors and their Uses Isrd 2018     2018

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    A feasibility study of an application of scintillation fiber imager to realtime range monitoring system for particle therapy was carried out. Monte Carlo simulation using PHITS suggested that reconstructed vertex distribution shows good correlation with Bragg peak depth, which could allow us to perform realtime range monitoring. As a performance test, scintillation fiber imager successfully provided 2D image of proton beam.

    DOI: 10.7566/JPSCP.24.011030

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  277. SMILE-2+: The 2018 balloon flight and the instrument design of the electron-tracking Compton camera

    Nakamura, Y; Tanimori, T; Takada, A; Mizumura, Y; Komura, S; Kishimoto, T; Takemura, T; Yoshikawa, K; Taniguchi, T; Onozaka, K; Saito, K; Mizumoto, T; Sonoda, S; Kubo, H; Matsuoka, Y; Nakamasu, Y; Kurosawa, S; Miuchic, K; Sawano, T

    SPACE TELESCOPES AND INSTRUMENTATION 2018: ULTRAVIOLET TO GAMMA RAY   Vol. 10699   2018

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    Publisher:Proceedings of SPIE the International Society for Optical Engineering  

    To establish imaging spectroscopy of cosmic gamma-rays from a few hundreds of keV to a few tens MeV, we developed an electron-tracking Compton camera (ETCC). The ETCC consists of a time projection chamber (TPC) and pixelated scintillator arrays (PSAs). The ETCC is superior to conventional gamma-ray imaging detectors of this energy band in that the arrival direction of an incident gamma-ray is firmly determined at one point and realizes high noise rejection efficiency. We performed a campaign to demonstrate the gamma-ray imaging performance of the ETCC at balloon altitude via the sub-MeV gamma-ray imaging loaded-on-balloon experiment 2+ (SMILE-2+). The balloon was launched on April 7, 2018, at 6:26 ACST (UTC +9:30) from Alice Springs, Australia. We performed a level flight for 26 hours at an altitude of 39.6 km. The main observation targets were the Galactic Center region and the Crab Nebula and we succeeded in observing them without any critical problems. The configuration of the flight model ETCC and the housekeeping data are described in detail.

    DOI: 10.1117/12.2309920

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  278. Recent Development of Neutron Detectors for Pulsed Compact Neutron Sources Open Access

    M. SHIMIZU Hirohiko, ARIKAWA Yasunobu, IKEDA Yujiro, KUROSAWA Shunsuke, HANAYAMA Ryohei, KONDO Haruyasu

    The Review of Laser Engineering   Vol. 46 ( 11 ) page: 634   2018

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    Language:Japanese   Publisher:The Laser Society of Japan  

    Compact neutron sources have been used as a various diagnostics such as neutron diffraction, neutron
    resonant analysis, and neutron radiography. The developments of the neutron detectors are essential for
    all of these applications, while the techniques are strongly dependent on the neutron energy and the aim
    of the measurement. This paper reviews neutron detection techniques pertinent to promote compact
    neutron source uses. Along with general neutron detection systems with conventional counters for slow
    neutrons, we have highlighted detectors for high energy neutrons with high time resolution and high
    sensitivity which could be applied in a laser-driven compact neutron source.

    DOI: 10.2184/lsj.46.11_634

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  279. Development of Red Emitting Powder Ceramic Phosphors with Good Temperature Dependence

    HORIAI Takahiko, KUROSAWA Shunsuke

    Hosokawa Powder Technology Foundation ANNUAL REPORT   Vol. 26 ( 0 ) page: 187 - 190   2018

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    DOI: 10.14356/hptf.17511

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  280. Anisotropy Measurements of ZnWO<sub>4</sub> Crystals for Developing the Direction-Sensitive Dark Matter Detector Open Access

    Sekiya Hiroyuki, Kurosawa Shunsuke, Yoshikawa Akira, Kodama Shohei, Yamato Shinnosuke, Shoji Ikuhiro, Ohashi Yuji, Tsukahara Misa, Yamaji Akihiro, Yokota Yui, Horiai Takehiko, Pedersen Juan, Onishi Akimasa, Kamata Kei, Kitaura Mamoru

    Meeting Abstracts of the Physical Society of Japan   Vol. 73.1 ( 0 ) page: 364 - 364   2018

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    DOI: 10.11316/jpsgaiyo.73.1.0_364

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  281. Development and melt growth of novel scintillating halide crystals Open Access

    Yoshikawa, A; Yokota, Y; Shoji, Y; Kral, R; Kamada, K; Kurosawa, S; Ohashi, Y; Arakawa, M; Chani, VI; Kochurikhin, VV; Yamaji, A; Andrey, M; Nikl, M

    OPTICAL MATERIALS   Vol. 74   page: 109 - 119   2017.12

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    Melt growth of scintillating halide crystals is reviewed. The vertical Bridgman growth technique is still considered as very popular method that enables production of relatively large and commercially attractive crystals. On the other hand, the micro-pulling-down method is preferable when fabrication of small samples, sufficient for preliminary characterization of their optical and/or scintillation performance, is required. Moreover, bulk crystal growth is also available using the micro-pulling-down furnace. The examples of growths of various halide crystals by industrially friendly melt growth techniques including Czochralski and edge-defined film-fed growth methods are also discussed. Finally, traveling molten zone growth that in some degree corresponds to horizontal zone melting is briefly overviewed.

    DOI: 10.1016/j.optmat.2017.03.043

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  282. Engineering of Eu dopant segregation in colquiriite-type fluoride single crystal scintillators Open Access

    Yokota, Y; Yamaji, A; Kurosawa, S; Ohashi, Y; Kamada, K; Yoshikawa, A

    AIP ADVANCES   Vol. 7 ( 12 )   2017.12

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    Colquiriite-type Eu-doped LiCaAlF<inf>6</inf> and LiSrAlF<inf>6</inf> (Eu:LiCAF and Eu:LiSAF) scintillator single crystals were grown using Al metal as a starting material to improve the Eu dopant segregation. All Eu:LiCAF and Eu:LiSAF single crystals using Al metal (Eu,Al<sup>M</sup>:LiCAF and Eu,Al<sup>M</sup>:LiSAF) indicated high transparency and effective segregation coefficients (k<inf>eff</inf>) of Eu2%,Al<sup>M</sup>1%:LiCAF and Eu2%,Al<sup>M</sup>1%:LiSAF single crystals were significantly improved to the value of 0.40 and 0.99, respectively. EuF<inf>3</inf> starting material reacted with Al metal before colquiriite-type phase was generated. As a result, Eu<sup>3+</sup> ion in EuF<inf>3</inf> was changed to Eu<sup>2+</sup> ion which could be incorporated into Ca<sup>2+</sup> and Sr<sup>2+</sup> sites easily.

    DOI: 10.1063/1.5006996

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  283. Difference in distribution of eu ions doped CaF2 single crystal caused by two types of grown method by measurement of multi-photon luminescence

    Tanaka M., Ono S., Yamaji A., Kurosawa S., Yoshikawa A.

    2017 Conference on Lasers and Electro Optics Pacific Rim CLEO PR 2017   Vol. 2017-January   page: 1 - 2   2017.11

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    We report on distribution of Eu ions doped CaF<inf>2</inf> single crystal by measurement of multi-photon luminescence. Distribution of Eu<sup>2+</sup> and Eu<sup>3+</sup> ions is measured respectively because the luminescence peak due to Eu<sup>2+</sup> and Eu<sup>3+</sup> ions is different. We observed the difference in distribution of Eu<sup>2+</sup> and Eu<sup>3+</sup> ions doped CaF<inf>2</inf> which is grown by Annealing method and micro pulling-down method.

    DOI: 10.1109/CLEOPR.2017.8119055

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  284. Development of a real-time dose monitor with Cr-doped Gd<sub>3</sub>Ga<sub>5</sub>O<sub>12</sub> infrared scintillator

    Kurosawa, S; Yamaji, A; Kochurikhin, VV; Ivanov, M; Pejchal, J; Murakami, R; Shoji, Y; Ohashi, Y; Yokota, Y; Kamada, K; Yoshikawa, A

    RADIATION MEASUREMENTS   Vol. 106   page: 187 - 191   2017.11

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    The development of a real-time dose monitor system is one of the important issues in medical engineering to reduce medical accidents such as overdose or incorrect positioning of the treated human tissue during radiation therapy. One of the challenging solutions is to use an infrared scintillator, which is sufficiently bright so that the light can be detected outside the human tissue. In this study, a novel infrared scintillator, Cr-doped Gd<inf>3</inf>Ga<inf>5</inf>O<inf>12</inf>, was tested with pork meat as a phantom of human tissue to prove its feasibility for the dose monitor. The scintillation photons of Cr:Gd<inf>3</inf>Ga<inf>5</inf>O<inf>12</inf> were observed through even 50-mm thick pork meat. The emission peak originated from d-d emission of Cr<sup>3+</sup>. The emission intensity of Cr:Gd<inf>3</inf>Ga<inf>5</inf>O<inf>12</inf> was approximately 3.5 times larger than that of the conventional infrared scintillator Cr:α-Al<inf>2</inf>O<inf>3</inf>. Moreover, we succeeded in performing the infrared imaging for Cr:Gd<inf>3</inf>Ga<inf>5</inf>O<inf>12</inf> irradiated with alpha-rays using a complementary metal oxide semiconductor camera.

    DOI: 10.1016/j.radmeas.2017.03.028

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  285. D816 mutation of the KIT gene in core binding factor acute myeloid leukemia is associated with poorer prognosis than other KIT gene mutations

    Yui S., Kurosawa S., Yamaguchi H., Kanamori H., Ueki T., Uoshima N., Mizuno I., Shono K., Usuki K., Chiba S., Nakamura Y., Yanada M., Kanda J., Tajika K., Gomi S., Fukunaga K., Wakita S., Ryotokuji T., Fukuda T., Inokuchi K.

    Annals of Hematology   Vol. 96 ( 10 ) page: 1641 - 1652   2017.10

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    The clinical impact of KIT mutations in core binding factor acute myeloid leukemia (CBF-AML) is still unclear. In the present study, we analyzed the prognostic significance of each KIT mutation (D816, N822K, and other mutations) in Japanese patients with CBF-AML. We retrospectively analyzed 136 cases of CBF-AML that had gone into complete remission (CR). KIT mutations were found in 61 (45%) of the patients with CBF-AML. D816, N822K, D816 and N822K, and other mutations of the KIT gene were detected in 29 cases (21%), 20 cases (15%), 7 cases (5%), and 5 cases (4%), respectively. The rate of relapse-free survival (RFS) and overall survival (OS) in patients with D816 and with both D816 and N822K mutations was significantly lower than in patients with other or with no KIT mutations (RFS: p < 0.001, OS: p < 0.001). Moreover, stratified analysis of the chromosomal abnormalities t(8;21)(q22;q22) and inv(16)(p13.1q22), t(16;16)(p13.1;q22) showed that D816 mutation was associated with a significantly worse prognosis. In a further multivariate analysis of RFS and OS, D816 mutation was found to be an independent risk factor for significantly poorer prognosis. In the present study, we were able to establish that, of all KIT mutations, D816 mutation alone is an unfavorable prognostic factor.

    DOI: 10.1007/s00277-017-3074-y

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  286. Quality of Life after Allogeneic Hematopoietic Cell Transplantation According to Affected Organ and Severity of Chronic Graft-versus-Host Disease

    Kurosawa, S; Oshima, K; Yamaguchi, T; Yanagisawa, A; Fukuda, T; Kanamori, H; Mori, T; Takahashi, S; Kondo, T; Kohno, A; Miyamura, K; Umemoto, Y; Teshima, T; Taniguchi, S; Yamashita, T; Inamoto, Y; Kanda, Y; Okamoto, S; Atsuta, Y

    BIOLOGY OF BLOOD AND MARROW TRANSPLANTATION   Vol. 23 ( 10 ) page: 1749 - 1758   2017.10

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    Knowing the impact of chronic graft-versus-host disease (GVHD) on quality of life (QoL) after allogeneic hematopoietic stem cell transplantation (allo-HCT) by GVHD type and severity is critical for providing care to transplant survivors. We conducted a cross-sectional questionnaire study to examine the relationship between patient-reported QoL as measured by the Medical Outcomes Study 36-Item Short-Form Health Survey, Functional Assessment of Cancer Therapy-Bone Marrow Transplant, and visual analogue scale (VAS) and chronic GVHD defined by the National Institutes of Health (NIH) criteria. Recipients of allo-HCT for hematologic disease between 1995 and 2009 aged ≥ 16 years at transplant and ≥20 years at the time of the survey who were relapse-free were eligible. A total of 1140 pairs of patient and physician questionnaires were included in the analysis. By NIH global severity score, QoL scores in all aspects were significantly lower in patients with higher global and organ-specific severity grades, independent of background variables. Compared with patients without GVHD symptoms, those with mild symptoms had impaired physical and general QoL according to global severity score and organ-specific scores except for the genital tract. Mild symptoms in the lungs, gastrointestinal tract, and joints and fascia were associated with clinically meaningful deterioration of physical QoL. VAS scores provided by physicians were generally higher than those provided by patients. Differences between scores reported by patients and physicians were larger for patients with no or mild GVHD symptoms. Our findings based on more than 1000 long-term survivors after HCT enabled us to identify a target of care, informing survivorship care protocols to improve post-transplantation QoL.

    DOI: 10.1016/j.bbmt.2017.06.011

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  287. Improvement of dopant distribution in radial direction of single crystals grown by micro-pulling-down method

    Yokota, Y; Kudo, T; Chani, V; Ohashi, Y; Kurosawa, S; Kamada, K; Zeng, Z; Kawazoe, Y; Yoshikawa, A

    JOURNAL OF CRYSTAL GROWTH   Vol. 474   page: 178 - 182   2017.9

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    Two iridium crucibles with one and five capillaries at a nozzle were developed for the growth of Ce-doped Y<inf>3</inf>Al<inf>5</inf>O<inf>12</inf> [Ce:YAG] single crystals by the micro-pulling-down [μ-PD] method. The purpose of the study was to examine the effect of the capillary number on the Ce distribution in the radial direction of the crystals. The crystals grown from 2 mol% and 5 mol% Ce-doped YAG melts were then cut perpendicular to the growth direction and polished to produce specimens suitable for the measurement of Ce distribution. The Ce:YAG crystals grown using the crucible with one capillary [Ce:YAG(1 C)] had greater Ce content in the central portion of the crystal when compared to its peripheral parts. On the other hand, in the case of the Ce:YAG crystal grown using the crucible with five capillaries [Ce:YAG(5 C)], the increased Ce concentration was detected in five specimen sections positioned just below the capillaries. The results indicated that increase of the number of capillaries is effective practice that results in an improvement of the radial homogeneity of the single crystals grown by the μ-PD method.

    DOI: 10.1016/j.jcrysgro.2016.11.119

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  288. Growth and scintillation properties of Eu and Ce doped LiSrI<sub>3</sub> single crystals

    Kamada, K; Yoshino, M; Murakami, R; Chiba, H; Yamaji, A; Shoji, Y; Kurosawa, S; Yokota, Y; Ohashi, Y; Kochurikhin, VV; Yoshikawa, A

    JOURNAL OF MATERIALS SCIENCE-MATERIALS IN ELECTRONICS   Vol. 28 ( 17 ) page: 13157 - 13160   2017.9

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    Publisher:Journal of Materials Science Materials in Electronics  

    In this study, Eu and Ce doped LiSrI<inf>3</inf> single crystals were explored and the scintillation performance was reported at the first time. Eu and Ce doped LiSrI<inf>3</inf> single crystals were grown by the Bridgman–Stockbarger method in a quartz ampoule with 3 mm inner diameter. Growth rate was 0.06 mm/min. Circular samples with 1 mm thickness were obtained from the grown crystal. The grown Eu doped LiSrI<inf>3</inf> crystal demonstrated Eu<sup>2+</sup> 4f–5d emission peak at 420 nm under alpha-ray excitation. In the case of Ce doped one, double emission peaks at 360 and 400 nm were observed. The light yield of the Eu doped LiSrI<inf>3</inf> was around 35,000 photon/MeV for 662 keV gamma-ray and 24,000 photon/5.5 MeV for alpha-ray. Energy resolution of the Eu doped LiSrI<inf>3</inf> was 5.2%@662 keV. Scintillation decay time of the grown Ce and Eu doped LiSrI<inf>3</inf> under 662 keV gamma-ray was 23.8 ns (50%) 212 ns (50%) and 545 ns 100%, respectively.

    DOI: 10.1007/s10854-017-7150-9

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  289. Development of a modified prognostic index for patients with aggressive adult T-cell leukemia-lymphoma aged 70 years or younger: possible risk-adapted management strategies including allogeneic transplantation Open Access

    Fuji, S; Yamaguchi, T; Inoue, Y; Utsunomiya, A; Moriuchi, Y; Uchimaru, K; Owatari, S; Miyagi, T; Taguchi, J; Choi, I; Otsuka, E; Nakachi, S; Yamamoto, H; Kurosawa, S; Tobinai, K; Fukuda, T

    HAEMATOLOGICA   Vol. 102 ( 7 ) page: 1258 - 1265   2017.7

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    Adult T-cell leukemia-lymphoma is a distinct type of peripheral Tcell lymphoma caused by human T-cell lymphotropic virus type I. Although allogeneic stem cell transplantation after chemotherapy is a recommended treatment option for patients with aggressive adult T-cell leukemia-lymphoma, there is no consensus about indications for allogeneic stem cell transplantation because there is no established risk stratification system for transplant eligible patients. We conducted a nationwide survey of patients with aggressive adult T-cell leukemia-lymphoma in order to construct a new, large database that includes 1,792 patients aged 70 years or younger with aggressive adult T-cell leukemialymphoma who were diagnosed between 2000 and 2013 and received intensive first-line chemotherapy. We randomly divided patients into two groups (training and validation sets). Acute type, poor performance status, high soluble interleukin-2 receptor levels (> 5,000 U/mL), high adjusted calcium levels (≥ 12 mg/dL), and high C-reactive protein levels (≥ 2.5 mg/dL) were independent adverse prognostic factors used in the training set. We used these five variables to divide patients into three risk groups. In the validation set, median overall survival for the low-, intermediate-, and high-risk groups was 626 days, 322 days, and 197 days, respectively. In the intermediate- and high-risk groups, transplanted recipients had significantly better overall survival than non-transplanted patients. We developed a promising new risk stratification system to identify patients aged 70 years or younger with aggressive adult T-cell leukemia-lymphoma who may benefit from upfront allogeneic stem cell transplantation. Prospective studies are warranted to confirm the benefit of this treatment strategy.

    DOI: 10.3324/haematol.2017.164996

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  290. Development of Eu:SrI<sub>2</sub> Scintillator Array for Gamma-Ray Imaging Applications

    Yoshino, M; Kamada, K; Shoji, Y; Kurosawa, S; Yokota, Y; Ohashi, Y; Yoshikawa, A; Yamamoto, S

    IEEE TRANSACTIONS ON NUCLEAR SCIENCE   Vol. 64 ( 7 ) page: 1647 - 1651   2017.7

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    Eu:SrI<inf>2</inf> bulk single crystals with 1.5-in diameter were grown using the Bridgman-Stockbarger technique and special-shaped crucibles. We will report on the growth of the 1.5-in size Eu:SrI<inf>2</inf> single crystal and the preliminary test of the same sample cut in size of 10 × 10 × 10 mm<sup>3</sup> with polishing. An energy resolution of 3.2% full width at half maximum (FWHM) was obtained for <sup>137</sup>Cs. After cutting and polishing the grown crystal to the size of 3 × 3 × 3 mm<sup>3</sup>, 8 × 8 matrix Eu:SrI<inf>2</inf> arrays were fabricated. We made a test module consisting of Eu:SrI<inf>2</inf> arrays, which was optically coupled with position sensitive photomultiplier tube (PSPMT) and multi-pixel photon counter (MPPC) array. The position and energy performance of the test module were evaluated using <sup>137</sup>Cs and <sup>57</sup>Co radioactive sources. As a result, we were able to resolve all pixels clearly. A good energy resolution of 6.7% ± 0.7% (FWHM) and 8.2% ± 2.5% (FWHM) for 662 keV was obtained using PSPMT and MPPC arrays, respectively. In the same way, energy resolution of 12.7% ± 1.3% and 14.7% ± 3.4% (FWHM) for 122 keV was obtained using PSPMT and MPPC-array, respectively. These energy resolutions considerably degraded compared with an energy resolution of the single piece of Eu:SrI<inf>2</inf> sample owing to the thinness of the Teflon reflector. This conclusion can be considered as a strong motivation for future research on the choice of reflector materials and structure of the Eu:SrI<inf>2</inf> array.

    DOI: 10.1109/TNS.2017.2676769

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  291. Temperature dependence of acoustic property of Ca<sub>3</sub>Ta( Ga, Al)<sub>3</sub>Si<sub>2</sub>O<sub>14</sub> single crystals

    Ohashi, Y; Arakawa, M; Yokota, Y; Shoji, Y; Yamaji, A; Kurosawa, S; Kamada, K; Yoshikawa, A

    JAPANESE JOURNAL OF APPLIED PHYSICS   Vol. 56 ( 7 )   2017.7

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    The temperature dependences of the acoustic properties of Ca<inf>3</inf>Ta(Ga<inf>1-x</inf>Al<inf>x</inf>)<inf>3</inf>Si<inf>2</inf>O<inf>14</inf> [CTGAS(x)] were experimentally studied as a function of the Al substitution content x. Five specimens, i.e., one each of X-, Y-, and Z-, and two rotated Y-cut specimens, were prepared from each crystal ingot of CTGAS(x) (x = 0, 0.25, 0.50, and 0.75) grown by the Czochralski technique. The longitudinal wave and shear wave velocities of CTGAS (x) were measured at three temperatures ranging from 291 to 300 K, then acoustically related physical constants (elastic, piezoelectric, and dielectric constants and coefficient of thermal expansion) were determined at approximately room temperature. The results revealed that the temperature coefficients of all the constants linearly changed with Al content. By one of the calculations using the constants and their temperature coefficients determined in this study, we demonstrated their capability to predict suitable conditions (i.e., cut angle, propagation direction, and chemical composition) for acoustic wave devices although they were determined in a narrow temperature range.

    DOI: 10.7567/JJAP.56.07JB03

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  292. ROLE OF UPFRONT ALLOGENEIC HEMATOPOIETIC STEM CELL TRANSPLANTATION IN PATIENTS WITH AGGRESSIVE ADULT T-CELL LEUKEMIA-LYMPHOMA: A DECISION ANALYSIS

    Fuji, S; Kurosawa, S; Inamoto, Y; Murata, T; Utsunomiya, A; Uchimaru, K; Yamasaki, S; Inoue, Y; Moriuchi, Y; Choi, I; Ogata, M; Hidaka, M; Yamaguchi, T; Fukuda, T

    HAEMATOLOGICA   Vol. 102   page: 132 - 133   2017.6

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  293. Energy location of Ce<SUP>3+</SUP> 4f level and majority carrier type in Gd<sub>3</sub>Al<sub>2</sub>Ga<sub>3</sub>O<sub>12</sub>:Ce crystals studied by surface photovoltage spectroscopy

    Kitaura, M; Azuma, J; Ishizaki, M; Kamada, K; Kurosawa, S; Watanabe, S; Ohnishi, A; Hara, K

    APPLIED PHYSICS LETTERS   Vol. 110 ( 25 )   2017.6

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    Publisher:Applied Physics Letters  

    Gd<inf>3</inf>Al<inf>2</inf>Ga<inf>3</inf>O<inf>12</inf>:Ce (GAGG:Ce) was studied by surface photovoltage spectroscopy using the ultraviolet photoelectron spectroscopy technique with synchrotron radiation and a laser source. The lowest Ce<sup>3+</sup> 4f level is located below the conduction band minimum by 3.02 eV. This result is supported by the excitation spectrum for photo-stimulated luminescence and is compatible with the value predicted by the vacuum-referred binding energy scheme for GAGG:Ce. It is also found that GAGG:Ce is of the p-type. The information on the energy location of the Ce<sup>3+</sup> 4f level and majority carrier type provides us with hints on how to improve the optical properties of GAGG:Ce for photonic device applications.

    DOI: 10.1063/1.4987141

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  294. Control of the solid-liquid interface during growth of a Ce-doped Gd<sub>2</sub>Si<sub>2</sub>O<sub>7</sub> crystal by the traveling solvent floating zone method

    Watauchi, S; Matsuya, K; Nagao, M; Tanaka, I; Kurosawa, S; Yokota, Y; Yoshikawa, A

    JOURNAL OF CRYSTAL GROWTH   Vol. 468   page: 465 - 468   2017.6

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    Publisher:Journal of Crystal Growth  

    The growth conditions of Ce-doped Gd<inf>2</inf>Si<inf>2</inf>O<inf>7</inf> crystals, using the infrared convergent heating floating zone method, were optimized to make the shape of the crystal-melt interface flat or convex. The shape of the crystal-melt interface, meaning the interface between the molten zone and the grown crystal, was evaluated quantitatively using the convexity (h/r) as a parameter. The h/r value was found to be systematically dependent on the crystal diameter, the focus position of the ellipsoidal mirror for infrared convergent heating, and the lamp power used during crystal growth. For an 8.2-mm-diameter crystal grown using conventional conditions, the h/r value was −0.8, which indicates that the crystal-melt interface had a concave shape. The h/r value increased with the position of the ellipsoidal mirror, going from −0.8 for the −8 mm mirror position, to −0.5 for the +6 mm mirror position. Lastly, when the lamp power increased from 5.8 to 7.0 kW, the h/r value increased from −0.6 to −0.3, which was the maximum value observed, indicating that a flat or convex crystal-melt interface was not obtained.

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  295. Crystal growth and optical properties of Gd admixed Ce-doepd Lu<sub>2</sub>Si<sub>2</sub>O<sub>7</sub> single crystals

    Horiai, T; Kurosawa, S; Murakami, R; Yamaji, A; Shoji, Y; Ohashi, Y; Pejchal, J; Kamada, K; Yokota, Y; Yoshikawa, A

    JOURNAL OF CRYSTAL GROWTH   Vol. 468   page: 391 - 394   2017.6

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    Ce-doped Lu<inf>2</inf>Si<inf>2</inf>O<inf>7</inf> scintillator contains radioactive isotope <sup>176</sup>Lu which causes an unwanted intrinsic background signal. The development of scintillators with reduced Lu concentration were required in some applications. In this study, we developed the Gd admixed lutetium pyrosilicate, where the average ion radius at the rare earth site was similar to the Tm<sup>3+</sup> ion radius, for which the RE<inf>2</inf>Si<inf>2</inf>O<inf>7</inf> (RE=Tm, Yb, Lu) crystal structure is stable from room temperature to melting point. We have grown (Ce<inf>x</inf> Lu<inf>1−x−y</inf> Gd<inf>y</inf>)<inf>2</inf>Si<inf>2</inf>O<inf>7</inf> (x=0.01, y=0.00, 0.05, 0.10) single crystals. Their crystal systems were monoclinic with a space group C2/m. The absorption spectra revealed the energy transitions in Ce and Gd ions might be occurred. The light output was degraded and decay time was accelerated comparing the Gd 5% admixed sample with the Gd 10% one.

    DOI: 10.1016/j.jcrysgro.2016.10.074

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  296. Effect of Mg co-doping on scintillation properties of Ce:Gd<sub>3</sub>(Ga, Al)<sub>5</sub>O<sub>12</sub> single crystals with various Ga/Al ratios

    Yoshino, M; Kamada, K; Shoji, Y; Yamaji, A; Kurosawa, S; Yokota, Y; Ohashi, Y; Yoshikawa, A; Chani, VI

    JOURNAL OF CRYSTAL GROWTH   Vol. 468   page: 420 - 423   2017.6

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    Mg co-doped Ce1%:Gd<inf>3</inf>Ga<inf>x</inf>Al<inf>5−x</inf>O<inf>12</inf> (Ce:GAGG) crystals (x=2.4, 2.7, 3.0) were successfully grown by the Czochralski (Cz) method. Effect of Mg co-doping on the scintillation properties of Ce:GAGG was examined. This study covers measurements of solidification fraction and scintillation properties such as light yield, energy resolution and non-proportionality for each crystal. Pulse-height spectra of various gamma and X-ray sources with energies ranged from 30 keV to 662 keV were measured. Regardless of the presence/absence of Mg dopant, the non-proportionality curves with lower content of gallium in the crystal structure tend to improve. Mg co-doped Ce:GAGG samples did not show a significant difference as compared with non co-doped Ce:GAGG. Mg co-doped crystals with x=2.4 and 2.7 showed the promising scintillation properties of faster decay time and higher energy resolution than those with x=3.0.

    DOI: 10.1016/j.jcrysgro.2016.12.054

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  297. Effects of Na co-doping on optical and scintillation properties of Eu: LiCaAlF<sub>6</sub> scintillator single crystals Open Access

    Tanaka, C; Yokota, Y; Kurosawa, S; Yamaji, A; Ohashi, Y; Kamada, K; Nikl, M; Yoshikawa, A

    JOURNAL OF CRYSTAL GROWTH   Vol. 468   page: 399 - 402   2017.6

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    Na co-doped Eu: LiCaAlF<inf>6</inf> (Eu, Na: LiCAF) single crystals were grown by the micro-pulling-down (μ-PD) method, and their optical and scintillation properties were examined to reveal the effects of the Na co-doping. The crystals were single-phase materials demonstrating structure isomorphic with that of undoped LiCAF. To perform the crystals characterization, the specimens with dimensions of several millimeters were cut from highly transparent and crack free fragments of the crystals and polished. It was observed that Na co-doping resulted modification of the transmittance and the excitation spectra, and increased the light yield detected under neutron irradiation.

    DOI: 10.1016/j.jcrysgro.2016.11.012

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  298. Effects of Al substitution for Ca<sub>3</sub>Ta(Ga<sub>1-<i>x</i></sub>Al<i><sub>x</sub></i>)<sub>3</sub>Si<sub>2</sub>O<sub>14</sub> piezoelectric single crystals

    Yokota, Y; Ohashi, Y; Kudo, T; Kochurikhin, VV; Medvedev, A; Kurosawa, S; Kamada, K; Yoshikawa, A

    JOURNAL OF CRYSTAL GROWTH   Vol. 468   page: 321 - 325   2017.6

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    Ca<inf>3</inf>Ta(Ga<inf>1-x</inf>Al<inf>x</inf>)<inf>3</inf>Si<inf>2</inf>O<inf>14</inf> [CTGAS] material is a piezoelectric material belonging to the Langasite-type group (space group: P321).and the CTGAS single crystals (x=0, 0.25, 0.50, 0.75) with a diameter of 1 in. were grown by a Czochralski [Cz] method using an Ir crucible under Ar+2%O<inf>2</inf>. The CTGAS single crystals without any cracks could be grown using a CTGAS seed crystal in the x range of 0≤x≤0.75. Cell parameters, a and c, decrease while the a/c ratio increased with the Al concentration. Piezoelectric constant d<inf>11</inf> and electromechanical coupling factor k<inf>12</inf> for the X-cut specimens of the CTGAS single crystals were increased by the Al substitution.

    DOI: 10.1016/j.jcrysgro.2016.10.044

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  299. Growth of platinum fibers using the micro-pulling-down method

    Nihei, T; Yokota, Y; Arakawa, M; Ohashi, Y; Kurosawa, S; Kamada, K; Chani, V; Yoshikawa, A

    JOURNAL OF CRYSTAL GROWTH   Vol. 468   page: 403 - 406   2017.6

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    Platinum (Pt) crystalline fibers were grown from the melt by the micro-pulling-down (μ-PD) method using the ZrO<inf>2</inf> ceramics crucible. The diameter of the grown Pt fiber was controlled by the ϕ1 mm outlet made at the bottom of the crucible and the Pt fiber of 0.95±0.03 mm in diameter and over 5 m in length was obtained at 10 mm/min pulling-down rate. In addition, the Pt fiber was grown at 1–110 mm/min pulling rates while the liquid-solid interface reached the bottom of the crucible and the crystal growth became unstable at 120 mm/min pulling rate. Few grain boundaries were observed in the scanning electron microscopy image of the Pt fibers and there were some spots with high intensity in the pole figures.

    DOI: 10.1016/j.jcrysgro.2016.10.088

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  300. Q Relationships among chemical composition, lattice constants, and acoustic properties for Ca<sub>3</sub>Ta(Ga<sub>1-</sub> <sub>x</sub>Al<sub>x</sub>)<sub>3</sub>Si<sub>2</sub>O<sub>14</sub> single crystals

    Ohashi, Y; Kitahara, M; Kudo, T; Arakawa, M; Yokota, Y; Shoji, Y; Yamaji, A; Kurosawa, S; Kamada, K; Yoshikawa, A

    JOURNAL OF CRYSTAL GROWTH   Vol. 468   page: 376 - 381   2017.6

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    The relationship among lattice constant a, Al content, and acoustic properties were experimentally examined using a plate specimen perpendicular to Y-axis prepared from Ca<inf>3</inf>Ta(Ga<inf>0.75</inf>Al<inf>0.25</inf>)<inf>3</inf>Si<inf>2</inf>O<inf>14</inf> [CTGAS(0.25)] single crystal grown by Czochralski method. As the acoustic properties, leaky surface acoustic wave (LSAW) velocities with different propagation directions, X- and Z-propagations, and longitudinal wave velocity propagating along Y-axis direction were measured by the line-focus-beam/plane-wave ultrasonic-material-characterization (LFB/PW-UMC) system. The measured results of LSAW velocity distributions revealed inhomogeneity in radial direction of the crystal ingot exhibiting lower velocity area at the center of the ingot. In addition, the distributions of lattice constant a and chemical composition (especially Al content) were measured along the radial direction. Abnormal changes suggesting existence of residual stresses concentrated on the central part of the crystal ingot other than the effect of chemical composition change were detected from the relationships among the measured parameters.

    DOI: 10.1016/j.jcrysgro.2016.10.040

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  301. Single crystal growth of Ce:Gd<sub>3</sub>(Ga,Al)<sub>5</sub>O<sub>12</sub> with various Mg concentration and their scintillation properties Open Access

    Kamada, K; Shoji, Y; Kochurikhin, VV; Nagura, A; Okumura, S; Yamamoto, S; Yeom, JY; Kurosawa, S; Pejchal, J; Yokota, Y; Ohashi, Y; Nikl, M; Yoshino, M; Yoshikawa, A

    JOURNAL OF CRYSTAL GROWTH   Vol. 468   page: 407 - 410   2017.6

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    1 in. diameter Mg 0.05, 0.1, 0.2, 0.5 mol% and Zr 0.015% co-doped Ce1%:GGAG crystals were grown by Cz method. Relationship between Mg concentration and absorption, luminescence, light output, decay time, timing resolution was investigated. Mg 0.2 mol% co-doped sample showed the fastest timing resolution of 165 ps among the Mg-co-doped samples.

    DOI: 10.1016/j.jcrysgro.2016.11.026

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  302. Development of the growth technique on cerium bromide single crystal by Halide-micro-pulling-down method

    Ito, T; Yokota, Y; Kurosawa, S; Kamada, K; Ohashi, Y; Yoshikawa, A

    CRYSTAL RESEARCH AND TECHNOLOGY   Vol. 52 ( 6 )   2017.6

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    We developed the growth technique of the CeBr<inf>3</inf> scintillator single crystal by a Halide-micro-pulling-down (H-μ-PD) method using a carbon crucible with a die under suitable temperature gradient. Four-types after-heaters with different configurations were prepared to control the temperature gradient around the liquid-solid interface during crystal growth. The high temperature gradient resulted in the stable meniscus during the crystal growth and the CeBr<inf>3</inf> single crystal with high transparency could be obtained. The light yield and the decay time under γ-ray irradiation were ∼68,000 ph/MeV and 19 ns, respectively.

    DOI: 10.1002/crat.201600401

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  303. Growth and scintillation properties of Eu doped LiSrI<sub>3</sub>/LiI eutectics

    Kamada, K; Chiba, H; Yoshino, M; Yamaji, A; Shoji, Y; Kurosawa, S; Yokota, Y; Ohashi, Y; Yoshikawa, A

    OPTICAL MATERIALS   Vol. 68   page: 70 - 74   2017.6

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    Eu doped LiSrI<inf>3</inf>/LiI eutectics were grown by the Bridgman method in a quartz ample with 4 mm inner diameter. and their directionally solidified eutectic system has been investigated. Growth rate was 0.3 mm/min. The eutectic showed well aligned eutectic structure and optically transparent. Grown Eu doped LiSrI3/LiI eutectic shows 400 nm emission ascribed to Eu<sup>2+</sup> 4f-5d transition under X-ray excitation. The light yield was around 26,000 photon/MeV for 662 keV gamma-ray and 35,000 photons for 5.5 MeV alpha-ray.

    DOI: 10.1016/j.optmat.2017.05.010

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  304. mFOLFOX6 Plus Panitumumab Versus 5-FU/LV Plus Panitumumab After Six Cycles of Frontline mFOLFOX6 Plus Panitumumab: A Randomized Phase II Study of Patients With Unresectable or Advanced/Recurrent, RAS Wild-type Colorectal Carcinoma (SAPPHIRE)—Study Design and Rationale Open Access

    Nagata N., Mishima H., Kurosawa S., Oba K., Sakamoto J.

    Clinical Colorectal Cancer   Vol. 16 ( 2 ) page: 154 - 157.e1   2017.6

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    Background In Japan, oxaliplatin (OXA)/5-fluorouracil (5-FU)/leucovorin (LV)—the mFOLFOX6 regimen—is the most frequently used first-line chemotherapy backbone for metastatic colorectal cancer. However, peripheral nerve disorders caused by OXA during mFOLFOX6 therapy can decrease patients’ quality of life. OXA can be safely discontinued from a FOLFOX regimen after 6 cycles during first-line therapy. Also, for patients who discontinue OXA without having experienced peripheral nerve disorders, reintroducing OXA in the later stages of treatment could remain an option. Patients and Methods The study is a phase II, multicenter, open-label, parallel-group, randomized, controlled exploratory study comparing the efficacy and safety of mFOLFOX6 plus panitumumab and 5-FU/LV plus panitumumab in patients with chemotherapy-naïve, unresectable, advanced or recurrent colorectal carcinoma of RAS wild-type (SAPPHIRE; ClinicalTrials.gov identifier, NCT02337946). Eligible patients will receive 6 cycles of mFOLFOX6 plus panitumumab combination therapy, followed by 1:1 randomization to either further treatment with mFOLFOX6 plus panitumumab or discontinuation of OXA and treatment with 5-FU/LV plus panitumumab. Up to 100 randomized patients will receive treatment for approximately 12 months or until any of the criteria for treatment discontinuation have been met. The primary endpoint is progression-free survival rate at 9 months after the day of randomization. The secondary endpoints are progression-free survival, overall survival, response rate, and interval to treatment failure. Safety will be evaluated according to the incidence and severity of adverse events, including the incidence of peripheral nerve and skin disorders. Additional endpoints will include maintenance of performance status, continuation of OXA in the mFOLFOX6 plus panitumumab group, and continuation of panitumumab in both groups.

    DOI: 10.1016/j.clcc.2017.02.001

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  305. Reduced- intensity conditioning allogeneic hematopoietic cell transplantation for younger patients with acute myeloid leukemia: a registry- based study Open Access

    Yanada, M; Kurosawa, S; Kobayashi, T; Ozawa, Y; Kanamori, H; Kobayashi, N; Sawa, M; Nakamae, H; Uchida, N; Hashimoto, H; Fukuda, T; Hirokawa, M; Atsuta, Y; Yano, S

    BONE MARROW TRANSPLANTATION   Vol. 52 ( 6 ) page: 818 - 824   2017.6

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    Clinical efficacy of allogeneic hematopoietic cell transplantation (HCT) using reduced-intensity conditioning (RIC) for younger patients remains unclear. We therefore performed a retrospective registry-based study to evaluate outcomes for patients with AML aged between 16 and 49 years who underwent RIC allogeneic HCT. Patients receiving RIC (N=125) showed significantly worse survival than those receiving myeloablative conditioning (MAC; N=1,554) (47.7% for RIC and 54.2% for MAC at 4 years, P=0.047). However, the difference became marginal after adjustment for patient characteristics (P=0.080), and inclusion in the multivariate analysis of the HCT comorbidity index or the propensity score for estimating the likelihood of choosing RIC or MAC further reduced statistical significance (P=0.371 and 0.206, respectively), indicating the existence of a selection bias against RIC. Nevertheless, outcomes for our patients receiving RIC were still acceptable, so that RIC constitutes a potential therapeutic option for younger AML patients who are deemed unsuitable for MAC. Subgroup analyses showed that patients aged between 40 and 49 years as well as those in first or second CR at the time of transplantation exhibited similar outcomes regardless of whether they were treated with RIC or MAC.

    DOI: 10.1038/bmt.2016.358

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  306. The divalent ion codoping effect on Ce-doped (Gd, La)<sub>2</sub>Si<sub>2</sub>O<sub>7</sub> single crystals Open Access

    Horiai, T; Murakami, R; Kurosawa, S; Shoji, Y; Yamaji, A; Pejchal, J; Ohashi, Y; Arakawa, M; Kamada, K; Yokota, Y; Yoshikawa, A

    OPTICAL MATERIALS   Vol. 68   page: 42 - 46   2017.6

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    Ce-doped (Gd, La)<inf>2</inf>Si<inf>2</inf>O<inf>7</inf> scintillators have fast decay time and keep high light output even at high temperature (∼150°C). To improve the scintillation properties such as light output and decay time, Ce-doped (Gd, La)<inf>2</inf>Si<inf>2</inf>O<inf>7</inf> scintillators codoped with the divalent ions (e.g. Mg<sup>2+</sup>, Ca<sup>2+</sup>) have been studied. In this study, we focused on the other divalent ions (Sr<sup>2+</sup> and Ba<sup>2+</sup>), and investigated their effect on the scintillation properties and temperature dependence of light output. The absorption due to Ce<sup>4+</sup> was not observed for Sr or Ba codoping. The light outputs were degraded by Sr<sup>2+</sup> or Ba<sup>2+</sup> codoping, while the decay times at room temperature were not changed for the samples codoped with divalent ions. On the other hand, the temperature dependence of light output for Ba-codoped sample was improved, and the light output value at 175°C was 36,000 photons/MeV, which was 93% of that at 25°C.

    DOI: 10.1016/j.optmat.2017.02.062

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  307. Effects of dopant distribution improvement on optical and scintillation properties for Ce-doped garnet-type single crystals

    Yokota, Y; Kudo, T; Ohashi, Y; Kurosawa, S; Kamada, K; Zeng, Z; Kawazoe, Y; Yoshikawa, A

    JOURNAL OF MATERIALS SCIENCE-MATERIALS IN ELECTRONICS   Vol. 28 ( 10 ) page: 7151 - 7156   2017.5

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    Ce-doped garnet-type single crystals with improved dopant distribution were grown by the micro-pulling-down method using a modified Iridium crucible and effects of dopant distribution improvement on the optical and scintillation properties were investigated. Ce-doped Y<inf>3</inf>Al<inf>5</inf>O<inf>12</inf> (Ce:YAG) and Gd<inf>3</inf>(Ga,Al)<inf>5</inf>O<inf>12</inf> (Ce:GGAG) single crystals with improved dopant distribution could be grown by a Iridium crucible with five capillaries (5C). The Ce:YAG and Ce:GGAG single crystals (5C) showed higher transmittance than the single crystals grown by an original Iridium crucible with one capillary (1C). In addition, a clear photo-peak could be observed in the pulse-height spectrum of the Ce:YAG single crystal (5C) under γ-ray irradiation while there was no peak in the spectrum of the Ce:YAG single crystal (1C).

    DOI: 10.1007/s10854-017-6696-x

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  308. Growth of LiF/LiBaF<sub>3</sub> eutectic scintillator crystals and their optical properties Open Access

    Kurosawa, S; Yamaji, A; Pejchal, J; Yokota, Y; Ohashi, Y; Kamada, K; Yoshikawa, A

    JOURNAL OF MATERIALS SCIENCE   Vol. 52 ( 10 ) page: 5531 - 5536   2017.5

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    Li-containing materials can be applied as neutron scintillators, and LiBaF<inf>3</inf> can discriminate neutron and gamma rays. Moreover, LIF/LiBaF<inf>3</inf> can have higher cross section of thermal-neutron capture compared with LiBaF<inf>3</inf>. In this study, LiF (82.5 mol%) and (Ba<inf>1−x</inf> RE<inf>x</inf>)F<inf>2</inf> (17.5 mol%, RE = Ce and Eu, x = 0.002) eutectic crystals, LiF/RE:LiBaF<inf>3</inf>, were grown by the micropulling down method with different pulling rates (growth rate) in order to observe the eutectic structure. Lamellar microstructure was formed for each pulling rate. LiF/Ce:LiBaF<inf>3</inf> excited by 5.5-MeV alpha rays had a broad peak at ~350 nm corresponding to 5d–4f transition of Ce<sup>3+</sup>. On the other hand, LiF/Eu:LiBaF<inf>3</inf> had two scintillation processes; a sharp emission was originated from <sup>6</sup>P<inf>7/2</inf> → <sup>8</sup>S<inf>7/2</inf> transitions in the 4f electronic configuration of Eu<sup>2+</sup> at 360 nm, and a broad one was attributed to Eu<sup>2+</sup> trapped exciton recombination at 400–450 nm. Since scintillation light was observed for these materials, these scintillators are sensitive to neutrons.

    DOI: 10.1007/s10853-017-0815-1

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  309. Imaging Polarimeter for a Sub-MeV Gamma-Ray All-sky Survey Using an Electron-tracking Compton Camera Open Access

    Komura, S; Takada, A; Mizumura, Y; Miyamoto, S; Takemura, T; Kishimoto, T; Kubo, H; Kurosawa, S; Matsuoka, Y; Miuchi, K; Mizumoto, T; Nakamasu, Y; Nakamura, K; Oda, M; Parker, JD; Sawano, T; Sonoda, S; Tanimori, T; Tomono, D; Yoshikawa, K

    ASTROPHYSICAL JOURNAL   Vol. 839 ( 1 )   2017.4

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    X-ray and gamma-ray polarimetry is a promising tool to study the geometry and the magnetic configuration of various celestial objects, such as binary black holes or gamma-ray bursts (GRBs). However, statistically significant polarizations have been detected in few of the brightest objects. Even though future polarimeters using X-ray telescopes are expected to observe weak persistent sources, there are no effective approaches to survey transient and serendipitous sources with a wide field of view (FoV). Here we present an electron-tracking Compton camera (ETCC) as a highly sensitive gamma-ray imaging polarimeter. The ETCC provides powerful background rejection and a high modulation factor over an FoV of up to 2π sr thanks to its excellent imaging based on a well-defined point-spread function. Importantly, we demonstrated for the first time the stability of the modulation factor under realistic conditions of off-axis incidence and huge backgrounds using the SPring-8 polarized X-ray beam. The measured modulation factor of the ETCC was 0.65 ±0.01 at 150 keV for an off-axis incidence with an oblique angle of 30° and was not degraded compared to the 0.58 ±0.02 at 130 keV for on-axis incidence. These measured results are consistent with the simulation results. Consequently, we found that the satellite-ETCC proposed in Tanimori et al. would provide all-sky surveys of weak persistent sources of 13 mCrab with 10% polarization for a 10<sup>7</sup> s exposure and over 20 GRBs down to a 6 ×10<sup>-6</sup> erg cm<sup>-2</sup> fluence and 10% polarization during a one-year observation.

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  310. Use of mycophenolate mofetil and a calcineurin inhibitor in allogeneic hematopoietic stem-cell transplantation from HLA-matched siblings or unrelated volunteer donors: Japanese multicenter phase II trials

    Nakane, T; Nakamae, H; Yamaguchi, T; Kurosawa, S; Okamura, A; Hidaka, M; Fuji, S; Kohno, A; Saito, T; Aoyama, Y; Hatanaka, K; Katayama, Y; Yakushijin, K; Matsui, T; Yamamori, M; Takami, A; Hino, M; Fukuda, T

    INTERNATIONAL JOURNAL OF HEMATOLOGY   Vol. 105 ( 4 ) page: 485 - 496   2017.4

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    To test the feasibility of mycophenolate mofetil (MMF) for graft-versus-host disease (GVHD) prophylaxis in Japanese patients, we conducted two multicenter prospective phase II trials of allogeneic hematopoietic stem-cell transplantation (HSCT) from HLA-matched related donors (MRD group) with MMF and cyclosporine or HLA 7–8/8 allele-matched unrelated bone-marrow donors (URD group) with MMF and tacrolimus. The cumulative incidences of grade II–IV acute GVHD on day 100, which was the primary endpoint in these trials, were 45.0% (90% CI 25.8–62.5) and 25.8% (90% CI 13.9–39.5) in the MRD (n = 20) and URD (n = 31) groups, respectively. The rates of 3-year overall survival and non-relapse mortality were 80.0 and 15.0% in the MRD group and 74.2 and 6.5% in the URD group, respectively. GVHD prophylaxis with MMF may lead to a lower incidence of severe mucositis and faster neutrophil engraftment compared to that with methotrexate. A pharmacokinetics study of mycophenolic acid (MPA) showed that a relatively higher plasma concentration of MPA was associated with a lower incidence of acute GVHD. In conclusion, the results of these studies suggest that GVHD prophylaxis with MMF may be useful as an alternative in Japanese patients who may benefit from faster engraftment or less severe mucositis after allogeneic HSCT.

    DOI: 10.1007/s12185-016-2154-4

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  311. High non-relapse mortality and low relapse incidence in gender-mismatched allogeneic hematopoietic stem cell transplantation from a parous female donor with a male child

    Shinohara A., Inamoto Y., Kurosawa S., Hiramoto N., Ueda R., Tanaka T., Tada K., Kobayashi Y., Morikawa N., Okinaka K., Kim S.W., Tajima K., Fukuda T.

    Leukemia and Lymphoma   Vol. 58 ( 3 ) page: 578 - 585   2017.3

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    To clarify the influence of exposure to a male fetus during a female donor’s (FD) pregnancy in allogeneic hematopoietic stem cell transplantation (HSCT), we retrospectively examined 292 HSCT patients. The 5-year non-relapse mortality (NRM) was 33.5% among 31 male recipients who had HSCT from FD with a male child (MC), 23.0% among 40 male recipients who had HSCT from FD without MC and 19.6% among 221 other recipients. The 5-year relapse incidence (RI) was 22.6%, 42.0%, and 43.1% for the respective group. In multivariate analysis, male recipients who had HSCT from FD with MC had an increased risk of NRM (hazard ratio [HR] 1.92, 95% CI 1.08–3.42, p =.03), a reduced risk of RI (HR 0.42, 95% CI 0.18–0.96, p =.04), resulting in no significant difference regarding overall survival. Male child of FD is suggested to influence NRM and RI in gender-mismatched HSCT.

    DOI: 10.1080/10428194.2016.1205743

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  312. 2 inch size Czochralski growth and scintillation properties of Li<SUP>+</SUP> co-doped Ce:Gd<sub>3</sub>Ga<sub>3</sub>Al<sub>2</sub>O<sub>12</sub>

    Kamada, K; Shoji, Y; Kochurikhin, VV; Yoshino, M; Okumura, S; Yamamoto, S; Yeom, JY; Kurosawa, S; Yokota, Y; Ohashi, Y; Nikl, M; Yoshino, M; Yoshikawa, A

    OPTICAL MATERIALS   Vol. 65   page: 52 - 55   2017.3

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    The 2 inch size Li 0.15 and 1.35 mol% co-doped Ce:Gd<inf>3</inf>Al<inf>2</inf>Ga<inf>3</inf>O<inf>12</inf> single crystals were prepared by the Czochralski (Cz) method. Absorption and luminescence spectra were measured together with several other scintillation characteristics, namely the scintillation decay and light yield to reveal the effect of Li co-doping. Ce<sup>4+</sup> CT absorption below 350 nm is clearly enhanced by Li co-doping as same as divalent ions co-doping. By 1.35 at.% Li co-doping, light yield was decrease to 88% of the Ce: GAGG standard and decay time was accelerated to 34.3ns 21.0%, 84.6ns 68.7%, 480ns 10.3%. The timing resolution measurement for a pair of 3 × 3 × 3mm<sup>3</sup> size Li,Ce:GAGG scintillator crystals was performed using Si-PMs and the timing resolution of the 1.35 at.% Li co-doped Ce:GAGG was 218ps.

    DOI: 10.1016/j.optmat.2016.09.005

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  313. Crystal growth and optical properties of indium doped LiCaAlF<sub>6</sub> scintillator single crystals Open Access

    Tanaka, C; Yokota, Y; Kurosawa, S; Yamaji, A; Jary, V; Babin, V; Pejchal, J; Ohashi, Y; Kamada, K; Nikl, M; Yoshikawa, A

    OPTICAL MATERIALS   Vol. 65   page: 69 - 72   2017.3

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    The In-doped LiCaAlF<inf>6</inf> [In:LiCAF] single crystals were grown by the micro-pulling-down (μ-PD) method, and the phases, chemical compositions, transmittance and radioluminescence spectra were investigated. All the grown crystals showed high transparency and single phase of LiCAF without visible cracks and inclusions except for the end part of In2%:LiCAF crystal which included the impurity phase. In the radioluminescence spectra of the In:LiCAF crystals under X-ray irradiation, the emission peak around 750 nm was revealed.

    DOI: 10.1016/j.optmat.2016.10.040

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  314. Development of novel growth methods for halide single crystals

    Yokota, Y; Kurosawa, S; Shoji, Y; Ohashi, Y; Kamada, K; Yoshikawa, A

    OPTICAL MATERIALS   Vol. 65   page: 46 - 51   2017.3

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    We developed novel growth methods for halide scintillator single crystals with hygroscopic nature, Halide micro-pulling-down [H-μ-PD] method and Halide Vertical Bridgman [H-VB] method. The H-μ-PD method with a removable chamber system can grow a single crystal of halide scintillator material with hygroscopicity at faster growth rate than the conventional methods. On the other hand, the H-VB method can grow a large bulk single crystal of halide scintillator without a quartz ampule. CeCl<inf>3</inf>, LaBr<inf>3</inf>, Ce:LaBr<inf>3</inf> and Eu:SrI<inf>2</inf> fiber single crystals could be grown by the H-μ-PD method and Eu:SrI<inf>2</inf> bulk single crystals of 1 and 1.5 inch in diameter could be grown by the H-VB method. The grown fiber and bulk single crystals showed comparable scintillation properties to the previous reports using the conventional methods.

    DOI: 10.1016/j.optmat.2016.08.035

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  315. Effects of Mg-codoping on luminescence and scintillation properties of Ce doped Lu<sub>3</sub>(Ga,Al)<sub>5</sub>O<sub>12</sub> single crystals Open Access

    Yamaguchi, H; Kamada, K; Pejchal, J; Kurosawa, S; Shoji, Y; Yokota, Y; Ohashi, Y; Yoshikawa, A

    OPTICAL MATERIALS   Vol. 65   page: 60 - 65   2017.3

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    Effects of Mg co-doping on scintillation properties of Ce:Lu<inf>3</inf>(Ga,Al)<inf>5</inf>O<inf>12</inf> (LGAG) were investigated. Mg 200 ppm co-doped Ce:LGAG single crystals were prepared by micro pulling down method. Absorption and radioluminescence spectra were measured together with several other scintillation characteristics, namely the scintillation decay and light yield to reveal the effect of Mg co-doping. Ce<sup>4+</sup> charge transfer absorption was observed below 340 nm in Mg,Ce:LGAG which is in good agreement with previous reports for other garnet-based crystals. The scintillation decay time showed the tendency to be accelerated and the light yield was enhanced by Mg co-doping.

    DOI: 10.1016/j.optmat.2016.08.030

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  316. Temperature dependence of Ce-doped (Gd<sub>0.6</sub> La<sub>0.4</sub>)<sub>2</sub>Si<sub>2</sub>O<sub>7</sub> scintillators Open Access

    Horiai, T; Kurosawa, S; Murakami, R; Yamaji, A; Shoji, Y; Ohashi, Y; Pejchal, J; Kamada, K; Yokota, Y; Yoshikawa, A

    OPTICAL MATERIALS   Vol. 65   page: 56 - 59   2017.3

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    Publisher:Optical Materials  

    (Ce<inf>0.01</inf> Gd<inf>0.59</inf> La<inf>0.40</inf>)<inf>2</inf>Si<inf>2</inf>O<inf>7</inf> single crystal (La40% sample) was grown by the micro-pulling-down method to study its scintillation properties and their temperature dependence. In addition, we investigated the relation between these properties and La concentration comparing the crystal with (Ce<inf>0.01</inf> Gd<inf>0.90</inf> La<inf>0.09</inf>)<inf>2</inf>Si<inf>2</inf>O<inf>7</inf> (La9% sample). As results, the light output of the La40% sample at 25°C was similar to that of the La9% sample. On the other hand, the decay time of the La40% sample was slower than that of the La9% sample at 25°C. The light output of La40% sample had a small decrease rate at high temperature when compared with that of La9% sample.

    DOI: 10.1016/j.optmat.2016.10.039

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  317. Establishment of Imaging Spectroscopy of Nuclear Gamma-Rays based on Geometrical Optics Open Access

    Tanimori, T; Mizumura, Y; Takada, A; Miyamoto, S; Takemura, T; Kishimoto, T; Komura, S; Kubo, H; Kurosawa, S; Matsuoka, Y; Miuchi, K; Mizumoto, T; Nakamasu, Y; Nakamura, K; Parker, JD; Sawano, T; Sonoda, S; Tomono, D; Yoshikawa, K

    SCIENTIFIC REPORTS   Vol. 7   page: 41511   2017.2

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    Since the discovery of nuclear gamma-rays, its imaging has been limited to pseudo imaging, such as Compton Camera (CC) and coded mask. Pseudo imaging does not keep physical information (intensity, or brightness in Optics) along a ray, and thus is capable of no more than qualitative imaging of bright objects. To attain quantitative imaging, cameras that realize geometrical optics is essential, which would be, for nuclear MeV gammas, only possible via complete reconstruction of the Compton process. Recently we have revealed that "Electron Tracking Compton Camera" (ETCC) provides a well-defined Point Spread Function (PSF). The information of an incoming gamma is kept along a ray with the PSF and that is equivalent to geometrical optics. Here we present an imaging-spectroscopic measurement with the ETCC. Our results highlight the intrinsic difficulty with CCs in performing accurate imaging, and show that the ETCC surmounts this problem. The imaging capability also helps the ETCC suppress the noise level dramatically by ∼3 orders of magnitude without a shielding structure. Furthermore, full reconstruction of Compton process with the ETCC provides spectra free of Compton edges. These results mark the first proper imaging of nuclear gammas based on the genuine geometrical optics.

    DOI: 10.1038/srep41511

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    PubMed

  318. Comparison of luminescence, energy resolution and light loss coefficient of Gd<sub>1.53</sub>La<sub>0.47</sub>Si<sub>2</sub>O<sub>7</sub>:Ce and Lu<sub>1.9</sub>Y<sub>0.1</sub>SiO<sub>5</sub>:Ce scintillators

    Yawai, N; Wantong, K; Chewpraditkul, W; Murakami, R; Horiai, T; Kurosawa, S; Yoshikawa, A; Nikl, M

    NUCLEAR INSTRUMENTS & METHODS IN PHYSICS RESEARCH SECTION A-ACCELERATORS SPECTROMETERS DETECTORS AND ASSOCIATED EQUIPMENT   Vol. 844   page: 129 - 134   2017.2

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    Publisher:Nuclear Instruments and Methods in Physics Research Section A Accelerators Spectrometers Detectors and Associated Equipment  

    The luminescence and scintillation properties of Gd<inf>1.53</inf>La<inf>0.47</inf>Si<inf>2</inf>O<inf>7</inf>:Ce (GPSLa23.5%:Ce) scintillators were investigated and compared to those of Lu<inf>1.9</inf>Y<inf>0.1</inf>SiO<inf>5</inf>:Ce (LYSO:Ce) scintillators. At 662 keV γ-rays, the light yield of 33,500±3300 ph/MeV obtained for GPSLa23.5%:Ce is higher than that of 28,100±2800 ph/MeV obtained for LYSO:Ce. The energy resolution of 4.8±0.2% obtained for GPSLa23.5%:Ce is much better than that of 8.2±0.3% obtained for LYSO:Ce due to its better intrinsic resolution and proportionality of light yield. The light yield and energy resolution for α- rays, as well as a light yield ratio under excitation with α - and γ - rays (α/γ ratio) were also determined. The intrinsic light yield and light loss coefficient under excitation with 662 keV γ-rays were evaluated. The total attenuation coefficient at 60 keV and 662 keV γ - rays was also determined and compared with the theoretical one calculated using the WinXCom program.

    DOI: 10.1016/j.nima.2016.11.040

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  319. Cesium hafnium chloride scintillator coupled with an avalanche photodiode photodetector Open Access

    Kurosawa, S; Kodama, S; Yokota, Y; Horiai, T; Yamaji, A; Shoji, Y; Král, R; Pejchal, J; Ohashi, Y; Kamada, K; Nikl, M; Yoshikawa, A

    JOURNAL OF INSTRUMENTATION   Vol. 12 ( 2 )   2017.2

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    Optical and scintillation properties of pure Cs<inf>2</inf>HfCl<inf>6</inf> (CHC) single crystals were investigated. In particular, light output and energy resolution were measured using a Si avalanche photodiode (Si-APD), since the Si-APD has sufficient quantum efficiency of around 70 % at emission wavelength region of CHC around 420 nm. This CHC single crystal grown using the vertical Bridgeman method showed light output of 37,000andplusmn; 2,000 photons/MeV . The FWHM energy resolution was determined to be 3.7andplusmn; 0.5andtimes; (E/662 keV)<sup>-0.85andplusmn; 0.03</sup>[%], where E [keV] is the gamma-ray energy. Moreover, the temperature dependence of the light output was stable from -5 to 30 <sup>-</sup>C, while the light output increased below -10 <sup>-</sup>C.

    DOI: 10.1088/1748-0221/12/02/C02042

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  320. Improvement of the growth of Li<sub>4</sub>SiO<sub>4</sub> single crystals for neutron detection and their scintillation and luminescence properties Open Access

    Pejchal, J; Babin, V; Beitlerova, A; Kurosawa, S; Yokota, Y; Yoshikawa, A; Nikl, M

    JOURNAL OF CRYSTAL GROWTH   Vol. 457   page: 143 - 150   2017.1

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    Publisher:Journal of Crystal Growth  

    We have investigated Li<inf>4</inf>SiO<inf>4</inf> scintillation crystals for their possible application in neutron detection due to high Li content and low density of 2.35 g/cm<sup>3</sup>. The micro-pulling-down method employing the Ir crucible and afterheater was optimized for crystal growth of Li<inf>4</inf>SiO<inf>4</inf> taking into account the Li evaporation. To grow high-quality crack-free single crystals, the heating power was increased to establish milder temperature gradient, thicker meniscus, smaller crystal diameter and resulting smaller stress in the as-grown crystals. The undoped, Ti-, Cr-, and Al- doped crystals were prepared and studied. Radioluminescence measurements under X-ray excitation showed quite high overall scintillation efficiency of the Ti-doped sample reaching as high as 250% of that of Bi<inf>4</inf>Ge<inf>3</inf>O<inf>12</inf> reference scintillator. The emission spectrum was dominated by one broad band peaking at 350 nm related to Ti<sup>4+</sup> impurity. Reasonable light yield of 10000 photons/neutron was found. However, its long decay time of 54 μs might be a limitation especially for high counting rate applications. The overall scintillation efficiency of the Cr<sup>3+</sup> sample was much lower and the spectrum shows one broad peak at 463 nm which does not correspond to Cr<sup>3+</sup> luminescence. The radioluminescence spectrum of the Al-doped sample resembled to that of the Ti-doped one, just its magnitude is considerably lower, which was explained by Ti contamination. Peculiarities and optimization of crystal growth and a preliminary sketch of luminescence mechanisms and dopant incorporation are discussed.

    DOI: 10.1016/j.jcrysgro.2016.02.008

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  321. Crystal growth and piezoelectric properties of Ca<sub>3</sub>Ta(Ga<sub>1-x</sub> Sc<sub>x</sub>)<sub>3</sub>Si<sub>2</sub>O<sub>14</sub> single crystals

    Igarashi, Y; Ohashi, Y; Yokota, Y; Arakawa, M; Inoue, K; Yamaji, A; Shoji, Y; Kamada, K; Kurosawa, S; Yoshikawa, A

    CERAMICS INTERNATIONAL   Vol. 43   page: S136 - S139   2017

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    Publisher:Ceramics International  

    Ca<inf>3</inf>Ta(Ga<inf>1-x</inf>Sc<inf>x</inf>)<inf>3</inf>Si<inf>2</inf>O<inf>14</inf> (CTGSS) single crystals with various Sc concentrations (x = 0, 0.1, 0.2, 0.3, and 0.4) were grown by the micro-pulling-down method and their structure and chemical composition were evaluated. Through the powder X-ray diffraction (XRD) measurement and backscattered electron (BSE) imaging, it was demonstrated that all the CTGSS crystals with different Sc concentration were successfully grown as langasite-type structure although some secondary phases were observed for the crystals with x = 0.2, 0.3 and 0.4. Lattice parameters calculated from the powder XRD pattern generally increased with Sc substitution. Measured parameters for CTGSS crystal with x = 0.1 were larger permittivity ε<inf>11</inf><sup>T</sup>/ε<inf>0</inf> and lower electromechanical coupling coefficient k<inf>12</inf> and piezoelectric constant d<inf>11</inf> than those for CTGS crystal with x = 0. It was also suggested that piezoelectric constant |d<inf>14</inf>| became larger due to the Sc substitution.

    DOI: 10.1016/j.ceramint.2017.05.272

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  322. Difference in distribution of Eu ions doped CaF2 single crystal caused by two types of grown method by measurement of multi-photon luminescence

    Tanaka M., Ono S., Yamaji A., Kurosawa S., Yoshikawa A.

    Optics Infobase Conference Papers   Vol. Part F122-CLEOPR 2017   2017

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    Publisher:Optics Infobase Conference Papers  

    We report on distribution of Eu ions doped CaF2 single crystal by measurement of multi-photon luminescence. Distribution of Eu<sup>2+</sup> and Eu<sup>3+</sup> ions is measured respectively because the luminescence peak due to Eu<sup>2+</sup> and Eu<sup>3+</sup> ions is different. We observed the difference in distribution of Eu<sup>2+</sup> and Eu<sup>3+</sup> ions doped CaF2 which is grown by Annealing method and micro pulling-down method.

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  323. Difference in Distribution of Eu Ions Doped CaF<sub>2</sub> Single Crystal Caused by Two Types of Grown Method by Measurement of Multi-photon Luminescence

    Tanaka, M; Ono, S; Yamaji, A; Kurosawa, S; Yoshikawa, A

    2017 CONFERENCE ON LASERS AND ELECTRO-OPTICS PACIFIC RIM (CLEO-PR)     2017

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  324. New readout and data-acquisition system for reducing dead ime in the Gamma Ray Compton Telescope

    Yoshikawa, K; Tanimori, T; Takada, A; Mizumoto, T; Mizumura, Y; Komura, S; Kishimoto, T; Takemura, T; Nakamasu, Y; Taniguchi, T; Nakamura, Y; Kubo, H; Sawano, T; Nakamura, K; Sonoda, S; Miuchi, K; Kurosawa, S; Parker, JD

    2017 IEEE NUCLEAR SCIENCE SYMPOSIUM AND MEDICAL IMAGING CONFERENCE (NSS/MIC)     2017

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  325. Single crystal growth and scintillation properties of Ca(Cl, Br, I)<sub>2</sub> single crystal

    Kamada, K; Iida, T; Ohata, T; Yoshino, M; Hayasaka, S; Shoji, Y; Sakuragi, S; Kurosawa, S; Yokota, Y; Ohashi, Y; Yoshikawa, A

    CERAMICS INTERNATIONAL   Vol. 43   page: S423 - S427   2017

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    Publisher:Ceramics International  

    Single crystal growth of undope CaCl<inf>2</inf>, CaBr<inf>2</inf> and CaI<inf>2</inf> was performed by Bridgman–Stockbarger (BS) method. Investigations of their crystal phases, luminescence and scintillation properties such light yield, energy resolution decay time were performed. In addition, linearity of gamma-ray response in 32–1275 keV range were also evaluated. The light output of 106,000 photon/MeV, energy resolution of 3.2%@662 keV, and scintillation decay time of 834 ns (84%) 1460 ns (16%) were observed. Luminescence properties of CaBr<inf>2</inf> also firstly reported.

    DOI: 10.1016/j.ceramint.2017.05.249

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  326. Transparent High-Density Oxide Ceramics Prepared by Spark Plasma Sintering

    Goto, T; Ito, A; Yoshikawa, A; Kurosawa, S; Pejchal, J

    NANOCOMPOSITE, CERAMIC, AND THIN FILM SCINTILLATORS     page: 107 - 154   2017

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  327. Improvement of scintillator's reflector toward the improvement of the performance for Compton scattering type polarimeter

    Saito Yo, Gunji Shuichi, Okumura Akira, Nakamori Takeshi, Nakazawa Kazuhiro, Watanabe Naoki, Karube Atsuhito, Kurosawa Shunsuke

    Meeting Abstracts of the Physical Society of Japan   Vol. 72.2 ( 0 ) page: 414 - 414   2017

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    Language:Japanese   Publisher:The Physical Society of Japan  

    DOI: 10.11316/jpsgaiyo.72.2.0_414

    CiNii Research

  328. Clinical Impact of Pre-Transplant Microbial Diversity on Transplant Outcomes

    Kurosawa, S; Doki, N; Suyama, M; Sasajima, S; Igarashi, A; Mimura, I; Morita, H; Fujioka, Y; Nishikawa, H; Shimazu, Y; Suda, W; Hattori, M; Najima, Y; Kakihana, K; Sakamaki, H; Honda, K; Ohashi, K

    BLOOD   Vol. 128 ( 22 )   2016.12

  329. Al content dependence of acoustic properties for Ca3Nb(Ga1-xAlx)3Si2O14 single crystals

    Ohashi Y., Arakawa M., Yokota Y., Inoue K., Yamaji A., Kurosawa S., Kamada K., Yoshikawa A.

    IEEE International Ultrasonics Symposium Ius   Vol. 2016-November   2016.11

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    Publisher:IEEE International Ultrasonics Symposium Ius  

    Acoustic properties for Ca<inf>3</inf>Nb(Ga<inf>1-x</inf>Al<inf>x</inf>)<inf>3</inf>Si<inf>2</inf>O<inf>14</inf> [CNGAS(x)] single crystals were experimentally investigated as a function of Al substitution content. Several plate specimens of the X-, Y-, Z-, 40°Y-, and 145°Y-cut were prepared from CNGAS(x) single crystal ingots (x=0, 0.25, and 0.50) grown by Czochralski technique. Velocities of longitudinal wave, shear wave, and leaky surface acoustic wave (LSAW) were measured for the CNGAS(x) specimens at 23°C using the ultrasonic microspectroscopy (UMS) system. Densities were also measured. It was experimentally demonstrated that all of acoustic properties were linearly changed as a function of Al substitution content.

    DOI: 10.1109/ULTSYM.2016.7728806

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  330. Co-doping effects on luminescence and scintillation properties of Ce doped (Lu,Gd)<sub>3</sub>(Ga,Al)<sub>5</sub>O<sub>12</sub> scintillator

    Yamaguchi, H; Kamada, K; Kurosawa, S; Pejchal, J; Shoji, Y; Yokota, Y; Ohashi, Y; Yoshikawa, A

    OPTICAL MATERIALS   Vol. 61   page: 129 - 133   2016.11

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    Publisher:Optical Materials  

    Mg co-doping effects on scintillation properties of Ce:Lu<inf>1</inf>Gd<inf>2</inf>(Ga,Al)<inf>5</inf>O<inf>12</inf> (LGGAG) were investigated. Mg 200 ppm co-doped Ce:LGGAG single crystals were prepared by micro pulling down method. Absorption and luminescence spectra were measured together with several other scintillation characteristics, namely the scintillation decay and light yield to reveal the effect of Mg co-doping. Ce<sup>4+</sup> charge transfer absorption was observed below 300 nm in Mg,Ce:LGGAG which is in good agreement with previous reports. The scintillation decay times were accelerated by Mg co-doping.

    DOI: 10.1016/j.optmat.2016.05.025

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  331. Growth and scintillation properties of Tb doped LiGdF<sub>4</sub>/LiF eutectic scintillator

    Kamada, K; Hishinuma, K; Kurosawa, S; Yamaji, A; Shoji, Y; Ohashi, Y; Yokota, Y; Yoshikawa, A

    OPTICAL MATERIALS   Vol. 61   page: 134 - 138   2016.11

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    Tb-doped LiGdF<inf>4</inf>-LiF eutectics were grown at various growth rate and their directionally solidified eutectic (DSE) system has been investigated. Well aligned fiber like eutectic structure with around 1.7 μm in diameter and 1200 μm in maximum length was obtained the growth speed of 0.15 mm/min. The sample showed optical transparency like bundle optical fibers and around 40% of transmittance at 1.5 mm thick was achieved in 380–630 nm range. The expected 380–630 nm emission exited by UV and α-ray, and 270–330 nm excitation of Tb<sup>3+8</sup>S -<sup>6</sup>P transition have been observed. The weak emission of Gd<sup>3+</sup> 4f-4f transition at 310 nm was also observed under alpha-ray excitation. The Observed excitation bands peaking at around 275 nm and 310 nm correspond respectively to the <sup>8</sup>S<sup>7/2</sup>- <sup>6</sup>I<inf>7/2</inf> and <sup>8</sup>S<inf>7/2</inf>-<sup>6</sup>P<inf>J</inf> absorption bands of Gd<sup>3+</sup>.

    DOI: 10.1016/j.optmat.2016.09.019

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  332. Chemical composition characterization of Ca<sub>3</sub>Ta(Ga<sub>0.5</sub>Al<sub>0.5</sub>)<sub>3</sub>Si<sub>2</sub>O<sub>14</sub> single crystal by the line-focus-beam ultrasonic material characterization system

    Ohashi, Y; Kudo, T; Yokota, Y; Shoji, Y; Kurosawa, S; Kamada, K; Yoshikawa, A

    JOURNAL OF CRYSTAL GROWTH   Vol. 452   page: 141 - 145   2016.10

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    Publisher:Journal of Crystal Growth  

    A new method for evaluation of homogeneity of Ca<inf>3</inf>Ta(Ga<inf>0.5</inf>Al<inf>0.5</inf>)<inf>3</inf>Si<inf>2</inf>O<inf>14</inf> (CTGAS) single crystals was established based on leaky surface acoustic wave (LSAW) velocity measurements performed by the line-focus-beam ultrasonic material characterization (LFB-UMC) system. Three plate specimens cut perpendicular to X-, Y-, and Z-axes were prepared from the CTGAS crystal ingot and LSAW velocity distributions were examined for these specimens. LSAW velocity changes due to Al-substitution effect were successfully extracted by using a relationship between two LSAW velocities propagating along different directions for Ca<inf>3</inf>TaGa<inf>3</inf>Si<inf>2</inf>O<inf>14</inf> (CTGS) and Al-substituted CTGS. Comparison of measured LSAW velocities and the results of chemical composition analysis performed by electron probe microanalysis (EPMA) demonstrated that LSAW velocity is mainly affected by Al-content change in CTGAS. Maximum velocity variation was observed in radial direction of the crystal ingot through the Z-axis propagating LSAW velocity measurements for Y-cut CTGAS specimen corresponding to Al-content change of 0.226 mol%. Accuracy of evaluation of Al content by velocity measurement for Y-cut Z-propagating LSAW is estimated to be ±0.0047 mol% and is superior to that by EPMA.

    DOI: 10.1016/j.jcrysgro.2016.04.003

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  333. Crystal growth and scintillation properties of Lu substituted CeBr<sub>3</sub> single crystals

    Ito, T; Yokota, Y; Kurosawa, S; Král, R; Kamada, K; Pejchal, J; Ohashi, Y; Yoshikawa, A

    JOURNAL OF CRYSTAL GROWTH   Vol. 452   page: 65 - 68   2016.10

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    Publisher:Journal of Crystal Growth  

    We grew Lu-substituted CeBr<inf>3</inf> [(Ce<inf>1−x</inf>Lu<inf>x</inf>)Br<inf>3</inf>] crystals by a modified micro-pulling-down method to increase the effective atomic number and to investigate effects of the Lu substitution on the crystal growth, phase generation, chemical composition, and optical and scintillation properties. The (Ce<inf>1−x</inf>Lu<inf>x</inf>)Br<inf>3</inf> crystals with x=0 and 0.01 had high transparency while the milky parts were generated in the crystals with x=0.05 and 0.20. By the analysis of chemical composition, the estimated Z<inf>eff</inf> increased to 47.9. On the other hand, the light yields were systematically decreased and decay times were increased with increasing Lu concentration.

    DOI: 10.1016/j.jcrysgro.2016.04.059

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  334. Czochralski growth of 2 in. Ce-doped (La,Gd)<sub>2</sub>Si<sub>2</sub>O<sub>7</sub> for scintillator application

    Yoshikawa, A; Shoji, Y; Kurosawa, S; Chani, VI; Murakami, R; Horiai, T; Kamada, K; Yokota, Y; Ohashi, Y; Kochurikhin, V

    JOURNAL OF CRYSTAL GROWTH   Vol. 452   page: 57 - 64   2016.10

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    Growth of 2-in. diameter Ce-doped (La<inf>,</inf>Gd)<inf>2</inf>Si<inf>2</inf>O<inf>7</inf> (La-GPS) scintillating crystals by Czochralski method using Ir crucible is reported. The composition of the host material was approximately equal to La<inf>0.5</inf>Gd<inf>1.5</inf>Si<inf>2</inf>O<inf>7</inf> and the concentration of the Ce<sup>3+</sup>-activator was either 0.5 or 1.5 at.% with respect to the total content of the rare-earths forming the host crystal matrix. Effects of the hot zone construction including inductive coil position, presence/absence of the after-heater, rotation rate and other growth parameters on the crystal quality are discussed in some details. The crystals produced in optimized conditions were colorless, transparent, uniform in their shape, crack- and inclusions-free, and demonstrated smooth glass-like surface. The length of the crystals’ cylindrically-shaped body parts exceed 100 mm. The growth results were well reproducible. The main disadvantage of the growth process is associated with short lifetime of the Ir crucible and its deformation caused by thermal expansion of the pre-solidified melt at each heating stage.

    DOI: 10.1016/j.jcrysgro.2016.06.016

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  335. Czochralski growth of 2 in. Ca<sub>3</sub>Ta(Ga,Al)<sub>3</sub>Si<sub>2</sub>O<sub>14</sub> single crystals for piezoelectric applications

    Yoshikawa, A; Shoji, Y; Ohashi, Y; Yokota, Y; Chani, VI; Kitahara, M; Kudo, T; Kamada, K; Kurosawa, S; Medvedev, A; Kochurikhin, V

    JOURNAL OF CRYSTAL GROWTH   Vol. 452   page: 135 - 140   2016.10

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    Growth of 2-in. diameter Al-substituted Ca<inf>3</inf>TaGa<inf>3</inf>Si<inf>2</inf>O<inf>14</inf> crystals by Czochralski method is reported. The crystals were grown from the melt of Ca<inf>3</inf>TaGa<inf>1.5</inf>Al<inf>1.5</inf>Si<inf>2</inf>O<inf>14</inf> composition and had langasite structure. No inclusions of secondary phases were detected in these crystals. The Ca<inf>3</inf>Ta(Ga,Al)<inf>3</inf>Si<inf>2</inf>O<inf>14</inf> mixed crystals produced using non-substituted Ca<inf>3</inf>TaGa<inf>3</inf>Si<inf>2</inf>O<inf>14</inf> seeds were defective. They had cracks and/or poly-crystalline structure. However, those grown on the seed of approximately Ca<inf>3</inf>TaGa<inf>1.5</inf>Al<inf>1.5</inf>Si<inf>2</inf>O<inf>14</inf> composition were defect-free. Phase diagram of the Ca<inf>3</inf>TaGa<inf>3</inf>Si<inf>2</inf>O<inf>14</inf>–Ca<inf>3</inf>TaAl<inf>3</inf>Si<inf>2</inf>O<inf>14</inf> pseudo-binary system and segregation phenomenon are discussed in some details. Homogeneity of the crystals was evaluated by measuring 2D-mapping of leaky surface acoustic wave (LSAW) velocities for Y-cut Ca<inf>3</inf>TaGa<inf>1.5</inf>Al<inf>1.5</inf>Si<inf>2</inf>O<inf>14</inf> substrate. Although some inhomogeneities were observed due to slight variations in chemical composition, the crystal had acceptable homogeneity for applications in acoustic wave devices exhibiting the LSAW velocity variation within ±0.048%.

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  336. Growth and scintillation properties of 3 in. diameter Ce doped Gd<sub>3</sub>Ga<sub>3</sub>Al<sub>2</sub>O<sub>12</sub> scintillation single crystal Open Access

    Kamada, K; Shoji, Y; Kochurikhin, VV; Okumura, S; Yamamoto, S; Nagura, A; Yeom, JY; Kurosawa, S; Yokota, Y; Ohashi, Y; Nikl, M; Yoshikawa, A

    JOURNAL OF CRYSTAL GROWTH   Vol. 452   page: 81 - 84   2016.10

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    The 3 in. size Ce1%:Gd<inf>3</inf>Al<inf>2</inf>Ga<inf>3</inf>O<inf>12</inf> single crystals were prepared by the Czochralski (Cz) method. Optical constants were measured. Chemical composition analysis and uniformity of scintillation decay and light yield along growth direction were evaluated. The timing resolution measurement for a pair of 3 mm×3 mm×3 mm size Ce:GAGG scintillator crystals was performed using Si-PMs.

    DOI: 10.1016/j.jcrysgro.2016.04.037

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  337. Growth and scintillation properties of Li and Ce co-doped Lu<sub>3</sub>Al<sub>5</sub>O<sub>12</sub> scintillator Open Access

    Kamada, K; Nikl, M; Kurosawa, S; Beitlerova, A; Nagura, A; Shoji, Y; Pejchal, J; Ohashi, Y; Yokota, Y; Yoshikawa, A

    JOURNAL OF CRYSTAL GROWTH   Vol. 452   page: 85 - 88   2016.10

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    The Li<sup>+</sup> co-doped Ce:Lu<inf>3</inf>Al<inf>5</inf>O<inf>12</inf> single crystals were prepared by micro pulling down method. Absorption and luminescence spectra were measured together with several other scintillation characteristics, namely the scintillation decay and light yield to reveal the effect of the co-doping. The smooth Ce<sup>4+</sup>CT absorption below 350 nm is clearly enhanced with increasing concentration of Li. The scintillation decays were accelerated and light yields were increased by Li co-doping.

    DOI: 10.1016/j.jcrysgro.2016.04.036

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  338. Growth of 2 Inch Eu-doped SrI<sub>2</sub> single crystals for scintillator applications

    Yoshikawa, A; Shoji, Y; Yokota, Y; Kurosawa, S; Hayasaka, S; Chani, VI; Ito, T; Kamada, K; Ohashi, Y; Kochurikhin, V

    JOURNAL OF CRYSTAL GROWTH   Vol. 452   page: 73 - 80   2016.10

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    A vertical Bridgman (VB) crystal growth process was established using modified micro-pulling-down (μ-PD) crystal growth system with a removable chamber that was developed for the growth of deliquescent halide single crystals because conventional μ-PD method does not allow growth of large bulk single crystals. Eu:SrI<inf>2</inf> crystals were grown from the melt of (Sr<inf>0.98</inf>Eu<inf>0.02</inf>)I<inf>2</inf> composition using carbon crucibles. Undoped μ-PD SrI<inf>2</inf> crystals were used as seeds that were affixed to the bottom of the crucible. All the preparations preceding the growths and the hot zone assembling were performed in a glove box with Ar gas. Then the removable chamber was taken out of the glove box, attached to the μ-PD system, connected with a Turbo Molecular pump, and evacuated down to 10<sup>−4</sup> Pa at ~300 °C. After the baking procedure, high purity Ar gas (6N) was injected into the chamber. The crucible was heated by a high frequency induction coil up to the melting point of Eu:SrI<inf>2</inf>. After melting the starting materials, the crucible was displaced in downward direction for the crystal growth and then cooled down to room temperature. Thus, 2 in. and crack-free Eu:SrI<inf>2</inf> bulk crystals were produced. The crystals had high transparency and did not contain any visible inclusions. The crystals were cut and polished in the glove box and then sealed in an aluminum container with an optical window for characterization. The details of the crystal growth are discussed.

    DOI: 10.1016/j.jcrysgro.2016.04.040

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  339. Growth of shape-controlled Ce:Y<sub>3</sub>Al<sub>5</sub>O<sub>12</sub> scintillator crystal and their scintillation properties

    Yokota, Y; Kurosawa, S; Ohasi, Y; Kamada, K; Yoshikawa, A

    JOURNAL OF CRYSTAL GROWTH   Vol. 452   page: 69 - 72   2016.10

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    A shape-controlled Ce doped Y<inf>3</inf>Al<inf>5</inf>O<inf>12</inf> (Ce:YAG) single crystal has been grown by a micro-pulling-down method using an Ir crucible with a square die. The as-grown Ce:YAG single crystal has square-shape and flat surfaces with high transparency. The shape-controlled Ce:YAG single crystal showed more than 70% transmittance from 530 nm to 900 nm without any cutting and polishing. An emission peak around 540 nm was observed in the radioluminescence spectrum under X-ray irradiation. In addition, the light yield and energy resolution under γ-ray irradiation of the as-grown crystal without any cutting and polishing were approximately 23,000 pH/MeV and 16%, respectively.

    DOI: 10.1016/j.jcrysgro.2016.02.041

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  340. Growth of N-benzyl-2-methyl-4-nitroaniline (BNA) single crystal fibers by micro-pulling down method

    Kamada, K; Takida, Y; Minamide, H; Shoji, Y; Kurosawa, S; Yokota, Y; Ohashi, Y; Yoshikawa, A

    JOURNAL OF CRYSTAL GROWTH   Vol. 452   page: 162 - 165   2016.10

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    N-benzyl-2-methyl-4-nitroaniline (BNA) fiber single crystals were grown by the micro-pulling down (µ-PD) method. Crucible material and its shape were selected based on wetting of the crucible material by liquid BNA. As a result, BNA fiber single crystal with about 1–2 mm diameter was successfully grown. Powder XRD analysis and X-ray rocking curve measurements were performed. Widely-tunable THz-wave generation from 4 THz to 14 THz was demonstrated using the BNA fiber crystal grown by µ-PD method.

    DOI: 10.1016/j.jcrysgro.2016.04.041

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  341. Luminescent properties of Cr-doped gallium garnet crystals grown by the micro-pulling-down method

    Kurosawa, S; Suzuki, A; Yamaji, A; Kamada, K; Pejchal, J; Ohashi, Y; Yokota, Y; Chani, VI; Yoshikawa, A

    JOURNAL OF CRYSTAL GROWTH   Vol. 452   page: 95 - 100   2016.10

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    Cr-doped (Gd<inf>x</inf>Y<inf>1−x</inf>)<inf>3</inf>Ga<inf>5</inf>O<inf>12</inf> crystals (x=0.00, 0.25, 0.50, 0.75 and 1.00) were grown by the micro-pulling-down method and examined for their possible application as red and infrared scintillating detectors in medical field. Although Cr:(Gd<inf>0.75</inf>Y<inf>0.25</inf>)<inf>3</inf>Ga<inf>5</inf>O<inf>12</inf> and Cr:Gd<inf>3</inf>Ga<inf>5</inf>O<inf>12</inf> had similar X-ray diffraction patterns, other samples showed some change in lattice constant. All the crystals had broad emission bands in the red and infrared region when excited by either 450 nm photons or X rays. These bands were associated with <sup>4</sup>T<inf>2</inf>→A<inf>2</inf> transitions. Moreover, redshift of the emission-peak wavelengths (<sup>4</sup>T<inf>2</inf>→<sup>4</sup>A<inf>2</inf>) and absorption peaks (<sup>4</sup>A<inf>2</inf>→<sup>4</sup>T<inf>1</inf> and <sup>4</sup>T<inf>2</inf>) was observed with increase of Gd content (x) in Cr-doped (Gd<inf>x</inf>Y<inf>1−x</inf>)<inf>3</inf>Ga<inf>5</inf>O<inf>12</inf> due to the change of the crystal fields. The crystals had scintillation emissions in the wavelength region suitable for the real time dose monitoring in radiation therapy.

    DOI: 10.1016/j.jcrysgro.2016.02.004

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  342. Pretransplantation Anti-CCR4 Antibody Mogamulizumab Against Adult T-Cell Leukemia/Lymphoma Is Associated With Significantly Increased Risks of Severe and Corticosteroid-Refractory Graft-Versus-Host Disease, Nonrelapse Mortality, and Overall Mortality

    Fuji, S; Inoue, Y; Utsunomiya, A; Moriuchi, Y; Uchimaru, K; Choi, I; Otsuka, E; Henzan, H; Kato, K; Tomoyose, T; Yamamoto, H; Kurosawa, S; Matsuoka, K; Yamaguchi, T; Fukuda, T

    JOURNAL OF CLINICAL ONCOLOGY   Vol. 34 ( 28 ) page: 3426 - +   2016.10

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    Purpose: Allogeneic hematopoietic stem-cell transplantation (allo-HSCT) is one important treatment option for patients with aggressive adult T-cell leukemia/lymphoma (ATLL). Mogamulizumab (anti-CCR4 monoclonal antibody; Mog) was recently approved as a treatment for ATLL in Japan. Major concerns exist about the possible adverse effects of pretransplantation Mog because Mog depletes regulatory T cells for several months. We assessed the impact of pretransplantation Mog on clinical outcomes after allo-HSCT. Patients and Methods: We included 996 allo-HSCT recipients age 70 years or younger with aggressive ATLL who were given the diagnosis between 2000 and 2013 and who received intensive chemotherapy by multiple chemotherapeutic drugs as first-line therapy. Before allo-HSCT, 82 patients received Mog with a median interval of 45 days from the last Mog to allo-HSCT. Results: Pretransplantation Mog was associated with an increased risk of grade 3 to 4 acute graft-versus-host disease (GVHD; relative risk, 1.80; P < .01) and refractoriness to systemic corticosteroid for acute GVHD (relative risk, 2.09; P < .01). One-year cumulative incidence of nonrelapse mortality was significantly higher in patients with pretransplantation Mog compared with those without (43.7% v 25.1%; P < .01). The probability of 1-year overall survival was also significantly inferior in patients with pretransplantation Mog compared with those without (32.3% v 49.4%; P < .01). In particular, use of Mog with intervals < 50 days to allo-HSCT was associated with a dismal clinical outcome. Conclusion: Pretransplantation Mog was significantly associated with an increased risk of GVHD-related mortality, which supports the relevance of CCR4-expressing Tregs after allo-HSCT in humans. In clinical practice, Mog should be cautiously used for patients with ATLL who are eligible for allo-HSCT.

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  343. Evaluation of Acoustic Properties for Ca<sub>3</sub>Nb(Ga<sub>0.7</sub> <sub>5</sub>Al<sub>0.25</sub>)<sub>3</sub>Si<sub>2</sub>O<sub>14</sub> Single Crystal Using the Ultrasonic Microspectroscopy System

    Ohashi, Y; Yokota, Y; Kudo, T; Kurosawa, S; Kamada, K; Yoshikawa, A

    IEEE TRANSACTIONS ON ULTRASONICS FERROELECTRICS AND FREQUENCY CONTROL   Vol. 63 ( 10 ) page: 1575 - 1580   2016.10

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    Acoustically related physical constants were experimentally determined for Ca<inf>3</inf>Nb(Ga<inf>0.75</inf>Al<inf>0.25</inf>)<inf>3</inf>Si<inf>2</inf>O<inf>14</inf> (CNGAS) single crystal for the first time. Several plate specimens of the X-, Y-, Z-, 40.24° Y-, and 144.98° Y-cut were prepared from a CNGAS single crystal ingot grown by Czochralski technique. Elastic constants, piezoelectric constants, and their temperature coefficients for CNGAS were determined from longitudinal wave and shear wave velocities at around room temperature, measured by the ultrasonic microspectroscopy system. Dielectric constants, density, and coefficients of thermal expansion were also measured. It was demonstrated that the determined constants could provide calculation accuracy within ±0.12% in leaky surface acoustic wave velocity. The piezoelectric constants for CNGAS were a 7.2% increase in e<inf>11</inf> and a 1.7% decrease in e<inf>14</inf> due to Al-substitution effect, compared with those of Ca<inf>3</inf>NbGa<inf>3</inf>Si<inf>2</inf>O<inf>14</inf>. The appropriate cut angle for thickness-shear mode resonator with zero temperature coefficient of velocity was estimated to be around 150° Y-cut from calculations using the determined constants of CNGAS exhibiting electromechanical coupling factor k<sup>2</sup> of 3.19% and power flow angle of -1.70°.

    DOI: 10.1109/TUFFC.2016.2573051

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  344. Late Mortality and Causes of Death among Long-Term Survivors after Allogeneic Stem Cell Transplantation Open Access

    Atsuta, Y; Hirakawa, A; Nakasone, H; Kurosawa, S; Oshima, K; Sakai, R; Ohashi, K; Takahashi, S; Mori, T; Ozawa, Y; Fukuda, T; Kanamori, H; Morishima, Y; Kato, K; Yabe, H; Sakamaki, H; Taniguchi, S; Yamashita, T

    BIOLOGY OF BLOOD AND MARROW TRANSPLANTATION   Vol. 22 ( 9 ) page: 1702 - 1709   2016.9

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    We sought to assess the late mortality risks and causes of death among long-term survivors of allogeneic hematopoietic stem cell transplantation (HCT). The cases of 11,047 relapse-free survivors of a first HCT at least 2 years after HCT were analyzed. Standardized mortality ratios (SMR) were calculated and specific causes of death were compared with those of the Japanese population. Among relapse-free survivors at 2 years, overall survival percentages at 10 and 15 years were 87% and 83%, respectively. The overall risk of mortality was significantly higher compared with that of the general population. The risk of mortality was significantly higher from infection (SMR = 57.0), new hematologic malignancies (SMR = 2.2), other new malignancies (SMR = 3.0), respiratory causes (SMR = 109.3), gastrointestinal causes (SMR = 3.8), liver dysfunction (SMR = 6.1), genitourinary dysfunction (SMR = 17.6), and external or accidental causes (SMR = 2.3). The overall annual mortality rate showed a steep decrease from 2 to 5 years after HCT; however, the decrease rate slowed after 10 years but was still higher than that of the general population at 20 years after HCT. SMRs in the earlier period of 2 to 4 years after HCT and 5 years or longer after HCT were 16.1 and 7.4, respectively. Long-term survivors after allogeneic HCT are at higher risk of mortality from various causes other than the underlying disease that led to HCT. Screening and preventive measures should be given a central role in reducing the morbidity and mortality of HCT recipients on long-term follow-up.

    DOI: 10.1016/j.bbmt.2016.05.019

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  345. Scintillation timing characteristics of (La,Gd)<sub>2</sub>Si<sub>2</sub>O<sub>7</sub>:Ce and Gd<sub>2</sub>SiO<sub>5</sub>:Ce single crystal scintillators: A comparative study

    Chewpraditkul, W; Sakthong, O; Chewpraditkul, W; Yawai, N; Szczesniak, T; Swiderski, L; Moszynski, M; Kurosawa, S; Murakami, R; Horiai, T; Yoshikawa, A; Nikl, M

    RADIATION MEASUREMENTS   Vol. 92   page: 49 - 53   2016.9

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    The scintillation timing characteristics of (La,Gd)<inf>2</inf>Si<inf>2</inf>O<inf>7</inf>:Ce (GPSLa23.5%:Ce) single crystal were studied and compared with Gd<inf>2</inf>SiO<inf>5</inf>:Ce (GSO:Ce) single crystal. The photoelectron yield, scintillation decay times and coincidence time resolution were measured. At 511 keV γ-rays, the photoelectron yield of 10,770 ± 500 phe MeV<sup>−1</sup> and energy resolution of 5.4 ± 0.2% obtained for GPSLa23.5%:Ce are much better than those of 3350 ± 160 phe MeV<sup>−1</sup> and 7.8 ± 0.3% obtained for GSO:Ce. The scintillation decay time profile was measured by the time-correlated single photon counting technique using a fast-slow coincidence setup. In both materials the comparable rise times of several nanoseconds are present. The fast component decay time of 56 ns with relative intensity of 49% obtained for GPSLa23.5%:Ce is inferior to that of 32 ns(88%) obtained for GSO:Ce. Consequently, the coincidence time resolution of GPSLa23.5%:Ce is slightly worse than that of GSO:Ce. The normalized time resolution was also discussed in terms of a number of photoelectrons and decay time of the scintillation pulse.

    DOI: 10.1016/j.radmeas.2016.06.008

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  346. Coronary artery bypass grafting in a patient with hemophilia B: continuous recombinant factor IX infusion as per the Japanese guidelines for replacement therapy

    Suzuki, T; Kawamoto, S; Kumagai, K; Adachi, O; Kanda, K; Ishikawa, M; Okitsu, Y; Harigae, H; Kurosawa, S; Saiki, Y

    GENERAL THORACIC AND CARDIOVASCULAR SURGERY   Vol. 64 ( 8 ) page: 481 - 483   2016.8

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    We herein report our experience of successfully managing the hemostatic system by controlling serum factor IX levels throughout the perioperative period in a patient with hemophilia B. Coronary artery bypass grafting with cardiopulmonary bypass was planned for a 52-year-old man with moderate severity of hemophilia B. During surgery, recombinant factor IX (rFIX; BeneFIX<sup>®</sup> Pfizer Japan inc., Tokyo, Japan) was administered by bolus infusion followed by continuous infusion as per the guidelines of the Japanese Society on Thrombosis and Hemostasis. The operative course was uneventful without any considerable bleeding or complications.

    DOI: 10.1007/s11748-014-0509-4

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  347. Crystal growth and luminescence properties of Yb<sub>2</sub>Si<sub>2</sub>O<sub>7</sub> infra-red emission scintillator

    Horiai, T; Kurosawa, S; Murakami, R; Pejchal, J; Yamaji, A; Shoji, Y; Chani, VI; Ohashi, Y; Kamada, K; Yokota, Y; Yoshikawa, A

    OPTICAL MATERIALS   Vol. 58   page: 14 - 17   2016.8

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    (Ce<inf>x</inf>Yb<inf>1-x</inf>)<inf>2</inf>Si<inf>2</inf>O<inf>7</inf> (x = 0.00, 0.01) single crystals were grown by the micro-pulling-down method to test the possibility of its application as infra-red scintillator for medical imaging. Powder X-ray diffraction analysis indicated that the crystals were single-phase materials. The radioluminescence spectra of the crystals demonstrated presence of two near infra-red emission peaks (at 1010 and 1030 nm). The emission peaks at 420 and 580 nm ascribed to defects were also observed in the crystals. The human body has maximum transmission in wavelength range from 650 to 1200 nm. Therefore, Yb<inf>2</inf>Si<inf>2</inf>O<inf>7</inf> is expected to be used as efficient infra-red scintillator for medical applications.

    DOI: 10.1016/j.optmat.2016.04.032

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  348. Growth and luminescence properties of Eu-doped HfO<sub>2</sub>/α-Al<sub>2</sub>O<sub>3</sub> eutectic scintillator Open Access

    Kamada, K; Hishinuma, K; Kurosawa, S; Yamaji, A; Shoji, Y; Pejchal, J; Ohashi, Y; Yokota, Y; Yoshikawa, A

    JOURNAL OF RARE EARTHS   Vol. 34 ( 8 ) page: 796 - 801   2016.8

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    HfO<inf>2</inf>/α-Al<inf>2</inf>O<inf>3</inf> eutectics were grown by the micro-pulling down (μ-PD) method at the composition of 63.2 mol.% α-Al<inf>2</inf>O<inf>3</inf>, 35.512 mol.% HfO<inf>2</inf>, 0.92 mol.% Eu<inf>2</inf>O<inf>3</inf> and 0.368 mol.% Y<inf>2</inf>O<inf>3</inf>. Rod phases with around 3–4 μm diameter were observed on the transverse cross-section. The phase-separated scintillator fibers (PSSFs) structure with fibers of around 3–4 μm diameter and 10–20 μm length was observed. The electron back scattering patterns indicated crystal orientation of [101] for monoclinic HfO<inf>2</inf> rod phase and [0001] for α-Al<inf>2</inf>O<inf>3</inf> matrix in the transverse cross-section. Eu<sup>3+</sup> 4f-4f emission was observed at 550–750 nm.

    DOI: 10.1016/S1002-0721(16)60096-0

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  349. Dependence of acoustic property on Al substitution for Ca<sub>3</sub>Ta(Ga<sub>1-<i>x</i></sub>Al<i><sub>x</sub></i>)<sub>3</sub>Si<sub>2</sub>O<sub>14</sub> single crystals

    Ohashi, Y; Arakawa, M; Kudo, T; Yokota, Y; Shoji, Y; Kurosawa, S; Kamada, K; Kushibiki, J; Yoshikawa, A

    JAPANESE JOURNAL OF APPLIED PHYSICS   Vol. 55 ( 7 )   2016.7

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    The acoustic properties of Ca<inf>3</inf>Ta(Ga<inf>1-x</inf>Al<inf>x</inf>)<inf>3</inf>Si<inf>2</inf>O<inf>14</inf> (CTGAS<inf>x</inf>) were experimentally studied as a function of the Al substitution content x in the ranges from x = 0 to 0.50. Five specimens, X-, Y-, Z-, 35°Y-, and 140°Y-cut, were prepared from each crystal of CTGAS<inf>x</inf> (x = 0, 0.25, and 0.50) grown by the Czochralski technique. Longitudinal wave and shear wave velocities for CTGAS<inf>x</inf> linearly increase with Al content for all propagation directions. Dielectric constants and density were measured and then elastic and piezoelectric constants were determined from the measured velocities for each crystal. The results revealed that all of the constants change linearly with Al content. From the relationship, the constants for CTAS (x = 1) were estimated. Calculations of the velocities using the determined constants also suggested that the maximum electromechanical coupling factor k<sup>2</sup> for the slow shear wave mode propagating along the rotated Y-axis direction of CTAS was improved to 4.42-compared with 3.83-for CTGS, owing to the Al substitution effect.

    DOI: 10.7567/JJAP.55.07KB06

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  350. Effects of Na and K co-doping on growth and scintillation properties of Eu:SrI<sub>2</sub> crystals Open Access

    Ito, T; Yokota, Y; Kurosawa, S; Kral, R; Pejchal, J; Ohashi, Y; Kamada, K; Nikl, M; Yoshikawa, A

    RADIATION MEASUREMENTS   Vol. 90   page: 157 - 161   2016.7

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    We grew Na and K co-doped Eu:SrI<inf>2</inf> [Na,Eu:SrI<inf>2</inf> and K,Eu:SrI<inf>2</inf>] crystals by a modified micro-pulling-down method to reveal the co-doping effects on the crystal growth and scintillation properties. The non-codoped, Na0.5%, Na1.0%, K0.5% and K1.0%,Eu:SrI<inf>2</inf> crystals indicated high transparency while the milky parts were generated in the Na5.0% and K5.0%,Eu:SrI<inf>2</inf> crystals. The light yields of Na,Eu:SrI<inf>2</inf> and K,Eu:SrI<inf>2</inf> crystals under γ-ray irradiation were decreased by the Na and K co-doping. On the other hand, there was a small change within 940–1020 ns in the decay times by the Na and K co-doping. In the light yield proportionality under γ-ray irradiation, the non-proportionality in the low energy region was improved by Na and K co-doping.

    DOI: 10.1016/j.radmeas.2016.01.025

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  351. Growth and radioluminescence of metal elements doped LiCaAlF<sub>6</sub> single crystals for neutron scintillator

    Tanaka, C; Yokota, Y; Kurosawa, S; Yamaji, A; Jary, V; Babin, V; Pejchal, J; Ohashi, Y; Kamada, K; Nikl, M; Yoshikawa, A

    RADIATION MEASUREMENTS   Vol. 90   page: 170 - 173   2016.7

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    The ns<sup>2</sup>-type metal elements (Pb and Sn) doped LiCaAlF<inf>6</inf> single crystals were grown by a micro-pulling-down (μ-PD) method. Pb doped LiCaAlF<inf>6</inf> [Pb:LiCAF] crystals showed high transparency and single phase of the LiCAF structure. However, we could not obtain Sn:LiCAF crystals due to the evaporation of SnF<inf>2</inf> during the crystal growth. There was an absorption peak around 193 nm in the transmittance spectrum of Pb:LiCAF crystal. In the radioluminescence spectrum of the Pb:LiCAF crystal under X-ray irradiation, two emission peaks around 200 and 830 nm were observed.

    DOI: 10.1016/j.radmeas.2016.02.021

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  352. Luminescence properties of the Mg co-doped Ce:SrHfO<sub>3</sub> ceramics prepared by the Spark Plasma Sintering Method

    Chiba, H; Kurosawa, S; Harata, K; Murakami, R; Yamaji, A; Ohashi, Y; Pejchal, J; Kamada, K; Yokota, Y; Yoshikawa, A

    RADIATION MEASUREMENTS   Vol. 90   page: 287 - 291   2016.7

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    1300 or 1400 °C pre–sintered Al/Ce/Mg:SrHfO<inf>3</inf> and Al/Ce:SrHfO<inf>3</inf> ceramics were prepared by the Spark Plasma Sintering (SPS) in order to search for a new scintillation material with a high–effective atomic number(Z<inf>eff</inf>) and good light output. The SrHfO<inf>3</inf> has a high Z<inf>eff</inf> of 60, and high gamma–ray detection efficiency is expected. Meanwhile it has a high melting point of over 2500 °C, and single crystal is hard to be grown. On the other hand, high melting materials can be prepared as ceramics, and the SPS method is a simple process to fabricate the ceramics within a few hours. Thus, we prepared the samples using the SPS method, and their optical and scintillation properties were investigated. We found that Al/Ce/Mg:SrHfO<inf>3</inf> and Al/Ce:SrHfO<inf>3</inf> ceramics had an emission wavelength at around 400 nm originating from 5d–4f transition of Ce<sup>3+</sup>. Moreover, Al/Ce/Mg:SrHfO<inf>3</inf> pre-sintered at a temperature of 1400 °C had a light output of approximately 5,000 ph/MeV. In this paper, the light output of Mg-co-doped samples was improved compared with the Mg-free ones. The light output also depends on the pre-sintering temperature.

    DOI: 10.1016/j.radmeas.2016.02.025

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  353. Optical and scintillation properties of Sr<sub>3</sub><i>B</i>Ga<sub>3</sub>Si<sub>2</sub>O<sub>14</sub> (<i>B</i> = Nb, Ta) single crystals

    Yokota, Y; Ito, T; Kurosawa, S; Ohashi, Y; Kamada, K; Yoshikawa, A

    RADIATION MEASUREMENTS   Vol. 90   page: 334 - 337   2016.7

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    Optical and scintillation properties of Sr<inf>3</inf>NbGa<inf>3</inf>Si<inf>2</inf>O<inf>14</inf> [SNGS] and Sr<inf>3</inf>TaGa<inf>3</inf>Si<inf>2</inf>O<inf>14</inf> [STGS] single crystals with the langasite-type crystal structure were investigated as a novel scintillator materials. In the transmittance spectra of the SNGS and STGS polished specimens, absorption peaks around 380 and 505 nm were observed and the absorptions are considered to be attributable to the excess oxygen in the crystals. An emission peak around 420 nm was observed in the X-ray radioluminescence spectrum of the SNGS crystal. On the other hand, there was an emission peak around 335 nm in the X-ray radioluminescence spectrum of the STGS crystal.

    DOI: 10.1016/j.radmeas.2015.12.026

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  354. Probing shallow electron traps in cerium-doped Gd<sub>3</sub>Al<sub>2</sub>Ga<sub>3</sub>O<sub>12</sub> scintillators by UV-induced absorption spectroscopy

    Kitaura, M; Kamada, K; Kurosawa, S; Azuma, J; Ohnishi, A; Yamaji, A; Hara, K

    APPLIED PHYSICS EXPRESS   Vol. 9 ( 7 )   2016.7

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    Publisher:Applied Physics Express  

    From measuring absorption spectra of cerium-doped Gd<inf>3</inf>Al<inf>2</inf>Ga<inf>3</inf>O<inf>12</inf> (Ce:GAGG) and undoped GAGG crystals at low temperatures under UV-light irradiation, we find that they exhibit a broad band at around 12000 cm%1. This band is enhanced by high-temperature annealing under a hydrogen atmosphere. On the basis of present experimental results, the UV-induced band is assigned to shallow electron traps of defect complexes associated with oxygen vacancies. The UV-induced band completely disappears with Mg2+ codoping. We conclude that the Mg2+ codoping has the effect of inhibiting the formation of shallow electron traps, which realizes a faster scintillation response of Ce:GAGG.

    DOI: 10.7567/APEX.9.072602

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  355. Scintillation properties of Zr co-doped Ce:(Gd, La)<sub>2</sub>Si<sub>2</sub>O<sub>7</sub> grown by the Czochralski process

    Murakami, R; Kurosawa, S; Shoji, Y; Jary, V; Ohashi, Y; Pejchal, J; Yokota, Y; Kamada, K; Nikl, M; Yoshikawa, A

    RADIATION MEASUREMENTS   Vol. 90   page: 162 - 165   2016.7

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    Publisher:Radiation Measurements  

    (Gd<inf>0.75</inf>,Ce<inf>0.015</inf>,La<inf>0.235</inf>)<inf>2</inf>Si<inf>2</inf>O<inf>7</inf> (Ce:La-GPS) single crystals co-doped with 0, 100, 200, 500 and 1000 ppm Zr were grown by the Czochralski process, and their scintillation properties were investigated. We investigated the co-doping effect of a stable tetravalent ion in Ce:La-GPS for the first time. The scintillation decay times in the faster component were shortened with increasing the Zr concentration. While the non-co-doped sample showed ∼63 ns day time, the Zr 100, 200, 500 and 1000 ppm co-doped samples showed ∼61, ∼59, ∼57, ∼54 ns, respectively. Additionally, light output, photon nonproportional response (PNR) and other optical properties were investigated.

    DOI: 10.1016/j.radmeas.2016.02.019

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  356. Association of Cumulative Steroid Dose with Risk of Infection after Treatment for Severe Acute Graft-versus-Host Disease Open Access

    Matsumura-Kimoto Y., Inamoto Y., Tajima K., Kawajiri A., Tanaka T., Hirakawa T., Ino K., Asao Y., Tamogami H., Kono C., Takeda W., Okinaka K., Fuji S., Kurosawa S., Kim S., Tanosaki R., Yamashita T., Fukuda T.

    Biology of Blood and Marrow Transplantation   Vol. 22 ( 6 ) page: 1102 - 1107   2016.6

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    This study aimed to characterize the incidence and risk factors of invasive fungal disease, cytomegalovirus infection, other viral diseases, and gram-negative rod infection after glucocorticoid treatment for severe acute graft-versus-host disease (GVHD) after allogeneic hematopoietic cell transplantation and to elucidate the associations of cumulative steroid dose with the risks of individual infections. The study cohort included 91 consecutive patients who developed maximum grades III and IV acute GVHD at our center. The mean cumulative prednisolone-equivalent dose was 41 mg/kg during the first 4 weeks. The cumulative incidence rates of fungal disease, cytomegalovirus disease, other viral diseases, and gram-negative rod infection at 6 months after glucocorticoid treatment were remarkably high, at 14%, 21%, 28%, and 20%, respectively. GVHD within 26 days after transplantation and low lymphocyte count at GVHD treatment were associated with increased risks of several infections. Cumulative prednisolone-equivalent steroid doses ≥ 55 mg/kg during the first 4 weeks were associated with an increased risk of fungal disease (hazard ratio, 3.65; P = .03) and cumulative doses ≥ 23 mg/kg were associated with an increased risk of non-cytomegalovirus viral diseases (hazard ratio, 4.14; P = .02). Strategies to reduce the risk of infectious complications are needed, particularly for patients who have risk factors and those who receive high cumulative steroid doses.

    DOI: 10.1016/j.bbmt.2016.02.020

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  357. Decision Analysis of Postremission Therapy in Cytogenetically Intermediate-Risk Acute Myeloid Leukemia: The Impact of <i>FLT3</i> Internal Tandem Duplication, Nucleophosmin, and CCAAT/Enhancer Binding Protein Alpha Open Access

    Kurosawa, S; Yamaguchi, H; Yamaguchi, T; Fukunaga, K; Yui, S; Wakita, S; Kanamori, H; Usuki, K; Uoshima, N; Yanada, M; Shono, K; Ueki, T; Mizuno, I; Yano, S; Takeuchi, J; Kanda, J; Okamura, H; Inamoto, Y; Inokuchi, K; Fukuda, T

    BIOLOGY OF BLOOD AND MARROW TRANSPLANTATION   Vol. 22 ( 6 ) page: 1125 - 1132   2016.6

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    We performed a decision analysis comparing allogeneic hematopoietic cell transplantation (allo-HCT) versus chemotherapy in first complete remission for patients with cytogenetically intermediate-risk acute myeloid leukemia, depending on the presence or absence of FLT3-internal tandem duplication (ITD), nucleophosmin (NPM1), and CCAAT/enhancer binding protein alpha (CEBPA) mutations. Adjusted means of the patient-reported EQ-5D index were used as quality-of-life (QOL) estimates. In 332 patients for which FLT3-ITD status was available, FLT3-ITD was present in 60. In 272 patients without FLT3-ITD, NPM1 mutations were present in 83. CEBPA biallelic mutations were detected in 53 patients. For patients harboring FLT3-ITD, allo-HCT improved life expectancy (LE) (52 versus 32 months during 10-year observation) and QOL-adjusted life expectancy (QALE, 36 versus 21). Monte-Carlo simulation identified allo-HCT as the favored strategy in 100% of simulations. In patients without FLT3-ITD, allo-HCT improved LE/QALE with or without NPM1 mutations. However, sensitivity analyses showed that the results were not robust enough. For patients harboring CEBPA biallelic mutations, chemotherapy was favored (LE, 53 versus 84; QALE, 37 versus 59), whereas, for patients with monoallelic mutations or wild-type CEBPA, allo-HCT was favored (LE, 68 versus 54; QALE, 48 versus 37). Sensitivity analyses did not change the results in either group. In conclusion, based on a Markov decision analysis, allo-HCT was a favored postremission strategy in patients with FLT3-ITD, and chemotherapy was favored in patients with biallelic CEBPA mutations. A prospective study is warranted to determine the value of allo-HCT, especially in FLT3-ITD-negative patients.

    DOI: 10.1016/j.bbmt.2016.03.015

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  358. PRETRANSPLANT ANTI-CCR4 ANTIBODY AGAINST ADULT T CELL LEUKEMIA/LYMPHOMA WAS ASSOCIATED WITH SIGNIFICANTLY INCREASED RISKS OF SEVERE/STEROID-REFRACTORY GVHD, NON-RELAPSE MORTALITY AND OVERALL MORTALITY

    Fuji, S; Inoue, Y; Utsunomiya, A; Moriuchi, Y; Uchimaru, K; Choi, I; Otsuka, E; Henzan, H; Kato, K; Tomoyose, T; Yamamoto, H; Kurosawa, S; Matsuoka, KI; Yamaguchi, T; Fukuda, T

    HAEMATOLOGICA   Vol. 101   page: 330 - 330   2016.6

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  359. Growth and Luminescence Properties of Eu : SrI<sub>2</sub> Single Crystals Prepared by Modified Micro-Pulling-Down Method

    Král, R; Jary, V; Pejchal, J; Kurosawa, S; Nitsch, K; Yokota, Y; Nikl, M; Yoshikawa, A

    IEEE TRANSACTIONS ON NUCLEAR SCIENCE   Vol. 63 ( 2 ) page: 453 - 458   2016.4

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    Publisher:IEEE Transactions on Nuclear Science  

    This paper reports on the preparation and growth of Eu-doped strontium iodide (SrI<inf>2</inf>) single crystals by modified micro-pulling-down method. Influence of the Eu<sup>2+</sup> and Eu<sup>3+</sup> (introduced in form of EuI<inf>2</inf> and EuCl<inf>3</inf>) on the luminescence and scintillation properties is analyzed. Sufficient optical quality of prepared single crystals was obtained allowing further characterization of their absorption, radio- and photoluminescence spectra. Photoluminescence and scintillation decay time of grown SrI<inf>2</inf> crystals irradiated under γ-ray source were evaluated as well.

    DOI: 10.1109/TNS.2015.2514058

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  360. Growth of 1.5-In Eu : SrI<sub>2</sub> Single Crystal and Scintillation Properties

    Yokota, Y; Ito, T; Yasuhiro, S; Kurosawa, S; Ohashi, Y; Kamada, K; Yoshikawa, A

    IEEE TRANSACTIONS ON NUCLEAR SCIENCE   Vol. 63 ( 2 ) page: 467 - 470   2016.4

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    We grew 1.5-in Eu doped SrI<inf>2</inf> (Eu:SrI<inf>2</inf>) bulk single crystal by a modified vertical Bridgman (VB) method using a removable chamber and high-frequency induction heating. As-grown 1.5-in Eu:SrI<inf>2</inf> bulk single crystal had no visible crack and inclusion in the crystal. In the transmittance and α-ray radioluminescence spectra, large absorption below 433 nm and emission peak at 433 nm were observed, respectively. Each polished Eu:SrI<inf>2</inf> specimen indicated 56 000 ∼ 62 000 ph/MeV light yield and 3.3 ∼ 3.9% energy resolution. The decay times of the specimens were 0.61 ∼ 0.67 μs.

    DOI: 10.1109/TNS.2016.2527745

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  361. Large Size Czochralski Growth and Scintillation Properties of Mg<SUP>2+</SUP> Co-doped Ce : Gd<sub>3</sub>Ga<sub>3</sub>Al<sub>2</sub>O<sub>12</sub> Open Access

    Kamada, K; Shoji, Y; Kochurikhin, VV; Nagura, A; Okumura, S; Yamamoto, S; Yeom, JY; Kurosawa, S; Pejchal, J; Yokota, Y; Ohashi, Y; Nikl, M; Yoshino, M; Yoshikawa, A

    IEEE TRANSACTIONS ON NUCLEAR SCIENCE   Vol. 63 ( 2 ) page: 443 - 447   2016.4

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    The 3 inch size Mg co-doped Ce : Gd<inf>3</inf>Al<inf>2</inf>Ga<inf>3</inf> O<inf>12</inf> single crystals were prepared by the Czochralski (Cz) method. Absorption and luminescence spectra were measured together with several other scintillation characteristics, namely the scintillation decay and light yield to reveal the effect of Mg co-doping. The timing resolution measurement for a pair of 3 × 3 × 3 mm<sup>3</sup> size GAGG:Ce.Mg scintillator crystals was performed using Si-PMs.

    DOI: 10.1109/TNS.2016.2521399

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  362. Single Crystal Growth of Cerium and Praseodymium Doped YCa<sub>4</sub>O(BO<sub>3</sub>)<sub>3</sub> Scintillator by Micro-Pulling Down Method Open Access

    Kamada, K; Kurosawa, S; Yokota, Y; Pejchal, J; Ohashi, Y; Yoshino, M; Yoshikawa, A

    IEEE TRANSACTIONS ON NUCLEAR SCIENCE   Vol. 63 ( 2 ) page: 486 - 489   2016.4

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    Ce and Pr doped YCOB single crystals were grown by the micro-pulling down (μ-PD) method and characterized as for the structure and chemical composition. The expected 420 nm emission of Ce<sup>3+</sup> 4f-5d has been observed in Ce:YCOB. Pr:YCOB shows broad emission spectrum peaking around 350 nm and this emission can be well ascribed to the 5d-4f emission of Pr<sup>3+</sup>. Luminescence and scintillation characteristics of these crystals were also investigated.

    DOI: 10.1109/TNS.2016.2521402

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  363. The Stable Ce<SUP>4+</SUP> Center: A New Tool to Optimize Ce-Doped Oxide Scintillators Open Access

    Nikl, M; Babin, V; Pejchal, J; Laguta, VV; Buryi, M; Mares, JA; Kamada, K; Kurosawa, S; Yoshikawa, A; Panek, D; Parkman, T; Bruza, P; Mann, K; Müller, M

    IEEE TRANSACTIONS ON NUCLEAR SCIENCE   Vol. 63 ( 2 ) page: 433 - 438   2016.4

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    Publisher:IEEE Transactions on Nuclear Science  

    The role and effect of stable Ce<sup>4+</sup> centers in Ce-doped LuAG single crystal scintillator is further studied by means of measurements of several optical, luminescence and scintillation characteristics. Two LuAG:Ce single crystal samples are compared: in one of them the dominating Ce<sup>4+</sup> center is stabilized by high concentration Mg<sup>2+</sup> codoping while the other one shows only the presence of stable Ce<sup>3+</sup> center. Tailored (Eu, Mg)-doped LuAG single crystal is also prepared to test the presence and thermal stability of hole traps in the host which affect the timing characteristics of Ce<sup>4+</sup> scintillation cycle, namely its restoration back to 4+ charge state in last step of the cycle. EPR experiment was also employed at Mg-and (Eu, Mg) doped LuAG samples and the signature of the O<sup>-</sup> hole center stabilized by Mg<sup>2+</sup> ion was clearly obtained.

    DOI: 10.1109/TNS.2015.2495119

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  364. A prospective multicenter study of unrelated bone marrow transplants using a reduced-intensity conditioning regimen with low-dose ATG-F

    Fuji, S; Kim, SW; Yano, S; Hagiwara, S; Nakamae, H; Hidaka, M; Ito, T; Ohashi, K; Hatanaka, K; Takami, A; Kurosawa, S; Yamashita, T; Yamaguchi, T; Fukuda, T

    BONE MARROW TRANSPLANTATION   Vol. 51 ( 3 ) page: 451 - 453   2016.3

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    DOI: 10.1038/bmt.2015.268

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  365. Luminescence and scintillation properties of Lu<sub>3</sub>Al<sub>5</sub>O<sub>12</sub> nanoceramics sintered by SPS method

    Pejchal, J; Babin, V; Beitlerova, A; Kucerkova, R; Panek, D; Barta, J; Cuba, V; Yamaji, A; Kurosawa, S; Mihokova, E; Ito, A; Goto, T; Nikl, M; Yoshikawa, A

    OPTICAL MATERIALS   Vol. 53   page: 54 - 63   2016.3

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    Publisher:Optical Materials  

    Ce-doped lutetium aluminum garnet Lu<inf>3</inf>Al<inf>5</inf>O<inf>12</inf> (LuAG) nanoceramics were fabricated at 1600°C and 1700°C by spark-plasma sintering (SPS) method from nano-powders prepared by radiation synthesis. Both undoped and Ce-doped LuAG ceramic samples were also prepared from the nano-powders at 1700°C with significantly increased pre-heating rate. The backscattered electron images revealed large amount of pores in all the Ce-doped samples causing their significant opacity. On the other hand, very large grains and no pores were revealed in the undoped sample, which was the only transparent one. The radioluminescence measurements revealed superior overall scintillation efficiency of the samples sintered at the temperature 1700°C, and their defect emission in the UV region was ascribed to oxygen-vacancy-related defects such as F<sup>+</sup> centers. The photoluminescence decay of the defect emission was characterized by an extremely fast decay time of a few nanoseconds. Influence of sintering procedure and subsequent annealing on the luminescence and scintillation properties is discussed.

    DOI: 10.1016/j.optmat.2016.01.024

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  366. Nationwide Survey of Aggressive Adult T-Cell Leukemia/Lymphoma to Compare the Clinical Outcome Between Non-Transplanted and Transplanted Patients Open Access

    Fuji, S; Inoue, Y; Utsunomiya, A; Moriuchi, Y; Uchimaru, K; Hanada, S; Miyagi, T; Taguchi, J; Choi, I; Otsuka, E; Tomoyose, T; Yamamoto, H; Kurosawa, S; Yamaguchi, T; Fukuda, T

    BIOLOGY OF BLOOD AND MARROW TRANSPLANTATION   Vol. 22 ( 3 ) page: S39 - S39   2016.3

  367. Qualitative Analysis of Patient-Reported Free Comments on Quality of Life in Patients Who Completed Treatment for Acute Leukemia Open Access

    Mori, A; Tsukagoshi, M; Kurosawa, S; Mori, T; Kanamori, H; Onishi, Y; Emi, N; Fujisawa, S; Kohno, A; Nakaseko, C; Saito, B; Kondo, T; Hino, M; Nawa, Y; Kato, S; Hashimoto, A; Inamoto, Y; Fukuda, T

    BIOLOGY OF BLOOD AND MARROW TRANSPLANTATION   Vol. 22 ( 3 ) page: S454 - S455   2016.3

  368. BiI<sub>3</sub> single crystal for room-temperature gamma ray detectors

    Saito, T; Iwasaki, T; Kurosawa, S; Yoshikawa, A; Den, T

    NUCLEAR INSTRUMENTS & METHODS IN PHYSICS RESEARCH SECTION A-ACCELERATORS SPECTROMETERS DETECTORS AND ASSOCIATED EQUIPMENT   Vol. 806   page: 395 - 400   2016.1

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    Publisher:Nuclear Instruments and Methods in Physics Research Section A Accelerators Spectrometers Detectors and Associated Equipment  

    BiI<inf>3</inf> single crystals were grown by the physical vapor transport method. The repeated sublimation of the starting material reduced impurities in the BiI<inf>3</inf> single crystal to sub-ppm levels. The detector was fabricated by depositing Au electrodes on both surfaces of the 100-μm-thick BiI<inf>3</inf> single crystal platelet. The resistivity of the BiI<inf>3</inf> single crystal was increased by post-annealing in an iodine atmosphere (ρ=1.6×10<sup>11</sup> Ω cm). Pulse height spectroscopy measurements showed clear peaks in the energy spectrum of alpha particles or gamma rays. It was estimated that the mobility-lifetime product was μ<inf>e</inf>τ<inf>e</inf>=3.4-8.5×10<sup>-6</sup> cm<sup>2</sup>/V and the electron-hole pair creation energy was 5.8 eV. Our results show that BiI<inf>3</inf> single crystals are promising candidates for detectors used in radiographic imaging or gamma ray spectroscopy.

    DOI: 10.1016/j.nima.2015.10.036

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  369. Crystal growth and scintillation properties of multi-component oxide single crystals: Ce:GGAG and Ce:La-GPS

    Yoshikawa, A; Kamada, K; Kurosawa, S; Shoji, Y; Yokota, Y; Chani, VI; Nikl, M

    JOURNAL OF LUMINESCENCE   Vol. 169   page: 387 - 393   2016.1

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    Publisher:Journal of Luminescence  

    Crystal growth by micro-pulling-down, Czochralski, and floating zone methods and scintillation properties of Ce:Gd<inf>3</inf>(Ga,Al)<inf>5</inf>O<inf>12</inf> (Ce:GGAG) multi-component oxide garnets, and Ce:Gd<inf>2</inf>Si<inf>2</inf>O<inf>7</inf> (Ce:GPS) or Ce:(La,Gd)<inf>2</inf>Si<inf>2</inf>O<inf>7</inf> (Ce:La-GPS) pyro-silicates are reviewed. GGAG crystals demonstrated practically linear dependences of some of the parameters including lattice constant, emission wavelength, and band gap on Ga content. However, emission intensity, light yield and energy resolution showed maxima for intermediate compositions. GGAG crystals had the highest light yield of 56,000 photon/MeV for Ga content of 2.7 atoms per garnet formula unit. Similarly the light yield and energy resolution of La-GPS showed the highest values of 40,000 photon/MeV and 4.4%@662 keV, respectively, for La-GPS containing 10% of La. Moreover, La-GPS demonstrated stable scintillation performance up to 200°C.

    DOI: 10.1016/j.jlumin.2015.04.001

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  370. Growth and scintillation properties of praseodymium doped (Lu,Gd)<sub>3</sub>(Ga,Al)<sub>5</sub>O<sub>12</sub> single crystals

    Kamada, K; Nikl, M; Kurosawa, S; Shoji, Y; Pejchal, J; Ohashi, Y; Yokota, Y; Yoshikawa, A

    JOURNAL OF LUMINESCENCE   Vol. 169   page: 811 - 815   2016.1

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    Pr doped (Lu,Gd)<inf>3</inf>(Ga,Al)<inf>5</inf>O<inf>12</inf> single crystals were grown by the micro-pulling down (μ-PD) method. The crystals were greenish and transparent with 3.0 mm in diameter, 10-30 mm in length. Neither visible inclusions nor cracks were observed. Luminescence and scintillation properties were measured. The substitution at the Al<sup>3+</sup> sites by Ga<sup>3+</sup> in garnet structure has been studied. The Pr<sup>3+</sup> 5d-4f emission is observed within 300-380 nm wavelength superposed with 312 nm emission line of Gd<sup>3+</sup>. Pr0.2%:Lu<inf>2.5</inf>Gd<inf>1</inf>Ga<inf>3</inf>Al<inf>2</inf>O<inf>12</inf> shows highest emission intensity. The light yield of Pr0.2%:Lu<inf>2.5</inf>Gd<inf>0.5</inf>Ga<inf>2</inf>Al<inf>3</inf>O<inf>12</inf> sample with diameter 3 mm×1 mm size was around 8000 ph/MeV. Two-exponential approximations of scintillation decay showed 39.6 ns (30.6%) and 151 ns (69.4%) decay times.

    DOI: 10.1016/j.jlumin.2015.05.057

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  371. Luminescence mechanism in doubly Gd, Nd-codoped fluoride crystals for VUV scintillators

    Pejchal, J; Fukuda, K; Babin, V; Kurosawa, S; Yokota, Y; Yoshikawa, A; Nikl, M

    JOURNAL OF LUMINESCENCE   Vol. 169   page: 682 - 689   2016.1

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    The Nd-doped, Gd-doped and doubly Nd, Gd-codoped BaLu<inf>1.2</inf>Y<inf>0.8</inf>F<inf>8</inf> (BaLuYF) and LuF<inf>3</inf> single crystals were grown by a micro-pulling-down method. Their photoluminescence, radioluminescence and alpha-ray-excited pulse-height spectra were studied in the vacuum-ultra-violet (VUV) region to confirm their possible application as fast VUV scintillators. Complementary photoluminescence measurements in the ultra-violet/visible spectral region were performed as well. The possibility of scintillation performance improvement by Gd codoping was tested. The overall scintillation efficiency of BaLuYF:Nd1% was comparable to that of the LaF<inf>3</inf>:Nd8% reference sample and only slight improvement was observed after Gd1% codoping. The positive effect of Gd codoping was confirmed for higher dopant concentrations. This was explained by an energy transfer from the high-energy Gd<sup>3+</sup> 4f <sup>2</sup>G(0)<inf>7/2</inf> level to the Nd<sup>3+</sup> 5d state. On the other hand, pulse-height spectra showed degradation of the light yield under alpha-ray excitation, which was explained by introduction of slow components due to Gd codoping. On the other hand, no positive effect of Gd codoping was found for the overall scintillation efficiency of Nd-doped LuF<inf>3</inf>, despite the same energy transfer process was confirmed. Slight improvement of the light yield under alpha-ray excitation was confirmed.

    DOI: 10.1016/j.jlumin.2015.04.008

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  372. The role of cerium variable charge state in the luminescence and scintillation mechanism in complex oxide scintillators: The effect of air annealing

    Nikl, M; Babin, V; Mares, JA; Kamada, K; Kurosawa, S; Yoshikawa, A; Tous, J; Houzvicka, J; Blazek, K

    JOURNAL OF LUMINESCENCE   Vol. 169   page: 539 - 543   2016.1

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    Publisher:Journal of Luminescence  

    The influence of annealing in air at elevated temperatures on the absorption, luminescence and scintillation characteristics was studied for a set of Ce-doped aluminum garnet and perovskite single crystals. Positive effects consisting mainly in increase of light yield and decrease of afterglow were found to varying extent in all the materials. It is explained by the positive role of created stable Ce<sup>4+</sup> center in scintillation mechanism and by decrease of deep trap concentration based on oxygen vacancies.

    DOI: 10.1016/j.jlumin.2015.01.008

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  373. A prototype of aerial radiation monitoring system using an unmanned helicopter mounting a GAGG scintillator Compton camera

    Jiang, JY; Shimazoe, K; Nakamura, Y; Takahashi, H; Shikaze, Y; Nishizawa, Y; Yoshida, M; Sanada, Y; Torii, T; Yoshino, M; Ito, S; Endo, T; Tsutsumi, K; Kato, S; Sato, H; Usuki, Y; Kurosawa, S; Kamada, K; Yoshikawa, A

    JOURNAL OF NUCLEAR SCIENCE AND TECHNOLOGY   Vol. 53 ( 7 ) page: 1067 - 1075   2016

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    Publisher:Journal of Nuclear Science and Technology  

    Due to the accident of Fukushima Daiichi Nuclear Power Plant, some areas were contaminated by released radioisotopes (mainly <sup>1</sup><sup>3</sup><sup>7</sup>Cs and <sup>1</sup><sup>3</sup><sup>4</sup>Cs). Effective decontamination is demanded to encourage evacuated people to return. This paper proposes a new survey system using an unmanned helicopter equipped with a Compton camera for localizing radionuclides. As a prototype, 32 Ce:Gd<inf>3</inf>(Al,Ga)<inf>5</inf>O<inf>1</inf><inf>2</inf> (GAGG) crystals were coupled to 16 silicon photomultipliers and 16 avalanched photodiodes as the scatterer and absorber, respectively. A new Dynamic Time-over-Threshold (dToT) method was applied to convert CR-RC shaping signals to digital signals for multi-channel spectra and coincidence acquisition. The system was designed to work in two modes: one is Compton-camera mode (CCM) which obtains the radiation distribution maps through Compton imaging using hovering flights, while the other one is Gamma-camera mode (GCM) which maps the radiation distribution via measured coincidence events using programmed flights. For point source in CCM, an intrinsic efficiency of 1.68% with a combined standard uncertainty of 0.04% and an angular resolution of about 14° (FWHM, full width at half maximum) was achieved. In GCM, a spatial resolution of about 11 cm (FWHM) was obtained when detecting area is 11.2 cm away from the detector, while it was about 28 cm (FWHM) in single detector mode (SDM). Promising results were obtained in field in Fukushima.

    DOI: 10.1080/00223131.2015.1089796

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  374. Al Content Dependence of Acoustic Properties for Ca<sub>3</sub>Nb(Ga<sub>1-x</sub>Al<sub>x</sub>)<sub>3</sub>Si<sub>2</sub>O<sub>14</sub> Single Crystals

    Ohashi, Y; Arakawa, M; Yokota, Y; Inoue, K; Yamaji, A; Kurosawa, S; Kamada, K; Yoshikawa, A

    2016 IEEE INTERNATIONAL ULTRASONICS SYMPOSIUM (IUS)     2016

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  375. Clinical characteristics and prognosis of acute myeloid leukemia associated with DNA-methylation regulatory gene mutations Open Access

    Ryotokuji T., Yamaguchi H., Ueki T., Usuki K., Kurosawa S., Kobayashi Y., Kawata E., Tajika K., Gomi S., Kanda J., Kobayashi A., Omori I., Marumo A., Fujiwara Y., Yui S., Terada K., Fukunaga K., Hirakawa T., Arai K., Kitano T., Kosaka F., Tamai H., Nakayama K., Wakita S., Fukuda T., Inokuchi K.

    Haematologica   Vol. 101 ( 9 ) page: 1074 - 1081   2016

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    Publisher:Haematologica  

    In recent years, it has been reported that the frequency of DNAmethylation regulatory gene mutations - mutations of the genes that regulate gene expression through DNA methylation - is high in acute myeloid leukemia. The objective of the present study was to elucidate the clinical characteristics and prognosis of acute myeloid leukemia with associated DNA-methylation regulatory gene mutation. We studied 308 patients with acute myeloid leukemia. DNA-methylation regulatory gene mutations were observed in 135 of the 308 cases (43.8%). Acute myeloid leukemia associated with a DNA-methylation regulatory gene mutation was more frequent in older patients (P<0.0001) and in patients with intermediate cytogenetic risk (P<0.0001) accompanied by a high white blood cell count (P=0.0032). DNA-methylation regulatory gene mutation was an unfavorable prognostic factor for overall survival in the whole cohort (P=0.0018), in patients aged ≤70 years, in patients with intermediate cytogenetic risk, and in FLT3-ITD-negative patients (P=0.0409). Among the patients with DNA-methylation regulatory gene mutations, 26.7% were found to have two or more such mutations and prognosis worsened with increasing number of mutations. In multivariate analysis DNA-methylation regulatory gene mutation was an independent unfavorable prognostic factor for overall survival (P=0.0424). However, patients with a DNA-methylation regulatory gene mutation who underwent allogeneic stem cell transplantation in first remission had a significantly better prognosis than those who did not undergo such transplantation (P=0.0254). Our study establishes that DNA-methylation regulatory gene mutation is an important unfavorable prognostic factor in acute myeloid leukemia.

    DOI: 10.3324/haematol.2016.143073

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  376. Field test around Fukushima Daiichi nuclear power plant site using improved Ce:Gd<sub>3</sub>(Al,Ga)<sub>5</sub>O<sub>12</sub> scintillator Compton camera mounted on an unmanned helicopter Open Access

    Shikaze, Y; Nishizawa, Y; Sanada, Y; Torii, T; Jiang, JY; Shimazoe, K; Takahashi, H; Yoshino, M; Ito, S; Endo, T; Tsutsumi, K; Kato, S; Sato, H; Usuki, Y; Kurosawa, S; Kamada, K; Yoshikawa, A

    JOURNAL OF NUCLEAR SCIENCE AND TECHNOLOGY   Vol. 53 ( 12 ) page: 1907 - 1918   2016

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    Publisher:Journal of Nuclear Science and Technology  

    An improved light-weight Compton camera exhibiting low power consumption was developed to be mountable on an unmanned helicopter to detect cesium radiation hot spots and confirm the decontamination effect of cesium-affected areas. An increase in the Ce:Gd<inf>3</inf>(Al,Ga)<inf>5</inf>O<inf>12</inf> scintillator array from 4 × 4 to 8 × 8 and expansion of the interlayer distance enhanced the detection efficiency and angular resolution, respectively. Measurements were performed over the Ukedo riverbed in Namie, Fukushima Prefecture (Japan). The helicopter's flight path and speed were pre-programmed to lines interspaced by 5 and 10 m intervals and 1 m/s, respectively, facilitating measurements over areas of 65 × 60 m<sup>2</sup> and 65 × 180 m<sup>2</sup> at a height of 10 m for approximately 20 and 30 min, respectively. Results provided accurate ambient dose equivalent rate maps at a height of 1 m with an angular resolution corresponding to a position resolution of approximately 10 m from a height of 10 m. Hovering flights were executed over hot-spot areas for 10–20 min at a height of 5–20 m. Gamma-ray images of these hot spots were obtained using a reconstruction software. Comparison between position-shifted measurement results showed that the angular resolution coincided with that evaluated in the laboratory (approximately 10°).

    DOI: 10.1080/00223131.2016.1185980

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  377. MeV gamma-ray observation with a well-defined point spread function based on electron tracking

    Takada, A; Tanimori, T; Kubo, H; Mizumoto, T; Mizumura, Y; Komura, S; Kishimoto, T; Takemura, T; Yoshikawa, K; Nakamasu, Y; Matsuoka, Y; Oda, M; Miyamoto, S; Sonoda, S; Tomono, D; Miuchi, K; Kurosawa, S; Sawano, T

    SPACE TELESCOPES AND INSTRUMENTATION 2016: ULTRAVIOLET TO GAMMA RAY   Vol. 9905   2016

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    Publisher:Proceedings of SPIE the International Society for Optical Engineering  

    The field of MeV gamma-ray astronomy has not opened up until recently owing to imaging difficulties. Compton telescopes and coded-aperture imaging cameras are used as conventional MeV gamma-ray telescopes; however their observations are obstructed by huge background, leading to uncertainty of the point spread function (PSF). Conventional MeV gamma-ray telescopes imaging utilize optimizing algorithms such as the ML-EM method, making it difficult to define the correct PSF, which is the uncertainty of a gamma-ray image on the celestial sphere. Recently, we have defined and evaluated the PSF of an electron-tracking Compton camera (ETCC) and a conventional Compton telescope, and thereby obtained an important result: The PSF strongly depends on the precision of the recoil direction of electron (scatter plane deviation, SPD) and is not equal to the angular resolution measure (ARM). Now, we are constructing a 30 cm-cubic ETCC for a second balloon experiment, Sub-MeV gamma ray Imaging Loaded-on-balloon Experiment: SMILE-II. The current ETCC has an effective area of ∼1 cm<sup>2</sup> at 300 keV, a PSF of ∼10° at FWHM for 662 keV, and a large field of view of ∼3 sr. We will upgrade this ETCC to have an effective area of several cm<sup>2</sup> and a PSF of ∼5° using a CF<inf>4</inf>-based gas. Using the upgraded ETCC, our observation plan for SMILE-II is to map of the electron-positron annihilation line and the 1.8 MeV line from <sup>26</sup>Al. In this paper, we will report on the current performance of the ETCC and on our observation plan.

    DOI: 10.1117/12.2232171

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  378. Radiation Hardness of Ce:(Gd, La)2Si2O7 Scintillator Using 80-MeV Alpha Rays Open Access

    Kurosawa S., Murakami R., Yamaji A., Shoji Y., Pejchal J., Ohashi Y., Yokota Y., Kamada K., Yoshikawa A.

    Proceedings of International Symposium on Radiation Detectors and their Uses Isrd 2016     2016

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    Publisher:Proceedings of International Symposium on Radiation Detectors and their Uses Isrd 2016  

    Ce-doped (Gd, La)<inf>2</inf>Si<inf>2</inf>O<inf>7</inf> scintillator has a high light output, fast decay time, and it has been expected to be applied in various fields. One of the applications is to use in the space for astronomy, and therefore, the evaluation of the radiation hardness is required. We grew a Ce-doped (Gd, La)<inf>2</inf>Si<inf>2</inf>O<inf>7</inf> single crystal by the Czochralski technique, and evaluated its radiation hardness using 80-MeV alpha rays in Tohoku University with a total dose of approximately 20,000 Gy. The light outputs and decay times were slightly degraded after the irradiation by few %. Only the energy resolution was degraded dramatically in the 80-MeV alpha-ray range, and Ce-doped (Gd, La)<inf>2</inf>Si<inf>2</inf>O<inf>7</inf> scintillator was found to have good radiation hardness for alpha rays.

    DOI: 10.7566/JPSCP.11.020002

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  379. Temperature Dependence of Luminescence Properties for Zr codoped Ce:(Gd, La)2Si2O7 Scintillator Open Access

    Horiai T., Kurosawa S., Murakami R., Jary V., Yamaji A., Shoji Y., Ohashi Y., Pejchal J., Kamada K., Yokota Y., Nikl M., Yoshikawa A.

    Proceedings of International Symposium on Radiation Detectors and their Uses Isrd 2016     2016

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    Publisher:Proceedings of International Symposium on Radiation Detectors and their Uses Isrd 2016  

    Since Ce-doped (Gd, La)<inf>2</inf>Si<inf>2</inf>O<inf>7</inf> scintillator was reported to have high light output, fast decay time and good temperature stability of the scintillation properties, it was expected to find application in various fields. In this study, we evaluated Zr codoping effect by measuring temperature dependence of photoluminescence and scintillation characteristics. The single crystals were grown by Czochralski technique and the light output at 448 K was around 80% of that at 298 K.

    DOI: 10.7566/JPSCP.11.020007

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  380. Growth of shape-controlled single crystals and effects of Al substitution on langasite-type piezoelectric single crystals with ordered structure

    Yokota Yuui, Kamada Kei, Shoji Yasuhiro, Kurosawa Shunsuke, Yoshikawa Akira, Ohashi Yuji

    Journal of the Japanese Association for Crystal Growth   Vol. 43 ( 3 ) page: 139 - 147   2016

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    Language:Japanese   Publisher:The Japanese Association for Crystal Growth  

    <p>  Shape-controlled langasite-type piezoelectric single crystals have been developed by the micro-pulling-down (μ-PD) method using specially designed Pt-Rh-Au crucibles with suitable wetting to the melt of langasite-type materials. The shape-controlled langasite-type piezoelectric single crystals indicated the comparable piezoelectric properties to the crystals grown by the conventional methods.</p><p>  Ca<sub>3</sub>Nb(Ga<sub>1-</sub><i><sub>x</sub></i>Al<i><sub>x</sub></i>)<sub>3</sub>Si<sub>2</sub>O<sub>14</sub> (CNGAS) and Ca<sub>3</sub>Ta(Ga<sub>1-</sub><i><sub>x</sub></i>Al<i><sub>x</sub></i>)<sub>3</sub>Si<sub>2</sub>O<sub>14</sub> (CTGAS) single crystals have been developed and the effects of Al substitution on their crystal growth, phase formation and piezoelectric properties were revealed. CNGAS and CTGAS single crystals could be grown by the μ-PD method in the range of 0 ≤ <i>x</i> ≤ 0.6 and 0 ≤ <i>x</i> ≤ 1, respectively. Piezoelectric properties of the CNGAS and CTGAS bulk single crystals grown by the Czochralski (Cz) method were investigated, and the piezoelectric constant <i>d</i><sub>11</sub> and electromechanical coupling factor <i>k</i><sub>12</sub> were increased by the Al substitution. In addition, the precise material constants of the CNGAS and CTGAS single crystals have been clarified by the ultrasonic material characterization system, and the 2 inch bulk single crystals have been developed by the Cz method.</p>

    DOI: 10.19009/jjacg.43.3_139

    CiNii Research

  381. Development of Ce-doped (Gd, La)<sub>2</sub>Si<sub>2</sub>O<sub>7</sub> for Well Logging Reviewed

    Shoji Yasuhiro, Kurosawa Shunsuke, Murakami Rikito, Shishido Toetsu, Horiai Takahiko, Yokota Yuui, Kamada Kei, Yoshikawa Akira

    Journal of the Japanese Association for Crystal Growth   Vol. 43 ( 1 ) page: 47 - 53   2016

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    Language:Japanese   Publisher:The Japanese Association for Crystal Growth  

    <p>  We have developed novel scintillation crystals based on Ce-doped (Gd,La)<sub>2</sub>Si<sub>2</sub>O<sub>7</sub> grown by the floating zone and Czochralski methods for oil well logging. The light output of 35,000 photons/MeV or more was kept in the temperature range from 25 to 150 ºC for these crystals. Ce: (Gd, La)<sub>2</sub>Si<sub>2</sub>O<sub>7</sub> single crystals can be applied to oil well logging and other radiation detection application under high temperature conditions.</p>

    DOI: 10.19009/jjacg.43.1_47

    CiNii Research

  382. Rare-earth Activated Pyrosilicate-type Powder Scintillator

    MURAKAMI Rikito, KUROSAWA Shunsuke

    Hosokawa Powder Technology Foundation ANNUAL REPORT   Vol. 24 ( 0 ) page: 170 - 173   2016

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    Language:Japanese   Publisher:Hosokawa Powder Technology Foundation  

    <p></p>

    DOI: 10.14356/hptf.15509

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  383. Directionally solidified Eu doped CaF<sub>2</sub>/Li<sub>3</sub>AlF<sub>6</sub> eutectic scintillator for neutron detection

    Kamada, K; Hishinuma, K; Kurosawa, S; Shoji, Y; Pejchal, J; Ohashi, Y; Yokota, Y; Yoshikawa, A

    OPTICAL MATERIALS   Vol. 50   page: 71 - 75   2015.12

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    Publisher:Optical Materials  

    Eu doped CaF<inf>2</inf>/Li<inf>3</inf>AlF<inf>6</inf> eutectics were grown by μ-PD method. The directionally solidified eutectic with well-aligned 600 nm diameter Eu:CaF<inf>2</inf> scintillator fibers surrounded with Li<inf>3</inf>AlF<inf>6</inf> was prepared. The grown eutectics showed an emission peak at 422 nm ascribed to Eu<sup>2+</sup> 4f-5d transition from Eu:CaF<inf>2</inf> scintillation fiber. Li concentration in the Eu:CaF<inf>2</inf>-Li<inf>3</inf>AlF<inf>6</inf> eutectic is around 0.038 mol/cm<sup>3</sup>,which is two times higher than that of LiCaAlF<inf>6</inf> single crystal (0.016 mol/cm<sup>3</sup>). The light yield of Eu:CaF<inf>2</inf>-Li<inf>3</inf>AlF<inf>6</inf> eutectic was around 7000 ph/neutron. The decay time was about 550 ns (89%) and 1450 ns (11%).

    DOI: 10.1016/j.optmat.2015.06.004

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  384. Growth and scintillation properties of Eu doped BaCl<sub>2</sub>/LiF eutectic scintillator

    Kamada, K; Hishinuma, K; Kurosawa, S; Yamaji, A; Shoji, Y; Pejchal, J; Yokota, Y; Ohashi, Y; Yoshikawa, A

    OPTICAL MATERIALS   Vol. 50   page: 76 - 80   2015.12

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    Publisher:Optical Materials  

    Eu doped BaCl<inf>2</inf>/LiF eutectics were grown by the micro-pulling down method and their directionally solidified eutectic (DSE) system has been investigated. The grown eutectic showed main phases of cubic LiF and orthorhombic BaCl<inf>2</inf>. In these eutectics, the 399 nm emission of Eu<sup>2+</sup> 4f5d was obtained. It shows the intrinsic decay time of about 410 ns. The light yield of the 1-mm-thick eutectic showed 7000 ph/5.5 MeV alpha-ray.

    DOI: 10.1016/j.optmat.2015.09.028

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  385. Two cases of bilateral lung transplantation combined with intracardiac repair and pulmonary artery replacement: perioperative managements based on the left ventricular function Open Access

    Toyama, H; Saitoh, K; Takei, Y; Ejima, Y; Kurosawa, S; Yamauchi, M

    JOURNAL OF ANESTHESIA   Vol. 29 ( 6 ) page: 957 - 961   2015.12

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    Language:English   Publisher:Journal of Anesthesia  

    We report on two patients who underwent bilateral lung transplantation (BLTx) combined with cardiac surgery. Patient 1 was a female whose pulmonary hypertension resulted from a congenital atrial septal defect (ASD) and idiopathic pulmonary arterial hypertension. She had a very small left ventricle (LV). We initiated venoarterial extracorporeal membrane oxygenation (ECMO) before induction of general anesthesia. She underwent ASD patch closure, pulmonary artery replacement, and BLTx under cardiopulmonary bypass (CPB). At the weaning from CPB, primary graft dysfunction and pulmonary edema induced by LV diastolic dysfunction was apparent. We gradually decreased the ECMO support and eventually weaned off the ECMO on the 4th postoperative day (POD) and the ventilator on the 29th POD. Patient 2 was a male with Eisenmenger syndrome, which resulted from ASD and ventricular septal defect (VSD). He had a normal LV. General anesthesia was induced smoothly without ECMO. He underwent ASD and VSD patch closure, pulmonary artery replacement, and BLTx under CPB. Weaning from CPB proceeded smoothly. These patients needed different management because of their different LV function. Especially, perioperative management of the BLTx patient with LV diastolic dysfunction was difficult. Assessment of perioperative cardiac function is very important in BLTx combined with cardiac surgery.

    DOI: 10.1007/s00540-015-2043-7

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  386. Acoustical physical constants around room temperature for Ca<sub>3</sub>TaGa<sub>1.5</sub>Al<sub>1.5</sub>Si<sub>2</sub>O<sub>14</sub> single crystal

    Ohashi, Y; Kudo, T; Yokota, Y; Shoji, Y; Kurosawa, S; Kamada, K; Yoshikawa, A

    ELECTRONICS LETTERS   Vol. 51 ( 24 ) page: 1957 - +   2015.11

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    Publisher:Electronics Letters  

    A full set of acoustical physical constants was determined for Ca<inf>3</inf>TaGa<inf>1.5</inf>Al<inf>1.5</inf>Si<inf>2</inf>O<inf>14</inf> (CTGAS) single crystal from bulk wave velocities measured by the ultrasonic micro-spectroscopy method. Several plate specimens were cut perpendicular to the X-, Y-, Z-, 35.25°Y-, and 139.74°Y-directions from a CTGAS single crystal ingot grown by Czochralski technique. Following measurements of dielectric constants and density, elastic constants, piezoelectric constants, and their temperature coefficients were determined from longitudinal wave and shear wave velocities measured for the CTGAS specimens at around room temperature. It was demonstrated that the as found constants could provide calculation accuracy within ±0.15% in leaky surface acoustic wave velocity. The determined constants were used for numerical calculation of the cut angle, at which the temperature coefficient of shear wave velocity becomes zero. This angle corresponded to 147.9°Y-cut substrate that had electromechanical coupling factor of k<sup>2</sup> = 3.2%. This parameter is about four times greater than that of AT-cut α-quartz.

    DOI: 10.1049/el.2015.2693

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  387. New readout and data-acquisition system in an electron-tracking Compton camera for MeV gamma-ray astronomy (SMILE-II) Open Access

    Mizumoto, T; Matsuoka, Y; Mizumura, Y; Tanimori, T; Kubo, H; Takada, A; Iwaki, S; Sawano, T; Nakamura, K; Komura, S; Nakamura, S; Kishimoto, T; Oda, M; Miyamoto, S; Takemura, T; Parker, JD; Tomono, D; Sonoda, S; Miuchi, K; Kurosawa, S

    NUCLEAR INSTRUMENTS & METHODS IN PHYSICS RESEARCH SECTION A-ACCELERATORS SPECTROMETERS DETECTORS AND ASSOCIATED EQUIPMENT   Vol. 800   page: 40 - 50   2015.11

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    Publisher:Nuclear Instruments and Methods in Physics Research Section A Accelerators Spectrometers Detectors and Associated Equipment  

    For MeV gamma-ray astronomy, we have developed an electron-tracking Compton camera (ETCC) as a MeV gamma-ray telescope capable of rejecting the radiation background and attaining the high sensitivity of near 1 mCrab in space. Our ETCC comprises a gaseous time-projection chamber (TPC) with a micro pattern gas detector for tracking recoil electrons and a position-sensitive scintillation camera for detecting scattered gamma rays. After the success of a first balloon experiment in 2006 with a small ETCC (using a 10×10×15 cm<sup>3</sup> TPC) for measuring diffuse cosmic and atmospheric sub-MeV gamma rays (Sub-MeV gamma-ray Imaging Loaded-on-balloon Experiment I; SMILE-I), a (30 cm)<sup>3</sup> medium-sized ETCC was developed to measure MeV gamma-ray spectra from celestial sources, such as the Crab Nebula, with single-day balloon flights (SMILE-II). To achieve this goal, a 100-times-larger detection area compared with that of SMILE-I is required without changing the weight or power consumption of the detector system. In addition, the event rate is also expected to dramatically increase during observation. Here, we describe both the concept and the performance of the new data-acquisition system with this (30 cm)<sup>3</sup> ETCC to manage 100 times more data while satisfying the severe restrictions regarding the weight and power consumption imposed by a balloon-borne observation. In particular, to improve the detection efficiency of the fine tracks in the TPC from ∼10% to ∼100%, we introduce a new data-handling algorithm in the TPC. Therefore, for efficient management of such large amounts of data, we developed a data-acquisition system with parallel data flow.

    DOI: 10.1016/j.nima.2015.08.004

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  388. Growth and piezoelectric properties of Ca<sub>3</sub>Nb(Ga<sub>1-<i>x</i></sub>Al<i><sub>x</sub></i>)<sub>3</sub>Si<sub>2</sub>O<sub>14</sub>(<i>x</i>=0.25 and 0.50) single crystals

    Yokota, Y; Ohashi, Y; Kudo, T; Kochurikhin, VV; Kurosawa, S; Kamada, K; Yoshikawa, A

    JAPANESE JOURNAL OF APPLIED PHYSICS   Vol. 54 ( 10 )   2015.10

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    Publisher:Japanese Journal of Applied Physics  

    One inch Ca<inf>3</inf>NbGa<inf>3</inf>Si<inf>2</inf>O<inf>14</inf> (CNGS) and Ca<inf>3</inf>Nb(Ga<inf>1-x</inf>Al<inf>x</inf>)<inf>3</inf>Si<inf>2</inf>O<inf>14</inf> (CNGAS) bulk crystals with an ordered langasite-type structure were grown by a Czochralski method. CNGS bulk single crystals without cracks could be grown, while CNGAS bulk crystals with x = 0.25 and 0.50 included some cracks even under improved growth conditions. Lattice parameters and anisotropy on the structure of grown crystals were systematically decreased and increased by increasing the Al concentration, respectively. Although the density and dielectric constant ε11 of an X-cut sample of the CNGAS crystal with x = 0.25 were decreased by Al substitution, the electromechanical coupling factor k<inf>12</inf> and piezoelectric constant d<inf>11</inf> were increased. The effects of Al substitution on piezoelectric properties were almost consistent with previous reports on the disordered langasite-type crystals except for their amount of change.

    DOI: 10.7567/JJAP.54.10ND13

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  389. AN ELECTRON-TRACKING COMPTON TELESCOPE FOR A SURVEY OF THE DEEP UNIVERSE BY MeV GAMMA-RAYS Open Access

    Tanimori, T; Kubo, H; Takada, A; Iwaki, S; Komura, S; Kurosawa, S; Matsuoka, Y; Miuchi, K; Miyamoto, S; Mizumoto, T; Mizumura, Y; Nakamura, K; Nakamura, S; Oda, M; Parker, JD; Sawano, T; Sonoda, S; Takemura, T; Tomono, D; Ueno, K

    ASTROPHYSICAL JOURNAL   Vol. 810 ( 1 )   2015.9

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    Publisher:Astrophysical Journal  

    Photon imaging for MeV gammas has serious difficulties due to huge backgrounds and unclearness in images, which originate from incompleteness in determining the physical parameters of Compton scattering in detection, e.g., lack of the directional information of the recoil electrons. The recent major mission/instrument in the MeV band, Compton Gamma Ray Observatory/COMPTEL, which was Compton Camera (CC), detected a mere ∼30 persistent sources. It is in stark contrast with the ∼2000 sources in the GeV band. Here we report the performance of an Electron-Tracking Compton Camera (ETCC), and prove that it has a good potential to break through this stagnation in MeV gamma-ray astronomy. The ETCC provides all the parameters of Compton-scattering by measuring 3D recoil electron tracks; then the Scatter Plane Deviation (SPD) lost in CCs is recovered. The energy loss rate (dE/dx), which CCs cannot measure, is also obtained, and is found to be helpful to reduce the background under conditions similar to those in space. Accordingly, the significance in gamma detection is improved severalfold. On the other hand, SPD is essential to determine the point-spread function (PSF) quantitatively. The SPD resolution is improved close to the theoretical limit for multiple scattering of recoil electrons. With such a well-determined PSF, we demonstrate for the first time that it is possible to provide reliable sensitivity in Compton imaging without utilizing an optimization algorithm. As such, this study highlights the fundamental weak-points of CCs. In contrast we demonstrate the possibility of ETCC reaching the sensitivity below 1 × 10<sup>-12</sup> erg cm<sup>-2</sup> s<sup>-1</sup> at 1 MeV.

    DOI: 10.1088/0004-637X/810/1/28

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  390. Crystal Growth of Ca<sub>3</sub>Nb(Ga<sub>1-<i>x</i></sub>Al<i><sub>x</sub></i>)<sub>3</sub>Si<sub>2</sub>O<sub>14</sub> Piezoelectric Single Crystals with Various Al Concentrations Open Access

    Yokota, Y; Kudo, T; Ohashi, Y; Medvedev, A; Kurosawa, S; Kamada, K; Yoshikawa, A

    MATERIALS   Vol. 8 ( 9 ) page: 5597 - 5605   2015.9

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    Language:English   Publisher:Materials  

    Ca<inf>3</inf>Nb(Ga<inf>1-x</inf>Al<inf>x</inf>)<inf>3</inf>Si<inf>2</inf>O<inf>14</inf> (CNGAS) single crystals with various Al concentrations were grown by a micro-pulling-down (μ-PD) method and their crystal structures, chemical compositions, crystallinities were investigated. CNGAS crystals with x = 0.2, 0.4 and 0.6 indicated a single phase of langasite-type structure without any secondary phases. In contrast, the crystals with x = 0.8 and 1 included some secondary phases in addition to the langasite-type phase. Lattice parameters, a- and c-axes lengths, of the langasite-type phase systematically decreased with an increase of Al concentration. The results of chemical composition analysis revealed that the actual Al concentrations in as-grown crystals were almost consistent with the nominal compositions. In addition, there was no large segregation of each cation along the growth direction.

    DOI: 10.3390/ma8095264

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  391. Patient-reported quality of life after allogeneic hematopoietic cell transplantation or chemotherapy for acute leukemia

    Kurosawa, S; Yamaguchi, T; Mori, T; Kanamori, H; Onishi, Y; Emi, N; Fujisawa, S; Kohno, A; Nakaseko, C; Saito, B; Kondo, T; Hino, M; Nawa, Y; Kato, S; Hashimoto, A; Fukuda, T

    BONE MARROW TRANSPLANTATION   Vol. 50 ( 9 ) page: 1241 - 1249   2015.9

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    Language:English   Publisher:Bone Marrow Transplantation  

    When discussing treatment options for patients with acute leukemia, it is important to acknowledge the impact of allogeneic hematopoietic cell transplantation (allo-HCT) or chemotherapy on quality of life (QOL). We performed a cross-sectional questionnaire study that administered SF-36, FACT-Leukemia and EuroQOL5D to 524 acute leukemia survivors, to compare patient-reported QOL between chemotherapy and allo-HCT, and to elucidate predictors of QOL. Patients who received chemotherapy alone had a better physical QOL than those who received allo-HCT. On the other hand, the allo-HCT group reported a better mental QOL. In the comparison of QOL in the allo-HCT patients according to the presence of GVHD at survey, patients who had GVHD symptoms experienced statistically and clinically significantly worse QOL than those who did not. In the allo-HCT patients without GVHD, the physical QOL was comparable to that in the chemotherapy patients, and they experienced significantly better mental and general QOL than the chemotherapy patients. GVHD and immunosuppressive drugs at survey were strongly associated with worse QOL after allo-HCT. In the chemotherapy group, a shorter time between treatment completion and survey was significantly associated with worse QOL. Further evaluation of QOL by a longitudinal assessment with quantitative and qualitative analyses are warranted.

    DOI: 10.1038/bmt.2015.137

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    PubMed

  392. Crystal growth of Ca3Nb(Ga0.75Al0.25)3O14 piezoelectric bulk single crystal

    Yokota Y., Kamada K., Kudo T., Ohashi Y., Kurosawa S., Yoshikawa A.

    2015 Joint IEEE International Symposium on the Applications of Ferroelectric International Symposium on Integrated Functionalities and Piezoelectric Force Microscopy Workshop Isaf Isif Pfm 2015     page: 102 - 104   2015.7

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    Publisher:2015 Joint IEEE International Symposium on the Applications of Ferroelectric International Symposium on Integrated Functionalities and Piezoelectric Force Microscopy Workshop Isaf Isif Pfm 2015  

    We grew a Al 25% substituted Ca<inf>3</inf>NbGa<inf>3</inf>Si<inf>2</inf>O<inf>14</inf>, Ca<inf>3</inf>Nb(Ga<inf>0.75</inf>Al<inf>0.25</inf>)<inf>3</inf>Si<inf>2</inf>O<inf>14</inf> (CNGAS) bulk single crystal with a diameter of 1 inch by Czochralski (Cz) method. Cracks in the crystal were dramatically decreased by the optimization of temperature gradient. Result of powder X-ray measurement indicated the grown CNGAS bulk single crystal was a single phase of langasite-type phase and lattice parameters, a- and c-axes lengths, decreased by the Al substitution. X-ray rocking curve of polished CNGS specimen indicated the grown CNGS bulk single crystal had great crystallinity.

    DOI: 10.1109/ISAF.2015.7172679

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  393. Homogeneity evaluation of Ca3Ta(Ga0.5Al0.5)3Si2O14 single crystal by the line-focus-beam ultrasonic material characterization system

    Ohashi Y., Kudo T., Shoji Y., Kurosawa S., Yoshikawa A., Yokota Y., Kamada K.

    2015 Joint IEEE International Symposium on the Applications of Ferroelectric International Symposium on Integrated Functionalities and Piezoelectric Force Microscopy Workshop Isaf Isif Pfm 2015     page: 190 - 192   2015.7

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    Publisher:2015 Joint IEEE International Symposium on the Applications of Ferroelectric International Symposium on Integrated Functionalities and Piezoelectric Force Microscopy Workshop Isaf Isif Pfm 2015  

    A new method for evaluating homogeneities of Ca<inf>3</inf>Ta(Ga<inf>0.5</inf>Al<inf>0.5</inf>)<inf>3</inf>Si<inf>2</inf>O<inf>14</inf> (CTGAS) single crystal was investigated using leaky surface acoustic wave (LSAW) velocities measured by the line-focus-beam ultrasonic material characterization (LFB-UMC) system. LSAW velocity changes due to Al-substitution effect were successfully extracted by using a relationship between two LSAW velocities propagating along different directions for Ca<inf>3</inf>TaGa<inf>3</inf>Si<inf>2</inf>O<inf>14</inf> (CTGS) and Al-doped CTGS. Al-concentration variation of 0.219 at% was detected in diameter direction of the crystal ingot through the LSAW velocity measurements for Y-cut CTGAS specimen. The velocity resolution to Al-concentration is estimated to be ±0.0046 at% for Y-cut Z-propagating LSAW.

    DOI: 10.1109/ISAF.2015.7172702

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  394. Eu concentration dependence on scintillation properties of Eu doped SrI<sub>2</sub> single crystals grown by modified micro-pulling-down method (vol 36, pg 1946, 2014)

    Nishimoto, K; Yokota, Y; Kurosawa, S; Kamada, K; Ymaji, A; Yoshikawa, A

    OPTICAL MATERIALS   Vol. 45   page: 258 - 258   2015.7

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    Publisher:Optical Materials  

    DOI: 10.1016/j.optmat.2015.01.016

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  395. Scintillation properties of a La, Lu-admix gadolinium pyrosilicate crystal

    Kurosawa, S; Shishido, T; Suzuki, A; Sugawara, T; Nomura, A; Yubuta, K; Shoji, Y; Yokota, Y; Pejchal, J; Ohashi, Y; Kamada, K; Yoshikawa, A

    NUCLEAR INSTRUMENTS & METHODS IN PHYSICS RESEARCH SECTION A-ACCELERATORS SPECTROMETERS DETECTORS AND ASSOCIATED EQUIPMENT   Vol. 784   page: 115 - 118   2015.6

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    Publisher:Nuclear Instruments and Methods in Physics Research Section A Accelerators Spectrometers Detectors and Associated Equipment  

    In order to obtain new scintillator with higher effective atomic number, a pyrosilicate crystal with a composition (Ce<inf>0.01</inf>, Gd<inf>0.54</inf>, La<inf>0.25</inf>, Lu<inf>0.20</inf>)<inf>2</inf>Si<inf>2</inf>O<inf>7</inf> (Ce:LaLu-GPS) was grown by the floating zone method. Emission wavelengths of this material were at 370 and 390 nm. Gamma-ray-excited pulse height and scintillation decay measurement showed that Ce:LaLu-GPS had a light output of 34,000±2000 photons/MeV, an FWHM energy resolution of 6.9±0.2%, and the decay time components of 59±1 ns (13%) and 570±20 ns (87%).

    DOI: 10.1016/j.nima.2014.12.108

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  396. Co-doping effects on luminescence and scintillation properties of Ce doped Lu<sub>3</sub>Al<sub>5</sub>O<sub>12</sub> scintillator

    Kamada, K; Nikl, M; Kurosawa, S; Beitlerova, A; Nagura, A; Shoji, Y; Pejchal, J; Ohashi, Y; Yokota, Y; Yoshikawa, A

    NUCLEAR INSTRUMENTS & METHODS IN PHYSICS RESEARCH SECTION A-ACCELERATORS SPECTROMETERS DETECTORS AND ASSOCIATED EQUIPMENT   Vol. 782   page: 9 - 12   2015.5

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    Publisher:Nuclear Instruments and Methods in Physics Research Section A Accelerators Spectrometers Detectors and Associated Equipment  

    The Mg, Ca, Sr and Ba 200 ppm co-doped Ce:Lu<inf>3</inf>Al<inf>5</inf>O<inf>12</inf> single crystals were prepared by micro pulling down method. Absorption and luminescence spectra were measured together with several other scintillation characteristics, namely the scintillation decay and light yield to reveal the effect of the co-doping. The scintillation decays were accelerated by both Mg and Ca co-dopants. The Mg co-doped samples showed the fastest decay and the highest light yield among the co-doped samples.

    DOI: 10.1016/j.nima.2015.01.105

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  397. Luminescence properties of Pr-doped (La, Gd)<sub>2</sub>Si<sub>2</sub>O<sub>7</sub> grown by the floating zone method

    Murakami, R; Kurosawa, S; Shishido, T; Sugawara, T; Nomura, A; Yubuta, K; Suzuki, A; Shoji, Y; Ohashi, Y; Pejchal, J; Kamada, K; Yokota, Y; Yoshikawa, A

    JAPANESE JOURNAL OF APPLIED PHYSICS   Vol. 54 ( 5 )   2015.5

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    Publisher:Japanese Journal of Applied Physics  

    Scintillation properties of a Pr-doped gadolinium lanthanum pyrosilicate (Pr:La-GPS) crystal grown by the floating zone (FZ) method were investigated, because the Pr<sup>3+</sup> 5d-4f transition is expected to show a shorter decay time than the Ce<sup>3+</sup> 5d-4f transition. In both α-ray radioluminescence and photoluminescence spectra, the emission peak related to the Pr<sup>3+</sup> 5d-4f transition was observed at around 350 nm. The photoluminescence decay time of Pr:La-GPS was found to be as short as ∼ 23 ns, whereas Ce:La-GPS had a decay time of ∼ 31 ns.

    DOI: 10.7567/JJAP.54.052401

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  398. Effects of anesthetics on perioperative short-term outcomes in patients undergoing thoracic surgery with one-lung ventilation

    Okada Y., Wagatsuma T., Yoshida A., Yamamoto Y., Saito K., Kurosawa S.

    Japanese Journal of Anesthesiology   Vol. 64 ( 4 ) page: 368 - 372   2015.4

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    Publisher:Japanese Journal of Anesthesiology  

    Background: The present study was designed to evaluate the postoperative values such as body temperature (BT), white blood cells (WBC), P/F ratio and C-reactive protein (CRP) associated with propofol or sevoflurane in patients undergoing thoracic surgery with one-lung ventilation. Methods: We retrospectively reviewed outcomes of patients undergoing video-associated thoracic surgery of the esophagus (VATS-E) with propofol (group P, n=71) or sevoflurane (group S, n=34). Data were taken at 1 POD and 2 POD in ICU. In addition, data of WBC and CRP were taken just before the operation and on 5 POD. Statistical analyses used t-value and two-way ANOVA with statistic significance as P<0.05. Results: There was no significant difference between the two groups and we could not find the correlation between anesthetics and each factor. Conclusions: Propofol and sevoflurane had similar effect on BT, WBC, P/F ratio and CRP in patients undergoing thoracic surgery with one-lung ventilation.

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  399. Growth, Structural Considerations, and Characterization of Ce-Doped (La,Gd)<sub>2</sub>Si<sub>2</sub>O<sub>7</sub> Scintillating Crystals

    Yoshikawa, A; Kurosawa, S; Shoji, Y; Chani, VI; Kamada, K; Yokota, Y; Ohashi, Y

    CRYSTAL GROWTH & DESIGN   Vol. 15 ( 4 ) page: 1642 - 1651   2015.4

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    Publisher:Crystal Growth and Design  

    Ce-doped lantanium-gadolinium pyrosilicate (La,Ce,Gd)<inf>2</inf>Si<inf>2</inf>O<inf>7</inf> (Ce:La-GPS), crystals with various content of rare-earth elements were produced from the melt, and their optimal La/Gd ratio was examined. It was found that Ce:La-GPS single crystals of acceptable optical quality can be produced from the melts ranging from La<inf>0.5</inf>Gd<inf>1.5</inf>Si<inf>2</inf>O<inf>7</inf> to La<inf>1.0</inf>Gd<inf>1.0</inf>Si<inf>2</inf>O<inf>7</inf> and containing about 1 atom % Ce with respect to the host rare-earths of La and Gd. The crystal growth was performed by the micro-pulling-down and Czochralski methods. The crystals were chemically uniform along the growth axis, and their composition was equal to that of the melt, thus corresponding to vicinity of congruent melting composition. Spatial distribution of Ce in La-GPS was also inspected, and no variation of Ce content was detected as a result of its similarity to one of the host cations (La) regarding the size. Basic optical and scintillation properties of the Ce:La-GPS crystals are also reported, and it is demonstrated that partial substitution of Gd with La has no negative impact on crystal growth and physical performance of the crystals.

    DOI: 10.1021/cg501416u

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  400. Improvement of scintillation properties on Ce doped Y<sub>3</sub>Al<sub>5</sub>O<sub>12</sub> scintillator by divalent cations co-doping

    Nagura, A; Kamada, K; Nikl, M; Kurosawa, S; Pejchal, J; Yokota, Y; Ohashi, Y; Yoshikawa, A

    JAPANESE JOURNAL OF APPLIED PHYSICS   Vol. 54 ( 4 )   2015.4

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    Publisher:Japanese Journal of Applied Physics  

    The Mg co-doped Y<inf>3</inf>Al<inf>5</inf>O<inf>12</inf>:Ce single crystal scintillators were prepared by micro pulling down method in a wide concentration range 0-3000 ppm of Mg co-dopant. Absorption and luminescence spectra were measured together with several other scintillation characteristics, namely the scintillation decay, light yield to reveal the effect of Mg co-doping. The scintillation decays were accelerated by Mg co-doping. The Mg co-doped samples showed much faster decay with increasing Mg.

    DOI: 10.7567/JJAP.54.04DH17

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  401. LiF/CaF<sub>2</sub>/LiBaF<sub>3</sub> ternary fluoride eutectic scintillator

    Hishinuma, K; Kamada, K; Kurosawa, S; Yamaji, A; Pejchal, J; Yokota, Y; Ohashi, Y; Yoshikawa, A

    JAPANESE JOURNAL OF APPLIED PHYSICS   Vol. 54 ( 4 )   2015.4

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    Publisher:Japanese Journal of Applied Physics  

    LiF/CaF<inf>2</inf>/LiBaF<inf>3</inf> ternary eutectic scintillators were grown by the μ-PD method. In the solidified eutectic the phases were uniformly distributed in the transverse direction and aligned along the growth direction. For the Eu-doped samples, the expected emission peak observed at 425nm was ascribed to Eu<sup>2+</sup> 5d-4f transition from Eu:CaF<inf>2</inf> under X-ray excitation. The LiF/CaF<inf>2</inf>/LiBaF<inf>3</inf> ternary eutectic scintillators showed a light yield around 7,000 photons/neutron and decay time of 260 ns (73.6%) and 50 ns (26.4%).

    DOI: 10.7567/JJAP.54.04DH04

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  402. Alkali earth co-doping effects on luminescence and scintillation properties of Ce doped Gd<sub>3</sub>Al<sub>2</sub>Ga<sub>3</sub>O<sub>12</sub> scintillator

    Kamada, K; Nikl, M; Kurosawa, S; Beitlerova, A; Nagura, A; Shoji, Y; Pejchal, J; Ohashi, Y; Yokota, Y; Yoshikawa, A

    OPTICAL MATERIALS   Vol. 41   page: 63 - 66   2015.3

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    Publisher:Optical Materials  

    The Mg and Ca co-doped Ce:Gd<inf>3</inf>Al<inf>2</inf>Ga<inf>3</inf>O<inf>12</inf> single crystals were prepared by micro pulling down method with a wide concentration range 0-1000 ppm of the codopants. Absorption and luminescence spectra were measured together with several other scintillation characteristics, namely the scintillation decay and light yield to reveal the effect of Mg and Ca co-doping. The scintillation decays were accelerated by both Mg and Ca codopants. Comparing to Ca co-doping, the Mg co-doped samples showed much faster decay and comparatively smaller light output decrease with increasing Mg dopant concentration.

    DOI: 10.1016/j.optmat.2014.10.008

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  403. Growth of Nd doped (Lu, Gd)<sub>3</sub>(Ga, Al)<sub>5</sub>O<sub>12</sub> single crystal by the micro pulling down method and their scintillation properties Open Access

    Kamada, K; Kurosawa, S; Yamaji, A; Shoji, Y; Pejchal, J; Ohashi, Y; Yokota, Y; Yoshikawa, A

    OPTICAL MATERIALS   Vol. 41   page: 32 - 35   2015.3

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    Publisher:Optical Materials  

    Nd 1 mol% doped (Lu, Gd)<inf>3</inf>(Ga, Al)<inf>5</inf>O<inf>12</inf> (LGGAG) single crystals were grown by the micro-pulling down (μ-PD) method. Luminescence and scintillation properties such as absorption, excitation and emission spectra, light yield and decay time were evaluated. Nd1%:Lu<inf>3</inf>Al<inf>5</inf>O<inf>12</inf> showed the highest light output of around 8200 photons/MeV among the grown crystals. Scintillation decay time of Nd:Y<inf>3</inf>Al<inf>5</inf>O<inf>12</inf> was 1.32 μs (36%) 2.02 μs (64%). Nd:Lu<inf>3</inf>Ga<inf>3</inf>Al<inf>2</inf>O<inf>12</inf> was relatively high dense scintillator of 7.38 g/cm<sup>3</sup> with good light yield of 6800 photons/MeV and scintillation decay time of 0.20 μs (5%) 2.60 μs (95%).

    DOI: 10.1016/j.optmat.2014.10.007

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  404. Luminescence and scintillation properties of Ce dope SrHfO<sub>3</sub> based eutectics

    Kamada, K; Kurosawa, S; Shoji, Y; Pejchal, J; Ohashi, Y; Yokota, Y; Yoshikawa, A

    OPTICAL MATERIALS   Vol. 41   page: 41 - 44   2015.3

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    Publisher:Optical Materials  

    Ce doped SrHfO<inf>3</inf>/SrAl<inf>12</inf>O<inf>19</inf> eutectics were grown by the micro pulling down (μ-PD) method and their directionally solidified eutectic system has been investigated. Investigations of obtained eutectic structure, luminescence and scintillation performances were also performed. Eutectics were grown at the speed of 0.60-0.90 mm/min. In the eutectics, Ce<sup>3+</sup> 4f-5d emission was observed at 410 nm. The eutectics showed light yield of around 300 photon/5.5 meV alpha-ray by <sup>241</sup>Am excitation. Scintillation decay time was 26.4 ns (45%) with slower decay component of 263 ns (55%).

    DOI: 10.1016/j.optmat.2014.10.010

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  405. Luminescence study on Eu or Tb doped lanthanum-gadolinium pyrosilicate crystal

    Kurosawa, S; Shishido, T; Sugawara, T; Nomura, A; Yubuta, K; Pejchal, J; Murakami, R; Yokota, Y; Shoji, Y; Ohashi, Y; Kamada, K; Yoshikawa, A

    OPTICAL MATERIALS   Vol. 41   page: 80 - 83   2015.3

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    Publisher:Optical Materials  

    (Eu<inf>0.01</inf>, Gd<inf>0.90</inf>, La<inf>0.09</inf>)<inf>2</inf>Si<inf>2</inf>O<inf>7</inf> (Eu:La-GPS) and (Tb<inf>0.01</inf>, Gd<inf>0.9</inf><inf>0</inf>, La<inf>0.09</inf>)<inf>2</inf>Si<inf>2</inf>O<inf>7</inf> (Tb:La-GPS) crystals were grown by the floating zone method, and their optical and scintillation properties were investigated. Gd<sup>3+</sup>-to-Tb<sup>3+</sup> or -Eu<sup>3+</sup> energy transfer processes were found, and photo-luminescence and radio-luminescence emission spectra showed <sup>5</sup>D<inf>0</inf>-<sup>7</sup>F<inf>i</inf> (i = 1-4) Eu<sup>3+</sup> transitions in Eu:La-GPS, and <sup>5</sup>D<inf>3</inf>-<sup>7</sup>F<inf>i</inf> (i = 3-6) and <sup>5</sup>D<inf>4</inf>-<sup>7</sup>F<inf>i</inf> (i = 3-6) transitions in Tb:La-GPS. Using these scintillators, alpha-ray imaging was possible with a CMOS camera. These materials can be used for X-ray detection as well.

    DOI: 10.1016/j.optmat.2014.12.006

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  406. Luminescence and scintillation properties of rare-earth-doped LuF<sub>3</sub> scintillation crystals

    Pejchal, J; Fukuda, K; Kurosawa, S; Yokota, Y; Yoshikawa, A

    OPTICAL MATERIALS   Vol. 41   page: 58 - 62   2015.3

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    Publisher:Optical Materials  

    The Nd-doped and Er-doped LuF<inf>3</inf> single crystals were grown by the micro-pulling-down method to study their scintillation properties in the vacuum-ultraviolet (VUV) region. The doubly Nd-Er codoped single crystal was grown to study possibility of scintillation performance improvement by energy transfer from Er<sup>3+</sup> to Nd<sup>3+</sup> ions. The LiF flux was to avoid phase transition below melting temperature. The 1%Nd-doped sample showed the highest overall scintillation efficiency under X-ray excitation which was 7 times as high as that of the LaF<inf>3</inf>:Nd 8% standard. The leading Nd<sup>3+</sup> 5d-4f emission was situated at 176 nm, while the Er<sup>3+</sup> 5d-4f emission for Er-doped samples was observed at 163 nm, which better matches the sensitivity of some VUV-sensitive photodetectors. The optimum Er concentration was determined to be around 1-3 mol%. No Er<sup>3+</sup> 5d-4f emission was observed for the doubly Er,Nd-codoped sample due to energy transfer from the Er<sup>3+</sup> to Nd<sup>3+</sup> ions. Slight improvement of the light yield was observed in the doubly-doped sample with respect to the Nd-only doped one.

    DOI: 10.1016/j.optmat.2014.10.009

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  407. Photoluminescence studies on energy transfer processes in cerium-doped Gd<sub>3</sub>Al<sub>2</sub>Ga<sub>3</sub>O<sub>12</sub> crystals

    Kitaura, M; Sato, A; Kamada, K; Kurosawa, S; Ohnishi, A; Sasaki, M; Hara, K

    OPTICAL MATERIALS   Vol. 41   page: 45 - 48   2015.3

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    Publisher:Optical Materials  

    We have measured photoluminescence properties of cerium-doped Gd<inf>3</inf>Al<inf>2</inf>Ga<inf>3</inf>O<inf>12</inf> (Ce:GAGG) crystals at low temperatures with use of synchrotron radiation. Excitation spectra for the Ce<sup>3+</sup> 5d-4f emission exhibit prominent peaks at Gd<sup>3+</sup> intra-4f absorption bands. The Gd<sup>3+</sup> intra-4f emission band is observed at 3.91 eV, but is not in resonance with the lowest energy Gd<sup>3+</sup> intra-4f absorption band at 3.95 eV. The temperature dependence of the Gd<sup>3+</sup> emission intensity is not correlated with that of the Ce<sup>3+</sup> emission intensity. Decay curves of the Ce<sup>3+</sup> emission were also measured at 9 K under excitation at various photon energies. The decay curve is remarkably changed, depending on the excitation photon energies. The present results give us hints to understand the whole of energy transfer processes in Ce:GAGG crystals.

    DOI: 10.1016/j.optmat.2014.12.040

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  408. Luminescence properties of SrI<sub>2</sub> single crystals doped with s<sup>2</sup>-group ions grown by modified micro-pulling-down method

    Kral Robert, Nitsch Karel, Pejchal Jan, Jary Vitezslav, Kurosawa Shunsuke, Yokota Yuui, Nikl Martin, Yoshikawa Akira

    JSAP Annual Meetings Extended Abstracts   Vol. 2015.1 ( 0 ) page: 535 - 535   2015.2

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    Language:English   Publisher:The Japan Society of Applied Physics  

    DOI: 10.11470/jsapmeeting.2015.1.0_535

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  409. Scintillation properties of Ce:(La,Gd)<sub>2</sub>Si<sub>2</sub>O<sub>7</sub> at high temperatures

    Kurosawa, S; Shishido, T; Sugawara, T; Nomura, A; Yubuta, K; Suzuki, A; Murakami, R; Pejchal, J; Yokota, Y; Kamada, K; Yoshikawa, A

    NUCLEAR INSTRUMENTS & METHODS IN PHYSICS RESEARCH SECTION A-ACCELERATORS SPECTROMETERS DETECTORS AND ASSOCIATED EQUIPMENT   Vol. 772   page: 72 - 75   2015.2

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    Publisher:Nuclear Instruments and Methods in Physics Research Section A Accelerators Spectrometers Detectors and Associated Equipment  

    Temperature dependence of scintillation properties was investigated for (Ce<inf>0.01</inf>, Gd<inf>0.90</inf>, La<inf>0.09</inf>)<inf>2</inf>Si<inf>2</inf>O<inf>7</inf> grown by floating zone method. The light output over 35,000 photons/MeV was found constant in the temperature range from 0 °C to 150 °C. In addition, FWHM energy resolution of Ce:La-GPS (roughly 7-8%) at 662 keV remained constant up to 100 °C. Thus, this crystal can be applied to oil well logging or other radiation detection application at high temperature conditions.

    DOI: 10.1016/j.nima.2014.10.008

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  410. Growth of 2-inch size Ce:doped Lu<sub>2</sub>Gd<sub>1</sub>Al<sub>2</sub>Ga<sub>3</sub>O<sub>12</sub> single crystal by the Czochralski method and their scintillation properties

    Kamada, K; Yoshikawa, A; Endo, T; Tsutsumi, K; Shoji, Y; Kurosawa, S; Yokota, Y; Prusa, P; Nikl, M

    JOURNAL OF CRYSTAL GROWTH   Vol. 410   page: 14 - 17   2015.1

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    Publisher:Journal of Crystal Growth  

    Ce 1% doped Lu<inf>2</inf>Gd<inf>1</inf>Al<inf>2</inf>Ga<inf>3</inf>O<inf>12</inf> (LGAGG) single crystals with a diameter of 50 mm and length of 150 mm were grown by the Czochralski (Cz) method using an RF heating system. The EPMA techniques is employed to check homogeniousity of chemical composition. Luminescence and scintillation properties were also evaluated. The grown LGAGG showed light yield of around 25,000 photon/MeV and energy resolution was 9.8%@662 keV. The scintillation decay time was 53.6 ns at room temperature.

    DOI: 10.1016/j.jcrysgro.2014.10.004

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  411. Performance of a new Electron-Tracking Compton Camera under intense radiations from a water target irradiated with a proton beam Open Access

    Matsuoka, Y; Tanimori, T; Kubo, H; Takada, A; Parker, JD; Mizumoto, T; Mizumura, Y; Iwaki, S; Sawano, T; Komura, S; Kishimoto, T; Oda, M; Takemura, T; Miyamoto, S; Sonoda, S; Tomono, D; Miuchi, K; Kabuki, S; Kurosawa, S

    JOURNAL OF INSTRUMENTATION   Vol. 10 ( 1 )   2015.1

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    Publisher:Journal of Instrumentation  

    We have developed an electron-tracking Compton camera (ETCC) for use in next generation MeV gamma ray telescopes. An ETCC consists of a gaseous time projection chamber (TPC) and pixel scintillator arrays (PSAs). Since the TPC measures the three dimensional tracks of Compton-recoil electrons, the ETCC can completely reconstruct the incident gamma rays. Moreover, the ETCC demonstrates efficient background rejection power in Compton-kinematics tests, identifies particle from the energy deposit rate (dE/dX) registered in the TPC, and provides high quality imaging by completely reconstructing the Compton scattering process. We are planning the "Sub-MeV gamma ray Imaging Loaded-on-balloon Experiment" (SMILE) for our proposed all-sky survey satellite. Performance tests of a mid-sized (30 cm)3 ETCC, constructed for observing the Crab nebula, are ongoing. However, observations at balloon altitudes or satellite orbits are obstructed by radiation background from the atmosphere and the detector itself [1]. The background rejection power was checked using proton accelerator experiments conducted at the Research Center for Nuclear Physics, Osaka University. To create the intense radiation fields encountered in space, which comprise gamma rays, neutrons, protons, and other energetic entities, we irradiated a water target with a 140MeV proton beam and placed a SMILE-II ETCC near the target. In this situation, the counting rate was five times than that expected at the balloon altitude. Nonetheless, the ETCC stably operated and identified particles sufficiently to obtain a clear gamma ray image of the checking source. Here, we report the performance of our detector and demonstrate its effective background rejection based in electron tracking experiments.

    DOI: 10.1088/1748-0221/10/01/C01053

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  412. Balloon-borne experiment for deep sky survey of MeV gamma rays using an electron-tracking Compton camera

    Komura S., Tanimori T., Takada A., Kubo H., Iwaki S., Matsuoka Y., Mizumoto T., Mizumura Y., Kishimoto T., Takemura T., Miyamoto S., Nakamura K., Nakamura S., Oda M., Sonoda S., Tomono D., Don Parke J., Miuchi K., Sawano T., Kurosawa S.

    Proceedings of Science   Vol. 30-July-2015   2015

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    Publisher:Proceedings of Science  

    Despite the scientific importance of MeV gamma-ray studies, sufficient observations have not been performed due to the large radiation backgrounds and the unclearness of MeV gamma-ray imaging. To advance the MeV gamma-ray astronomy, we have developed an Electron-Tracking Compton Camera (ETCC) with a gaseous electron tracker. By measuring three dimensional tracks of Compton-recoil electrons, our ETCC has attained the high-quality imaging and powerful background rejection. In order to verify such performance of an ETCC, we have carried out the balloon-borne experiments, Sub-MeV gamma-ray Imaging Loaded-on-balloon Experiment (SMILE) since 2006. The performance of current ETCC has already been surpassed the requirements to detect the Crab Nebula for 5 sigma level with several hours balloon observations. In addition, the ability of the polarization measurements has been revealed. The modulation factor is estimated to be 0.6 for the energy region below 200 keV by the Monte Carlo simulation. We have measured the polarization ability using the polarized X-ray beam-line at SPring-8, and then modulation factor of 0.6 is obtained at 130 keV, which is consistent with the results of the simulation and shows that the ETCC has an excellent performance as a sub-MeV gamma-ray polarimeter. By using the pressured CF4 based gas at 3 atm, the detection efficiency of the ETCC will be increased one order. Therefore we have a plan of the long duration observation for deep sky survey with polarization measurements of bright sources including Gamma-Ray Bursts. Here we present the concept of ETCC and the future prospects based on the performance of the current ETCC.

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  413. Crystal Growth of Ca<sub>3</sub>Nb(Ga<sub>0.75</sub>Al<sub>0.25</sub>)<sub>3</sub>O<sub>14</sub> Piezoelectric Bulk Single Crystal

    Yokota, Y; Kamada, K; Kudo, T; Ohashi, Y; Kurosawa, S; Yoshikawa, A

    2015 JOINT IEEE INTERNATIONAL SYMPOSIUM ON THE APPLICATIONS OF FERROELECTRIC, INTERNATIONAL SYMPOSIUM ON INTEGRATED FUNCTIONALITIES AND PIEZOELECTRIC FORCE MICROSCOPY WORKSHOP (ISAF/ISIF/PFM)     page: 102 - 104   2015

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  414. Homogeneity Evaluation of Ca<sub>3</sub>Ta(Ga<sub>0.5</sub>Al<sub>0.5</sub>)<sub>3</sub>Si<sub>2</sub>O<sub>14</sub> Single Crystal by the Line-Focus-Beam Ultrasonic Material Characterization System

    Ohashi, Y; Kudo, T; Shoji, Y; Kurosawa, S; Yoshikawa, A; Yokota, Y; Kamada, K

    2015 JOINT IEEE INTERNATIONAL SYMPOSIUM ON THE APPLICATIONS OF FERROELECTRIC, INTERNATIONAL SYMPOSIUM ON INTEGRATED FUNCTIONALITIES AND PIEZOELECTRIC FORCE MICROSCOPY WORKSHOP (ISAF/ISIF/PFM)     page: 190 - 192   2015

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  415. Measurements of Acoustical Physical Constants for Ca<sub>3</sub>Nb(Ga<sub>0.75</sub>Al<sub>0.25</sub>)<sub>3</sub>Si<sub>2</sub>O<sub>14</sub> Single Crystal Using the Ultrasonic Microspectroscopy System

    Ohashi, Y; Yokota, Y; Kudo, T; Kurosawa, S; Kamada, K; Yoshikawa, A

    2015 IEEE INTERNATIONAL ULTRASONICS SYMPOSIUM (IUS)     2015

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    Publisher:2015 IEEE International Ultrasonics Symposium Ius 2015  

    Acoustical physical constants were experimentally determined for Al-substituted Ca<inf>3</inf>NbGa<inf>3</inf>Si<inf>2</inf>O<inf>14</inf> (CNGAS) single crystal for the first time. Several plate specimens of the X-, Y-, Z-, 40.24°Y-, and 144.98°Y-cut were prepared from a CNGAS single crystal ingot grown by Czochralski technique. Elastic constants, piezoelectric constants, and their temperature coefficients were determined from longitudinal wave and shear wave velocities measured for the CNGAS specimens at around room temperature using the ultrasonic micro-spectroscopy (UMS) system. Dielectric constants, density, and coefficients of thermal expansion were also measured. It was demonstrated that the determined constants could provide calculation accuracy within ±0.12% in leaky surface acoustic wave (LSAW) velocity.

    DOI: 10.1109/ULTSYM.2015.0364

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  416. Decision Analysis of Allogeneic Hematopoietic Stem Cell Transplantation Versus Chemotherapy in Cytogenetically Standard-Risk Acute Myeloid Leukemia in First Complete Remission: The Impact of FLT3-ITD Profile

    Kurosawa, S; Yamaguchi, H; Yamaguchi, T; Fukunaga, K; Yui, S; Kanamori, H; Usuki, K; Uoshima, N; Yanada, M; Shono, K; Ueki, T; Mizuno, I; Yano, S; Takeuchi, J; Kanda, J; Okamura, H; Tajima, K; Inamoto, Y; Inokuchi, K; Fukuda, T

    BLOOD   Vol. 124 ( 21 )   2014.12

  417. Luminescence Characteristics of the Ce<SUP>3+</SUP>-Doped Pyrosilicates: The Case of La-Admixed Gd<sub>2</sub>Si<sub>2</sub>O<sub>7</sub> Single Crystals

    Jary, V; Nikl, M; Kurosawa, S; Shoji, Y; Mihokova, E; Beitlerova, A; Pazzi, GP; Yoshikawa, A

    JOURNAL OF PHYSICAL CHEMISTRY C   Vol. 118 ( 46 ) page: 26521 - 26529   2014.11

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    Publisher:Journal of Physical Chemistry C  

    We study Ce<sup>3+</sup> luminescence and scintillation characteristics in novel, high performing hosts among the oxide single crystal scintillators, the La-admixed Gd<inf>2</inf>Si<inf>2</inf>O<inf>7</inf>. Obtained characteristics are systematically compared with the earlier studied Lu<inf>2</inf>Si<inf>2</inf>O<inf>7</inf> host. We determine the barrier height of the thermal ionization of the Ce<sup>3+</sup> excited center, we address the effect of La-admixture on the physical characteristics, and we construct an energy level diagram of the material system. High scintillation efficiency, low afterglow, and the onset of Ce<sup>3+</sup> excited state ionization appearing well above room temperature indicate a large potential of La-admixed Gd<inf>2</inf>Si<inf>2</inf>O<inf>7</inf> in a variety of scintillating material applications. (Graph Presented).

    DOI: 10.1021/jp5080384

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  418. Growth and physical properties of Al doped Ca3NbGa3Si2O14 piezoelectric single crystals

    Yokota Y., Kamada K., Kudo T., Ohashi Y., Medvedev A., Kurosawa S., Yoshikawa A.

    2014 Joint IEEE International Symposium on the Applications of Ferroelectric International Workshop on Acoustic Transduction Materials and Devices and Workshop on Piezoresponse Force Microscopy Isaf Iwatmd Pfm 2014     2014.10

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    Publisher:2014 Joint IEEE International Symposium on the Applications of Ferroelectric International Workshop on Acoustic Transduction Materials and Devices and Workshop on Piezoresponse Force Microscopy Isaf Iwatmd Pfm 2014  

    Ca<inf>3</inf>Nb(Ga<inf>1-x</inf>Al<inf>x</inf>)<inf>3</inf>Si<inf>2</inf>O<inf>14</inf>(CNGAS) crystals with various Al concentrations were grown by a micro-pulling-down (μ-PD) method and their crystal structures, chemical compositions, crystallinities were investigated. CNGAS crystals with x = 0.2, 0.4 and 0.6 indicated a single phase of langasite-type structure and the crystals with x = 0.8 and 1 included some secondary phases in addition to the langasite-type phase by the powder X-ray diffraction measurements. Lattice parameters, a and c-axes lengths, of the langasite-type phase systematically decreased with an increase of Al concentration.

    DOI: 10.1109/ISAF.2014.6923019

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  419. Growth of Ca3Ta(Ga0.5Al0.5)3Si2O14 piezoelectric single crystal and the piezoelectric properties

    Kudo T., Shoji Y., Ohashi Y., Medvedev A., Kurosawa S., Yoshikawa A., Yokota Y., Kamada K.

    2014 Joint IEEE International Symposium on the Applications of Ferroelectric International Workshop on Acoustic Transduction Materials and Devices and Workshop on Piezoresponse Force Microscopy Isaf Iwatmd Pfm 2014     2014.10

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    Publisher:2014 Joint IEEE International Symposium on the Applications of Ferroelectric International Workshop on Acoustic Transduction Materials and Devices and Workshop on Piezoresponse Force Microscopy Isaf Iwatmd Pfm 2014  

    We grew Ca<inf>3</inf>Ta(Ga<inf>0.5</inf>Al<inf>0.5</inf>)<inf>3</inf>Si<inf>2</inf>O<inf>14</inf> piezoelectric single crystal with a diameter of 1 inch by Czochralski method and the physical properties were investigated. The grown crystal indicated high transparency with the yellow color. In addition, there was no crack in the crystal. By the powder X-ray diffraction measurement, the grown crystal was a single phase of langasite-type structure and lattice parameters, a- and c-axes lengths, were decreased by the Al substitution. The back-reflection Laue image revealed that the grown crystal was single crystal and crystalline facets derived from (0 0 1) plane. Actual chemical composition of grown crystal was little different from the nominal composition with stoichiometric composition.

    DOI: 10.1109/ISAF.2014.6922990

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  420. Control of mean ionic radius at Ca site by Sr co-doping for Ce doped LiCaAlF<sub>6</sub> single crystals and the effects on optical and scintillation properties

    Yokota, Y; Yamaji, A; Kurosawa, S; Kamada, K; Yoshikawa, A

    OPTICAL MATERIALS   Vol. 36 ( 12 ) page: 1950 - 1953   2014.10

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    Publisher:Optical Materials  

    Sr co-doped Ce:LiCaAlF<inf>6</inf> [Ce:Li(Ca,Sr)AlF<inf>6</inf>] crystals with various Ca/Sr ratios were grown by a micro-pulling-down (μ-PD) method and effects of Sr co-doping on crystal structure, chemical composition, optical and scintillation properties for Ce:LiCaAlF<inf>6</inf> crystals were investigated as a neutron scintillator. High transparent Ce2%:Li(Ca,Sr)AlF <inf>6</inf> crystals with 2% and 5% Sr contents were obtained while Ce2%:Li(Ca,Sr)AlF<inf>6</inf> crystals with 10% and 20% Sr contents included milky parts in the crystals. a- and c-axis lengths of Ce:Li(Ca,Sr)AlF <inf>6</inf> phase systematically increased with an increase of Sr content. In addition to the emission at 284 and 308 nm from Ce<sup>3+</sup> ion, emission peaks at 367 nm appeared by Sr co-doping. © 2014 Elsevier B.V. All rights reserved.

    DOI: 10.1016/j.optmat.2014.02.025

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  421. Cz grown 2-in. size Ce:Gd<sub>3</sub>(Al,Ga)<sub>5</sub>O<sub>12</sub> single crystal; relationship between Al, Ga site occupancy and scintillation properties

    Kamada, K; Kurosawa, S; Prusa, P; Nikl, M; Kochurikhin, VV; Endo, T; Tsutumi, K; Sato, H; Yokota, Y; Sugiyama, K; Yoshikawa, A

    OPTICAL MATERIALS   Vol. 36 ( 12 ) page: 1942 - 1945   2014.10

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    2-in. size Ce 1%:Gd<inf>3</inf>(Al<inf>1-</inf> <inf>x</inf>Ga<inf>x</inf>)<inf>5</inf>O<inf>12</inf> (GAGG) single crystals with various Ga concentration of x = 2, 2.4, 2.7 and 3 were grown by the Czochralski (Cz) method. Light yield has maximum value of 58,000 photon/MeV at x = 2.7 Ga concentration. Energy resolution was improved with decreasing Ga concentration and x = 2.4 sample showed best energy resolution of 4.2%@662 keV. The dependence of scintillation properties on crystal structure and Al-Ga was discussed. © 2014 Elsevier B.V. All rights reserved.

    DOI: 10.1016/j.optmat.2014.04.001

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  422. Effects of Eu concentration control on crystal growth and scintillation properties for Eu:LiSrAlF<sub>6</sub> crystals

    Suzuki, S; Yokota, Y; Yamaji, A; Kurosawa, S; Kamada, K; Yoshikawa, A

    OPTICAL MATERIALS   Vol. 36 ( 12 ) page: 1959 - 1962   2014.10

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    Publisher:Optical Materials  

    Eu doped LiSrAlF<inf>6</inf> (Eu:LiSAF) crystals with various Eu concentrations were grown by a micro-pulling-down (μ-PD) method and the effects of Eu concentration control on crystal growth and scintillation properties for Eu:LiSAF crystals were investigated as a neutron scintillator. As-grown Eu0.3%:LiSAF crystal had no visible inclusion while milky parts were observed in the crystals with higher Eu contents. The secondary phases with the chemical composition of EuF<inf>2</inf> or EuF<inf>3</inf> in the Eu:LiSAF matrix were observed for the crystals with high Eu contents while the secondary phase couldn't be observed in the powder XRD patterns. In the radioluminescence spectra of Eu:LiSAF crystals under α-ray irradiation, emission peaks around 375 nm originated from 5d-4f transition of Eu<sup>2+</sup> ion were observed. The light yields systematically increased with an increase of actual Eu contents in the crystals and the decay times were 1490-1620 ns. © 2014 Elsevier B.V. All rights reserved.

    DOI: 10.1016/j.optmat.2014.02.007

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  423. Eu concentration dependence on scintillation properties of Eu doped SrI<sub>2</sub> single crystals grown by modified micro-pulling-down method

    Nishimoto, K; Yokota, Y; Kurosawa, S; Kamada, K; Ymaji, A; Yoshikawa, A

    OPTICAL MATERIALS   Vol. 36 ( 12 ) page: 1946 - 1949   2014.10

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    Publisher:Optical Materials  

    Eu doped SrI<inf>2</inf> (Eu:SrI<inf>2</inf>) single crystals with various Eu contents were grown by a modified micro-pulling-down (μ-PD) method and effects of Eu concentration on scintillation properties were investigated. Eu 1%, 5%, 7.5%, 10% and 15%:SrI<inf>2</inf> single crystals were obtained and all as-grown crystals indicated high transparency without visible inclusion. Actual Eu contents in the grown crystals were almost same as nominal compositions. In the X-ray radioluminescence spectra, emission peaks around 435 nm were observed in all crystals. Eu7.5 mol%:SrI<inf>2</inf> crystals indicated the highest light yield, 78,000 ph/MeV, and the smallest energy resolution, 3.7%. © 2014 Elsevier B.V. All rights reserved.

    DOI: 10.1016/j.optmat.2014.02.026

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  424. Growth of Sc doped RE<sub>3</sub>Al<sub>5</sub>O<sub>12</sub> (RE = Y, Lu) single crystals by micro-pulling-down method and their scintillation properties

    Kamada, K; Pejchal, J; Nikl, M; Kurosawa, S; Yokota, Y; Yoshikawa, A

    OPTICAL MATERIALS   Vol. 36 ( 12 ) page: 1934 - 1937   2014.10

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    Publisher:Optical Materials  

    Sc doped Y<inf>y</inf>Lu<inf>3-y</inf>Al <inf>5</inf>O<inf>12</inf> (y = 0-1) single crystals were grown by the μ-PD method. EPMA techniques were employed to check their chemical composition. Luminescence characteristics were measured. Anti-site defect-related host emission was observed within 280-360 nm wavelength. The light yield was increasing with Y concentration and with an optimum for Sc2% concentration. The Sc 2% doped Y<inf>3</inf>Al<inf>5</inf>O<inf>12</inf> showed the highest light yield value around 30,000 photon/MeV and 670 ns scintillation decay time using a photomultiplier detector (R7600U). Substitution effects of the Lu site and their influence on luminescence and scintillation properties were studied. © 2014 Elsevier B.V. All rights reserved.

    DOI: 10.1016/j.optmat.2014.04.003

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  425. Luminescent properties of Cr-doped (Gd<i><sub>X</sub></i>, Y<sub>1-<i>X</i></sub>)<sub>3</sub>Al<sub>5</sub>O<sub>12</sub> infra-red scintillator crystals

    Suzuki, A; Kurosawa, S; Yamaji, A; Shoji, Y; Pejchal, J; Kamada, K; Yokota, Y; Yoshikawa, A

    OPTICAL MATERIALS   Vol. 36 ( 12 ) page: 1938 - 1941   2014.10

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    Publisher:Optical Materials  

    Cr-doped (Gd<inf>X</inf> Y<inf>1-X</inf>) <inf>3</inf>Al<inf>5</inf>O<inf>12</inf> (X = 0, 0.25, 0.50) crystals prepared by the micro-pulling down method were investigated to develop a infra-red scintillator for implantable patient dosimeter in radiation therapy. In order to evaluate their optical and scintillation performance, the following properties were measured: (i) transmittance between ultra-violet and near-infra red region, (ii) photoluminescence spectra under Xe-lamp excitation, and (iii) X-ray excited radio-luminescence spectra. Cr:Y<inf>3</inf>Al<inf>5</inf>O<inf>12</inf> and Cr:(Gd<inf>0.25</inf> Y<inf>0.75</inf>)<inf>3</inf>Al<inf>5</inf>O <inf>12</inf> crystals showed increased transmittance of 80%, while Cr:(Gd <inf>0.50</inf> Y<inf>0.50</inf>)<inf>3</inf>Al<inf>5</inf>O<inf>12</inf> had a lower transmittance of 40% due to its polycrystalline structure. In addition, all the Cr:(Gd<inf>X</inf> Y<inf>1-X</inf>)<inf>3</inf>Al <inf>5</inf>O<inf>12</inf> crystals showed sharp scintillation luminescence peaks ascribed to Cr<sup>3+</sup> d-d transitions. Therefore, these results suggested that Cr:Y<inf>3</inf>Al<inf>5</inf>O<inf>12</inf> and Cr:(Gd <inf>0.25</inf> Y<inf>0.75</inf>)<inf>3</inf>Al<inf>5</inf>O<inf>12</inf> crystals can be candidate materials for the dosimeter use. © 2014 Elsevier B.V. All rights reserved.

    DOI: 10.1016/j.optmat.2014.04.002

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  426. Crystal growth and scintillation properties of selected fluoride crystals for VUV scintillators

    Pejchal, J; Fukuda, K; Yamaji, A; Yokota, Y; Kurosawa, S; Kral, R; Nikl, M; Yoshikawa, A

    JOURNAL OF CRYSTAL GROWTH   Vol. 401   page: 833 - 838   2014.9

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    Publisher:Journal of Crystal Growth  

    Single crystals of orthorhombic and monoclinic BaLu<inf>2</inf>F<inf>8</inf>doped with Nd and Tm were grown by micro-pulling-down method. The monoclinic (low temperature modification) was grown using LiF flux, while the orthorhombic (high temperature modification) was grown with special hot-zone with shallow gradient and employing quenching process. Reasonable scintillation efficiency was achieved for the crystals of the former modification, while no rare-earth ion emission was observed in the latter due to preferential energy transfer to defects. The orthorhombic (low temperature) modification of ErF<inf>3</inf>was grown using LiF flux and hot zone with steep gradient. Quite low scintillation efficiency was found for the Nd-doped sample due to energy migration over the Er<sup>3+</sup>levels. Possibility of using pure ErF<inf>3</inf>as an infra-red scintillator is discussed.

    DOI: 10.1016/j.jcrysgro.2013.12.040

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  427. Crystal growth of pure and Sn-doped SrI<sub>2</sub> by atmosphere-controlled micro-pulling-down method and its luminescence and scintillation properties

    Kral Robert, Pejchal Jan, Nitsch Karel, Kurosawa Shunsuke, Babin Vladimir, Yokota Yuui, Yoshikawa Akira, Nikl Martin

    JSAP Annual Meetings Extended Abstracts   Vol. 2014.2 ( 0 ) page: 382 - 382   2014.9

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    DOI: 10.11470/jsapmeeting.2014.2.0_382

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  428. Effects of La, Gd, or Lu co-doping on crystal growth and scintillation properties of Eu:SrI<sub>2</sub> single crystals

    Nishimoto, K; Yokota, Y; Kurosawa, S; Pejchal, J; Kamada, K; Chani, V; Yoshikawa, A

    JOURNAL OF CRYSTAL GROWTH   Vol. 401   page: 484 - 488   2014.9

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    Eu:SrI<inf>2</inf>and La, Gd or Lu co-doped Eu:SrI<inf>2</inf>single crystals were grown by a modified micro-pulling-down method and the effects of rare-earth (RE) co-doping on the crystal growth and scintillation properties were investigated. RE-free Eu7.5 mol%:SrI<inf>2</inf>and La, Gd or Lu 1 mol% co-doped Eu7.5 mol:SrI<inf>2</inf>single crystals with high transparency were obtained. The powder X-ray diffraction measurements revealed that all the grown crystals had a single phase of SrI<inf>2</inf>structure. In the X-ray radioluminescence spectra, emission peaks around 435 nm were observed for the Eu:SrI<inf>2</inf>and La co-doped Eu:SrI<inf>2</inf>specimens. The light yield of the La co-doped Eu7.5%:SrI<inf>2</inf>specimens were lower than that of the RE-free Eu7.5%:SrI<inf>2</inf>specimen due to the generation of some defects by La co-doping.

    DOI: 10.1016/j.jcrysgro.2014.02.022

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  429. Growth of Al doped Ca<sub>3</sub>TaGa<sub>3</sub>Si<sub>2</sub>O<sub>14</sub> piezoelectric single crystals with various Al concentrations

    Kudo, T; Yokota, Y; Sato, M; Tota, K; Onodera, K; Kurosawa, S; Kamada, K; Yoshikawa, A

    JOURNAL OF CRYSTAL GROWTH   Vol. 401   page: 173 - 176   2014.9

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    Publisher:Journal of Crystal Growth  

    Al-doped Ca<inf>3</inf>TaGa<inf>3</inf>Si<inf>2</inf>O<inf>14</inf>single crystals with various Al concentrations were grown by the micro-pulling-down method and their structure and chemical composition were investigated. Ca<inf>3</inf>Ta(Ga<inf>1-x</inf>Al<inf>x</inf>)<inf>3</inf>Si<inf>2</inf>O<inf>14</inf>crystals with x=0, 0.2, 0.4, 0.6, 0.8 and 1 were grown. They were highly transparent and a single phase of langasite-type structure was confirmed in the powder X-ray diffraction measurement. Their lattice parameters related to the a- and c-axes systematically decreased with increase in Al concentration. It followed from the EPMA analysis that the real Al concentration in the crystals almost corresponded to the nominal compositions.

    DOI: 10.1016/j.jcrysgro.2014.02.021

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  430. Growth of Eu:SrI<sub>2</sub> bulk crystals and their scintillation properties

    Yokota, Y; Kurosawa, S; Nishimoto, K; Kamada, K; Yoshikawa, A

    JOURNAL OF CRYSTAL GROWTH   Vol. 401   page: 343 - 346   2014.9

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    Publisher:Journal of Crystal Growth  

    Eu doped SrI<inf>2</inf>[Eu:SrI<inf>2</inf>] bulk single crystals with 1 in. diameter were grown using a special-shaped carbon crucible and a modified micro-pulling-down furnace and their scintillation properties were investigated. As-grown Eu:SrI<inf>2</inf>bulk crystals indicated high transparency while they included several cracks in the crystals. Grown crystals indicated a single phase of SrI<inf>2</inf>structure in the powder X-ray diffraction measurement. In the X-ray radioluminescence spectrum, there was a sharp emission peak around 435 nm which originated from 5d-4f transition of Eu<sup>2+</sup>ion. Light yields of Eu5% and 7.5%:SrI<inf>2</inf>crystals under γ-ray irradiation from <sup>137</sup>Cs radiation source were 83,000 and 85,000 ph/MeV, respectively. Their decay times under γ-ray irradiation were approximately 2 μs.

    DOI: 10.1016/j.jcrysgro.2014.02.031

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  431. Luminescence and Scintillation Properties of Rare-earth-doped LuF<sub>3</sub>-based VUV Scintillation Crystals

    Fukuda Kentaro, Yamaji Akihiro, Pejchal Jan, Kurosawa Shunsuke, Yokota Yuui, Yoshikawa Akira

    JSAP Annual Meetings Extended Abstracts   Vol. 2014.2 ( 0 ) page: 383 - 383   2014.9

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    DOI: 10.11470/jsapmeeting.2014.2.0_383

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  432. Luminescence and Scintillation Properties of Selected Oxide Ceramics and Nanoceramics Sintered by SPS Method

    Barta Jan, Pejchal Jan, Cuba Vaclav, Kurosawa Shunsuke, Kucerkova Romana, Kamada Kei, Goto Takashi, Yokota Yuui, Ito Akihiko, Yoshikawa Akira

    JSAP Annual Meetings Extended Abstracts   Vol. 2014.2 ( 0 ) page: 361 - 361   2014.9

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    Language:English   Publisher:The Japan Society of Applied Physics  

    DOI: 10.11470/jsapmeeting.2014.2.0_361

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  433. Defect Engineering in Ce-Doped Aluminum Garnet Single Crystal Scintillators

    Nikl, M; Kamada, K; Babin, V; Pejchal, J; Pilarova, K; Mihokova, E; Beitlerova, A; Bartosiewicz, K; Kurosawa, S; Yoshikawa, A

    CRYSTAL GROWTH & DESIGN   Vol. 14 ( 9 ) page: 4827 - 4833   2014.9

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    Publisher:Crystal Growth and Design  

    Mg-codoped Lu<inf>3</inf>Al<inf>5</inf>O<inf>12</inf>:Ce single crystal scintillators were prepared by a micropulling down method in a wide concentration range from 0 to 3000 ppm of Mg codopant. Their structure and chemical composition were checked by X-ray diffraction and electron probe microanalysis techniques. Absorption and luminescence spectra, photoluminescence decays, and thermoluminescence glow curves were measured together with several other scintillation characteristics, namely, the scintillation decay, light yield, afterglow, and radiation damage to reveal the effect of Mg codoping. Several material characteristics manifest a beneficial effect of Mg codopant. We propose a model explaining the mechanism of material improvement which is based on the stabilization of a part of the cerium dopant in the tetravalent charge state. The stable Ce<sup>4+</sup> center provides an additional fast radiative recombination pathway in the scintillation mechanism and efficiently competes with electron traps in garnet scintillators. © 2014 American Chemical Society.

    DOI: 10.1021/cg501005s

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  434. Crystal growth of LiF/LiYF<sub>4</sub> eutectic crystals and their luminescent properties

    Nishimoto, K; Yokota, Y; Kurosawa, S; Fujimoto, Y; Kawaguchi, N; Fukuda, K; Yoshikawa, A

    JOURNAL OF THE EUROPEAN CERAMIC SOCIETY   Vol. 34 ( 9 ) page: 2117 - 2121   2014.8

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    Publisher:Journal of the European Ceramic Society  

    Undoped and 0.5mol% Ce-doped LiF-LiYF<inf>4</inf> eutectic crystals were grown by the micro-pulling-down method at different growth rates. The SEM images of all the eutectic crystals showed LiF with rod-like structure in the LiYF<inf>4</inf> matrix. The diameter of the rod phase systematically decreased with the increase of the growth rate. The radioluminescence spectra of cerium doped crystal under alpha-ray excitation showed emission peak at 325nm related to Ce<sup>3+</sup> 5d-4f transition. The white part in the cathodoluminescence image is considered to be due to Ce<sup>3+</sup> ion in LiYF<inf>4</inf> phase, according to the scanning electron microscopy (SEM) image in the same region. © 2014 Elsevier Ltd.

    DOI: 10.1016/j.jeurceramsoc.2014.02.029

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  435. Growth and luminescent properties of Ce-doped LiF/LiLuF<sub>4</sub> eutectic fibers grown by micro-pulling-down method

    Yokota, Y; Kurosawa, S; Nishimoto, K; Chani, V; Yoshikawa, A

    JOURNAL OF THE EUROPEAN CERAMIC SOCIETY   Vol. 34 ( 9 ) page: 2095 - 2099   2014.8

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    The undoped and Ce-doped LiF/LiLuF<inf>4</inf> eutectic fibers with various ratios of LuF<inf>3</inf> to LiF were grown by the micro-pulling-down method for their application as neutron scintillators with light guiding structure. The differential thermal analysis (DTA) of undoped eutectic materials indicated that the eutectic point of LiF/LiLuF<inf>4</inf> was positioned around LiF 80mol%-LuF<inf>3</inf> 20mol% composition. Some of the as-produced eutectic solids had rod-like regular array structures. This was observed using SEM images of cross-sectional and parallel cuts of the grown solids. In the range of x≥0.28, the dendrites appeared between the eutectic areas. Ce doped LiF/LiLuF<inf>4</inf> eutectic fibers demonstrated two emission peaks around 310 and 326nm in the photoluminescence spectrum, and the decay time of the emission at 326nm was 32.3ns. © 2014 Elsevier Ltd.

    DOI: 10.1016/j.jeurceramsoc.2013.12.047

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  436. Growth and optical properties of LiF/LaF<sub>3</sub> eutectic crystals

    Kurosawa, S; Yamaji, A; Yokota, Y; Futami, Y; Nishimoto, K; Kawaguchi, N; Fukuda, K; Yoshikawa, A

    JOURNAL OF THE EUROPEAN CERAMIC SOCIETY   Vol. 34 ( 9 ) page: 2111 - 2115   2014.8

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    Neutron imaging devices employing a scintillator can be used in various fields, and eutectic crystals can be suitable for the imaging with a fine position resolution of a few hundred micrometers. Since LiF and LaF<inf>3</inf> have different refractive indexes of 1.41 and 1.64 at 300nm, respectively, the eutectic crystal is expected to behave as a scintillator with light guiding properties. Thus, the optical properties of Ce-doped LiF/LaF<inf>3</inf> eutectic crystal grown by micro-pulling down method were investigated. The light output of LiF/Ce:LaF<inf>3</inf> eutectic crystal was relatively small. The emission peaks at 300nm originating from Ce<sup>3+</sup> of 5d-4f transition were observed under excitation by UV photons and 5.5MeV alpha rays. Moreover, the photo-luminescence decay time of Ce-doped LiF/LaF<inf>3</inf> eutectic crystal was estimated to be 17±1ns. © 2014 Elsevier Ltd.

    DOI: 10.1016/j.jeurceramsoc.2014.01.037

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  437. Crystal Growth and Luminescence Properties of Yb-doped Gd<sub>3</sub>Al<sub>2</sub>Ga<sub>3</sub>O<sub>12</sub> Infra-red Scintillator

    Suzuki, A; Kurosawa, S; Nagata, S; Yamamura, T; Pejchal, J; Yamaji, A; Yokota, Y; Shirasaki, K; Homma, Y; Aoki, D; Shikama, T; Yoshikawa, A

    OPTICAL MATERIALS   Vol. 36 ( 9 ) page: 1484 - 1487   2014.7

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    1-mol%-Yb-doped Gd<inf>3</inf>Al<inf>2</inf>Ga<inf>3</inf>O<inf>12</inf> infra-red scintillator crystal has been studied as a novel implantable radiation monitor in radiation therapy. Powder X-ray diffraction measurement and chemical analysis with a field emission scanning microscope and wavelength dispersive spectrometer determined its garnet structure and average chemical composition of Yb<inf>0.03±0.01</inf>Gd<inf>2.99±0.07</inf>Al <inf>2.21±0.08</inf>Ga<inf>2.64±0.09</inf>O <inf>12.10±0.09</inf>. Transmittance measurements reached high values of approximately 70% in the human body transparency region between 650 to 1200 nm. Photoluminescence peaks were detected around 970 and 1030 nm under the 940 nm excitation with a Xe lamp. Infra-red scintillation emissions were clearly observed around 970 and 1030 nm due to Yb<sup>3+</sup> 4f-4f transitions under X-ray excitation. Therefore, these results suggest that Yb-doped Gd <inf>3</inf>Al<inf>2</inf>Ga<inf>3</inf>O<inf>12</inf> might be used as an infra-red scintillator material. © 2014 Elsevier B.V. All rights reserved.

    DOI: 10.1016/j.optmat.2014.04.007

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  438. Radiation imaging with a new scintillator and a CMOS camera

    Kurosawa, S; Shoji, Y; Pejchal, J; Yokota, Y; Yoshikawa, A

    JOURNAL OF INSTRUMENTATION   Vol. 9 ( 7 )   2014.7

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    A new imaging system consisting of a high-sensitivity complementary metal-oxide semiconductor (CMOS) sensor, a microscope and a new scintillator, Ce-doped Gd<inf>3</inf>(Al,Ga)<inf>5</inf>O<inf>12</inf> (Ce:GAGG) grown by the Czochralski process, has been developed. The noise, the dark current and the sensitivity of the CMOS camera (ORCA-Flash4.0, Hamamatsu) was revised and compared to a conventional CMOS, whose sensitivity is at the same level as that of a charge coupled device (CCD) camera. Without the scintillator, this system had a good position resolution of 2.1 ± 0.4 μm and we succeeded in obtaining the alpha-ray images using 1-mm thick Ce:GAGG crystal. This system can be applied for example to high energy X-ray beam profile monitor, etc. © 2014 IOP Publishing Ltd and Sissa Medialab srl.

    DOI: 10.1088/1748-0221/9/07/C07015

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  439. Dislocated dental bridge covering the larynx: usefulness of tracheal tube guides under video-assisted laryngoscopy for induction of general anesthesia, thus avoiding tracheostomy Open Access

    Hidaka, H; Suzuki, T; Toyama, H; Kurosawa, S; Nomura, K; Katori, Y

    HEAD & FACE MEDICINE   Vol. 10 ( 1 ) page: 23   2014.6

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    Background: To describe a case with dislodgement of dental bridge with clasps covering the vocal cords, in a patient who was successfully intubated using tube exchanger under video-assisted laryngoscopy.Study design, methods: Clinical case record with a video clip.Setting: University hospital.Case presentation: A 83-year-old woman presented with dislodgement of her dental bridge whilst eating. Laryngoscopy revealed a foreign body almost entirely covering the vocal cords, with the clasps of the dislodged partial denture piercing the pharyngeal wall. Before induction of general anesthesia, a tracheal tube introducer combined with video-assisted laryngoscopy was introduced into the trachea in the awake condition, followed by successful endotracheal intubation. Thereafter, the dislodged denture was extracted via the oral cavity.Conclusions: Tracheal tube introducers combined with video-assisted laryngoscopy appear to be useful for airway management, decreasing the number of avoidable tracheostomies performed. © 2014 Hidaka et al.; licensee BioMed Central Ltd.

    DOI: 10.1186/1746-160X-10-23

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  440. Crystal growth and optical properties of Ce:(La,Gd)<sub>2</sub>Ge<sub>2</sub>O<sub>7</sub> grown by the floating zone method

    Kurosawa, S; Shishido, T; Sugawara, T; Yubuta, K; Jan, P; Suzuki, A; Yokota, Y; Shoji, Y; Kamada, K; Yoshikawa, A

    JOURNAL OF CRYSTAL GROWTH   Vol. 393   page: 142 - 144   2014.5

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    Some pyrosilicate scintillators such as Ce:Gd<inf>2</inf>Si <inf>2</inf>O<inf>7</inf> and Ce:Lu<inf>2</inf>Si<inf>2</inf>O<inf>7</inf> have a good light output, and especially Ce:(Gd,La)<inf>2</inf>Si<inf>2</inf>O <inf>7</inf> has an excellent light output of over 36,000 ph/MeV. In order to search novel scintilators, we have developed a pyrogermanate-based scintillation material (Ce<inf>0.01</inf>,Gd<inf>0.90</inf>,La<inf>0.09</inf>) <inf>2</inf>Ge<inf>2</inf>O<inf>7</inf> using the floating zone method. Although the light output was decreased due to quenching, 5d-4f transition of Ce <sup>3+</sup> was observed around 480 nm in photo- and radio-luminescence spectra. This emission wavelength was longer than that of (Ce <inf>0.01</inf>,Gd<inf>0.90</inf>,La<inf>0.09</inf>)<inf>2</inf>Si <inf>2</inf>O<inf>7</inf> with an emission wavelength of 390 nm. © 2013 Elsevier B.V.

    DOI: 10.1016/j.jcrysgro.2013.12.038

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  441. Crystal growth of CaYAlO<sub>4</sub> single crystals grown by the micro-pulling down method and their luminescent properties

    Yamaji, A; Suzuki, A; Shoji, Y; Kurosawa, S; Pejchal, J; Kamada, K; Yokota, Y; Yoshikawa, A

    JOURNAL OF CRYSTAL GROWTH   Vol. 393   page: 138 - 141   2014.5

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    Nd and Yb doped CaYAlO<inf>4</inf> crystals have been grown by the micro-pulling down method. The segregation coefficient along the growth direction and the radial dopant distribution were measured by using electron probe micro-analysis (EPMA). The X-ray induced luminescence spectra in the spectral range from 300 to 1500 nm were measured: Nd and Yb doped CaYAlO <inf>4</inf> showed intense peaks at 990 and 1045 nm, respectively. These crystals would be promising materials for near infrared emission scintillators. © 2013 Elsevier B.V.

    DOI: 10.1016/j.jcrysgro.2013.11.089

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  442. Czochralski growth of Gd<sub>3</sub>(Al<sub>5-<i>x</i></sub>,Ga<i><sub>x</sub></i>)O<sub>12</sub> (GAGG) single crystals and their scintillation properties

    Kurosawa, S; Shoji, Y; Yokota, Y; Kamada, K; Chani, VI; Yoshikawa, A

    JOURNAL OF CRYSTAL GROWTH   Vol. 393   page: 134 - 137   2014.5

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    Ce:Gd<inf>3</inf>(Al<inf>x</inf>Ga<inf>1-x</inf>)<inf>5</inf>O<inf>12</inf> (x=2.5/5 and 3/5, Ce:GAGG-2.5 and Ce:GAGG-3) crystals were grown by the Czochralski process in order to reduce cost of the starting materials as compared with conventional Ce:Gd<inf>3</inf>Al<inf>2</inf>Ga<inf>3</inf>O <inf>12</inf> (Ce:GAGG-2) crystal which have high light output. Although perovskite phase was detected in Ce:GAGG-3, Ce:GAGG-2.5 had single-phase garnet structure. Solidification fraction for the Ce:GAGG-2.5 growth was 0.52. Optical properties including transmittance, emission, and excitation spectra of 30 samples cut from the Ce:GAGG-2.5 bulk ingot did not depend on their original position along the growth axis. These samples had light outputs of approximately 58,000±3000 photons/MeV. However, scintillation decay times varied from 140 to 200 ns and depended on the position clearly. © 2013 Elsevier B.V.

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  443. Optical properties of a Nd-doped SrBr<sub>2</sub> crystal grown by the Bridgman technique

    Kurosawa, S; Yokota, Y; Yanagida, Y; Pejchal, J; Yamaji, A; Shoji, Y; Kamada, K; Yoshikawa, A

    JOURNAL OF CRYSTAL GROWTH   Vol. 393   page: 163 - 166   2014.5

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    We have investigated the optical properties of 1 mol% Nd-doped SrBr <inf>2</inf> crystal grown by the Bridgman technique for an X-ray scintillator application. We succeeded in obtaining a transparent crystal, whose X-ray diffraction was measured under dry condition because of its hygroscopic nature. Roughly, we estimated that 90% of this crystal dissolved within 300 min. under 25 °C and 65-70% humidity. Under excitation by 270 and 400 nm photons several emission peaks originating from <sup>4</sup>F<inf>3/2</inf> or <sup>4</sup>G<inf>i1</inf>→<sup>4</sup>I<inf>i2</inf> (i1=5/2 and 7/2 and i2=13/2, 11/2, and 9/2) transitions of Nd<sup>3+</sup> were observed. 1 mol% Nd:SrBr<inf>2</inf> had a maximum quantum yield of approximately 45%. Additional emission peaks were observed under X-ray excitation. © 2013 Elsevier B.V.

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  444. Development of a 30 cm-cube Electron-Tracking Compton Camera for the SMILE-II Experiment Open Access

    Mizumura, Y; Tanimori, T; Kubo, H; Takada, A; Parker, JD; Mizumoto, T; Sonoda, S; Tomono, D; Sawano, T; Nakamura, K; Matsuoka, Y; Komura, S; Nakamura, S; Oda, M; Miuchi, K; Kabuki, S; Kishimoto, Y; Kurosawa, S; Iwaki, S

    JOURNAL OF INSTRUMENTATION   Vol. 9 ( 5 )   2014.5

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    To explore the sub-MeV/MeV gamma-ray window for astronomy, we have developed the Electron-Tracking Compton Camera (ETCC), and carried out the first performance test in laboratory conditions using several gamma-ray sources in the sub-MeV energy band. Using a simple track analysis for a quick first test of the performance, the gamma-ray imaging capability was demonstrated with clear images and 5.3 degrees of angular resolution measure (ARM) measured at 662 keV. As the greatest impact of this work, a gamma-ray detection efficiency on the order of 10<sup>-4</sup> was achieved at the sub-MeV gamma-ray band, which is one order of magnitude higher than our previous experiment. This angular resolution and detection efficiency enables us to detect the Crab Nebula at the 5σ level with several hours observation at balloon altitude in middle latitude. Furthermore, good consistency of efficiencies between this performance test and simulation including only physical processes is very important; it means we achieve nearly 100% detection of Compton recoil electrons and means that our predictions of performance enhancement resulting from future upgrades are more realistic. We are planning to confirm the imaging capability of the ETCC by observation of celestial objects in the SMILE-II (Sub-MeV gamma ray Imaging Loaded-on-balloon Experiment II). The SMILE-II and following SMILE-III project will be an important key of sub-MeV/MeV gamma-ray astronomy. © 2014 IOP Publishing Ltd and Sissa Medialab srl.

    DOI: 10.1088/1748-0221/9/05/C05045

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  445. Glucocorticoid mediates the transcription of OAT-PG, a kidney-specific prostaglandin transporter

    Hatano, R; Mukouchi, H; Matsumoto, Y; Kawaguchi, K; Kazama, I; Endo, Y; Toyama, H; Ejima, Y; Kurosawa, S; Kanai, Y; Matsubara, M; Asano, S

    PFLUGERS ARCHIV-EUROPEAN JOURNAL OF PHYSIOLOGY   Vol. 466 ( 5 ) page: 925 - 935   2014.5

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    OAT-PG is a kidney-specific prostaglandin transporter and exclusively expressed at the basolateral membrane of proximal tubules in rodent kidneys. We previously reported that OAT-PG was dominantly expressed in the male kidney similar to the other SLC22 family proteins as organic anion transporter (OAT) 1 and OAT3. Recently, Wegner et al. revealed that a transcription factor, B-cell CLL/lymphoma 6 (BCL6), is associated with the male-dominant expressions of OAT1 and OAT3 in the rat kidney. Here, we performed the luciferase assay to investigate whether OAT-PG is also transcriptionally regulated by BCL6. However, the promoter activity of OAT-PG was not directly affected by BCL6 overexpression nor the testosterone treatment, suggesting that different regulatory mechanisms underlie the male-dominant transcriptional regulation of OAT-PG compared to those of OAT1 and OAT3. We newly found that adrenalectomy (Adx) of male rat caused a significant reduction of OAT-PG expression without any significant changes in the OAT1 and OAT3 expressions, and it was recovered by the dexamethasone administration. Furthermore, the renocortical PGE <inf>2</inf> concentration was markedly increased in Adx male rat, concomitant with the downregulation of OAT-PG, and it was reduced to the basal level by dexamethasone treatment. In the luciferase assay, dexamethasone stimulated OAT-PG promoter activity but not OAT1. The luciferase activity responsiveness to dexamethasone was significantly reduced by the deletion of glucocorticoid response elements in the OAT-PG promoter region. These results suggest that glucocorticoid plays an important role in the regulation of the renocortical PGE<inf>2</inf> concentration by the transcriptional regulation of OAT-PG in the rat kidney. © 2013 Springer-Verlag.

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  446. Performance of Ce-doped (La, Gd)<sub>2</sub>Si<sub>2</sub>O<sub>7</sub> scintillator with an avalanche photodiode

    Kurosawa, S; Shishido, T; Suzuki, A; Pejchal, J; Yokota, Y; Yoshikawa, A

    NUCLEAR INSTRUMENTS & METHODS IN PHYSICS RESEARCH SECTION A-ACCELERATORS SPECTROMETERS DETECTORS AND ASSOCIATED EQUIPMENT   Vol. 744   page: 30 - 34   2014.4

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    Publisher:Nuclear Instruments and Methods in Physics Research Section A Accelerators Spectrometers Detectors and Associated Equipment  

    Scintillation properties of Ce-doped (La, Gd)<inf>2</inf>Si <inf>2</inf>O<inf>7</inf> (Ce:La-GPS) crystal were measured with Si avalanche photodiode (APD, Hamamatsu S8664-55). Since Ce:La-GPS is a novel scintillator, its scintillation properties have been evaluated using the APD for the first time. This crystal grown by floating zone method had a good light output of 41,000±1000 photons/MeV and FWHM energy resolution at 662 keV was 4.4±0.1% at 23.0±0.2 C. The photon non-proportional response (PNR) of Ce:La-GPS was approximately 65% at 32 keV, where light output at 662 keV was normalized to 100%. Moreover, the temperature dependence of the light outputs was determined to be approximately 0.15%/ C from -10 to 30 C. © 2014 Elsevier B.V.

    DOI: 10.1016/j.nima.2014.01.018

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  447. Anesthetic management of six patients with surgically repaired tetralogy of fallot undergoing the second intra-cardiac surgery

    Adachi K., Kurosawa S., Kameyama E., Nakata Y.

    Japanese Journal of Anesthesiology   Vol. 63 ( 4 ) page: 373 - 379   2014.4

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    In Japan, more than 9,000 patients with congenital heart disease reach adulthood every year with improved medical treatment, and perioperative encounter with patients requiring the second intra-cardiac operation in adulthood is more often. Tetralogy of Fallot (TOF) is the most common form of cyanotic congenital heart disease, and long-term prognosis is good. Therefore, we have more chances to care the postoperative adult patients with TOF. This is a retrospective study in 6 patients with TOF who underwent the second intra-cardiac operation in adulthood from 2008 to 2012. Among the six patients, six had pulmonary valve replacement; four had tricuspid valve replacements or valvuloplastys; four had ventricular septal defect closures; two had right ventricular outflow tract obstruction releases; one had aortic valve replacement; and three had cryoablations. Right ventricular end-diastolic volume was 194.1±83.5 ml·m<sup>-2</sup> (mean±SD), and right ventricular ejection fraction was 38.2±4.8%. The factors which influence the anesthetic management were as follows: right cardiac failure by abnormality of the pulmonary valve; residual disease and deuteropathy of two or more combination; the risks associated with the second open chest surgery such as long operative time and severe bleeding. Perioperative management of an adult with congenital heart disease requires full understanding of its pathophysiology such as congenital heart disease, adult-specific complications, and the second open chest surgery.

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  448. Fundamental study of inorganic-organic hybrid scintillator using Pr:Lu<sub>3</sub>Al<sub>5</sub>O<sub>12</sub> and plastic scintillator

    Kamada, K; Kurosawa, S; Yokota, Y; Yanagida, T; Nikl, M; Yoshikawa, A

    JAPANESE JOURNAL OF APPLIED PHYSICS   Vol. 53 ( 4 )   2014.4

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    Read out test of inorganic-organic hybrid scintillator; Pr:LuAG single crystal covered with plastic scintillator BC-499 is demonstrated. Emission peaks of the hybrid scintillator was observed around 430 nm, which suit to the sensitive wavelength of photomultiplier tube (PMT). The Pr:LuAG sample coated with BC-499 showed the better light output than the that of Pr:LuAG itself. Light output was increased up to 30% sing PMT (Hamamatsu R9800). Decay curve of the hybrid scintillator was also measured and successfully modeled. Corporation. © 2014 The Japan Society of Applied Physics.

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  449. Luminescent properties of Ce:Gd<sub>3</sub>(Al,Ga,Mg,M)<sub>5</sub>O<sub>12</sub> crystal (M = Zr, Hf)

    Kurosawa, S; Kamada, K; Yokota, Y; Yoshikawa, A

    JAPANESE JOURNAL OF APPLIED PHYSICS   Vol. 53 ( 4 )   2014.4

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    To obtain a new scintillator with a higher gamma-ray stopping power than conventional Ce:Gd<inf>3</inf>Al<inf>2</inf>Ga<inf>3</inf>O<inf>12</inf> (Ce:GAGG), which has excellent light output and energy resolution, new scintillators based on Ce:GAGG, Ce:Gd3Al2Mg0.5Hf0.5Ga2O12, and Ce:Gd3Al2Mg0.5Zr0.5Ga2O12 were grown by the micro-pulling down method as the first step. We found that the emission wavelengths of these crystals became slightly longer than that of Ce:GAGG by approximately 10-20nm owing to the change in energy band structure. © 2014 The Japan Society of Applied Physics.

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  450. Optical and scintillating properties of Ce:Li(Y,Lu)F<sub>4</sub> single crystals

    Yokota, Y; Kurosawa, S; Chani, V; Kamada, K; Yoshikawa, A

    RADIATION MEASUREMENTS   Vol. 62   page: 6 - 9   2014.3

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    We have investigated the optical and scintillating properties of Lu co-doped Ce:LiYF<inf>4</inf> single crystals with various Lu content. In the transmittance and absorption spectra, the absorption peaks at 243 nm get systematically red shifted in contrast to the peaks at 197 and 200 nm which get blue shifted with the increase in Lu content. At the same time, emission peaks at 306 nm and 200 nm under 295 nm excitation also get red shifted. The decay time of Ce:Li(Y,Lu)F<inf>4</inf> crystals under 295 nm excitation is found to be faster than that of Ce:LiYF<inf>4</inf> and Ce:LiLuF<inf>4</inf> crystals. The alpha-peak positions in the pulse-height spectra and decay times of crystals under alpha-ray irradiation are found to vary with the Lu content. © 2014 Elsevier Ltd. All rights reserved.

    DOI: 10.1016/j.radmeas.2013.12.003

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  451. Czochralski Growth and Scintillation Properties of Ce : (Gd, Y, Lu)<sub>3</sub> (Al, Ga)<sub>5</sub>O<sub>12</sub> Single Crystals

    Kamada, K; Prusa, P; Nikl, M; Blazek, K; Endo, T; Tsutsumi, K; Kurosawa, S; Yokota, Y; Yoshikawa, A

    IEEE TRANSACTIONS ON NUCLEAR SCIENCE   Vol. 61 ( 1 ) page: 293 - 296   2014.2

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    1-inch size Ce1%: Gd<inf>2</inf>Lu<inf>1</inf>Al<inf>2</inf>Ga <inf>3</inf>O<inf>12</inf>, Gd<inf>1</inf>Lu<inf>2</inf>Al<inf>2</inf>Ga <inf>3</inf>O<inf>12</inf>, Gd<inf>1</inf>Y<inf>2</inf>Al<inf>1.5</inf>Ga <inf>3.5</inf>O<inf>12</inf> and Lu<inf>2</inf>Y<inf>1</inf>Al <inf>2</inf>Ga<inf>3</inf>O<inf>12</inf> were grown by the Czhocralski (Cz) method. The EPMA techniques is employed to check their chemical composition. Luminescence and scintillation properties were also evaluated. The Ce1%: Gd <inf>1</inf>Y<inf>2</inf>Al<inf>2</inf>Ga<inf>3</inf>O<inf>12</inf> sample showed the highest light yield of around 40 000 photon/MeV. The scintillation decay time was 46.6 ns(63%) and 157 ns(37%). © 2014 IEEE.

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  452. Development of a Prototype Detector Using APD-Arrays Coupled With Pixelized Ce:GAGG Scintillator for High Resolution Radiation Imaging

    Kamada, K; Shimazoe, K; Ito, S; Yoshino, M; Endo, T; Tsutsumi, K; Kataoka, J; Kurosawa, S; Yokota, Y; Takahashi, H; Yoshikawa, A

    IEEE TRANSACTIONS ON NUCLEAR SCIENCE   Vol. 61 ( 1 ) page: 348 - 352   2014.2

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    A novel digital PET scanner based on Time over Threshold method is developed. The positron emission tomography (PET) is composed of 144channel Ce:Gd<inf>3</inf>Al<inf>2</inf>Ga<inf>3</inf>O<inf>12</inf> (GAGG)-Avaranche photodiode (APD) detector arrays individually coupled with custom designed Time over Threshold (ToT) application-specific integrated circuit (ASIC) to realize the high count rate and good spatial resolution. Such an imaging system provides a simple front-end circuit and flexible digital signal processing like multiplexing such as a pulse train method. The measured energy resolution of the detector system was 6.7% for the 511 keV peak, and 4.25 ns time resolution was measured with a single detector module. The measured spatial resolution for a point source was 1.37 mm FWHM for our initial data with a columnar <sup>22</sup>Na source. © 2014 IEEE.

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  453. Growth and Scintillation Properties of Ce:Li(Ca, Ba)AlF<sub>6</sub> Scintillator Crystals

    Yokota, Y; Kurosawa, S; Fukuda, K; Kamada, K; Yoshikawa, A

    IEEE TRANSACTIONS ON NUCLEAR SCIENCE   Vol. 61 ( 1 ) page: 419 - 423   2014.2

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    Ba co-doped Ce:LiCaAlF<inf>6</inf>[Ce:Li(Ca,Ba)AlF<inf>6</inf>] and LiCaAlF<inf>6</inf> [Li(Ca,Ba)AlF<inf>6</inf>] crystals with various Ba concentrations were grown and their structures, optical and scintillation properties were investigated. As-grown Ce2%Ba1% and Ce2%Ba2%:Li(Ca,Ba)AlF <inf>6</inf> crystals were high transparency in all parts while an end part of as-grown Ce2%Ba5%:Li(Ca,Ba)AlF<inf>6</inf> crystal and all parts of as-grown Ba5%:Li(Ca,Ba)AlF<inf>6</inf> crystal included milky parts which decreased transmittance. Ce:Li(Ca,Ba)AlF<inf>6</inf> crystals indicated the emission peaks at 288 and 308 nm from which was attributable to the 5d-4f transition of Ce<sup>3+</sup> ion in the radioluminescence spectra under α-ray irradiation. In the case of Ce1%Ba2%:Li(Ca,Ba)AlF<inf>6</inf> crystal, light yield under thermal neutron irradiation were improved. Decay times of Ce:Ce:Li(Ca,Ba)AlF<inf>6</inf> under thermal neutron irradiation systematically increased with an increase of Ba concentration. © 2013 IEEE.

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  454. Lower incidence of emergence agitation in children after propofol anesthesia compared with sevoflurane: a meta-analysis of randomized controlled trials

    Kanaya, A; Kuratani, N; Satoh, D; Kurosawa, S

    JOURNAL OF ANESTHESIA   Vol. 28 ( 1 ) page: 4 - 11   2014.2

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    Background: Emergence agitation (EA) from general anesthesia has been reported as an adverse effect of sevoflurane in children. We describe a meta-analysis of randomized controlled trials that compared the incidence of EA between children who underwent sevoflurane anesthesia and those who underwent propofol anesthesia. Methods: A literature search was conducted to identify clinical trials that met our inclusion criteria. Prospective randomized trials comparing sevoflurane and propofol anesthesia in children less than 15 years of age were included in the meta-analysis. Data from each trial were combined using the random effects model to calculate pooled odds ratios (ORs) and their corresponding 95 % confidence intervals (CIs). The heterogeneity of data was assessed by Cochran's Q and I <sup>2</sup> tests. Sensitivity analysis was conducted for study quality, patient age, and type of surgical procedure. Results: The meta-analysis included 14 studies, in which 560 patients received sevoflurane and 548 received propofol. The pooled OR for EA was 0.25 with a 95 % CI of 0.16-0.39 (P = 0.000), which indicates that propofol anesthesia resulted in a lower incidence of EA. The heterogeneity of data was not statistically supported (P = 0.191). All sensitivity analyses strengthened the evidence for the lower incidence of EA with propofol. Conclusions: Our meta-analysis demonstrated that EA in children is less likely to occur after propofol anesthesia compared with sevoflurane anesthesia. © 2013 Japanese Society of Anesthesiologists.

    DOI: 10.1007/s00540-013-1656-y

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  455. Luminescence Properties of Gd<sub>3</sub>Ga<sub>5</sub>O<sub>12</sub>:Cr Single Crystals

    Yamaji, A; Kochurikhin, VV; Kurosawa, S; Suzuki, A; Fujimoto, Y; Yokota, Y; Yoshikawa, A

    IEEE TRANSACTIONS ON NUCLEAR SCIENCE   Vol. 61 ( 1 ) page: 320 - 322   2014.2

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    We evaluated optical and scintillation properties of a 0.03% Cr-doped Gd<inf>3</inf>Ga<inf>5</inf>O<inf>12</inf> (GGG:Cr) single crystal grown by Czochralsk method for medical use. Since human body has low absorption region from approximately 700-1100 nm, near infrared scintillators would be applied to the real time dose monitor system. In the X-ray excited radioluminescence, the emissions related to <sup>2</sup>E→<sup>4</sup> A<inf>2</inf> transitions of Cr<sup>3+</sup> were observed at around 725 nm. The scintillation light yield of GGG: Cr 0.03% single crystal under 5.5 MeV alpha-ray excitation was determined to be 30% of BGO. © 2014 IEEE.

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  456. Luminescence and Scintillation Properties of Scintillators Based on Orthorhombic and Monoclinic BaLu<sub>2</sub>F<sub>8</sub> Single Crystals

    Pejchal, J; Fukuda, K; Kurosawa, S; Yokota, Y; Kral, R; Nikl, M; Yoshikawa, A

    IEEE TRANSACTIONS ON NUCLEAR SCIENCE   Vol. 61 ( 1 ) page: 411 - 418   2014.2

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    The rare-earth-doped orthorhombic BaLu<inf>2</inf>F<inf>8</inf> vacuum-ultra-violet scintillator crystals have been studied. The fast emission around 185 nm with a decay time of several nanoseconds was due to the allowed 5d-4f transition of the Nd<sup>3+</sup> ion. The high temperature phase BaLu<inf>2</inf> F<inf>8</inf> orthorhombic crystals have been prepared by micro-pulling-down method. Unfortunately, no 5d-4f emission (neither from Nd<sup>3+</sup> nor from Tm<sup>3+</sup>) was observed in the crystals under excitation by ionizing radiation at all. This was explained by preferential energy transfer from the host to the lattice defect states. Further improvement of the scintillation efficiency by facilitating the energy transfer from the host matrix to the Nd<sup>3+</sup> luminescence center by Tm<sup>3+</sup> -codoping was attempted. The energy transfer from the Tm<sup>3+</sup> ions to the Nd<sup>3+</sup> ones has been proved, however, no improvement of the overall scintillation efficiency was observed. © 2013 IEEE.

    DOI: 10.1109/TNS.2013.2280505

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  457. Perovskite fluoride crystals as light emitting materials in vacuum ultraviolet region

    Yamanoi, K; Nishi, R; Takeda, K; Shinzato, Y; Tsuboi, M; Luong, MV; Nakazato, T; Shimizu, T; Sarukura, N; Cadatal-Raduban, M; Pham, MH; Nguyen, HD; Kurosawa, S; Yokota, Y; Yoshikawa, A; Togashi, T; Nagasono, M; Ishikawa, T

    OPTICAL MATERIALS   Vol. 36 ( 4 ) page: 769 - 772   2014.2

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    Vacuum-ultraviolet (VUV) fluorescence from KMgF<inf>3</inf> and BaLiF <inf>3</inf> crystals excited by an extreme ultraviolet free electron laser (EUV-FEL) with 61-nm emission wavelength is studied. Cross-luminescence (CL) peaks at 8.5 eV and 7.5 eV, due to an electron from the valence band recombining with a hole in the F2p core band edge are observed in KMgF<inf>3</inf>. On the other hand, BaLiF<inf>3</inf> exhibited a fluorescence peak at 7.75 eV. The band gap energy of BaLiF<inf>3</inf> is estimated from its absorption spectrum to be around 8.41 eV. Results suggest the possibility of developing VUV solid-state devices including light emitting diodes. © 2013 Elsevier B.V. All rights reserved.

    DOI: 10.1016/j.optmat.2013.11.023

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  458. Read Out Test of Pr:LuAG Scintillator Coupled to Organic Wavelength Shifter Using Si Based Photodetectors

    Kamada, K; Yanagida, T; Kurosawa, S; Yokota, Y; Endo, T; Tsutsumi, K; Yoshikawa, A

    IEEE TRANSACTIONS ON NUCLEAR SCIENCE   Vol. 61 ( 1 ) page: 452 - 455   2014.2

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    Functional possibilities of Pr:LuAG single crystal covered with plastic scintillators are demonstrated. Shift of luminescence wavelength of the hybrid scintillators towards the region of higher spectral sensitivity of photodetectors and radiation responses of the hybrid scintillators were investigated. The Pr:LuAG sample coated with bis-MSBPVD showed the better light output and energy resolution than the Pr:LuAG itself. Light output was increased up to 55% and energy resolution was also improved to 6.5%@662 keV using APD (Hamamatsu S8664-8220). In the case of MPPC (Hamamatsu S10362-33-050 3600 pixel-type), light output was increased up to 35% and energy resolution was also improved to 9.8%@662 keV. Decay curve of the Pr:LuAG sample coupled with the WLS was also measured and successfully modeled. © 2013 IEEE.

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  459. Scintillation Properties of Nd<SUP>3+</SUP>-Doped Lu<sub>2</sub>O<sub>3</sub> Ceramics in the Visible and Infrared Regions

    Kurosawa, S; An, LQ; Yamaji, A; Suzuki, A; Yokota, Y; Shirasaki, K; Yamamura, T; Ito, A; Goto, T; Boulon, G; Yoshikawa, A

    IEEE TRANSACTIONS ON NUCLEAR SCIENCE   Vol. 61 ( 1 ) page: 316 - 319   2014.2

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    Nd<sup>3+</sup> -doped Lu<inf>2</inf>O<inf>3</inf> (Nd: Lu <inf>2</inf>O<inf>3</inf>) is a candidate for an infrared scintillator because (i) Lu<inf>2</inf>O<inf>3</inf> has a high density of 9.5g/cm<sup>3</sup> and a high atomic number of 67 and (ii) Nd<sup>3+</sup>-doped materials emit in the infrared range and the emission lines from Nd<sup>3+</sup> can be used in medical applications since human body has a transparency window between 600 and 1,100 nm. However, it is extremely difficult to fabricate Lu<inf>2</inf>O <inf>3</inf> single crystals using conventional crystal growth methods because of the high melting point (2,510 °C). Using solid-state reactions, it is much easier to fabricate Lu<inf>2</inf>O<inf>3</inf> into a ceramic structure. Therefore, Nd: Lu<inf>2</inf>O<inf>3</inf> transparent ceramics were fabricated using a spark plasma sintering method. This technique is comparatively simple and consumes less time than other methods such as vacuum hot pressing. The scintillation properties and transmittance spectra of the as-produced ceramics were studied in both the visible and infrared regions. Radioluminescence spectra were measured in the range 800-1,200 nm. Nd<sup>3+</sup> emission lines were observed in the transparency window of human body. Thus, these ceramic materials could be a candidate for medical imaging applications. © 2014 IEEE.

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  460. Scintillation Properties of a Non-Doped Ca<sub>3</sub>TaGa<sub>3</sub>Si<sub>2</sub>O<sub>14</sub> Crystal

    Kurosawa, S; Kitahara, M; Yokota, Y; Hishinuma, K; Kudo, T; Buzanov, O; Medvedev, A; Chani, VI; Yoshikawa, A

    IEEE TRANSACTIONS ON NUCLEAR SCIENCE   Vol. 61 ( 1 ) page: 339 - 342   2014.2

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    In order to search for a new scintillation material consisting of tantalum (Ta) with a high atomic number of 73, we have investigated scintillation properties of langasite type crystal containing Ta. Non-doped Ca <inf>3</inf>TaGa<inf>3</inf>Si<inf>2</inf>O<inf>14</inf> (CTGS), which is well known as a piezoelectric material, was grown by the Czochralski method. Radio-luminescence spectrum of this crystal peaked around 340 nm. Its light output was approximately 1,200 photons/MeV. This crystal is expected to be a scintillation host material. © 2014 IEEE.

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  461. Annual FEV<sub>1</sub> changes and numbers of circulating endothelial microparticles in patients with COPD: a prospective study Open Access

    Takahashi, T; Kobayashi, S; Fujino, N; Suzuki, T; Ota, C; Tando, Y; Yamada, M; Yanai, M; Yamaya, M; Kurosawa, S; Yamauchi, M; Kubo, H

    BMJ OPEN   Vol. 4 ( 3 ) page: e004571   2014

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    Objective: Growing evidence suggests that endothelial injury is involved in the pathophysiology of chronic obstructive pulmonary disease (COPD). Circulating endothelial microparticles (EMPs) increase in patients with COPD because of the presence of endothelial injury. We examined the relationship between EMP number and changes in forced expiratory volume in 1 s (FEV <inf>1</inf>) in patients with COPD. Design: Prospective study. Setting: One hospital in Japan. Participants: A total 48 outpatients with stable COPD coming to the hospital from September 2010 to September 2011. Primary and secondary outcomes measured: Blood samples were collected and vascular endothelial (VE)-cadherin EMPs (CD144+ EMPs), E-selectin EMPs (CD62E+ EMPs) and platelet endothelial cell adhesion molecule EMPs (CD31+/CD41- EMPs) were measured using fluorescence-activated cell sorting. Annual FEV<inf>1</inf> changes were evaluated using FEV<inf>1</inf> data acquired a year before and a year after sample collection. Results: The number of E-selectin and VE-cadherin EMPs showed significant negative correlations with annual FEV<inf>1</inf> changes (r <inf>s</inf>=-0.65, p<0.001, r<inf>s</inf>=-0.43, p=0.003, respectively). Leucocyte counts tended to be correlated with annual FEV<inf>1</inf> changes, but this correlation was not significant (r<inf>s</inf>=-0.28, p=0.057). There were significant differences in annual FEV<inf>1</inf> changes between with and without history of frequent exacerbation (p=0.006), and among Global Initiative for Chronic Obstructive Lung Disease (GOLD) stages (p=0.009). Multiple linear regression analysis revealed E-selectin EMP to be the only significant parameter associated with annual FEV<inf>1</inf> changes, independent of VE-cadherin EMP, GOLD stages, leucocyte counts, and history of frequent exacerbation. Receiver operating characteristic curves showed the optimum E-selectin EMP cut-off level for prediction of rapid FEV<inf>1</inf> decline (>66 mL/year) to be 153.0/μL (areas under curve 0.78 (95% CI 0.60 to 0.89); sensitivity, 67%; specificity, 81%). Conclusions: The high E-selectin EMP levels in stable patients with COPD are predictive of rapid FEV<inf>1</inf> decline. Trial registration number: UMIN000005168.

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  462. Growth and Luminescence Properties of Ce and Ca co-doped LiGdF<sub>4</sub>-LiF Eutectic Scintillator

    Hishinuma, K; Kamada, K; Kurosawa, S; Suzuki, S; Yamaji, A; Yokota, Y; Yoshikawa, A

    ADVANCED CERAMICS AND NOVEL PROCESSING   Vol. 616   page: 96 - 103   2014

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    Ce and Ca co-doped LiGdF4-LiF eutectics were grown and their directionally solidified eutectic (DSE) system has been investigated. In these eutectics, apart from the expected 305 nm emission of the regular Ce<sup>3+</sup>, 310 nm emission of the Gd<sup>3+</sup> and Ce<sup>3+</sup> -perturbed emission around 320-380 nm was observed. Ce<sup>3+</sup>-perturbed emission at 340 nm shows the intrinsic decay time of about 27 ns. In photoluminescence mechanism the observed decay time shortening of the regular Ce<sup>3+</sup> and Gd<sup>3+</sup> centers point to the energy transfer in the sequence the regular Ce <sup>3+</sup>?→ (Gd<sup>3+</sup>)<inf>n</inf>?→ the perturbed Ce <sup>3+</sup> sites. © (2014) Trans Tech Publications, Switzerland.

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  463. Growth and physical properties of Al doped Ca<sub>3</sub>NbGa<sub>3</sub>Si<sub>2</sub>O<sub>14</sub> piezoelectric single crystals

    Yokota, Y; Kamada, K; Kudo, T; Ohashi, Y; Medvedev, A; Kurosawa, S; Yoshikawa, A

    2014 JOINT IEEE INTERNATIONAL SYMPOSIUM ON THE APPLICATIONS OF FERROELECTRICS, INTERNATIONAL WORKSHOP ON ACOUSTIC TRANSDUCTION MATERIALS AND DEVICES & WORKSHOP ON PIEZORESPONSE FORCE MICROSCOPY (ISAF/IWATMD/PFM)     page: 244 - 247   2014

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  464. Growth of Ca<sub>3</sub>Ta(Ga<sub>0.5</sub>Al<sub>0.5</sub>)<sub>3</sub>Si<sub>2</sub>O<sub>14</sub> piezoelectric single crystal and the piezoelectric properties

    Kudo, T; Shoji, Y; Ohashi, Y; Medvedev, A; Kurosawa, S; Yoshikawa, A; Yokota, Y; Kamada, K

    2014 JOINT IEEE INTERNATIONAL SYMPOSIUM ON THE APPLICATIONS OF FERROELECTRICS, INTERNATIONAL WORKSHOP ON ACOUSTIC TRANSDUCTION MATERIALS AND DEVICES & WORKSHOP ON PIEZORESPONSE FORCE MICROSCOPY (ISAF/IWATMD/PFM)     page: 131 - 133   2014

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  465. High-z gamma-ray bursts for unraveling the dark ages mission HiZ-GUNDAM Open Access

    Yonetoku, D; Mihara, T; Sawano, T; Ikeda, H; Atsushi, H; Shunsuke, T; Yoshida, K; Seta, H; Toyanago, A; Kagawa, Y; Kawai, K; Kawai, N; Sakamoto, T; Serino, M; Kurosawa, S; Gunji, S; Tanimori, T; Murakami, T; Yatsu, Y; Yamaoka, K; Yoshida, A; Kawabata, K; Matsumoto, T; Tsumura, K; Matsuura, S; Shirahata, M; Okita, H; Yanagisawa, K; Yoshida, M; Motohara, K

    SPACE TELESCOPES AND INSTRUMENTATION 2014: ULTRAVIOLET TO GAMMA RAY   Vol. 9144   2014

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    We are now investigating and studying a small satellite mission HiZ-GUNDAM for future observation of gamma-ray bursts (GRBs). The mission concept is to probe the end of dark ages and the dawn of formation of astronomical objects, i.e. the physical condition of early universe beyond the redshift z > 7. We will consider two kinds of mission payloads, (1) wide field X-ray imaging detectors for GRB discovery, and (2) a near infrared telescope with 30 cm in diameter to select the high-z GRB candidates effectively. In this paper, we explain some requirements to promote the GRB cosmology based on the past observations, and also introduce the mission concept of HiZ-GUNDAM and basic development of X-ray imaging detectors.

    DOI: 10.1117/12.2055041

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  466. MeV gamma-ray Compton camera using a gaseous electron tracker for background-suppressed observation

    Takada, A; Tanimori, T; Kubo, H; Parker, JD; Mizumoto, T; Mizumura, Y; Sawano, T; Nakamura, K; Matsuoka, Y; Komura, S; Nakamura, S; Oda, M; Miuchi, K; Kurosawa, S

    SPACE TELESCOPES AND INSTRUMENTATION 2014: ULTRAVIOLET TO GAMMA RAY   Vol. 9144   2014

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    As a next generation MeV gamma-ray telescope, we develop an electron-tracking Compton camera (ETCC) that consists of a gaseous electron tracker surrounded by pixel scintillator arrays. The tracks of the Compton-recoil electron measured by the tracker restrict the incident gamma-ray direction to an arc region on the sky and reject background by using the energy loss rate dE/dx and a Compton-kinematics test. In 2013, we constructed, for a balloon experiment, a 30-cm-cubic ETCC with an effective area of ∼1 cm<sup>2</sup> for detecting sub-MeV gamma rays (5 σ detection of the Crab Nebula for 4 h). In future work, we will extend this ETCC to an effective area of ∼10 cm<sup>2</sup>. In the present paper, we report the performance of the current ETCC.

    DOI: 10.1117/12.2055627

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  467. Optical and scintillation properties of Cr doped Y<sub>3</sub>Ga<sub>5</sub>O<sub>12</sub> crystal for infra-red scintillators

    Yamaji, A; Kurosawa, S; Suzuki, A; Pejchal, J; Kamada, K; Yokota, Y; Yoshikawa, A

    ADVANCED CERAMICS AND NOVEL PROCESSING   Vol. 616   page: 92 - 95   2014

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    We evaluated optical and scintillation properties of a Cr 0.5%:Y <inf>3</inf>Ga<inf>5</inf>O<inf>12</inf> (YGG) and Cr 0.5%:Y<inf>3</inf>Al <inf>5</inf>O<inf>12</inf> (YAG) crystals grown by the micro-pulling down method for infrared emission scintillators. In the photoluminescence and X-ray induced radioluminescence measurements, the emissions peaks of Cr:YGG were located in the longer wavelength than those of Cr:YAG. Radioluminescene spectrum of Cr:YGG had a broad peak at 716 nm related to Cr<sup>3+</sup> <sup>2</sup>E→ <sup>4</sup>A<inf>2</inf> and <sup>4</sup>T→<sup>4</sup>A<inf>2</inf> transitions. © (2014) Trans Tech Publications, Switzerland.

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  468. TL Properties of Pure Al<sub>2</sub>O<sub>3</sub> Grown by the Micro-Pulling Down Method

    Kurosawa, S; Bispo, L; Shoji, Y; Seki, M; Yokota, Y; Chubaci, JFD; Yoshikawa, A

    ADVANCED CERAMICS AND NOVEL PROCESSING   Vol. 616   page: 87 - 91   2014

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    Carbon-doped Al<inf>2</inf>O<inf>3</inf> is used as a material for dosimeter using thermoluminescence (TL) technique or optically stimulated luminescence (OSL) technique, and the emission bands are originated from defect emission. We have an original crystal growth named micro-pulling down (μ-PD) method which had higher temperature graduation during the crystal growth. Thus, crystal defect is easy to be formed without some dopant using the μ-PD method. We grew pure Al<inf>2</inf>O<inf>3</inf> samples with different heating condition, and different peaks in TL spectra were obtained among the pure Al<inf>2</inf>O<inf>3</inf>. © (2014) Trans Tech Publications, Switzerland.

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  469. Development of a single crystal with a high index of refraction

    Kurosawa, S; Kochurikhin, VV; Yamaji, A; Yokota, Y; Kubo, H; Tanimori, T; Yoshikawa, A

    NUCLEAR INSTRUMENTS & METHODS IN PHYSICS RESEARCH SECTION A-ACCELERATORS SPECTROMETERS DETECTORS AND ASSOCIATED EQUIPMENT   Vol. 732   page: 599 - 602   2013.12

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    Publisher:Nuclear Instruments and Methods in Physics Research Section A Accelerators Spectrometers Detectors and Associated Equipment  

    Time-of-flight Positron emission tomography (TOF-PET) is one of the next-generation medical imaging methods, which requires scintillators with a very short decay time. However, the shortest scintillation decay times are typically 20-30 ns, and these values are not sufficient for TOF-PET. Cherenkov counters are used in high energy physics and they are expected to be applied in medical imaging due to their short decay time. Here, high-refractive index materials are necessary for Cherenkov radiators to reach a high light output. We measured refractive indices of Gd<inf>3</inf>Ga<inf>5</inf>O<inf>12</inf> (GGG), Y<inf>3</inf>Ga<inf>5</inf>O<inf>12</inf> (YGG) and Lu<inf>3</inf>Ga <inf>5</inf>O<inf>12</inf> (LuGG) crystals grown by a micro-pulling-down (μ-PD) method. The GGG, YGG and LuGG crystals were found to have refractive indices of ~2.5, ~2.3 and ~2.3 at 400 nm, respectively. Then we grew a 40 mm diameter GGG crystal by the Czochralski method, and the emission decay times of the GGG crystals irradiated with muons and gamma rays were 10±1ns and 10±2ns, respectively, using a photomultiplier tube (Hamamatsu R6231-100). Cherenkov light of the GGG crystal could be observed for the gamma-ray irradiation. © 2013 Elsevier B.V.

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  470. Differential roles of prostaglandin E-type receptors in activation of hypoxia-inducible factor 1 by prostaglandin E<sub>1</sub> in vascular-derived cells under non-hypoxic conditions Open Access

    Suzuki, K; Nishi, K; Takabuchi, S; Kai, S; Matsuyama, T; Kurosawa, S; Adachi, T; Maruyama, T; Fukuda, K; Hirota, K

    PEERJ   Vol. 1 ( 1 ) page: e220   2013.11

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    Prostaglandin E1 (PGE<inf>1</inf>), known pharmaceutically as alprostadil, has vasodilatory properties and is used widely in various clinical settings. In addition to acute vasodilatory properties, PGE<inf>1</inf> may exert beneficial effects by altering protein expression of vascular cells. PGE<inf>1</inf> is reported to be a potent stimulator of angiogenesis via upregulation of VEGF expression, which is under the control of the transcription factor hypoxia-inducible factor 1 (HIF-1). However, the molecular mechanisms behind the phenomenon are largely unknown. In the present study, we investigated the mechanism by which PGE1 induces HIF-1 activation and VEGF gene expression in human aortic smooth muscle cells (HASMCs) and human umbilical vein endothelial cells (HUVECs), both vascular-derived cells. HUVECs and HASMCs were treated with PGE1 at clinically relevant concentrations under 20% O<inf>2</inf> conditions and HIF-1 protein expression was investigated. Expression of HIF-1α protein and the HIF-1-downstream genes were low under 20% O<inf>2</inf> conditions and increased in response to PGE<inf>1</inf> treatment in both HUVECs and HASMCs in a dose- and timedependent manner under 20% O<inf>2</inf> conditions as comparable to exposure to 1% O<inf>2</inf> conditions. Studies using EP-receptor-specific agonists and antagonists revealed that EP1 and EP3 are critical to PGE<inf>1</inf>-induced HIF-1 activation. In vitro vascular permeability assays using HUVECs indicated that PGE<inf>1</inf> increased vascular permeability in HUVECs. Thus, we demonstrate that PGE1 induces HIF-1α protein expression and HIF-1 activation under non-hypoxic conditions and also provide evidence that the activity of multiple signal transduction pathways downstream of EP1 and EP3 receptors is required for HIF-1 activation. © Copyright 2013 Suzuki et al.

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  471. Spatial resolution of a μPIC-based neutron imaging detector Open Access

    Parker, JD; Harada, M; Hattori, K; Iwaki, S; Kabuki, S; Kishimoto, Y; Kubo, H; Kurosawa, S; Matsuoka, Y; Miuchi, K; Mizumoto, T; Nishimura, H; Oku, T; Sawano, T; Shinohara, T; Suzuki, J; Takada, A; Tanimori, T; Ueno, K

    NUCLEAR INSTRUMENTS & METHODS IN PHYSICS RESEARCH SECTION A-ACCELERATORS SPECTROMETERS DETECTORS AND ASSOCIATED EQUIPMENT   Vol. 726   page: 155 - 161   2013.10

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    We present a detailed study of the spatial resolution of our time-resolved neutron imaging detector utilizing a new neutron position reconstruction method that improves both spatial resolution and event reconstruction efficiency. Our prototype detector system, employing a micro-pattern gaseous detector known as the micro-pixel chamber (μPIC) coupled with a field-programmable-gate-array- based data acquisition system, combines 100μm-level spatial and sub-μs time resolutions with excellent gamma rejection and high data rates, making it well suited for applications in neutron radiography at high-intensity, pulsed neutron sources. From data taken at the Materials and Life Science Experimental Facility within the Japan Proton Accelerator Research Complex (J-PARC), the spatial resolution was found to be approximately Gaussian with a sigma of 103.48±0.77μm (after correcting for beam divergence). This is a significant improvement over that achievable with our previous reconstruction method (334±13μm), and compares well with conventional neutron imaging detectors and with other high-rate detectors currently under development. Further, a detector simulation indicates that a spatial resolution of less than 60μm may be possible with optimization of the gas characteristics and μPIC structure. We also present an example of imaging combined with neutron resonance absorption spectroscopy. © 2013 Elsevier B.V.

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  472. Growth of column-shaped and plate-like langasite-type piezoelectric single crystals and their physical properties

    Yokota, Y; Sato, M; Chani, V; Futami, Y; Tota, K; Kurosawa, S; Onodera, K; Yoshikawa, A

    SENSORS AND ACTUATORS A-PHYSICAL   Vol. 200   page: 56 - 59   2013.10

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    Column-shaped Ca<inf>3</inf>TaGa<inf>3</inf>Si<inf>2</inf> O<inf>14</inf> (CTGS) and plate-like Ca<inf>3</inf>NbGa<inf>3</inf>Si<inf>2</inf> O <inf>14</inf> (CNGS) single crystals were grown by micro-pulling-down method using crucibles of original shape. The column-shaped CTGS crystals oriented along a- and c-axes were produced using the seeds of corresponding orientations. The plate-like CNGS crystal was grown along a-axis from the crucible equipped with a plate-shaped die at the bottom. The X-ray diffraction patterns of the grown CTGS and CNGS crystals corresponded to langasitetype structure and the lattice parameters were consistent with those of the crystals grown by Czochralski (Cz) method. The X-ray rocking curve analysis indicated that structural perfection of the grown CTGS and CNGS shaped crystals was comparable to that of the crystals produced by Cz method. The central part of the CTGS crystal was single phase material and had excess of Ca and Si with corresponding deficit of Ta and Ga. However, peripheral parts of the crystal contained secondary phase of calcium tantalate. In the transmission spectrum, two broad absorption peaks around 360 and 490 nm were observed that was associated with the color centers relevant to the oxygen content in the crystal. © 2012 Elsevier B.V. All rights reserved.

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  473. Logistic regression analysis of risk factors for prolonged pulmonary recovery in children from aspirated foreign body

    Hidaka, H; Obara, T; Kuriyama, S; Kurosawa, S; Katori, Y; Kobayashi, T

    INTERNATIONAL JOURNAL OF PEDIATRIC OTORHINOLARYNGOLOGY   Vol. 77 ( 10 ) page: 1677 - 1682   2013.10

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    Language:English   Publisher:International Journal of Pediatric Otorhinolaryngology  

    Objective: Foreign body aspiration is a life-threatening emergency for children. Fried chicken is commonly available all over the world, but no cases have previously been reported addressing this food as a tracheobronchial foreign body. We report an extremely rare case of tracheobronchial aspiration of fried chicken complicated by severe bronchitis and postoperative atelectasis. To clarify predisposing factors related to bronchopulmonary complications, we also reviewed paediatric cases of tracheobronchial foreign bodies treated in our department over the past 14 years. Methods: We retrospectively reviewed a total of 77 cases of tracheobronchial foreign bodies from 1988 to 2011. The main outcome measure was duration of hospitalisation, reflecting postoperative therapy. Logistic regression analyses were conducted to determine risk factors for longer hospitalisation. Results: Age, sex, and interval between the aspiration episode and bronchoscopy were not significantly associated with longer hospitalisation. Regarding kinds of foreign bodies, higher rates of longer hospitalisation were noted for patients who had aspirated peanut or animal material, as compared to patients who had aspirated non-organic material (odds ratio, 5.80; 95% confidence interval, 1.12-30.43). Conclusions: In terms of predicting the risk of pulmonary complications, the type of foreign body aspirated offers a more meaningful factor than the interval between aspiration and operation. Specifically, peanuts or animal material containing oils appear to be associated with a more prolonged pulmonary recovery even after retrieval of the foreign body. © 2013 Elsevier Ireland Ltd.

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  474. Prognosis of patients with core binding factor acute myeloid leukemia after first relapse Open Access

    Kurosawa, S; Miyawaki, S; Yamaguchi, T; Kanamori, H; Sakura, T; Moriuchi, Y; Sano, F; Kobayashi, T; Yasumoto, A; Hatanaka, K; Yanada, M; Nawa, Y; Takeuchi, J; Nakamura, Y; Fujisawa, S; Shibayama, H; Miura, I; Fukuda, T

    HAEMATOLOGICA   Vol. 98 ( 10 ) page: 1525 - 1531   2013.10

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    Core binding factor acute myeloid leukemia is known to have a favorable prognosis, however, there have been no detailed analyses on prognostic factors after first relapse. Using a nationwide database, we retrospectively analyzed core binding factor acute myeloid leukemia patients who relapsed after being treated with chemotherapy alone during their first complete remission. Of a total of 397 patients who were diagnosed with core binding factor acute myeloid leukemia, 208 experienced a first relapse, and analyses were performed in 139 patients for whom additional data were available. In the entire cohort, the overall survival rate after relapse was 48% at 3 years. By multivariate analysis, younger age at diagnosis, a longer interval before relapse, and inv(16) were shown to be independently associated with better survival after relapse. Although there was no significant difference in survival after relapse between patients who underwent allogeneic hematopoietic cell transplantation and those who did not in the overall series of relapsed patients, we found that transplantation significantly improved survival among patients who had t(8;21) (54% versus 26% at 3 years, P=0.002). In addition, among patients with t(8;21), those who had different cytogenetics at relapse had a significantly improved survival after transplantation, while those who had same cytogenetics did not. We showed that the prognosis differs significantly and optimal treatment strategies may vary between groups of patients with core binding factor acute myeloid leukemia with different cytogenetic profiles at relapse. These findings may help to guide therapeutic decisions after first relapse. © 2013 Ferrata Storti Foundation.

    DOI: 10.3324/haematol.2012.078030

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  475. Simulation of gas avalanche in a micro pixel chamber using Garfield plus Open Access

    Takada, A; Tanimori, T; Kubo, H; Parker, JD; Mizumoto, T; Mizumura, Y; Iwaki, S; Sawano, T; Nakamura, K; Taniue, K; Higashi, N; Matsuoka, Y; Komura, S; Sato, Y; Namamura, S; Oda, M; Sonoda, S; Tomono, D; Miuchi, K; Kabuki, S; Kishimoto, Y; Kurosawa, S

    JOURNAL OF INSTRUMENTATION   Vol. 8 ( 10 )   2013.10

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    A micro pixel chamber (μ-PIC), the development of which started in 2000 as a type of a micro pattern gas detector, has a high gas gain greater than 6000 in stable operation, a large detection area of 900 cm<sup>2</sup>, and a fine position resolution of about 120 μm. However, for its development, simulation verification has not been very useful, because conventional simulations explain only part of the experimental data. On the other hand, some μ-PIC applications require precise understanding of the fluctuation of the gas avalanche and signal waveform for their improvement; therefore, there is a need to update the μ-PIC simulation. Hence, we adopted Garfield++, which is developed for simulating a microscopic avalanche in an effort to explain experimental data. The simulated avalanche size was well consistent with the experimental gas gain. Moreover, we calculated a signal waveform and successfully explained the pulse height and time-over-threshold. These results clearly indicate that the simulation of μ-PIC applications will improve and that Garfield++ simulation will easily facilitate the μ-PIC development.© 2013 IOP Publishing Ltd and Sissa Medialab srl.

    DOI: 10.1088/1748-0221/8/10/C10023

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  476. Development of a High Sensitivity Gamma Camera with Unmanned Helicopter for Environmental Survey

    SHIMAZOE Kenji, TAKAHASHI Hiroyuki, KUROWSAWA Shunsuke, KAMADA Kei, YOSHIKAWA Akira, SATO Hiroki, USUKI Yoshiyuki, SHIKAZE Yoshiaki, TORII Tateo

      Vol. 2013 ( 1 ) page: 13 - 17   2013.9

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  477. Comparative study of optical and scintillation properties of Tm<SUP>3+</SUP>:YAG, and Tm<SUP>3+</SUP>:LuAG single crystals

    Fujimoto, Y; Sugiyama, M; Yanagida, T; Wakahara, S; Suzuki, S; Kurosawa, S; Chani, V; Yoshikawa, A

    OPTICAL MATERIALS   Vol. 35 ( 11 ) page: 2023 - 2026   2013.9

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    The optical and scintillation properties of Tm<sup>3+</sup>-doped yttrium aluminum garnet Y<inf>3</inf>Al<inf>5</inf>O<inf>12</inf> (YAG) and Tm <sup>3+</sup>-doped lutetium aluminum garnet Lu<inf>3</inf>Al<inf>5</inf>O <inf>12</inf> (LuAG) are compared. The Tm<sup>3+</sup>-doped single crystals were grown by the micro-pulling down (μ-PD) technique. Both crystals demonstrated some emission peaks originated from 4f-4f forbidden transition of Tm<sup>3+</sup> under <sup>241</sup>Am alpha-ray excitation. The scintillation decay time of Tm<sup>3+</sup>-doped YAG was similar to that of LuAG. When irradiated by the gamma-rays from a <sup>137</sup>Cs source, the relative scintillation light yields of Tm:YAG was 90% greater than that of Tm:LuAG. © 2012 Elsevier B.V. All rights reserved.

    DOI: 10.1016/j.optmat.2012.10.010

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  478. Crystal growth and characterization of Ce:Gd<sub>3</sub>(Ga,Al)<sub>5</sub>O<sub>12</sub> single crystal using floating zone method in different O<sub>2</sub> partial pressure

    Yoshikawa, A; Fujimoto, Y; Yamaji, A; Kurosawa, S; Pejchal, J; Sugiyama, M; Wakahara, S; Futami, Y; Yokota, Y; Kamada, K; Yubuta, K; Shishido, T; Nikl, M

    OPTICAL MATERIALS   Vol. 35 ( 11 ) page: 1882 - 1886   2013.9

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    Multicomponent garnet Ce:Gd<inf>3</inf>(Ga,Al)<inf>5</inf>O<inf>12</inf> (Ce:GAGG) single crystals show very high light yield with reasonably fast scintillation response. Therefore, they can be promising scintillators for gamma-ray detection. However, in the decay curve a very slow component does exist. Therefore, it is necessary to optimize further the crystal growth technology of Ce:GAGG. In this study, Ce:GAGG single crystals were grown by the floating zone (FZ) method under atmospheres of various compositions such as Ar 100%, Ar 80% + O<inf>2</inf> 20%, Ar 60% + O<inf>2</inf> 40% and O<inf>2</inf> 100%. Radioluminescence spectra are dominated by the band at about 540 nm due to Ce<sup>3+</sup> 5d<inf>1</inf>-4f transition. The Ce:GAGG single crystal grown under Ar atmosphere shows an intense slower decay component. It can be related to the processes of the delayed radiative recombination and thermally induced ionization of 5d<inf>1</inf> level of Ce<sup>3+</sup> center possibly further affected by oxygen vacancies. This slower decay process is significantly suppressed in the samples grown under the O<inf>2</inf> containing atmosphere. © 2012 Elsevier B.V. All rights reserved.

    DOI: 10.1016/j.optmat.2013.02.021

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  479. Doping concentration dependence on VUV luminescence of Tm:CaF<sub>2</sub> Open Access

    Kawaguchi, N; Yanagida, T; Futami, Y; Fujimoto, Y; Fukuda, K; Kajimoto, S; Fukumura, H; Kurosawa, S; Yokota, Y; Yoshikawa, A

    OPTICAL MATERIALS   Vol. 35 ( 11 ) page: 1898 - 1901   2013.9

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    Luminescence and scintillation properties of Tm<sup>3+</sup> 0.1-15% doped CaF<inf>2</inf> crystals were systematically investigated. The crystals were grown by a simple solidification method which allowed us to obtain single crystals conveniently. In X-ray induced radio luminescence spectra, the luminosity of the self-trapped-exciton (STE) emission of CaF<inf>2</inf> at 270 nm decreased with increasing of Tm<sup>3+</sup> concentration. The Tm <sup>3+</sup> 5d-4f transition based emission lines appeared at 175 nm (4f <sup>11</sup>5d high spin state (HS) → <sup>3</sup>H<inf>6</inf>) and at 165 nm (low spin state (LS) to <sup>3</sup>H<inf>6</inf>). Pulse height spectra were measured under α-ray irradiation by using vacuum ultra-violet (VUV) sensitive photomultiplier tube (PMT) R8778 and Tm<sup>3+</sup> 0.1% doped specimen exhibited the highest light yield. © 2012 Elsevier B.V. All rights reserved.

    DOI: 10.1016/j.optmat.2013.01.026

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  480. Evaluation of Ce<SUP>3+</SUP> and alkali metal ions Co-doped LiSrAlF<sub>6</sub> crystalline scintillators

    Wakahara, S; Yanagida, T; Fujimoto, Y; Yokota, Y; Pejchal, J; Kurosawa, S; Suzuki, S; Kawaguchi, N; Fukuda, K; Yoshikawa, A

    RADIATION MEASUREMENTS   Vol. 56   page: 111 - 115   2013.9

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    Publisher:Radiation Measurements  

    High scintillation efficiency of Eu-doped LiSrAlF<inf>6</inf> (LiSAF) and LiCaAlF<inf>6</inf> (LiCAF) codoped with alkali metal ions has been reported in our recent studies. Thus in this paper, we demonstrated the scintillation properties of 1% Ce-doped LiSAF crystals with 1% alkali metal ions co-doping to increase the light yield and understand the scintillation mechanism. The crystals showed intense emission band corresponding to the 5d-4f transition of Ce<sup>3+</sup>, and their light yields under thermal neutron excitation were higher than that of the Ce only doped crystal. Especially, the light yield of Ce-Na co-doped crystal exceeded about two times that of Ce only doped one. © 2013 Elsevier Ltd. All rights reserved.

    DOI: 10.1016/j.radmeas.2012.12.022

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  481. Optical properties and radiation response of Ce:SrHfO<sub>3</sub> prepared by the Spark Plasma Sintering Method

    Kurosawa, S; Pejchal, J; Wakahara, S; Yokota, Y; Yoshikawa, A

    RADIATION MEASUREMENTS   Vol. 56   page: 155 - 158   2013.9

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    SrHfO<inf>3</inf>, Ce<inf>0.02</inf>Sr<inf>0.98</inf>HfO<inf>3</inf> (Ce:SHO) and Ce<inf>0.02</inf>Al<inf>0.02</inf>Sr<inf>0.96</inf>HfO<inf>3</inf> (Ce/Al:SHO) ceramics were prepared by Spark Plasma Sintering (SPS) in order to search for a new material with a high-effective atomic number. Here, SrHfO <inf>3</inf> has high melting point, and single crystal cannot be grown by micro pulling down method (which usually enables growth within less than 1 day) due to its high melting temperature. Since SPS can be used for preparation of the ceramics within roughly 10 h at temperatures lower than the melting point, we use the SPS method for material preparation. Ce:SHO had a low transparency of less than 0.1% below 540-nm, while Ce/Al:SHO had a wider transparent region including the emission wavelength region of Ce<sup>3+</sup> (∼395 nm). Ce/Al:SHO ceramics had light output of ∼4000 photons/MeV, and decay time of 21.6 ± 0.9 ns. © 2013 Elsevier B.V. All rights reserved.

    DOI: 10.1016/j.radmeas.2013.01.051

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  482. Photo- and radio-excited luminescence properties of Eu-doped La<sub>2</sub>O<sub>3</sub>-Al<sub>2</sub>O<sub>3</sub> based eutectics

    Fujimoto, Y; Kamada, K; Yanagida, T; Wakahara, S; Suzuki, S; Kurosawa, S; Yoshikawa, A

    RADIATION MEASUREMENTS   Vol. 56   page: 107 - 110   2013.9

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    Eutectic crystal of 0.5% Eu-doped 30LaAlO<inf>3</inf>-70Al <inf>2</inf>O<inf>3</inf> (vol %) was prepared by micro-pulling down (μ-PD) technique under nitrogen atmosphere. Being excited at a wavelength of 320 nm, the crystal exhibited intense emission band with a maximum at 450 nm which is corresponding to 4f<sup>6</sup>5d-4f<sup>7</sup>(<sup>8</sup>S<inf>7/2</inf>) transitions of Eu<sup>2+</sup>. The decay time and fluorescence quantum efficiency (QE) were determined to be about 475 ns and 60%, respectively. When alpha-ray excited the crystal, both Eu<sup>2+</sup> 4f<sup>6</sup>5d-4f <sup>7</sup>(<sup>8</sup>S<inf>7/2</inf>) and Eu<sup>3+</sup> 4f <sup>6</sup>-4f<sup>6</sup> (<sup>5</sup>D<inf>0</inf>-<sup>7</sup>F <inf>1,2</inf>) emission peaks were observed at 435 nm and 600 nm. By the pulse height spectra, the relative scintillation light yield of the crystal was about 4% compared with that of BGO commercial scintillator. © 2013 Elsevier Ltd. All rights reserved.

    DOI: 10.1016/j.radmeas.2013.03.028

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  483. Recent decrease in non-relapse mortality due to GVHD and infection after allogeneic hematopoietic cell transplantation in non-remission acute leukemia

    Kurosawa, S; Yakushijin, K; Yamaguchi, T; Atsuta, Y; Nagamura-Inoue, T; Akiyama, H; Taniguchi, S; Miyamura, K; Takahashi, S; Eto, T; Ogawa, H; Kurokawa, M; Tanaka, J; Kawa, K; Kato, K; Suzuki, R; Morishima, Y; Sakamaki, H; Fukuda, T

    BONE MARROW TRANSPLANTATION   Vol. 48 ( 9 ) page: 1198 - 1204   2013.9

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    Although recent improvements have been indicated in the outcome after allogeneic hematopoietic cell transplantation (allo-HCT), little information is available on how changes in transplant modalities have affected the outcomes after allo-HCT in non-remission, based on patient age, donor source and disease type. We compared the incidence and causes of non-relapse mortality (NRM) after allo-HCT in non-remission among three consecutive four-year periods using a nationwide transplant outcome registry database. A total of 3308 patients with acute leukemia in non-remission were analyzed. The risk of NRM decreased over the three periods, and the hazard ratios (HRs) in 2001-2004 and 2005-2008 compared with 1997-2000 were 0.86 (95% CI, 0.70-1.06; P=0.16) and 0.65 (95% CI, 0.53-0.80; P<0.01), respectively. A significant decrease in the HR for overall mortality was also observed in 2005-2008 (HR 0.85; 95% CI, 0.75-0.97; P=0.02). We found that a decrease in the incidences of death due to GVHD and infection contributed to the reduction in NRM, to which high-resolution donor-recipient HLA matching and other improvements may have contributed. As none of the subgroups showed improved survival without a reduction in NRM, the effective prevention of transplant-related complications appears to be necessary for improving outcomes after allo-HCT in non-remission. © 2013 Macmillan Publishers Limited.

    DOI: 10.1038/bmt.2013.42

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  484. Scintillation properties of Er-doped Y<sub>3</sub>Al<sub>5</sub>O<sub>12</sub> single crystals

    Yamaji, A; Ogino, H; Fujimoto, Y; Suzuki, A; Yanagida, T; Yokota, Y; Kurosawa, S; Yoshikawa, A

    RADIATION MEASUREMENTS   Vol. 56   page: 116 - 119   2013.9

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    Er-doped Y<inf>3</inf>Al<inf>5</inf>O<inf>12</inf> single crystals with different Er concentrations of 0.1, 1.0, 10, 30, and 50% were grown by the micro-pulling down method. There were several absorption lines due to the Er<sup>3+</sup> 4f-4f transitions in the transmittance spectra and these lines correspond to the transitions from the ground state of <sup>4</sup>I <inf>15/2</inf> to the excited states. The photo- and radio-luminescence spectra showed Er<sup>3+</sup> 4f-4f emissions. Relative light yield under 5.5 MeV alpha-ray irradiation of Er 0.1%:Y<inf>3</inf>Al<inf>5</inf>O<inf>12</inf> was estimated to be 63% of that of Bi<inf>4</inf>Ge<inf>3</inf>O<inf>12</inf>. © 2013 Elsevier Ltd. All rights reserved.

    DOI: 10.1016/j.radmeas.2013.01.056

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  485. Crystal growth and luminescence properties of Pr-doped LuLiF<sub>4</sub> single crystal

    Sugiyama, M; Yanagida, T; Yokota, Y; Kurosawa, S; Fujimoto, Y; Yoshikawa, A

    RADIATION MEASUREMENTS   Vol. 55   page: 112 - 115   2013.8

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    0.1, 1, and 3% Pr (with respect to Lu) doped LuLiF<inf>4</inf> (Pr:LuLiF<inf>4</inf>) single crystals were grown by the micro-pulling-down (μ-PD) method. Transparency of the grown crystals was higher than 70% in the visible wavelength region with some absorption bands due to Pr<sup>3+</sup> 4f-4f transitions. Intense absorption bands related with the Pr<sup>3+</sup> 4f-5d transitions were observed at 190 and 215 nm. In radioluminescence spectra, Pr<sup>3+</sup> 5d-4f emissions were observed at 220, 240, 340, and 405 nm. In the pulse height spectra recorded under <sup>137</sup>Cs γ-ray excitation, the Pr 3% doped sample showed the highest light yield of 2050 photons/MeV and the scintillation decay time of it exhibited 23 and 72 ns also excited by <sup>137</sup>Cs γ-ray. © 2012 Elsevier Ltd. All rights reserved.

    DOI: 10.1016/j.radmeas.2013.01.020

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  486. Eu and Rb co-doped LiCaAlF<sub>6</sub> scintillators for neutron detection

    Yamaji, A; Yanagida, T; Kawaguchi, N; Yokota, Y; Fujimoto, Y; Kurosawa, S; Pejchal, J; Watanabe, K; Yamazaki, A; Yoshikawa, A

    RADIATION MEASUREMENTS   Vol. 55   page: 132 - 135   2013.8

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    Eu and Rb co-doped LiCaAlF<inf>6</inf> (LiCAF) single crystals with different dopant concentrations were grown by the micro-pulling-down method for neutron detection. Their transmittance spectra showed strong absorption bands at 200-220 and 290-350 nm, and under <sup>241</sup>Am alpha-ray excitation, their radioluminescence spectra exhibited an intense emission peak at 373 nm that was attributed to the Eu<sup>2+</sup> 5d-4f transition. These results were consistent with those for the Rb-free Eu:LiCAF. The highest light yield among the grown crystals was 36,000 ph/n, which was 20% greater than that of the Rb-free crystal. In addition, the neutron-excited scintillation decay times were 650-750 ns slower than that of the Rb-free Eu:LiCAF. © 2012 Elsevier Ltd. All rights reserved.

    DOI: 10.1016/j.radmeas.2013.04.021

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  487. Evaluation of Nd:BaY<sub>2</sub>F<sub>8</sub> for VUV scintillator

    Kurosawa, S; Yanagida, T; Pejchal, J; Fukuda, K; Kawaguchi, N; Ishizu, S; Suyama, T; Nakagawa, M; Yokota, Y; Nikl, M; Yoshikawa, A

    RADIATION MEASUREMENTS   Vol. 55   page: 108 - 111   2013.8

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    Vacuum Ultra violet (VUV) scintillators, have a short decay time around several ns, and therefore can be used in high counting rate applications. New Nd-doped BaY<inf>2</inf>F<inf>8</inf> VUV scintillator crystals were successfully grown by a micro-pulling down (μ-PD) method and their optical properties and radiation response were investigated. All the BaY <inf>2</inf>F<inf>8</inf> samples with 0.5, 1, 3, 7 and 10 mol% Nd concentration had 5d-4f luminescence peaks at 185, 237 and 270 nm. Although this scintillator has low light output around 70 photons/5.5-MeV alpha, which was determined from our pulse height measurement, we found that the decay time of this crystal reached 13 ns which is a typical value for the VUV scintillators. © 2012 Elsevier Ltd. All rights reserved.

    DOI: 10.1016/j.radmeas.2013.01.011

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  488. Luminescence properties and radiation response of sodium borate glasses scintillators

    Fujimoto, Y; Yanagida, T; Wakahara, S; Suzuki, S; Kurosawa, SU; Yoshikawa, A

    RADIATION MEASUREMENTS   Vol. 55   page: 124 - 127   2013.8

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    We examined basic luminescence properties and radiation response of sodium borate glass scintillators activated with Pb<sup>2+</sup>, Cu<sup>+</sup>, Ti<sup>4+</sup>, V<sup>5+</sup>, W<sup>6+</sup> and Yb<sup>3+</sup> ions, respectively. These glasses had more than 80% transparency for emission wavelength range, and strong absorption bands due to the charge transition of the ions were observed. In the photoluminescence spectra, all glasses demonstrated intense emission peak in visible region, which are corresponding to the ions with s<sup>2</sup> (Pb<sup>2+</sup>), d<sup>10</sup> (Cu<sup>+</sup>) and d<sup>0</sup> (Ti<sup>4+</sup>, V<sup>5+</sup>, W<sup>6+</sup>) configuration. Additionally charge transfer emission was observed in Yb <sup>3+</sup>-doped glass. When <sup>241</sup>Am 5.5 MeV alpha-ray excited the glasses, they showed weak emission intensity because of low energy transfer efficiency from host lattice to emission center. By <sup>241</sup>Am irradiated pulse height spectra, Cu<sup>+</sup>-doped glass demonstrated the highest scintillation output in the glasses. © 2012 Elsevier Ltd. All rights reserved.

    DOI: 10.1016/j.radmeas.2013.01.017

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  489. Neutron detection with LiCaAlF<sub>6</sub> scintillator doped with 3d-transition metal ions

    Kawaguchi, N; Yanagida, T; Fujimoto, Y; Furuya, Y; Futami, Y; Yamaji, A; Watanabe, K; Yamazaki, A; Uritani, A; Kajimoto, S; Fukumura, H; Kurosawa, S; Yokota, Y; Pejchal, J; Yoshikawa, A

    RADIATION MEASUREMENTS   Vol. 55   page: 128 - 131   2013.8

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    Capability of thermal neutron detection was examined for LiCaAlF <inf>6</inf> (LiCAF) scintillators doped with 3d-transition metal ions. Their radioluminescence spectra were measured with an 241-Am source to simulate <sup>6</sup>Li(n, α)<sup>3</sup>H reaction. The sufficiently intense radioluminescence was observed for the Mn, Co and Cu dopants, while only a weak one was observed for Ti, V, Fe and Ni. A Mn doped LiCAF crystal, which showed the highest radioluminescence intensity, was coupled with a Si avalanche photodiode for the examination of its neutron response. It was confirmed that the average current of the photodiode clearly increased under excitation with 13.5 meV neutron flux. © 2012 Elsevier Ltd. All rights reserved.

    DOI: 10.1016/j.radmeas.2013.03.024

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  490. Optical and scintillation property of Ce, Ho and Eu-doped PbF<sub>2</sub>

    Kurosawa, S; Yokota, Y; Yanagida, T; Yoshikawa, A

    RADIATION MEASUREMENTS   Vol. 55   page: 120 - 123   2013.8

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    PbF<inf>2</inf> crystal has favorable properties such as a high density and short radiation length, while the scintillation light output is too small to obtain a photo-absorption peak under gamma ray excitation. In this paper, we report scintillation response for 0.1 or 0.5-mol% Ce, Eu and Ho doped PbF <inf>2</inf> crystals grown by an annealing method under 5.5-MeV alpha ray excitation. Although Ce doped PbF<inf>2</inf> crystals did not show intense photo- and radio-luminescence, Eu and Ho doped ones showed several peaks excited under UV and 5.5-MeV alpha ray excitation, respectively. Additionally, full-absorption peaks in the pulse height spectra of 0.1-mol% Eu and Ho doped PbF<inf>2</inf> were ascribed to 5.5-MeV alpha-rays. © 2012 Elsevier Ltd. All rights reserved.

    DOI: 10.1016/j.radmeas.2013.03.005

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  491. Optical and scintillation properties of Sc<sub>2</sub>O<sub>3</sub>, Y<sub>2</sub>O<sub>3</sub> and Lu<sub>2</sub>O<sub>3</sub> transparent ceramics synthesized by SPS method

    Futami, Y; Yanagida, T; Fujimoto, Y; Pejchal, J; Sugiyama, M; Kurosawa, S; Yokota, Y; Ito, A; Yoshikawa, A; Goto, T

    RADIATION MEASUREMENTS   Vol. 55   page: 136 - 140   2013.8

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    Sc<inf>2</inf>O<inf>3</inf>, Y<inf>2</inf>O<inf>3</inf> and Lu <inf>2</inf>O<inf>3</inf> transparent ceramics were prepared by the spark plasma sintering (SPS) method. After polishing, the samples were semitransparent. Their optical transmittance was 10-40% at 500 nm which corresponded with their semi-transparency. In the X-ray induced emission spectra, a broad emission peak appeared around 335 nm in each sample. For this wavelength, scintillation decay time for Y<inf>2</inf>O<inf>3</inf> and Sc<inf>2</inf>O<inf>3</inf> were 22 and 48 ns, respectively. The light yield of Sc<inf>2</inf>O<inf>3</inf>, Y <inf>2</inf>O<inf>3</inf> and Lu<inf>2</inf>O<inf>3</inf> was 16,200, 2600, and 200 ph/5.5 MeV-alpha, respectively, which followed from the alpha-ray induced pulse height spectra. The gamma-ray induced light yield of Sc<inf>2</inf>O <inf>3</inf> was 11,500 ph/MeV, which is 1.4 times larger than that of conventional single crystal BGO (Bi<inf>4</inf>Ge<inf>3</inf>O<inf>12</inf>) scintillator. Light yield non-proportionality and energy resolution of Sc <inf>2</inf>O<inf>3</inf> were examined for the first time. © 2012 Elsevier Ltd. All rights reserved.

    DOI: 10.1016/j.radmeas.2013.01.014

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  492. Study of the correlation of scintillation decay and emission wavelength

    Yanagida, T; Fujimoto, Y; Yamaji, A; Kawaguchi, N; Kamada, K; Totsuka, D; Fukuda, K; Yamanoi, K; Nishi, R; Kurosawa, S; Shimizu, T; Sarukura, N

    RADIATION MEASUREMENTS   Vol. 55   page: 99 - 102   2013.8

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    In photoluminescence which directly excites the emission center of phosphor material is known to have a correlation between the emission wavelength and the decay time based on quantum mechanics. In scintillation phenomenon, host lattice of the material is first excited by ionizing radiation and then the excitation energy is transferred to emission centers. For the first time, we investigated the correlation between the scintillation decay and the emission wavelength by using pulse X-ray equipped streak camera system which could observe time and wavelength resolved scintillation phenomenon. Investigated materials were Ce<sup>3+</sup>, Pr<sup>3+</sup> and Nd<sup>3+</sup> doped oxides and fluorides which all showed 5d-4f transition based emission. As a result, we obtained the relation that τ (scintillation decay time) was proportional to the λ<sup>2.15</sup> (emission wavelength). © 2012 Elsevier Ltd. All rights reserved.

    DOI: 10.1016/j.radmeas.2012.05.014

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  493. Crystal growth of Eu:SrI<sub>2</sub> single crystals by micro-pulling-down method and the scintillation properties

    Yokota, Y; Nishimoto, K; Kurosawa, S; Totsuka, D; Yoshikawa, A

    JOURNAL OF CRYSTAL GROWTH   Vol. 375   page: 49 - 52   2013.7

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    Undoped and Eu doped SrI<inf>2</inf> (Eu:SrI<inf>2</inf>) single crystals were grown by the modified micro-pulling-down (μ-PD) method and their scintillation properties were investigated. Undoped and Eu:SrI<inf>2</inf> single crystals with Eu 1%, 2%, 3% and 5% concentrations were obtained by the modified μ-PD method with the removable chamber system and their crystals with approximately 2 mm diameter and 2-3 cm length indicated high transparency. Powder X-ray diffraction patterns of grown Eu:SrI<inf>2</inf> crystals revealed that the Eu:SrI<inf>2</inf> crystals had a single phase of SrI<inf>2</inf> structure and similar lattice parameters regardless of Eu concentrations. In the X-ray radioluminescence spectrum of Eu:SrI<inf>2</inf> crystal, the emission peak around 430 nm which was due to the 5d-4f transition of Eu<sup>2+</sup> ion was observed. Light yields, energy resolutions and decay times of grown Eu:SrI<inf>2</inf> crystals irradiated under γ-ray were evaluated. © 2013 Elsevier B.V.

    DOI: 10.1016/j.jcrysgro.2013.03.049

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  494. Temperature Dependence of Scintillation Properties of Bright Oxide Scintillators for Well-Logging

    Yanagida, T; Fujimoto, Y; Kurosawa, S; Kamada, K; Takahashi, H; Fukazawa, Y; Nikl, M; Chani, V

    JAPANESE JOURNAL OF APPLIED PHYSICS   Vol. 52 ( 7 )   2013.7

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    Scintillation characteristics such as the pulse height, energy resolution, and decay time of single crystals of Tl-doped NaI (Tl:NaI), Ce-doped Lu2SiO5 (Ce:LSO), Ce-doped YAlO<inf>3</inf> (Ce:YAP), Ce-doped Gd3(Al,Ga)5OL <inf>12</inf> (Ce:GAGG), Pr-doped Lu<inf>3</inf>Al<inf>5</inf>OL<inf>12</inf> (Pr:LuAG), undoped LuAG, and Ce-doped Y3Al<inf>5</inf>OL<inf>12</inf> (Ce:YAG) transparent ceramics were compared at 25-150°C to simulate well logging conditions. For increasing temperature, the light output of the scintillators decreased, mostly because of thermal quenching. Among these samples, Pr:LuAG demonstrated the highest scintillation performance at 150°C. © 2013 The Japan Society of Applied Physics.

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  495. Higher fraction of inspired oxygen in anesthesia induction does not affect functional residual capacity reduction after intubation: a comparative study of higher and lower oxygen concentration

    Kanaya, A; Satoh, D; Kurosawa, S

    JOURNAL OF ANESTHESIA   Vol. 27 ( 3 ) page: 385 - 389   2013.6

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    Background: Low fraction of inspired oxygen (F<inf>I</inf>O<inf>2</inf>) reduces the atelectasis area during anesthesia induction. However, atelectasis may occur during laryngoscopy and endotracheal intubation because lungs can collapse within a fraction of a second. We assessed the effects of ventilation with 100 and 40 % oxygen on functional residual capacity (FRC) in patients undergoing general anesthesia. Methods: Twenty patients scheduled for elective open abdominal surgery were randomized into 40 % oxygen (GI, n = 10) and 100 % oxygen (GII, n = 10) groups and FRC was measured. Preoxygenation and mask ventilation with 40 and 100 % oxygen were used in GI and GII, respectively. In both groups, 40 % oxygen was used for anesthesia maintenance after intubation. Bilateral lung ventilation was performed with volume guarantee and low tidal volume (7 ml/kg predicted body weight) using bilevel airway pressure. We measured FRC and blood gas in all patients during preoxygenation, after intubation, and during surgery. Results: FRC decreased from during preoxygenation (GI 2380 ml, GII 2313 ml) to after intubation (GI 1569 ml, GII 1586 ml) and significantly decreased during surgery (GI 1338 ml, GII 1417 ml) (P < 0.05). PaO<inf>2</inf>/F<inf>I</inf>O<inf>2</inf> decreased from during preoxygenation (GI 419 mmHg, GII 427 mmHg) to after intubation (GI 381 mmHg, GII 351 mmHg) and significantly decreased during surgery (GI 333 mmHg, GII 291 mmHg) (P < 0.05). No significant differences were found between the groups in both parameters. Conclusions: FRC significantly decreased from the awake state to surgery in both groups. FRC was not influenced by F<inf>I</inf>O<inf>2</inf> elevation at anesthesia induction. © 2013 Japanese Society of Anesthesiologists.

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  496. Impact of hepatitis C virus infection on clinical outcome in recipients after allogeneic hematopoietic cell transplantation Open Access

    Nakasone, H; Kurosawa, S; Yakushijin, K; Taniguchi, S; Murata, M; Ikegame, K; Kobayashi, T; Eto, T; Miyamura, K; Sakamaki, H; Morishima, Y; Nagamura, T; Suzuki, R; Fukuda, T

    AMERICAN JOURNAL OF HEMATOLOGY   Vol. 88 ( 6 ) page: 477 - 484   2013.6

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    The impact of hepatitis C virus (HCV) infection on outcomes following allogeneic hematopoietic cell transplantation (HCT) remains a matter of debate. We have retrospectively examined the significance of HCV infection among recipients who received allogeneic HCT, using a Japan transplant outcome registry database between 2006 and 2009. Among 7,831 recipients, 136 were HCV-positive. The rate of hematopoietic recovery was lower in the HCV-positive group (neutrophil recovery of 500 × 10<sup>6</sup>/L or higher: 79% vs. 87% at Day 30, P=0.087; platelet recovery of 50 × 10<sup>9</sup>/L or higher: 57% vs. 65% at Day 60, P=0.012). The HCV-positive group had a significantly higher incidence of nonrelapse mortality 38% vs. 25% at 2 years, P<0.01) and inferior overall survival (41% vs. 51% at 2 years, P<0.01). A multivariate analysis revealed that HCV seropositivity was associated with an independent risk for higher nonrelapse mortality (hazard ratio: 1.65, P<0.01) and inferior overall survival (hazard ratio: 1.39, P<0.01). The incidences of death due to hepatic problems (8% vs. 2%, P<0.01), bacterial infection (10% vs. 4%, P<0.01), or graft failure (5% vs. 2%, P=0.084) tended to be higher in the HCV-positive group. HCV infection had an adverse impact on the clinical outcome following HCT, especially in the setting of unrelated transplantation. Careful evaluation before embarking on HCT and intensive assessment against complications are warranted in HCV-infected recipients. © 2013 Wiley Periodicals, Inc.

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  497. [Perioperative management of lung transplantations in patients with pulmonary arterial hypertension compared with that in patients with lymphangiomyomatosis].

    Adachi K, Kurosawa S, Wagatsuma T, Yamamoto Y, Kameyama E, Nishino R

    Masui. The Japanese journal of anesthesiology   Vol. 62 ( 5 ) page: 573 - 9   2013.5

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  498. Differences in the released endothelial microparticle subtypes between human pulmonary microvascular endothelial cells and aortic endothelial cells in vitro

    Takahashi, T; Kobayashi, S; Fujino, N; Suzuki, T; Ota, C; Tando, Y; He, M; Yamada, M; Kurosawa, S; Yamaya, M; Kubo, H

    EXPERIMENTAL LUNG RESEARCH   Vol. 39 ( 4-5 ) page: 155 - 161   2013.5

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    Circulating endothelial microparticles (EMPs) are membrane vesicles that are shed into the blood stream from activated or apoptotic endothelial cells. We previously reported that circulating EMP numbers significantly increased in stable chronic obstructive pulmonary disease (COPD) patients and during exacerbation compared with healthy control subjects. However, different types of circulating EMPs with distinct time profiles were detectable during exacerbations. We hypothesized that the released EMP subtypes correlated with differences in the inflammatory stimuli and the endothelial cell type. We compared the EMP subtypes from human aortic endothelial cells (Aortic ECs) and human lung microvascular endothelial cells (Pulmonary microvascular ECs) released in response to various stimuli, including proinflammatory cytokines (TNFα), oxidative stress (H2O2), and cigarette smoke extracts (CSE) in vitro. We defined circulating EMPs by the expression of endothelial antigens: CD144<sup>+</sup> MPs (VE-cadherin EMPs), CD31<sup>+</sup>/CD41<sup>-</sup> MPs (PECAM EMPs), CD62E<sup>+</sup> MPs (E-selectin EMPs), and CD146<sup>+</sup> MPs (MCAM EMPs). E-selectin EMPs were released from both pulmonary microvascular and aortic ECs in response to TNFα but not to H2O2 or CSE stimulation. The amount of MCAM EMPs released from pulmonary microvascular ECs differed significantly between the cells stimulated with H2O2 and those stimulated with CSE. VE-cadherin EMPs were only released from aortic ECs, whereas PECAM EMPs were released exclusively from pulmonary microvascular ECs. The EMP subtypes released differ in vitro among TNFα, H2O2, and CSE stimulation as well as between pulmonary microvascular and aortic ECs. The differences in circulating EMP subtypes may reflect a condition or site of endothelial injury and may serve as markers for endothelial damage in COPD patients. Copyright © 2013 Informa Healthcare USA, Inc.

    DOI: 10.3109/01902148.2013.784932

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  499. Perioperative management of lung transplantations in patients with pulmonary arterial hypertension compared with that in patients with lymphangiomyomatosis

    Adachi K., Kurosawa S., Wagatsuma T., Yamamoto Y., Kameyama E., Nishino R.

    Japanese Journal of Anesthesiology   Vol. 62 ( 5 ) page: 573 - 579   2013.5

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    Background : 'The number of lung transplantation has tended to increase as a treatment for patients with pulmonary arterial hypertension (PAH) and lymphangiomyomatosis (LAM) in Japan. However, we have little evidence about the comparison of perioperative management in patients with PAH and that in patients with LAM. Methods : In this retrospective study, ten patients with PAH and seventeen patients with LAM who underwent the lung transplantations between 2006 and 2011 were enrolled. Results : PAH patients received double lung transplantation with intraoperative cardiopulmonary bypass (CPB) support. Before anesthesia induction, percutaneous cardiopulmonary support (PCPS) was begun. Most of LAM patients received single lung transplantation without using CPB support and PCPS support before anesthesia induction. But sometimes during an operation PCPS support was necessary. Postoperative PCPS support showed no significant differences between PAH and LAM. The four year survival rate was 80% (PAH) and 87.8% (LAM). Pa<inf>O2</inf>/F<inf>IO2</inf> in patients with PAH and in those with LAM, %FEV<inf>1.0</inf> in those with LAM after surgery improved when compared to those before surgery. Conclusions : The large difference in perioperative management between patients with PAH and those with LAM is an important knowledge for anesthesist.

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  500. [Assessment of the perioperative factors contributing to the hemodynamic changes during surgery in ten patients with pheochromocytoma].

    Konno D, Nishino R, Ejima Y, Ohnishi E, Sato K, Kurosawa S

    Masui. The Japanese journal of anesthesiology   Vol. 62 ( 4 ) page: 421 - 5   2013.4

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  501. Assessment of the perioperative factors contributing to the hemodynamic changes during surgery in ten patients with pheochromocytoma

    Konno D., Nishino R., Ejima Y., Ohnishi E., Sato K., Kurosawa S.

    Japanese Journal of Anesthesiology   Vol. 62 ( 4 ) page: 421 - 425   2013.4

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    Background : Intensive perioperative management is required for adrenalectomy in patients with pheocromocytoma because of the unstable hemodynamics and life threatening cardiovascular disturbances due to catecholamine surge from the neuroendocrine tumors. The aim of this study was to assess the perioperative factors contributing to the hemodynamic changes during surgery in pheochromocytoma. Methods : Ten patients with pheochromocytoma undergoing elective adrenalectomy were enrolled in this retrospective study. The circulating blood volume before surgery and the perioperative factors associated with hemodynamic changes during surgery were assessd by the pulse dye densitometry and Vigileo™/FroTrac™ system, respectively. Results : The decreases of blood pressure after resections of the central veins from tumors were significantly greater in laparotomy than those in laparoscopic surgery (P<0.05). In addition, the decreases of blood pressure after resection of the central were correlated with tumor sizes (R= -0.611), perioperative noradrenaline (NA) blood levels (R= -0.860), perioperative amounts of NA in urine (R=-0.743), and mean stroke volume variations for 5 min after resection of the veins(R= -0.679). Conclusions : The decreases of blood pressure after resections of the central veins are dependent on the perioperative blood NA levels, the level of NA in the perioperative urine testig, and tumor sizes.

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  502. Changes in incidence and causes of non-relapse mortality after allogeneic hematopoietic cell transplantation in patients with acute leukemia/myelodysplastic syndrome: an analysis of the Japan Transplant Outcome Registry

    Kurosawa, S; Yakushijin, K; Yamaguchi, T; Atsuta, Y; Nagamura-Inoue, T; Akiyama, H; Taniguchi, S; Miyamura, K; Takahashi, S; Eto, T; Ogawa, H; Kurokawa, M; Tanaka, J; Kawa, K; Kato, K; Suzuki, R; Morishima, Y; Sakamaki, H; Fukuda, T

    BONE MARROW TRANSPLANTATION   Vol. 48 ( 4 ) page: 529 - 536   2013.4

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    The outcomes for allogeneic hematopoietic cell transplantation (allo-HCT) are heavily influenced by non-relapse mortality (NRM). We retrospectively assessed the changes in the incidence and causes of NRM after allo-HCT over the past 12 years. NRM, relapse rate and OS were analyzed using the Japan transplant outcome database of 6501 adult patients with acute leukemia or myelodysplastic syndrome who received their first allo-HCT in remission from 1997 through 2008. In multivariate analysis in patients aged 16-49 years, the adjusted hazard ratios (HRs) for NRM for 2001-2004 and 2005-2008 were 0.78 (95% confidence interval, 0.65-0.93) and 0.64 (0.54-0.78), respectively, compared with 1997-2000. The HR for overall mortality in 2005-2008 was 0.81 (0.70-0.93) compared with 1997-2000. In patients aged 50-70 years, the HRs for NRM and overall mortality in 2005-2008 were 0.56 (0.46-0.68) and 0.66 (0.47-0.93), respectively, compared with those in 2001-2004. We found that causes of death that contributed to the changes in NRM varied among subgroups. In conclusion, our study indicated that the incidence of NRM after allo-HCT has significantly decreased over the past 12 years, which has led to an improvement of OS, and also showed reductions in NRM in subgroups consisting of older patients and those who received unrelated cord blood transplantation. © 2013 Macmillan Publishers Limited All rights reserved.

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  503. Crystal Growth and Scintillation Properties of Ce-Doped K<sub>2</sub>NaLuF<sub>6</sub>

    Yamaji, A; Fujimoto, Y; Yanagida, T; Kawaguchi, N; Yokota, Y; Kurosawa, S; Yoshikawa, A

    IEEE TRANSACTIONS ON NUCLEAR SCIENCE   Vol. 60 ( 2 ) page: 1024 - 1026   2013.4

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    Ce 0.1, 0.5, 1.0, and 2.0 mol%-doped K<inf>2</inf>NaLuF<inf>6</inf> crystals with 2 mm in diameter and 30-50 mm in length were grown by micro-pulling-down method. The photoluminescence spectra under ultraviolet excitation showed intense emission ascribed to 5d-4f transitions of Ce <sup>3+</sup> replacing Lu<sup>3+</sup> isolated octahedral site. In the radioluminescenced spectra under alpha-ray irradiation, the emission band is due to the transition from the lowest 5d excited state of Ce<sup>3+</sup> to 2F<inf>5/2</inf> ground state level is dominant. The light yields of Ce:K <inf>2</inf>NaLuF}<inf>6</inf> under 5.5-MeV alpha-ray excitation was estimated to be approximately 1.2 to 1.8% of those of BGO. © 1963-2012 IEEE.

    DOI: 10.1109/TNS.2013.2247061

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  504. Invasive fungal infections after allogeneic haematopoietic stem cell transplantation in Japan

    Oshima, K; Taniguchi, S; Kurosawa, S; Ogawa, H; Ohashi, K; Eto, T; Sakamaki, H; Yabe, H; Morishima, Y; Kato, K; Suzuki, R; Fukuda, T

    BONE MARROW TRANSPLANTATION   Vol. 48   page: S55 - S55   2013.4

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  505. Effect of related donor availability on outcome of AML in the context of related and unrelated hematopoietic cell transplantation

    Yanada, M; Kurosawa, S; Yamaguchi, T; Uchida, N; Miyawaki, S; Kanamori, H; Usuki, K; Kobayashi, T; Watanabe, M; Nagafuji, K; Yano, S; Nawa, Y; Tomiyama, J; Tashiro, H; Nakamura, Y; Fujisawa, S; Kimura, F; Emi, N; Miura, I; Fukuda, T

    BONE MARROW TRANSPLANTATION   Vol. 48 ( 3 ) page: 390 - 395   2013.3

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    Although allogeneic hematopoietic cell transplantation (HCT) from a related donor is effective therapy for younger patients with AML, it remains unknown how the availability of a related donor affects the outcome when unrelated HCT is a treatment option for patients without a related donor. To address this issue, we retrospectively analyzed 605 cytogenetically non-favorable AML patients younger than 50 years for whom a related donor search was performed during first CR (CR1). The 4-year OS was 62% in 253 patients with a related donor and 59% in 352 patients without a related donor (P=0.534). Allogeneic HCT was performed during CR1 in 62% and 41% of patients with and without a related donor, respectively. Among patients transplanted in CR1, the cumulative incidence of non-relapse mortality was significantly higher in patients without a related donor (P=0.022), but there was no difference in post-transplant OS between the groups (P=0.262). These findings show the usefulness of unrelated HCT in younger patients with cytogenetically non-favorable AML who do not have a related donor. The extensive use of unrelated HCT for such patients may minimize the potential disadvantage of lacking a related donor. © 2013 Macmillan Publishers Limited. All rights reserved.

    DOI: 10.1038/bmt.2012.159

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  506. Histology of symptomatic gastroesophageal reflux disease: Is it predictive of response to proton pump inhibitors?

    Miwa, H; Takubo, K; Shimatani, T; Furuta, T; Oshima, T; Tanaka, J; Aida, J; Ito, M; Kurosawa, S; Joh, T; Wada, T; Habu, Y; Watanabe, Y; Hongo, M; Chiba, T; Kinoshita, Y

    JOURNAL OF GASTROENTEROLOGY AND HEPATOLOGY   Vol. 28 ( 3 ) page: 479 - 487   2013.3

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    Background and Aim: To examine the differences in esophageal histopathology between non-erosive reflux disease (NERD) and reflux esophagitis (RE), and to investigate whether baseline esophageal histopathology can predict the therapeutic response to proton pump inhibitors (PPIs). Method: The subjects comprised 94 patients with NERD (n=71) or mild RE (n=23). Tissue was biopsied from 5cm above the squamo-columnar junction (SCJ), and the degree or presence of nine histopathological markers was assessed. The patients were treated with rabeprazole (RPZ) 10mg once daily for 4 weeks. If complete heartburn relief was not achieved, RPZ was increased to 10mg twice daily for another 2 weeks, and then to 20mg twice daily for another 2 weeks if heartburn remained. Results: Features of esophageal histopathology 5cm above the SCJ differed between NERD and RE patients. The esophageal histopathology in patients unresponsive to RPZ was characterized by Protein Gene Product (PGP) 9.5 negativity in those with NERD, and intraepithelial bleeding in those with RE. In addition, the combination of dilated intercellular spaces (DIS) (+)/PGP 9.5 (-) was indicative of strong resistance to PPI therapy in NERD patients. Conclusion: The therapeutic efficacy of PPI can be predicted from the features of biopsied esophageal tissue. Factors predictive of resistance to treatment with PPI are negativity for PGP 9.5 in NERD patients and intraepithelial bleeding in RE patients. © 2012 Journal of Gastroenterology and Hepatology Foundation and Wiley Publishing Asia Pty Ltd.

    DOI: 10.1111/j.1440-1746.2012.07266.x

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  507. Late Mortality and Causes of Death Among Long-Term Survivors After Allogeneic Stem Cell Transplantation Open Access

    Atsuta, Y; Nakasone, H; Kurosawa, S; Oshima, K; Sakai, R; Ohashi, K; Fukuda, T; Takahashi, S; Mori, T; Morishima, Y; Kato, K; Yabe, H; Sakamaki, H; Taniguchi, S

    BIOLOGY OF BLOOD AND MARROW TRANSPLANTATION   Vol. 19 ( 2 ) page: S150 - S151   2013.2

  508. Luminescence and scintillation mechanism in Ce3+ and Pr3+ doped (Lu,Y,Gd)3(Ga,Al)5O12 single crystal scintillators

    Nikl M., Kamada K., Kurosawa S., Yokota Y., Yoshikawa A., Pejchal J., Babin V.

    Physica Status Solidi C Current Topics in Solid State Physics   Vol. 10 ( 2 ) page: 172 - 175   2013.2

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    Luminescence processes occurring in the 5d<sup>1</sup> excited state of Ce<sup>3+</sup> and Pr<sup>3+</sup> centers in the (Gd,RE)<inf>3</inf>(Ga,Al)<inf>5</inf>O<inf>12</inf>, RE=Lu,Y, multicomponent garnet host were studied by purely optical contactless methods. Combination of measurements of the prompt nanosecond decay and slow delayed radiative recombination decay allows to resolve the presence of thermal quenching and thermally induced ionization processes acting upon the 5d<sup>1</sup> excited state. Additional energy transfer process depleting the 5d<sup>1</sup> state of Pr<sup>3+</sup> center was found and is due to the resonance of 5d<sup>1</sup>-<sup>3</sup>H<inf>4</inf> emission transition of Pr<sup>3+</sup> and <sup>8</sup>S-<sup>6</sup>P<inf>x</inf> absorption transition of Gd<sup>3+</sup> which might be responsible for noticeably lower light yield in Pr-doped multicomponent garnets. © 2013 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim.

    DOI: 10.1002/pssc.201200499

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  509. Scintillation properties of Yb<SUP>3+</SUP>-doped YAG transparent ceramics

    Fujimoto, Y; Yanagida, T; Wakahara, S; Yagi, H; Yanagidani, T; Kurosawa, S; Yoshikawa, A

    OPTICAL MATERIALS   Vol. 35 ( 4 ) page: 778 - 781   2013.2

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    We investigated scintillation properties of Yb<sup>3+</sup>-doped Y <inf>3</inf>A<inf>5</inf>O<inf>12</inf> (YAG) transparent ceramics with different dopant concentrations. The transparency of both 0.3% and 15% Yb <sup>3+</sup>-doped exceeded 70% in the wavelength range 300-800 nm, and two kinds of absorption bands due to charge transfer (CT) transition and 4f-4f forbidden transition of Yb<sup>3+</sup> were observed around 200-250 nm and 900 nm, respectively. Ultraviolet luminescence caused by the CT transition between Yb<sup>3+</sup> and O<sup>2-</sup> was observed under α-ray excitation from <sup>241</sup>Am sealed source. The scintillation decay times were determined to be about 2.2 ns (Yb 0.3%) and 1.4 ns (Yb 15%) using the streak camera system equipped with pulsed X-ray source. From <sup>241</sup>Am alpha-ray-excited pulse height spectra, the relative scintillation light yield of 0.3% and 15% Yb<sup>3+</sup>-doped ceramics was 7% and 10% compared with that of BGO commercial scintillator. © 2012 Elsevier B.V. All rights reserved.

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  510. Vacuum Ultraviolet Fluorescence Spectroscopy of Nd<SUP>3+</SUP>:LaF<sub>3</sub> Using Femtosecond Extreme Ultraviolet Free Electron Laser

    Shinzato, Y; Yamanoi, K; Nishi, R; Takeda, K; Nakazato, T; Shimizu, T; Sarukura, N; Cadatal-Raduban, M; Fukuda, K; Kurosawa, S; Yokota, Y; Yoshikawa, A; Togashi, T; Nagasono, M; Ishikawa, T

    APPLIED PHYSICS EXPRESS   Vol. 6 ( 2 )   2013.2

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    Time-resolved vacuum ultraviolet (VUV) fluorescence was observed from a Czochralski method-grown Nd<sup>3+</sup>:LaF<inf>3</inf> crystal excited by 61 nm femtosecond pulses from the extreme ultraviolet free-electron laser (EUV-FEL). The 172 nm fluorescence peak exhibited double exponential fluorescence decay with slow and fast decay components of 6.7 and 1.9 ns, respectively. The spectral profile is similar to those previously reported, but the double exponential nature has never been attained using conventional short-wavelength pulsed lasers. Our results demonstrate the importance of the EUV-FEL for short-wavelength spectroscopy, not just for rare-earth-doped fluorides but also for wide-band-gap semiconductors such as AlGaN. Copyright © 2013 The Japan Society of Applied Physics.

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  511. Annealing Effects for Ca<sub>3</sub>NbGa<sub>3</sub>Si<sub>2</sub>O<sub>14</sub> Piezoelectric Single Crystals Grown by Micro-Pulling-Down Method

    Yokota, Y; Kitahara, M; Kurosawa, S; Sato, M; Tota, K; Onodera, K; Yoshikawa, A

    FERROELECTRICS   Vol. 455 ( 1 ) page: 1 - 5   2013.1

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    The langasite-type Ca<inf>3</inf>NbGa<inf>3</inf>Si<inf>2</inf>O <inf>14</inf> [CNGS] piezoelectric crystals grown in Air and Ar were annealed under various temperatures and atmospheres and the effects of annealing on various properties were investigated. The absorption peaks around 360 and 500 nm of CNGS crystals grown in Air decreased by the annealing at 1300°C in Ar. On the other hand, the annealing at 1300°C in Air decreased transmittance in the range from 300 to 500 nm for the CNGS crystal grown in Ar. The results suggest that the absorptions around 350 and 500 nm originate from the excess oxygen and the post-annealing can control the oxygen content in the crystals. © 2013 Copyright Taylor and Francis Group, LLC.

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  512. Effects of Growth Atmosphere on Crystal Growth and Optical Properties for Ca<sub>3</sub>NbGa<sub>3</sub>Si<sub>2</sub>O<sub>14</sub> Single Crystals

    Yokota, Y; Sato, M; Tota, K; Kurosawa, S; Onodera, K; Yoshikawa, A

    FERROELECTRICS   Vol. 449 ( 1 ) page: 147 - 153   2013.1

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    Ca<inf>3</inf>NbGa<inf>3</inf>Si<inf>2</inf>O1<inf>4</inf> (CNGS) single crystals were grown by the micro-pulling-down (μ-PD) method under various atmosphere, Air, Ar + 3%O<inf>2</inf> and Ar 100%, and the effects of growth atmosphere on crystal growth and optical properties were investigated. While the CNGS crystal grown in Air indicated orange color, the crystal grown in Ar was colorless. CNGS crystal grown in Air indicated several large absorption peaks around 360 and 500 nm in the transmittance spectrum. In contrast, the crystal grown in Ar didn't indicate these absorption peaks. Copyright © Taylor and Francis Group, LLC.

    DOI: 10.1080/00150193.2013.822780

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  513. Neutron imaging detector based on the μPIC micro-pixel chamber Open Access

    Parker, JD; Hattori, K; Fujioka, H; Harada, M; Iwaki, S; Kabuki, S; Kishimoto, Y; Kubo, H; Kurosawa, S; Miuchi, K; Nagae, T; Nishimura, H; Oku, T; Sawano, T; Shinohara, T; Suzuki, J; Takada, A; Tanimori, T; Ueno, K

    NUCLEAR INSTRUMENTS & METHODS IN PHYSICS RESEARCH SECTION A-ACCELERATORS SPECTROMETERS DETECTORS AND ASSOCIATED EQUIPMENT   Vol. 697   page: 23 - 31   2013.1

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    Publisher:Nuclear Instruments and Methods in Physics Research Section A Accelerators Spectrometers Detectors and Associated Equipment  

    We have developed a prototype time-resolved neutron imaging detector employing the micro-pixel chamber (μPIC), a micro-pattern gaseous detector, coupled with a field programmable gate array-based data acquisition system for applications in neutron radiography at high-intensity neutron sources. The prototype system, with an active area of 10×10 cm <sup>2</sup> and operated at a gas pressure of 2 atm, measures both the energy deposition (via time-over-threshold) and three-dimensional track of each neutron-induced event, allowing the reconstruction of the neutron interaction point with improved accuracy. Using a simple position reconstruction algorithm, a spatial resolution of 349±36μm was achieved, with further improvement expected. The detailed tracking allows strong rejection of background gamma-rays, resulting in an effective gamma sensitivity of 10 <sup>-12</sup> or less, coupled with stable, robust neutron identification. The detector also features a time resolution of 0.6μs. © 2012 Elsevier B.V.

    DOI: 10.1016/j.nima.2012.08.036

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  514. 26aXZB-9 Recent Results for the μPIC Neutron Imaging Detector with DAQ Upgrade Open Access

    Parker J. D., Kabuki S., Harada M., Hattori K., Iwaki S., Kishimoto Y., Kubo H., Kurosawa S., Matsuoka Y., Miuchi K., Suzuki J., Tanimori T., Mizumoto T., Takada A., Oku T., Nishimura H., Sawano T., Shinohara T., Ueno K., Ikeno M., Tanaka M., Uchida T.

    Meeting Abstracts of the Physical Society of Japan   Vol. 68.1.1 ( 0 ) page: 147   2013

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    DOI: 10.11316/jpsgaiyo.68.1.1.0_147_4

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  515. 26aXZB-9 Recent Results for the μPIC Neutron Imaging Detector with DAQ Upgrade

    Kabuki S., Kishimoto Y., Kurosawa S., Kubo H., Matsuoka Y., Miuchi K., Mizumoto T., Nishimura H., Oku T., Sawano T., Suzuki J., Shinohara T., Takada A., Tanimori T., Ueno K., Ikeno M., Tanaka M., Uchida T., Hattori K., Parker J. D., Harada M., Iwaki S.

    Meeting Abstracts of the Physical Society of Japan   Vol. 68.1.4 ( 0 ) page: 1014   2013

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    DOI: 10.11316/jpsgaiyo.68.1.4.0_1014_2

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  516. Decreased Expression of a Novel Prostaglandin Transporter, OAT-PG, Facilitates Renocortical PGE<sub>2</sub> Accumulation during Rat Pregnancy

    Kazama, I; Matsubara, M; Kanai, Y; Hatano, R; Asano, S; Endo, Y; Toyama, H; Ejima, Y; Kurosawa, S; Maruyama, Y

    GYNECOLOGIC AND OBSTETRIC INVESTIGATION   Vol. 76 ( 3 ) page: 163 - 170   2013

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    Background: Prostaglandin (PG)-specific organic anion transporter (OAT-PG) is a recently identified renal transporter involved in the local clearance of prostaglandin E<inf>2</inf> (PGE<inf>2</inf>). Since the renal biosynthesis of PGE<inf>2</inf> is not increased during pregnancy, this transporter expression would affect the gestational changes in the renal PGE<inf>2</inf> content. Methods: Kidneys from rats at different gestational stages were used to examine gestational changes in the renocortical PGE<inf>2</inf> concentration. The renal expression of OAT-PG and the enzymes for PGE<inf>2</inf> synthesis was also examined sequentially, together with the gestational changes in renal renin production. Results: The renocortical PGE<inf>2</inf> concentration was significantly increased during midterm to late pregnancy, with a maximum increase of 47.6 ± 11.5% from the virgin value. Although the expression of the enzymes, such as cyclooxygenases and PG synthases, was not increased, that of OAT-PG was significantly decreased throughout pregnancy, inversely correlating with changes in the renocortical PGE<inf>2</inf> concentration. Renal renin production was significantly increased during pregnancy. Conclusion: This study demonstrated for the first time that the tissue PGE<inf>2</inf> concentration was increased in pregnant rat kidneys, which may be associated with the gestational rise in glomerular filtration rate. The decreased expression of OAT-PG was thought to be responsible for the increased tissue PGE<inf>2</inf> content. © 2013 S. Karger AG, Basel.

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  517. Evaluation of Relationships between Precipitation, Snow Depth, and Elevation

    Kikuchi, S; Kazama, S; Kurosawa, S

    PROCEEDINGS OF THE 35TH IAHR WORLD CONGRESS, VOLS III AND IV     2013

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  518. Performance Improvement of an Electron-Tracking Compton Camera by a New Track Reconstruction Method

    Komura, S; Tanimori, T; Kubo, H; Takada, A; Parker, JD; Mizumoto, T; Mizumura, Y; Sonoda, S; Tomono, D; Sawano, T; Nakamura, K; Matsuoka, Y; Nakamura, S; Oda, M; Kabuki, S; Kishimoto, Y; Kurosawa, S; Iwaki, S; Sato, Y; Tanaka, M; Ikeno, M; Uchida, T

    2013 IEEE NUCLEAR SCIENCE SYMPOSIUM AND MEDICAL IMAGING CONFERENCE (NSS/MIC)     2013

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  519. Precise low-energy electron tracking using a gaseous Time Projection Chamber for the balloon-borne gamma ray compton telescope

    Mizumoto T., Tanimori T., Kubo H., Takada A., Parker J.D., Sonoda S., Mizumura Y., Tomono D., Sawano T., Nakamura K., Matsuoka Y., Komura S., Nakamura S., Oda M., Miuchi K., Kabuki S., Kishimoto Y., Kurosawa S., Iwaki S., Sato Y., Tanaka M., Ikeno M., Uchida T.

    IEEE Nuclear Science Symposium Conference Record     2013

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    For MeV gamma ray astronomy, we have developed an Electron Tracking Compton Camera (ETCC) as a MeV gamma ray telescope in the next generation. Our detector consists of a gaseous Time Projection Chamber (TPC), which uses μ-PIC as the two-dimensional readout detector, and a position sensitive scintillation camera. We launched a small size ETCC with a 10 cm × 10 cm × 15 cm TPC loaded on a balloon in 2006, and obtained the fluxes of diffuse cosmic and atmospheric gamma rays (SMILE-I). As the next step of SMILE-I, we have a plan of the next measurement of MeV gamma ray celestial sources like Crab Nebula with a middle size (30 cm)<sup>3</sup> ETCC (SMILE-II) for the test of its imaging property. For SMILE-II, we developed the new Data AcQuisition (DAQ) system of an ETCC to reduce the dead time and power consumption, including the new data acquisition algorithm of electron tracking. The detection efficiency obtained using the new algorithm is about 10 times larger than the one based on the SMILE-I's algorithm. In this record, we report the new SMILE-II ETCC DAQ system and its performances. © 2013 IEEE.

    DOI: 10.1109/NSSMIC.2013.6829411

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  520. Precise Low-Energy Electron Tracking Using a Gaseous Time Projection Chamber for the Balloon-Borne Gamma Ray Compton Telescope

    Mizumoto, T; Tanimori, T; Kubo, H; Takada, A; Parker, JD; Sonoda, S; Mizumura, Y; Tomono, D; Sawano, T; Nakamura, K; Matsuoka, Y; Komura, S; Nakamura, S; Oda, M; Miuchi, K; Kabuki, S; Kishimoto, Y; Kurosawa, S; Iwaki, S; Sato, Y; Tanaka, M; Ikeno, M; Uchida, T

    2013 IEEE NUCLEAR SCIENCE SYMPOSIUM AND MEDICAL IMAGING CONFERENCE (NSS/MIC)     2013

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  521. Performance improvement of an Electron-Tracking Compton Camera by a new track reconstruction method

    Komura S., Tanimori T., Kubo H., Takada A., Parker J.D., Mizumoto T., Mizumura Y., Sonoda S., Tomono D., Sawano T., Nakamura K., Matsuoka Y., Nakamura S., Oda M., Kabuki S., Kishimoto Y., Kurosawa S., Iwaki S., Sato Y., Tanaka M., Ikeno M., Uchida T.

    IEEE Nuclear Science Symposium Conference Record     2013

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    For MeV gamma-ray Astronomy, we have developed an Electron Tracking Compton Camera (ETCC) as a next-generation MeV gamma-ray telescope. An ETCC consists of a three-dimensional electron tracker using a gaseous time projection chamber (TPC) and position-sensitive gamma-ray absorbers using pixel scintillator arrays (PSAs). We carried out the balloon borne experiment in 2006 with a small size ETCC and observed successfully the fluxes of the diffuse cosmic and atmospheric gamma rays. As the next flight, we plan to observe bright celestial sources like Crab nebula and have constructed a large size ETCC. To achieve this, an effective area must be larger than 0.5cm <sup>2</sup> for obtaining a 3 sigma level signal for 3 hours observation. To obtain the required sensitivity, we have improved the electron track reconstruction method by updating the track encoding logic and developing a simple track analysis for the new logic. We performed ground-based experiments in the new method using a test model ETCC and measured the detection efficiency, which is found to be 10 times higher than that in the previous method and consistent with the simulation. In addition, the measured angular resolution is improved remarkably. From these results, we expect that a large size ETCC will have more than 3 times better sensitivity than the original design performance. © 2013 IEEE.

    DOI: 10.1109/NSSMIC.2013.6829698

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  522. Relationships Between Annual Changes In Fev1 And Numbers Of Circulating Endothelial Microparticles In COPD Patients

    Takahashi, T; Kobayashi, S; Fujino, N; Suzuki, T; Tando, Y; Ota, C; Yamada, M; Kurosawa, S; Yanai, M; Yamaya, M; Kubo, H

    AMERICAN JOURNAL OF RESPIRATORY AND CRITICAL CARE MEDICINE   Vol. 187   2013

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  523. Development of a Time-resolved Neutron Imaging Detector Based on the μPIC Micro-Pixel Chamber

    Harada Masahide, Hattori Kaori, Don Parker Joseph, Iwaki Satoru, Miuchi Kentaro, Mizumoto Tetsuya, Matsuoka Yoshihiro, Kubo Hidetoshi, Kabuki Shigeto, Ikeno Masahiro, Kishimoto Yuji, Nishimura Hironobu, Tanimori Toru, Takada Atsushi, Suzuki Jun-ichi, Sawano Tatsuya, Shinohara Takenao, Ueno Kazuki, Kurosawa Shunsuke, Tanaka Manobu, Oku Takayuki, Uchida Tomohisa

    hamon   Vol. 23 ( 3 ) page: 218 - 222   2013

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    <p>We have developed a prototype time-resolved neutron imaging detector employing a micro-pattern gaseous detector known as the micro-pixel chamber (μPIC) coupled with a field-programmable-gate-array-based data acquisition system. Our detector system combines 100μm-level spatial and sub-μs time resolutions with a low gamma sensitivity of less than 10<sup>-12</sup> and high data rates, making it well suited for applications in neutron radiography at high-intensity, pulsed neutron sources. In the present paper, we introduce the detector system and present several test measurements performed at NOBORU (BL10), J-PARC to demonstrate the capabilities of our prototype. We also discuss future improvements to the spatial resolution and rate performance.</p>

    DOI: 10.5611/hamon.23.3_218

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  524. A case of congenital central hypoventilation syndrome

    Kameyama, Y; Wagatsuma, T; Nakamura, M; Kurosawa, S; Saito, K; Hoshi, K

    JOURNAL OF ANESTHESIA   Vol. 26 ( 6 ) page: 922 - 924   2012.12

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    We encountered a 2-year-old female infant with congenital central hypoventilation syndrome (CCHS) who underwent an abdominal operation for strangulated ileus. Prior to the surgery, at home, the infant had been receiving non-invasive positive-pressure ventilation (NPPV) support only during sleep. However, after postoperative extubation, the blood oxygen saturation (SpO <inf>2</inf>) decreased to approximately 90 % with NPPV during sleep alone, necessitating the use of biphasic cuirass ventilation (BCV) along with NPPV for 2 days. The infant was weaned from the BCV on hospital day 9, and was discharged from the intensive care unit (ICU) on hospital day 13. Although it has been said that CCHS is not under the control of the respiratory center, there are no reports of the true CO<inf>2</inf> response curves in these patients. Therefore, during respiratory management in the ICU post-surgery, we examined (with the consent of the mother) the relationship of the end-tidal carbon dioxide (ETCO<inf>2</inf>) to the tidal volume and respiratory rate, for a period of 6 min in the absence of sedation, using a respiratory profile monitor. Electrocardiographic and SpO<inf>2</inf> monitoring was also conducted at the same time, to ensure the patient's safety. In this patient, while the ETCO <inf>2</inf> increased, the tidal volume and respiratory rate remained unchanged. No relationship was found between the tidal volume and the respiratory rate. Various modalities have been used for the treatment of CCHS (tracheotomy, NPPV, and diaphragmatic pacing). Treatment of these patients in the ICU should be tailored to the needs of individual patients and their families. © 2012 Japanese Society of Anesthesiologists.

    DOI: 10.1007/s00540-012-1451-1

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  525. Increased circulating endothelial microparticles in COPD patients: a potential biomarker for COPD exacerbation susceptibility Open Access

    Takahashi, T; Kobayashi, S; Fujino, N; Suzuki, T; Ota, C; He, M; Yamada, M; Suzuki, S; Yanai, M; Kurosawa, S; Yamaya, M; Kubo, H

    THORAX   Vol. 67 ( 12 ) page: 1067 - 1074   2012.12

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    Rationale: The influence of COPD exacerbation on the endothelium is not completely understood. Circulating endothelial microparticles (EMPs) are membrane vesicles in circulating blood that are shed by activated or apoptotic endothelial cells. Objective: To compare EMP numbers in stable COPD patients with those during and after exacerbation. Methods: We examined the EMP numbers in 80 stable COPD patients, 27 patients with exacerbated COPD, and 20 healthy non-COPD volunteers. EMPs were defined as CD144+ MPs (VE-cadherin EMPs), CD31+/CD41- MPs (PECAM EMPs), CD146 MPs (MCAM EMPs) and CD62E + EMPs (E-selectin EMPs) as analysed by FACS. Von Willebrand factor (vWF) expression was utilised to identify the origins of the EMPs. Results: VE-cadherin, PECAM and E-selectin EMP numbers were significantly higher in the stable COPD patients than in the non-COPD volunteers, and they were significantly higher in the patients with exacerbated COPD than in the stable COPD patients. The majority of these increased EMPs were vWF-negative, indicating a pulmonary capillary origin. Baseline E-selectin EMP levels were significantly higher in COPD patients who experienced frequent exacerbations than in those who did not have frequent exacerbations (p<0.001). Twenty-eight days after the onset of exacerbation, E-selectin EMP levels returned to those observed in stable COPD patients, whereas PECAM EMP levels remained high. MCAM EMP numbers were not elevated in stable or exacerbated-COPD patients. Conclusions: Endothelial damage, mainly in pulmonary capillaries, occurs during exacerbation and continues even after clinical symptoms disappear. Higher baseline E-selectin EMP levels may indicate COPD patients who are susceptible to exacerbation.

    DOI: 10.1136/thoraxjnl-2011-201395

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  526. [Seventeen cases of lung transplantations for lymphangioleiomyomatosis].

    Adachi K, Kurosawa S, Wagatsuma T, Kameyama E

    Masui. The Japanese journal of anesthesiology   Vol. 61 ( 11 ) page: 1239 - 44   2012.11

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  527. Seventeen cases of lung transplantations for lymphangioleiomyomatosis

    Adachi K., Kurosawa S., Wagatsuma T., Kameyama E.

    Japanese Journal of Anesthesiology   Vol. 61 ( 11 ) page: 1239 - 1244   2012.11

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    Background : The number of lung transplantation has tended to increase as a treatment for patients with pulmonary lymphangioleiomyomatosis (LAM) in Japan. However, we have little evidence about the correlation between preoperative medical parameters and intraoperative complications. Methods : A retrospective study was performed in 17 patients with LAM undergoing the lung transplantations between 2006 and 2011. Results : Major intraoperative complications were as follows : hypotension, pulmonary hypertension, hypoxemia and blood loss of more than 1,000 ml. According to the medical records, no patients was diagnosed pulmonary hypertension before surgery and no preoperative parameters predicted intraoperative pulmonary hypertension. Therefore, according to the medical records it seemed difficult to predict the risk of the intraoperative pulmonary hypertension and hypotension. Intraoperative hypoxemia and the requirements of percutaneous cardiopulmonary support (PCPS) are not associated with preoperative Pa<inf>O2</inf> and %FEV<inf>1.0</inf>. Pleurodesis and the use of PCPS were significantly correlated with an increased risk of intraoperative massive bleeding. The four year survival rate was 87.8%. %FEV<inf>1.0</inf>, Pa <inf>O2</inf>/F<inf>IO</inf> and %DL<inf>CO</inf> after surgery improved when compared to those before surgery. Conclusions : Although the intraoperative complications such as hypotension, pulmonary hypertension, hypoxemia and/or massive bleeding frequently occurred in patients with LAM during the lung transplantations, it was difficult to predict them except the massive bleeding of more than 1,000 ml before surgery. However, lung transplantation is a valuable therapy for patients with end-stage LAM.

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  528. Crystal growth and optical properties of Ca 3NbGa 3Si 2O 14 single crystals grown under various atmosphere

    Yokota Y., Kurosawa S., Yoshikawa A., Sato M., Tota K., Onodera K.

    Proceedings of 2012 21st IEEE Int Symp on Applications of Ferroelectrics Held Jointly with 11th IEEE European Conference on the Applications of Polar Dielectrics and IEEE Pfm Isaf Ecapd Pfm 2012     2012.10

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    We grew Ca <inf>3</inf>NbGa <inf>3</inf>Si <inf>2</inf>O <inf>14</inf> (CNGS) single crystals in Air, Ar+3%O <inf>2</inf> and Ar atmosphere by the micro-pulling-down (μ-PD) method in order to clarify the origin of the crystal color. While the CNGS crystal grown in Air indicated orange color, the crystal grown in Ar was colorless. CNGS crystal grown in Air indicated several large absorption peaks around 360 and 500 nm in the transmittance spectrum. In contrast, the crystal grown in Ar didn't indicate these absorption peaks. © 2012 IEEE.

    DOI: 10.1109/ISAF.2012.6297847

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  529. Temperature dependence of the scintillation properties of Ce:GSO and Ce:GSOZ

    Kurosawa, S; Sugiyama, M; Yanagida, T; Yokota, Y; Yoshikawa, A

    NUCLEAR INSTRUMENTS & METHODS IN PHYSICS RESEARCH SECTION A-ACCELERATORS SPECTROMETERS DETECTORS AND ASSOCIATED EQUIPMENT   Vol. 690   page: 53 - 57   2012.10

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    The light output and decay times of Ce:GSO and Ce:GSOZ scintillators depend on Ce concentration and temperature. We investigated the temperature dependence of the light output and the decay time for Ce:GSO and Ce:GSOZ doped with 0.3 (only GSO), 0.5, 1.0, and 1.5 mol% Ce. These samples were measured with a ruggedized photomultiplier (PMT) (Hamamatsu R6877A) at 175 °C (in the thermostat chamber). Up to 100 °C, the relative light output of all of the samples remained within 10% after correcting the PMT gain, which depends on the temperature. The decay times of the GSO and GSOZ samples with the identical Ce concentrations were equal. Moreover, the quenching energy values for all the samples were equivalent. © 2012 Elsevier B.V. All rights reserved.

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  530. Crystal Growth and Scintillation Properties of Fluoride Scintillators

    Kurosawa, S; Yanagida, T; Yokota, Y; Yoshikawa, A

    IEEE TRANSACTIONS ON NUCLEAR SCIENCE   Vol. 59 ( 5 ) page: 2173 - 2176   2012.10

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    Fluoride single crystals have a wide band gap. Thus, we were interested in studying the scintillation properties of fluoride single crystals. We investigated the scintillation properties of fluoride crystals grown by the micro-pulling-down and annealing methods. The time required to grow crystals using these methods is lesser than that using conventional methods such as the Czochralski and Bridgman methods. Both ZnF <inf>2</inf> and PbF <inf>2</inf> exhibited small light outputs of less than 1,000 photons/MeV, while BaF <inf>2</inf> and CeF <inf>3</inf> exhibited light outputs of ∼6,000 and ∼2,000 photons/MeV, respectively. In addition, BaF <inf>2</inf> is a well-known fast scintillator, but it also has a slow component. We tested a BaF <inf>2</inf> crystal with a Ce/La co-dopant and observed the suppression of the slow component. © 2012 IEEE.

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  531. Crystal Growth and Scintillation Properties of Ho-Doped Lu<sub>3</sub>Al<sub>5</sub>O<sub>12</sub> Single Crystals

    Sugiyama, M; Yanagida, T; Fujimoto, Y; Totsuka, D; Yokota, Y; Kurosawa, S; Futami, Y; Yoshikawa, A

    IEEE TRANSACTIONS ON NUCLEAR SCIENCE   Vol. 59 ( 5 ) page: 2141 - 2145   2012.10

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    The crystals of 0.1, 0.5, 1, and 3% Ho doped Lu <inf>3</inf>Al <inf>5</inf>O <inf>12</inf> (Ho:LuAG) grown by the micro-pulling-down method were examined for their scintillation properties. At wavelengths longer than 300 nm, Ho:LuAG crystals demonstrated around 60% transparency with many absorption peaks attributed to Ho <sup>3+</sup> 4f <sup>10</sup>-4f <sup>10</sup> transitions. When excited by <sup>241</sup>Am α-ray to obtain radio luminescence spectra, broad host emission and four sharp Ho <sup>3+</sup> 4f <sup>10</sup>-4f <sup>10</sup> emission peaks were detected in the visible region. Light yields and decay time profiles of the samples irradiated by <sup>137</sup>Cs\gamma-ray were measured using photomultiplier tubes R7600 (Hamamatsu). Ho 0.5%:LuAG showed the highest light yield of 3100 ±310 photons/MeV among the present samples. The decay time profiles were well reproduced by two components exponential approximation consisting of 0.5-1 μs and 3-6 μs. © 2012 IEEE.

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  532. Fast and High-Energy-Resolution Oxide Scintillator: Ce-Doped (La,Gd)<sub>2</sub>Si<sub>2</sub>O<sub>7</sub>

    Suzuki, A; Kurosawa, S; Shishido, T; Pejchal, J; Yokota, Y; Futami, Y; Yoshikawa, A

    APPLIED PHYSICS EXPRESS   Vol. 5 ( 10 )   2012.10

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    A novel scintillation crystal (Ce <inf>0.01</inf>,Gd <inf>0.90</inf>,La <inf>0.09</inf>) <inf>2</inf>Si <inf>2</inf>O <inf>7</inf> (Ce:La-GPS) was grown by the floating zone method, and its optical and scintillation properties were investigated. The emission wavelength of this material was 390 nm. Gamma ray excited pulse height and scintillation decay measurement showed that Ce:La-GPS had a high energy resolution (FWHM) of 5% at 662 keV, high light output of 36,000 photons/MeV and fast scintillation decay time of 46 ns. © 2012 The Japan Society of Applied Physics.

    DOI: 10.1143/APEX.5.102601

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  533. Impact of changes of positive end-expiratory pressure on functional residual capacity at low tidal volume ventilation during general anesthesia Open Access

    Satoh, D; Kurosawa, S; Kirino, W; Wagatsuma, T; Ejima, Y; Yoshida, A; Toyama, H; Nagaya, K

    JOURNAL OF ANESTHESIA   Vol. 26 ( 5 ) page: 664 - 669   2012.10

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    Purpose: Several reports in the literature have described the effects of positive end-expiratory pressure (PEEP) level upon functional residual capacity (FRC) in ventilated patients during general anesthesia. This study compares FRC in mechanically low tidal volume ventilation with different PEEP levels during upper abdominal surgery. Methods: Before induction of anesthesia (awake) for nine patients with upper abdominal surgery, a tight-seal facemask was applied with 2 cmH<inf>2</inf>O pressure support ventilation and 100 % O<inf>2</inf> during FRC measurements conducted on patients in a supine position. After tracheal intubation, lungs were ventilated with bilevel airway pressure with a volume guarantee (7 ml/kg predicted body weight) and with an inspired oxygen fraction (FIO<inf>2</inf>) of 0.4. PEEP levels of 0, 5, and 10 cmH<inf>2</inf>O were used. Each level of 5 and 10 cmH<inf>2</inf>O PEEP was maintained for 2 h. FRC was measured at each PEEP level. Results: FRC awake was significantly higher than that at PEEP 0 cmH<inf>2</inf>O (P < 0.01). FRC at PEEP 0 cmH <inf>2</inf>O was significantly lower than that at 10 cmH<inf>2</inf>O (P < 0.01). PaO<inf>2</inf>/FIO<inf>2</inf> awake was significantly higher than that for PEEP 0 cmH<inf>2</inf>O (P < 0.01). PaO<inf>2</inf>/FIO<inf>2</inf> at PEEP 0 cmH<inf>2</inf>O was significantly lower than that for PEEP 5 cmH <inf>2</inf>O or PEEP 10 cmH<inf>2</inf>O (P < 0.01). Furthermore, PEEP 0 cmH<inf>2</inf>O, PEEP 5 cmH<inf>2</inf>O after 2 h, and PEEP 10 cmH <inf>2</inf>O after 2 h were correlated with FRC (R = 0.671, P < 0.01) and PaO<inf>2</inf>/FIO<inf>2</inf> (R = 0.642, P < 0.01). Conclusions: Results suggest that PEEP at 10 cmH<inf>2</inf>O is necessary to maintain lung function if low tidal volume ventilation is used during upper abdominal surgery. © 2012 The Author(s).

    DOI: 10.1007/s00540-012-1411-9

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  534. Lithium Aluminate Crystals as Scintillator for Thermal Neutron Detection

    Fujimoto, Y; Kamada, K; Yanagida, T; Kawaguchi, N; Kurosawa, S; Totsuka, D; Fukuda, K; Watanabe, K; Yamazaki, A; Yokota, Y; Yoshikawa, A

    IEEE TRANSACTIONS ON NUCLEAR SCIENCE   Vol. 59 ( 5 ) page: 2252 - 2255   2012.10

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    Undoped and Cu <sup>+</sup>-doped lithium aluminate LiAlO <inf>2</inf> singe crystals have been grown using micro-pulling down (μ-PD) technique. After cutting and polishing, optical properties and scintillation characteristics of the crystals were examined. From the transmittance measurements, Cu <sup>+</sup>-doped crystal showed absorption band around 270 nm, which is corresponding to the transition between Cu <sup>+</sup> 3d <sup>10</sup> and 3 d <sup>9</sup> 4s states. Ultra violet emission peak appeared around 360 nm under 270 nm excitation. The emission decay time was calculated to be about 17.3 μ s. <sup>241</sup> Am 5.5 MeV alpha-ray excited radioluminescence spectra exhibited intense luminescence band at 360 nm due to the Cu <sup>+</sup>3d <sup>9</sup>4s-3d <sup>10</sup> transitions. By the pulse height spectra <sup>252</sup> Cf neutron source excitation, the scintillation light output of Cu <sup>+</sup>-doped LiAlO <inf>2</inf> was found to be about 8700 ph/n. © 2012 IEEE.

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  535. LPE Growth and Scintillation Properties of (Zn,Mg)O Single Crystalline Film

    Yoshikawa, A; Yanagida, T; Fujimoto, Y; Kurosawa, S; Yokota, Y; Yamaji, A; Sugiyama, M; Wakahara, S; Futami, Y; Kikuchi, M; Miyamoto, M; Sekiwa, H; Nikl, M

    IEEE TRANSACTIONS ON NUCLEAR SCIENCE   Vol. 59 ( 5 ) page: 2286 - 2289   2012.10

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    Among the direct wide band-gap semiconductors, ZnO is an attractive scintillator for alpha particle monitoring. However, the undoped ZnO has a dominant slow luminescence around 500-600 nm due to lattice defects. In this study, the Mg-substituted ZnO ((Zn,Mg)O) single crystalline films with high crystallinity are investigated. Mg doping is found to improve the lattice order and suppress slow luminescent component around 500-600 nm. (Zn,Mg)O single crystalline films were grown by the Liquid Phase Epitaxy (LPE) method. Alpha-ray excited radioluminescence spectra of (Zn,Mg)O film show only one emission peak around 400 nm and decay time of a few nanoseconds. This emission is assigned to free exciton. Light yield of LPE grown (Zn,Mg)O film is evaluated of about 90% of BGO. © 2012 IEEE.

    DOI: 10.1109/TNS.2012.2194743

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  536. Scintillation Properties of Transparent Ceramic Pr:LuAG for Different Pr Concentration

    Yanagida, T; Fujimoto, Y; Kamada, K; Totsuka, D; Yagi, H; Yanagitani, T; Futami, Y; Yanagida, S; Kurosawa, S; Yokota, Y; Yoshikawa, A; Nikl, M

    IEEE TRANSACTIONS ON NUCLEAR SCIENCE   Vol. 59 ( 5 ) page: 2146 - 2151   2012.10

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    We manufactured transparent optical ceramic of Pr 0.2-1% doped Lu <inf>3</inf> Al <inf>5</inf> O <inf>12</inf> (Pr:LuAG) by the sintering method. We compare its optical and scintillation properties with the single crystal counterpart grown by the conventional Czochralski method. So far the scintillation ceramic of Pr:LuAG appeared inferior to its single crystal analog especially in terms of light yield. However, in the present case our ceramic Pr 0.25%-doped sample exhibited by 20% higher light yield compared to single crystal under γ-ray excitation. Furthermore, in the ceramic sample the slower scintillation decay components were suppressed and the defect related host emission as well. The optimized technology of optical ceramics thus appears very competitive to single crystals and opens great practical prospectives for the former materials in the field of fast scintillators. © 2012 IEEE.

    DOI: 10.1109/TNS.2012.2189583

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  537. Overexpression of delayed rectifier K + channels promotes in situ proliferation of leukocytes in rat kidneys with advanced chronic renal failure Open Access

    Kazama I., Maruyama Y., Endo Y., Toyama H., Ejima Y., Matsubara M., Kurosawa S.

    International Journal of Nephrology   Vol. 2012   page: 581581   2012.9

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    Leukocytes, such as lymphocytes and macrophages, predominantly express delayed rectifier K <sup>+</sup> channels (Kv1.3), and the channels play crucial roles in the activation and proliferation of the cells. Since lymphocytes are activated in patients with end-stage renal disease (ESRD), the channels expressed in those cells would contribute to the progression of renal fibrosis in advanced-stage chronic renal failure (CRF). In the present study, using a rat model with advanced CRF that underwent 5/6 nephrectomy followed by a 14-week recovery period, we examined the histopathological features of the kidneys and the leukocyte expression of Kv1.3-channels and cell cycle markers. Age-matched sham-operated rats were used as controls. In the cortical interstitium of advanced CRF rat kidneys, leukocytes proliferated in situ and overexpressed Kv1.3 channel protein in their cytoplasm. Treatment with margatoxin, a selective Kv1.3-channel inhibitor, significantly suppressed the number of leukocytes and the progression of renal fibrosis with a significant decrease in the cortical cell cycle marker expression. This study demonstrated for the first time that the number of leukocytes was dramatically increased in rat kidneys with advanced CRF. The overexpression of Kv1.3 channels in the leukocytes was thought to contribute to the progression of renal fibrosis by stimulating cell cycling and promoting cellular proliferation. © 2012 Itsuro Kazama et al.

    DOI: 10.1155/2012/581581

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  538. Dopant segregation in rare earth doped lutetium aluminum garnet single crystals grown by the micro-pulling down method

    Sugiyama, M; Yokota, Y; Fujimoto, Y; Yanagida, T; Futami, Y; Kurosawa, S; Yoshikawa, A

    JOURNAL OF CRYSTAL GROWTH   Vol. 352 ( 1 ) page: 110 - 114   2012.8

  539. [Use of sugammadex in patients undergoing caesarean section using general anesthesia with rocuronium].

    Shibusawa M, Ejima Y, Nishino R, Toyama H, Kurosawa S

    Masui. The Japanese journal of anesthesiology   Vol. 61 ( 8 ) page: 805 - 9   2012.8

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  540. Use of sugammadex in patients for caesarean section undergoing general anesthesia with rocuronium

    Shibusawa M., Ejima Y., Nishino R., Toyama H., Kurosawa S.

    Japanese Journal of Anesthesiology   Vol. 61 ( 8 ) page: 805 - 809   2012.8

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    Recently, rocuronium is being used in patients for caesarean section undergoing general anesthesia instead of suxamethonium. An increased dose of rocuronium improves intubating conditions but prolongs neuromuscular blockade. Sugammadex reverses rapidly and predictably even profound rocuronium-induced neuromuscular blockade. We experienced 13 cases of caesarean section patients undergoing general anesthesia with thiopental (3.5 mg·kg <sup>-1</sup>) and rocuronium (0.9 mg·kg <sup>-1</sup>). At the end of surgery, sugammadex (2 mg·kg <sup>-1</sup>) was administered every 3 minutes repeatedly until TOF>0.9. In two patients, neuromuscular blockade spontaneously recovered to TOF>0.9 at the end of surgery. In most patients administered sugammadex, TOF recovered to more than 0.9 within a few minutes. However, in one patient who had chronic renal failure (creatinine clearance rate : 12 ml·min <sup>-1</sup>), 10 minutes were required for TOF to recover to more than 0.7, and TOF never reached 0.9. All patients were successfully intubated at the first attempt. No signs of recurarization or adverse effects related to sugammadex were noted in the perioperative period.

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  541. Two principal components, coping and independence, comprise patient enablement in Japan: Cross sectional study in Tohoku area Open Access

    Kurosawa S., Matsushima M., Fujinuma Y., Hayashi D., Noro I., Kanaya T., Watanabe T., Tominaga T., Nagata T., Kawasaki A., Hosoya T., Yanagisawa H.

    Tohoku Journal of Experimental Medicine   Vol. 227 ( 2 ) page: 97 - 104   2012.7

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    The concept of "patient enablement" involves patients perceptions of ability to understand and cope with illness. Improving enablement is an important goal of medical consultations for patients with chronic illness. To measure "enablement," a post-medical-consultation patient-reported questionnaire was developed and named "Patient Enablement Instrument (PEI)" in the United Kingdom. Unfortunately, there has been no tool to evaluate patient enablement in Japan. Therefore, this study aimed to develop PEI Japanese version, to examine its validity and reliability, and to clarify the constitution of concept about patient enablement among Japanese patients. The translation process included forward translation, expert panel back-translation, following the standard WHO process. Participants were 256 individuals (157 men and 99 women; mean age 62.9 ± 11.8 years) receiving a regular outpatient treatment due to chronic illness at the Department of Cardiology, Respiratory, or Endocrinology and Metabolism in a regional hospital. To assess validity, we compared PEI with Medical Interview Satisfaction Scale (MISS) by correlation coefficient, which was 0.55 (P < 0.01). Furthermore, factor analysis indicated that PEI had two principal factors labeled "coping with illness and health maintenance" and "confidence in oneself and independence". For an evaluation of reliability, internal consistency was calculated (Cronbach's alpha = 0.875). In conclusion, two principal factors comprise patient enablement measured by PEI with satisfactory validity and reliability. PEI Japanese version will be a useful tool to evaluate and improve medical consultations in Japan. © 2012 Tohoku University Medical Press.

    DOI: 10.1620/tjem.227.97

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  542. Anesthesia in patients with cancer disorders

    Kurosawa, S

    CURRENT OPINION IN ANESTHESIOLOGY   Vol. 25 ( 3 ) page: 376 - 384   2012.6

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    Purpose of review: Along with the increasing population of elderly people in developed countries, anesthesiologists have increasing opportunities to anesthetize cancer patients in their routine work. However, no guideline of anesthesia procedures for cancer patients is available even though guidelines of operative procedures have been formulated for different types of cancer. This review provides Recent findings related to the optimal choice of anesthetics and adequate anesthesia management for cancer patients. Recent findings: The intrinsic weapon fighting cancer cells is competent immune cells, particularly CD4 <sup>+</sup> T helper 1-type cells, CD8 <sup>+</sup> cytotoxic T cells, and natural killer cells. However, surgical inflammation, some anesthetics, and inadvertent anesthesia management suppress these effector cells and induce suppressive immune cells, which render cancer patients susceptible to tumor recurrence and metastasis after surgery. Summary: Accumulated basic and clinical data suggest that total intravenous anesthesia with propofol, cyclooxygenase antagonists, and regional anesthesia can decrease negative consequences associated with perioperative immunosuppression. Volatile anesthesia, systemic morphine administration, unnecessary blood transfusions, intraoperative hypoxia, hypotension, hypothermia, and hyperglycemia should be avoided. © 2012 Wolters Kluwer Health | Lippincott Williams & Wilkins.

    DOI: 10.1097/ACO.0b013e328352b4a8

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  543. Prognosis of acute myeloid leukemia harboring monosomal karyotype in patients treated with or without allogeneic hematopoietic cell transplantation after achieving complete remission Open Access

    Yanada, M; Kurosawa, S; Yamaguchi, T; Yamashita, T; Moriuchi, Y; Ago, H; Takeuchi, J; Nakamae, H; Taguchi, J; Sakura, T; Takamatsu, Y; Waki, F; Yokoyama, H; Watanabe, M; Emi, N; Fukuda, T

    HAEMATOLOGICA-THE HEMATOLOGY JOURNAL   Vol. 97 ( 6 ) page: 915 - 918   2012.6

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    To evaluate the prognostic impact of monosomal karyotype on post-remission outcome in acute myeloid leukemia, we retrospectively analyzed 2,099 patients who had achieved complete remission. Monosomal karyotype was noted in 73 patients (4%). Of these, the probability of overall survival from first complete remission was 14% at four years, which was significantly lower than that reported in patients without monosomal karyotype, primarily due to a high relapse rate (86%). Monosomal karyotype remained significantly associated with worse overall survival among patients with unfavorable cytogenetics or complex karyotype, and even in patients who underwent allogeneic hematopoietic cell transplantation during first complete remission. These findings confirm that monosomal karyotype has a significantly adverse effect on post-remission outcome in patients with acute myeloid leukemia treated with and without allogeneic hematopoietic cell transplantation in first complete remission, emphasizing the need for the development of alternative therapies for this patient population. © 2012 Ferrata Storti Foundation.

    DOI: 10.3324/haematol.2011.058289

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  544. Predicting the efficacy of proton pump inhibitors in patients with non-erosive reflux disease before therapy using dual-channel 24-h esophageal pH monitoring

    Shimatani, T; Sugimoto, M; Nishino, M; Adachi, K; Furuta, K; Ito, M; Kurosawa, S; Manabe, N; Mannen, K; Hongo, M; Chiba, T; Kinoshita, Y

    JOURNAL OF GASTROENTEROLOGY AND HEPATOLOGY   Vol. 27 ( 5 ) page: 899 - 906   2012.5

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    Background and Aim: We aimed to determine whether reflux- and symptom-related parameters can predict the efficacy of proton pump inhibitors (PPI) in non-erosive reflux disease (NERD). Methods: Twenty-seven NERD patients who had experienced heartburn more than once a week within the previous month were enrolled. Intraesophageal pH before therapy was measured simultaneously at 5 and 15cm above the esophagogastric junction (EGJ) for 24h. The PPI rabeprazole was administered at a dose of 10mg once daily for 4weeks. In the event that heartburn was not relieved, the dose was increased to 10mg twice daily for an additional 2weeks, and again to 20mg twice daily for another 2weeks. Results: Univariate analysis demonstrated no significant associations between any reflux- or symptom-related parameters at either site and complete heartburn relief after 4weeks, or cumulative complete heartburn relief after 8weeks. However, post-hoc analysis demonstrated more satisfactory heartburn relief after 4weeks in patients with a high symptom index compared with those with a low symptom index, at 5cm above the EGJ (P=0.009). Cumulative satisfactory heartburn relief after 8weeks was also greater in patients with a high total number of acid reflux episodes compared with those with a low total number of episodes, at 15cm above the EGJ (P=0.037). Conclusions: Pre-therapeutic pH monitoring in the lower and mid-esophagus is useful for predicting the efficacy of PPI in NERD patients. © 2011 Journal of Gastroenterology and Hepatology Foundation and Blackwell Publishing Asia Pty Ltd.

    DOI: 10.1111/j.1440-1746.2011.06975.x

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  545. Hyperglycaemia during the early phase after haematopoietic stem cell transplantation is caused by the elevation of insulin resistance

    Yakushijin, K; Fuji, S; Kim, S; Yoshimura, K; Kurosawa, S; Asakura, Y; Hiramoto, N; Mori, M; Fukuhara, S; Kamiyama, Y; Ueno, N; Tada, K; Maeda, T; Nakamura, D; Nishinohara, M; Furuta, K; Mori, S; Tanosaki, R; Heike, Y; Takaue, Y; Tobinai, K; Fukuda, T

    BONE MARROW TRANSPLANTATION   Vol. 47   page: S201 - S202   2012.4

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  546. Remifentanil use for cesarean section in a patient with intracranial re-ruptured arteriovenous malformation

    Onishi, E; Kojima, A; Saishu, T; Kurosawa, S

    JOURNAL OF ANESTHESIA   Vol. 26 ( 2 ) page: 275 - 279   2012.4

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    We describe the successful administration of remifentanil as part of the anesthetic technique used for cesarean section performed under general anesthesia in a 24-year-old woman with intracranial re-hemorrhage caused by re-ruptured arteriovenous malformation. A low dose of remifentanil was useful to obtund the hypertensive response during induction and maintenance of anesthesia without neonatal respiratory depression. © 2011 Japanese Society of Anesthesiologists.

    DOI: 10.1007/s00540-011-1295-0

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  547. Development of a new imaging device using a VUV scintillator and a gas photomultiplier with a μ-PIC and GEM Open Access

    Kurosawa, S; Taniue, K; Sekiya, H; Kubo, H; Ida, C; Miuchi, K; Tanimori, T; Yanagida, T; Yokota, Y; Yoshikawa, A; Fukuda, K; Kawaguchi, N; Ishizu, S; Nakagawa, M; Suyama, T; Pejchal, J

    JOURNAL OF INSTRUMENTATION   Vol. 7 ( 3 )   2012.3

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    We have developed a new imaging device consisting of a VUV scintillator coupled to a gas photomultiplier (gas PMT) with a CsI photocathode, micro pixel chamber (μ-PIC) and gas electron multipliers (GEMs). Generally, the VUV scintillator has a short decay time of less than ∼ 10 nsec. Thus the new detector could be used under the high rate counting ( ∼ 10 MHz) in the hard X-ray to soft-gamma ray region. Our goal in this paper is to obtain a soft gamma-ray image at 0.1 MeV with our gas PMT combined with the VUV scintillator as a high rate counter, and we have optimized electric fields in the gas PMT and developed a new VUV scintillator with a higher light output. In order to obtain a higher collection efficiency of photoelectrons and suppress the ion feedback in the gas PMT, we first optimized the electric field. Then we decided the electric field in the drift, transfer, and induction region to be 0.25, 1.0 and 3.0 kV/cm, respectively. The total gas gain of the gas PMT was approximately 2 × 10<sup>5</sup>, and the gas PMT was estimated to have a quantum efficiency (QE) of 0.7% at 178nm. Additionally, as a consequence of new VUV scintillators search, Nd:LuLiF<inf>4</inf> and Nd:LuF<inf>3</inf> with a volume of 10mm × 10mm × 5mm were found to have higher light outputs than Nd:LaF<inf>3</inf>, which is a conventional VUV scintillator, by a factor of 2.1, and 2.6, respectively, and the Nd:LuF<inf>3</inf> irradiated with 5.5-MeV alpha-rays had a light output of approximately 400 photons. Finally, we succeeded in obtaining the crystal images upon 5.5MeV alpha and 0.122MeV gamma rays excitation from <sup>241</sup>Am- and <sup>57</sup>Co sources, respectively, using the gas PMT with the Nd:LuF<inf>3</inf>. © 2012 IOP Publishing Ltd and Sissa Medialab srl.

    DOI: 10.1088/1748-0221/7/03/C03013

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  548. Eu-doped <SUP>6</SUP>LiF-SrF<sub>2</sub> eutectic scintillators for neutron detection

    Yanagida, T; Fukuda, K; Fujimoto, Y; Kawaguchi, N; Kurosawa, S; Yamazaki, A; Watanabe, K; Futami, Y; Yokota, Y; Pejchal, J; Yoshikawa, A; Uritani, A; Iguchi, T

    OPTICAL MATERIALS   Vol. 34 ( 5 ) page: 868 - 871   2012.3

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    Eu<sup>2+</sup> 0.05%, 0.1%, and 0.2% activated LiF-SrF<inf>2</inf> eutectic scintillators were prepared by the Bridgman method using <sup>6</sup>Li enriched (95%) raw material. The α-ray-induced radio luminescence spectra showed intense emission peak at 430 nm due to an emission from Eu<sup>2+</sup> 5d-4f transition in the Eu:SrF<inf>2</inf> layers. When excited by <sup>252</sup>Cf neutrons, all the samples exhibited almost the same light yields of 5000-7000 ph/n with a typical decay times of several hundreds ns. © 2011 Elsevier B.V. All rights reserved.

    DOI: 10.1016/j.optmat.2011.11.022

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  549. Prompt gamma detection for range verification in proton therapy

    Kurosawa, S; Kubo, H; Ueno, K; Kabuki, S; Iwaki, S; Takahashi, M; Taniue, K; Higashi, N; Miuchi, K; Tanimori, T; Kim, D; Kim, J

    CURRENT APPLIED PHYSICS   Vol. 12 ( 2 ) page: 364 - 368   2012.3

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    It is an on-going challenge to verify the proton range in situ during proton therapy. Since the protons stop in target tissue, measurement of gamma-rays emitted either promptly from nuclear de-excitation or in pair from positron annihilation is the feasible method to monitor the proton range in-vivo. Using the technique of gamma collimation, we empirically demonstrated that the proton range and prompt gamma distribution are well correlated in the therapy energy range, and that measuring prompt gammas is a viable method for the clinical application. However, this collimation technique appears not to be applicable to passively scattered proton beams. The device chosen for gamma imaging in 2D is an electron tracking Compton camera, which images single-emission photons employing a gas chamber to induce Compton scattering. Images of prompt gammas were attained at the proton beam energy of 140 MeV. Measurements showed that gamma image in the energy range of 800-2000 keV provides a better match with the proton range compared to the image by lower energy gammas. © 2011 Elsevier B.V. All rights reserved.

    DOI: 10.1016/j.cap.2011.07.027

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  550. 束縛励起子準位の導入によるEu:LiCaAlF<sub>6</sub>のシンチレーション特性向上

    柳田 健之, 二見 能資, 藤本 裕, 河口 範明, 山崎 淳, 渡辺 賢一, 福田 健太郎, 黒澤 俊介, 横田 有為, 吉川 彰

    応用物理学会学術講演会講演予稿集   Vol. 2012.1 ( 0 ) page: 487 - 487   2012.2

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    DOI: 10.11470/jsapmeeting.2012.1.0_487

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  551. Crystal growth and scintillation properties of Er-doped Lu<sub>3</sub>Al<sub>5</sub>O<sub>12</sub> single crystals

    Sugiyama, M; Fujimoto, Y; Yanagida, T; Totsuka, D; Kurosawa, S; Futami, Y; Yokota, Y; Chani, V; Yoshikawa, A

    NUCLEAR INSTRUMENTS & METHODS IN PHYSICS RESEARCH SECTION A-ACCELERATORS SPECTROMETERS DETECTORS AND ASSOCIATED EQUIPMENT   Vol. 664 ( 1 ) page: 127 - 131   2012.2

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    Publisher:Nuclear Instruments and Methods in Physics Research Section A Accelerators Spectrometers Detectors and Associated Equipment  

    Er-doped Lu <inf>3</inf>Al <inf>5</inf>O <inf>12</inf> (Er:LuAG) single crystalline scintillators with different Er concentrations of 0.1, 0.5, 1, and 3% were grown by the micro-pulling-down (μ-PD) method. The grown crystals were composed of single-phase material, as demonstrated by powder X-ray diffraction (XRD). The radioluminescence spectra measured under <sup>241</sup>Am α-ray excitation indicated host emission at approximately 350 nm and Er <sup>3</sup> 4f4f emissions. According to the pulse height spectra recorded under γ-ray irradiation, the 0.5% Er:LuAG exhibited the highest peak channel among the samples. The γ-ray excited decay time profiles were well fitted by the two-component exponential approximation (0.8 μs and 610 μs). © 2011 Elsevier B.V. All rights reserved.

    DOI: 10.1016/j.nima.2011.10.063

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  552. THE IMPACT OF HCV SERO-POSITIVITY OF RECIPIENTS ON CLINICAL OUTCOMES FOLLOWING ALLOGENEIC HSCT IN JAPAN Open Access

    Nakasone, H; Yakushijin, K; Kurosawa, S; Ogawa, H; Ohashi, K; Eto, T; Sakamaki, H; Morishima, Y; Nagamura, T; Suzuki, R; Murata, M; Taniguchi, S; Fukuda, T

    BIOLOGY OF BLOOD AND MARROW TRANSPLANTATION   Vol. 18 ( 2 ) page: S328 - S329   2012.2

  553. Characterizations of Ce<SUP>3+</SUP>-Doped CaB<sub>2</sub>O<sub>4</sub> Crystalline Scintillator

    Fujimoto, Y; Yanagida, T; Kawaguchi, N; Kurosawa, S; Fukuda, K; Totsuka, D; Watanabe, K; Yamazaki, A; Yokota, Y; Yoshikawa, A

    CRYSTAL GROWTH & DESIGN   Vol. 12 ( 1 ) page: 142 - 146   2012.1

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    Single crystals of undoped and 0.5% Ce <sup>3+</sup>-doped calcium metaborate CaB <inf>2</inf>O <inf>4</inf> have been grown successfully by micropulling down (μ-PD) technique. The material can find its application in the neutron detection. After the single-phase of CaB <inf>2</inf>O <inf>4</inf> was confirmed using X-ray diffraction analysis, optical and scintillation characteristics were investigated. In the transmittance spectra, Ce <sup>3+</sup>-doped crystals showed absorption bands around 270 and 320 nm which are ascribed to the transition from 4f ground state to 5d excited state of Ce <sup>3+</sup>. Under the <sup>241</sup>Am 5.5 MeV α-ray excitation, strong emission peak at 370 nm because of the Ce <sup>3+</sup> 5d-4f transition was observed for Ce <sup>3+</sup>-doped crystal, while the undoped crystal showed broad intrinsic emission band around 300-400 nm which is caused by the lattice defects in the host crystal. The absolute light yield was calculated to be about 2200 photons per neutron under <sup>252</sup>Cf neutron irradiation. © 2011 American Chemical Society.

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  554. Development of the balloon-borne sub-MeV gamma-ray Compton camera using an electron-tracking gaseous TPC and a scintillation camera

    Ueno, K; Mizumoto, T; Hattori, K; Higashi, N; Iwaki, S; Kabuki, S; Kishimoto, Y; Komura, S; Kubo, H; Kurosawa, S; Matsuoka, Y; Miuchi, K; Nakamura, K; Nishimura, H; Parker, J; Sato, Y; Sawano, T; Takada, A; Tanimori, T

    JOURNAL OF INSTRUMENTATION   Vol. 7 ( 1 )   2012.1

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    We have developed an Electron-Tracking Compton Camera (ETCC) for use onboard a balloon to observe sub-MeV/MeV gamma rays from celestial objects. The ETCC is constructed with a three dimensional gaseous tracker for recoil electrons from Compton scattering, and GSO:Ce pixel scintillator arrays as absorber of the Compton-scattered gamma-ray. By using the ETCC, we can reconstruct the energy and direction of individual gamma rays. We have developed a prototype ETCC with a (30 cm)<sup>3</sup> TPC, and tested its performance in the range of 356 - 835 keV in the laboratory. As the result, we succeeded in taking images of gamma ray sources and determined a detection efficiency of 9.0 × 10<sup>-6</sup> and an effective area of 8.0 × 10<sup>-3</sup> cm<sup>2</sup> at 662 keV for the prototype ETCC. Furthermore, we developed a new power saving readout circuit for the scintillators that achieves the electric power consumption of 0.41 W/channel, an energy dynamic range of 81 - 1333 keV, and an energy resolution of 10.3% at full width at half maximum at 662 keV. © 2012 IOP Publishing Ltd and SISSA.

    DOI: 10.1088/1748-0221/7/01/C01088

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  555. 20aAG-12 Neutron Imaging Detector Based on the μPIC Micro-Pixel Gaseous Chamber

    Parker J. D., Hattori K., Kishimoto Y., Kamiyama T., Kubo H., Kiyanagi Y., Harada M., Kurosawa S., Matsuoka Y., Iwaki S., Miuchi K., Oku T., Sawano T., Nishimura H., Shinohara T., Suzuki J., Takada A., Kino K., Tanimori T., Kabuki S., Ueno K.

    Meeting Abstracts of the Physical Society of Japan   Vol. 67.2.4 ( 0 ) page: 869   2012

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    DOI: 10.11316/jpsgaiyo.67.2.4.0_869_1

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  556. Crystal growth and optical properties of Ca<sub>3</sub>NbGa<sub>3</sub>Si<sub>2</sub>O<sub>14</sub> single crystals grown under various atmosphere

    Yokota, Y; Kurosawa, S; Yoshikawa, A; Sato, M; Tota, K; Onodera, K

    2012 INTERNATIONAL SYMPOSIUM ON APPLICATIONS OF FERROELECTRICS HELD JOINTLY WITH 11TH IEEE ECAPD AND IEEE PFM (ISAF/ECAPD/PFM)     2012

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  557. Development of electron tracking Compton camera for both balloon and future satellite experiments for MeV gamma-ray astronomy Open Access

    Tanimori, T; Ikeno, M; Kubo, H; Miuchi, K; Kabuki, S; Parker, JD; Kishimoto, Y; Komura, S; Kurosawa, S; Iwaki, S; Sawano, T; Nakamura, K; Matsuoka, Y; Mizumoto, T; Sato, Y; Tanaka, M; Takada, A; Uchida, T; Ueno, K

    SPACE TELESCOPES AND INSTRUMENTATION 2012: ULTRAVIOLET TO GAMMA RAY   Vol. 8443   2012

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    Publisher:Proceedings of SPIE the International Society for Optical Engineering  

    In order to explore MeV gamma-ray astronomy, we have developed the Electron Tracking Compton Camera (ETCC) consisting of a Time projection Chamber based on the micro pixel gas counter and pixel array scintillators. By measuring the track of a recoil electron in the TPC event by event, the ETCC measures the direction of each gamma-ray, and provides both good background rejection and an angular resolution over ̃1 degree. A 1m-cubic size ETCC in satellite would be a good candidate for an All sky MeV gamma-ray survey of a wide band energy region of 0.1-100MeV with several ten times better sensitivity than COMPTEL. Already we carried out a balloon experiment with a small ETCC (Sub-MeV gamma ray Imaging Loaded-on-balloon Experiment: SMILE-I) in 2006, and measured diffuse cosmic and atmosphere gamma rays. We are now constructing a 30cm-cube ETCC to catch gamma-rays from the Crab and terrestrial gamma-ray bursts at the North Pole from 2013 (SMILE-II project). Terrestrial gamma-ray bursts are generated by relativistic electron precipitation in the Pole region. Recently performance of tracking a recoil electron has been dramatically improved, which may enable us to reach the ideal efficiency expected for the detector. In addition, we mention about the unique capability to find a high-z Gamma-Ray Bursts beyond z>10 by ETCC, in particular long duration GRBs over 1000 sec, which are expected to be due to POP-III stars. © 2012 SPIE.

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  558. Investigation of a Tb-doped HfO<sub>2</sub> Single Crystal Grown by a Skull Melting Method

    Kurosawa, S; Futami, Y; Kochurikhin, VV; Borik, MA; Yokota, Y; Yanagida, T; Yoshikawa, A

    MATERIALS INTEGRATION   Vol. 508   page: 81 - +   2012

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    HfO<inf>2</inf> has high effective atomic number and no radioactive-isotope as the background source, and it can be the candidate for the high-stopping scintillator instead of Lu<inf>2</inf>SiO<inf>5</inf>:Ce scintillator used in medical imaging, astronomy and etc. However, HfO<inf>2</inf> has an extremely high melting point of 2774 °C, and it is difficult to grow the crystal from the melt using crucible, as there is no suitable metals, which can survive around that temperature. Thus, Czochralski, Bridgman, and micro-pulling down method cannot be applied. Therefore we investigated optical properties of a 17-mol% b-doped (stabilized) HfO<inf>2</inf> crystal grown by the skull melting method, and this crystal had a high refractive index of 2.5 at 550 nm, and the maximum emission peak at ∼550 nm from <sup>5</sup>D<inf>4</inf> excited states of Tb<sup>3+</sup>. In addition, we found the radiation reaction of the crystal irradiated with alpha and gamma rays measuring with a photomultiplier. © (2012) Trans Tech Publications, Switzerland.

    DOI: 10.4028/www.scientific.net/KEM.508.81

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  559. Nd<SUP>3+</SUP> doped LiCaAlF<sub>6</sub> single crystal for scintillator application

    Yanagida, T; Futami, Y; Kawaguchi, N; Pejchal, J; Fujimoto, Y; Kurosawa, S; Yokota, Y; Yoshikawa, A

    MATERIALS INTEGRATION   Vol. 508   page: 224 - +   2012

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    Nd<sup>3+</sup> 0.5% doped single crystal LiCaAlF<inf>6</inf> scintillator was grown by the micro-pulling down (μ-PD) method. Powder X-ray diffraction analysis was done and the grown crystal was a single phase LiCaAlF<inf>6</inf>. It was cut and polished to the physical dimension of 1 × 2 × 7 mm<sup>3</sup>. In transmittance spectrum, Nd<sup>3+</sup> 5d-4f absorption observed at 175 nm and the transmittance became 80% at wavelength longer than 180 nm. Excited by 160 nm, Nd<sup>3+</sup> 5d-4f emission appeared at 180 nm. X-ray induced radio-luminescence spectrum showed the similar feature with the photoluminescence one. When coupled with PMT and irradiated by 241Am α-ray, the absolute light yield resulted 100 ph/5.5 MeV α. © (2012) Trans Tech Publications, Switzerland.

    DOI: 10.4028/www.scientific.net/KEM.508.224

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  560. Optical and Scintillation Properties of Eu-doped Calcium Orthoborate

    Fujimoto, Y; Futami, Y; Yanagida, T; Kurosawa, S; Kawaguch, N; Fukuda, K; Totsuka, D; Yoshikawa, A

    MATERIALS INTEGRATION   Vol. 508   page: 235 - +   2012

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    Publisher:Key Engineering Materials  

    Single crystals of Eu-doped calcium orthoborate have been grown by micro-pulling (μ-PD) technique with radio frequency heating system, and its transmittance, photoluminescence and radiation responses were investigated. In transmittance spectra, Eu-doped crystal showed broad absorption band around 200-450 nm, which is due to the complex of charge transfer (CT) transition and 4f-4f transition of Eu<sup>3+</sup>. Intense Eu<sup>2+</sup> 5f-4f and Eu <sup>3+</sup> 4f-4f emission peaks were observed when excited to 265 nm and 385 nm, and the calculated decay times were 230 ns and 1.5 ms, respectively. <sup>241</sup>Am 5.5 MeV α-ray excited radioluminescence spectra indicated both Eu<sup>2+</sup> 5f-4f and Eu<sup>3+</sup> 4f-4f emission peaks. © (2012) Trans Tech Publications, Switzerland.

    DOI: 10.4028/www.scientific.net/KEM.508.235

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  561. Survey Meter Using Novel Inorganic Scintillators Open Access

    YANAGIDA Takayuki, KAMADA Kei, KUROSAWA Shunsuke, FUKUDA Kentaro, FUJIMOTO Yutaka, YOKOTA Yuui, YOSHIKAWA Akira, KAWAGUCHI Noriaki

    The Review of Laser Engineering   Vol. 40 ( 3 ) page: 171   2012

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    Language:Japanese   Publisher:The Laser Society of Japan  

    Single crystal scintillator materials are widely used for detection of high-energy photons and particles.
    There is continuous demand for new scintillator materials with higher performance because of increasing
    number of medical, industrial, security and other applications. This article presents the recent
    development of three novel inorganic scintillators; Pr-doped Lu3Al5O12 (Pr:LuAG), Ce doped Gd3 (Al,
    Ga)5 O12 (Ce:GAGG) and Ce or Eu-doped 6LiCaAlF6 (Ce:LiCAF, Eu:LiCAF). Pr:LuAG shows very
    interesting scintillation properties including very fast decay time, high light yield and excellent energy
    resolution. Taking the advantage of these properties, positron emission mammography (PEM) equipped
    with Pr:LuAG were developed. Ce:GAGG shows very high light yield, which is much higher than that
    of Ce:LYSO. Survey meter using Ce:GAGG is developed using this scintillator. Ce:LiCAF and
    Eu:LiCAF were developed for neutron detection. The advantage and disadvantage are discussed
    comparing with halide scintillators. Eu-doped LiCAF indicated five times higher light yield than that of
    existing Li-glass. It is expected to be used as the alternative of 3He.

    DOI: 10.2184/lsj.40.3_171

    Open Access

    CiNii Research

  562. Development of a position-sensitive radiation detector using a VUV scintillator and gaseous detector

    Kurosawa S., Yokota Y., Yoshikawa A., Yanagida T., Taniue K., Kubo H., Nakagawa M., Fukuda K., Sekiya H., Ishizu S., Tanimori T., Kawaguchi N., Suyama T.

    Ionizing Radiation   Vol. 38 ( 1 ) page: 25 - 33   2012

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    Language:Japanese   Publisher:The Japan Society of Applied Physics  

    <p>  We have developed a new imaging device consisting of a VUV scintillator coupled to a gas photomultiplier (gas PMT) with a micro pixel chamber (μ-PIC) and gas electron multipliers (GEMs). Generally, the VUV scintillator has a short decay time of less than ~10 nsec, and the μ-PIC can be operated up to 10<sup>7</sup> Hz/mm<sup>2</sup>. Thus the new detector is expected to be used in high rate counting (~ 10<sup>4</sup> - 10<sup>5</sup> Hz) with higher detection efficiency than a gas detector only.</p><p>  The gas PMT had the order of 10-nm thick CsI photocathode vaporated and deposited on a 5-mm thick MgF<sub>2</sub> window with a diameter of 54 mm. Both of μ-PIC and two GEMs had a detection area of 10 cm × 10 cm, and the gas PMT was filled with Ar+C<sub>2</sub>H<sub>6</sub> mixture gas (9 : 1) at 1 atm. Total gas gain of the gas PMT was up to 7 × 10<sup>5</sup> with stable operation, and the gas PMT was estimated to have a quantum efficiency (QE) of 1% at 175 nm. As a VUV scintillator, we used an 8-mol% Nd doped LaF<sub>3</sub>. This crystal was coupled to the gas PMT, and we succeeded in detection of single photoelectrons and the image.</p>

    DOI: 10.11470/houshasen.38.1_25

    CiNii Research

  563. Scintillation properties of Nd<SUP>3+</SUP>, Tm<SUP>3+</SUP>, and Er<SUP>3+</SUP> doped LuF<sub>3</sub> scintillators in the vacuum ultra violet region

    Yanagida, T; Kawaguchi, N; Fukuda, K; Kurosawa, S; Fujimoto, Y; Futami, Y; Yokota, Y; Taniue, K; Sekiya, H; Kubo, H; Yoshikawa, A; Tanimori, T

    NUCLEAR INSTRUMENTS & METHODS IN PHYSICS RESEARCH SECTION A-ACCELERATORS SPECTROMETERS DETECTORS AND ASSOCIATED EQUIPMENT   Vol. 659 ( 1 ) page: 258 - 261   2011.12

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    Publisher:Nuclear Instruments and Methods in Physics Research Section A Accelerators Spectrometers Detectors and Associated Equipment  

    In order to develop novel vacuum ultra violet (VUV) emitting scintillators, we grew Nd 0.5%, Tm 0.5%, and Er 0.5% doped LuF<inf>3</inf> scintillators by the μ-pulling down method, because LuF<inf>3</inf> has a very wide band gap and Nd<sup>3+</sup>, Tm<sup>3+</sup>, and Er<sup>3+</sup> luminescence centers show fast and intense 5d4f emission in VUV region. Transmittance and X-ray induced radioluminescence were studied in these three samples using our original spectrometer made by Bunkou-Keiki company. In the VUV region, transmittance of 2060% was achieved for all the samples. The emission peaks appeared at approximately 180, 165, and 164 nm for Nd<sup>3+</sup>, Tm<sup>3+</sup>, and Er<sup>3+</sup> doped LuF<inf>3</inf>, respectively. Using PMT R8778 (Hamamatsu), we measured their light yields under <sup>241</sup>Am α-ray excitation. Compared with Nd:LaF<inf>3</inf> scintillator, which has 33 photoelectrons/5.5 MeV α, Nd:LuF<inf>3</inf> and Tm:LuF<inf>3</inf> showed 900±90 and 170±20 ph/5.5 MeV-α, respectively. Only for the Nd doped one, we can detect <sup>137</sup>Cs 662 keV γ-ray photoabsorption peak and the light yield of 1200±120 ph/MeV was measured. We also investigated their decay time profiles by picosecond pulse X-ray equipped streak camera, and the main decay component of Nd:LuF<inf>3</inf> turned out to be 7.63 ns. © 2011 Elsevier B.V. All rights reserved.

    DOI: 10.1016/j.nima.2011.08.056

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  564. SMILE-II: Observation of celestial and atmosphereic MeV gamma rays using a balloon-borne wide fields of view Electron-Tracking Compton Camera

    Takada A., Tanimori T., Kubo H., Miuchi K., Kabuki S., Parker J.D., Kishimoto Y., Mizumoto T., Ueno K., Kurosawa S., Iwaki S., Sawano T., Taniue K., Nakamura K., Higashi N., Matsuoka Y., Komura S., Sato Y., Arvelius S., Turunen E.

    European Space Agency Special Publication ESA SP   Vol. 700 SP   page: 567 - 571   2011.12

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    Publisher:European Space Agency Special Publication ESA SP  

    We have developed an Electron Tracking Compton Camera (ETCC) as an MeV gamma-ray telescope in the next generation. The ETCC consists of a gaseous time projection chamber and a position sensitive scintillation camera. We had launched a small size ETCC loaded on a balloon in 2006, and it was successful to obtain the fluxes of diffuse cosmic and atmospheric gamma rays in the energy range between 125 keV and 1.25 MeV. As the next flight (SMILE-II), we planned a long duration flight using a circumpolar balloon launched from Kiruna, and it will observe the celestial bright sources and the atmospheric gamma-ray burst due to the relativistic electron from the radiation belt. In this paper, we report the concepts of our detector and the performance of the SMILE-Il prototype.

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  565. Ultrafast Transparent Ceramic Scintillators Using the Yb<SUP>3+</SUP> Charge Transfer Luminescence in RE<sub>2</sub>O<sub>3</sub> Host

    Yanagida, T; Fujimoto, Y; Kurosawa, S; Watanabe, K; Yagi, H; Yanagitani, T; Jary, V; Futami, Y; Yokota, Y; Yoshikawa, A; Uritani, A; Iguchi, T; Nikl, M

    APPLIED PHYSICS EXPRESS   Vol. 4 ( 12 )   2011.12

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    Publisher:Applied Physics Express  

    We report a new discovery of Yb <sup>3+</sup>-doped ultrafast scintillators based on the Yb <sup>3+</sup> charge transfer luminescence. Transparent ceramic Yb <sup>3+</sup>-doped Y <inf>2</inf>O <inf>3</inf>, Sc <inf>2</inf>O <inf>3</inf>, Lu <inf>2</inf>O <inf>3</inf>, and Yb <inf>2</inf>O <inf>3</inf> were prepared by sintering. When irradiated by γ-and X-rays, they showed a well detectable photoabsorption peak in the pulse height spectra and ultrafast scintillation decay dominated by the decay time of about 1 ns. For the first time, the Yb <sup>3+</sup>-doped oxide materials show detectable scintillation in the pulse height measurement at room temperature with ultrafast scintillation decay. © 2011 The Japan Society of Applied Physics.

    DOI: 10.1143/APEX.4.126402

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  566. Airway management in a patient with Williams syndrome

    Kanaya A., Yasuda T., Kojima A., Saishu T., Kurosawa S.

    Japanese Journal of Anesthesiology   Vol. 60 ( 10 ) page: 1176 - 1179   2011.10

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    Publisher:Japanese Journal of Anesthesiology  

    Williams syndrome is characterized by the triad of supravalvular aortic stenosis (SAS), mental retardation and elfin facies. Generally, difficult airway is expected in patients with Williams syndrome by characteristic face. A 26-year-old female with Williams syndrome was scheduled for abdominal myomectomy under general anesthesia. Difficult mask ventilation and tracheal intubation were anticipated because of micrognathia, mandibular retrusion, and a Mallanpati classIII airway. Before induction of anesthesia the patient breathed 100% oxygen for 3 minutes. Anesthesia was induced and maintained with propofol, remifentanil and rocuronium bromide. Mask ventilation was easily performed. The direct laryngoscopy view was Cormack grade I and there was no difficulty in the tracheal intubation. After induction of anesthesia, anesthetic course was uneventful. According to the most previous clinical reports in patients with Williams syndrome in Japan, mask ventilation and tracheal intubation were performed easily contrary to preoperative airway assessment. In view of SAS, mental retardation, airway deformity and airway assessment in previous clinical reports, we should select the optimal strategy for airway management in patients with Williams syndrome.

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  567. The influence of tidal volume on functional residual capacity during general anesthesia

    Kanaya A., Satoh D., Kurosawa S.

    Japanese Journal of Anesthesiology   Vol. 60 ( 10 ) page: 1149 - 1152   2011.10

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    Publisher:Japanese Journal of Anesthesiology  

    Background : Ventilation with lower tidal volume improves outcome in acute respiratory distress syndrome (ARDS). However, it is questionable if ventilation strategy using lower tidal volumes created for patients with ARDS can be transferred to healthy patients undergoing general anesthesia. We assessed the effects of ventilation with lower tidal volumes and conventional tidal volumes on functional residual capacity (FRC) and Pa <inf>O2</inf>/FI <inf>O2</inf> (P/F) ratio in patients undergoing general anesthesia for upper abdominal surgery. Methods : We studied 16 patients undergoing general anesthesia for upper abdominal surgery. Patients were randomized to ventilation with low tidal volume group (7 ml·kg <sup>-1</sup> predicted body weight n=8) or conventional tidal volume group (10 ml·kg <sup>-1</sup> predicted body weight n=8). We measured FRC and P/F ratio after induction of general anesthesia and start of surgery in both groups. Results : There were no differences in FRC and P/F ratio between ventilation with lower tidal volume group and conventional tidal volume group (P > 0.05), but peak airway pressures with conventional tidal volume group were higher than those with lower tidal volume group only after induction of general anesthesia (P < 0.05). Conclusions : Lower tidal volumes are better than conventional tidal volumes in view of airway pressure and lung protective strategy during general anesthesia.

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  568. [Influence of tidal volume on functional residual capacity during general anesthesia].

    Kanaya A, Satoh D, Kurosawa S

    Masui. The Japanese journal of anesthesiology   Vol. 60 ( 10 ) page: 1149 - 52   2011.10

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    PubMed

  569. Europium and Sodium Codoped LiCaAlF<sub>6</sub> Scintillator for Neutron Detection

    Yanagida, T; Yamaji, A; Kawaguchi, N; Fujimoto, Y; Fukuda, K; Kurosawa, S; Yamazaki, A; Watanabe, K; Futami, Y; Yokota, Y; Uritani, A; Iguchi, T; Yoshikawa, A; Nikl, M

    APPLIED PHYSICS EXPRESS   Vol. 4 ( 10 )   2011.10

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    A recent study has revealed that a Eu-doped LiCaAlF<inf>6</inf> (Eu:LiCAF) crystalline scintillator showed good scintillation response under thermal neutron exposure. We discover here that Eu and Na codoped LiCAF exhibits superior scintillation properties to Eu:LiCAF. We grew Eu 2% and Na 0.5, 1, and 2% codoped LiCAF by the micropulling down method. In radioluminescence spectra, they showed intense emission peaking at 370nm due to Eu<sup>2+</sup> 5d-4f transition. In particular, the light yield of Eu 2% Na 2%-doped LiCAF reached 40000 ph/n, which was about 30% higher than that of Eu:LiCAF. © 2011 The Japan Society of Applied Physics.

    DOI: 10.1143/APEX.4.106401

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  570. Comparison of actual tidal volume in neonatal lung model volume control ventilation using three ventilators

    Toyama, H; Endo, Y; Ejima, Y; Matsubara, M; Kurosawa, S

    ANAESTHESIA AND INTENSIVE CARE   Vol. 39 ( 4 ) page: 599 - 606   2011.7

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  571. Comparison of actual tidal volume in neonatal lung model volume control ventilation using three ventilators

    Toyama H., Endo Y., Ejima Y., Matsubara M., Kurosawa S.

    Anaesthesia and Intensive Care   Vol. 39 ( 4 ) page: 599 - 606   2011.7

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    Publisher:Anaesthesia and Intensive Care  

    In neonates, small changes in tidal volumes (V<inf>T</inf>) may lead to complications. Previous studies have shown a significant difference between ventilator-measured tidal volume and tidal volume delivered (actual V <inf>T</inf>). We evaluated the accuracy of three different ventilators to deliver small V<inf>T</inf> during volume-controlled ventilation. We tested Servo 300, 840 ventilator and Evita 4 Neoflow ventilators with lung models simulating normal and injured neonatal lung compliance models. Gas volume delivered from the ventilator into the test circuit (V<inf>TV</inf>) and actual V<inf>T</inf> to the test lung were measured using Ventrak respiration monitors at set V<inf>T</inf> (30 ml). The gas volume increase of the breathing circuit was then calculated. Tidal volumes of the SV300 and PB840 in both lung models were similar to the set V<inf>T</inf> and the actual tidal volumes in the injured model (20.7 ml and 19.8 ml, respectively) were significantly less than that in the normal model (27.4 ml and 23.4 ml). PB840 with circuit compliance compensation could not improve the actual V<inf>T</inf> . V<inf>TV</inf> of the EV4N in the normal and the injured models (37.8 ml and 46.6 ml) were markedly increased compared with set V<inf>T</inf> , and actual V<inf>T</inf> were similar to set V<inf>T</inf> in the normal and injured model (30.2 ml and 31.9 ml, respectively). EV4N measuring V<inf>T</inf> close to the lung could match actual V<inf>T</inf> to almost the same value as the set V<inf>T</inf> , however the gas volume of the breathing circuit was increased. If an accurate value for the patient's actual V<inf>T</inf> is needed, this V<inf>T</inf> must be measured by a sensor located between the Y-piece and the tracheal tube.

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  572. OBSERVATION OF DIFFUSE COSMIC AND ATMOSPHERIC GAMMA RAYS AT BALLOON ALTITUDES WITH AN ELECTRON-TRACKING COMPTON CAMERA Open Access

    Takada, A; Kubo, H; Nishimura, H; Ueno, K; Hattori, K; Kabuki, S; Kurosawa, S; Miuchi, K; Mizuta, E; Nagayoshi, T; Nonaka, N; Okada, Y; Orito, R; Sekiya, H; Takeda, A; Tanimori, T

    ASTROPHYSICAL JOURNAL   Vol. 733 ( 1 )   2011.5

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    Publisher:Astrophysical Journal  

    We observed diffuse cosmic and atmospheric gamma rays at balloon altitudes with the Sub-MeV gamma-ray Imaging Loaded-on-balloon Experiment I (SMILE-I) as the first step toward a future all-sky survey with a high sensitivity. SMILE-I employed an electron-tracking Compton camera comprised of a gaseous electron tracker as a Compton-scattering target and a scintillation camera as an absorber. The balloon carrying the SMILE-I detector was launched from the Sanriku Balloon Center of the Institute of Space and Astronautical Science/Japan Aerospace Exploration Agency on 2006 September 1, and the flight lasted for 6.8hr, including level flight for 4.1hr at an altitude of 32-35km. During the level flight, we successfully detected 420 downward gamma rays between 100keV and 1MeV at zenith angles below 60°. To obtain the flux of diffuse cosmic gamma rays, we first simulated their scattering in the atmosphere using Geant4, and for gamma rays detected at an atmospheric depth of 7.0gcm<sup>-2</sup> we found that 50% and 21% of the gamma rays at energies of 150keV and 1MeV, respectively, were scattered in the atmosphere prior to reaching the detector. Moreover, by using Geant4 simulations and the QinetiQ atmospheric radiation model, we estimated that the detected events consisted of diffuse cosmic and atmospheric gamma rays (79%), secondary photons produced in the instrument through the interaction between cosmic rays and materials surrounding the detector (19%), and other particles (2%). The obtained growth curve was comparable to Ling's model, and the fluxes of diffuse cosmic and atmospheric gamma rays were consistent with the results of previous experiments. The expected detection sensitivity of a future SMILE experiment measuring gamma rays between 150keV and 20MeV was estimated from our SMILE-I results and was found to be 10 times better than that of other experiments at around 1MeV. © 2011. The American Astronomical Society. All rights reserved..

    DOI: 10.1088/0004-637X/733/1/13

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  573. A new imaging device based on UV scintillators and a large area gas photomultiplier

    Sekiya, H; Ida, C; Kubo, H; Kurosawa, S; Miuchi, K; Tanimori, T; Taniue, K; Yoshikawa, A; Yanagida, T; Yokota, Y; Fukuda, K; Ishizu, S; Kawaguchi, N; Suyama, T

    NUCLEAR INSTRUMENTS & METHODS IN PHYSICS RESEARCH SECTION A-ACCELERATORS SPECTROMETERS DETECTORS AND ASSOCIATED EQUIPMENT   Vol. 633 ( SUPPL. 1 ) page: S36 - S39   2011.5

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    Publisher:Nuclear Instruments and Methods in Physics Research Section A Accelerators Spectrometers Detectors and Associated Equipment  

    A new type high spatial resolution radiation detector based on a UV scintillatora UV imaging gas photomultiplier is presented. The prototype UV detector consists of a 10 cm×10 cm μPIC, 2 GEMs and a semitransparent CsI photocathode deposited on a MgF<inf>2</inf> window. The effective photo-sensitive area is φ34 mm and the readouts are 400 μm pitch strips. A newly developed 20 mm size LaF<inf>3</inf>(Nd) crystal which emits 172 nm photons is coupled to the detector for the first step. The detector was tested in pulse mode operation with 5.5 MeV α particles from <sup>241</sup>Am. The single photoelectrons were successfully detected and the images of the crystal shape were clearly obtained. © 2010 Elsevier B.V. All rights reserved.

    DOI: 10.1016/j.nima.2010.06.114

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  574. Impaired endothelial progenitor cell mobilization and colony-forming capacity in chronic obstructive pulmonary disease

    Takahashi, T; Suzuki, S; Kubo, H; Yamaya, M; Kurosawa, S; Kato, M

    RESPIROLOGY   Vol. 16 ( 4 ) page: 680 - 687   2011.5

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    Language:English   Publisher:Respirology  

    Background and objective: Recent studies suggest that there is endothelial impairment in both the systemic and pulmonary circulations of patients with COPD. Endothelial progenitor cells (EPC) are mobilized into the circulation by physiological stressors such as surgery, and are thought to play a role in the repair of damaged endothelium. There has been a steady increase in the frequency of surgery among COPD patients, due to the incidence of complications and lung cancer; however, the mobilization of EPC during lung resection has not been examined. We evaluated whether the mobilization and proliferation of EPC are impaired in COPD patients. Methods: The numbers of circulating EPC (CD34/KDR/AC133-positive mononuclear cells) were measured by flow cytometry, in COPD patients (n = 30) and non-COPD patients (n = 30) who were undergoing thoracic surgery. EPC colony-forming units (EPC-CFU) were also examined. Results: In non-COPD patients, both circulating EPC and EPC-CFU were significantly increased 2 h after the operation started, whereas in COPD patients there were no changes in circulating EPC or EPC-CFU, irrespective of the severity of COPD. Multiple linear regression analysis demonstrated that the presence of COPD was the only significant independent predictor of reduced mobilization of EPC during thoracic surgery. Conclusions: The number of circulating EPC and EPC-CFU was not increased during thoracic surgery in COPD patients. These results indicate that both the mobilization and proliferative capacity of EPC are severely impaired in COPD patients. Endothelial progenitor cell (EPC) numbers and colony-forming units (CFU) were compared in COPD and non-COPD patients undergoing thoracic surgery. Both circulating EPC numbers and EPC-CFU were increased during surgery in non-COPD patients, but not in COPD patients. The mobilization and proliferative capacity of EPC may be severely impaired in COPD patients. © 2011 Asian Pacific Society of Respirology.

    DOI: 10.1111/j.1440-1843.2011.01959.x

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  575. Development of an Electron-Tracking Compton Camera using CF<sub>4</sub> gas at high pressure for improved detection efficiency

    Takahashi, M; Kabuki, S; Hattori, K; Higashi, N; Iwaki, S; Kubo, H; Kurosawa, S; Miuchi, K; Nakamura, K; Nishimura, H; Parker, JD; Sawano, T; Takada, A; Tanimori, T; Taniue, K; Ueno, K

    NUCLEAR INSTRUMENTS & METHODS IN PHYSICS RESEARCH SECTION A-ACCELERATORS SPECTROMETERS DETECTORS AND ASSOCIATED EQUIPMENT   Vol. 628 ( 1 ) page: 150 - 153   2011.2

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    Publisher:Nuclear Instruments and Methods in Physics Research Section A Accelerators Spectrometers Detectors and Associated Equipment  

    We have developed an Electron-Tracking Compton Camera (ETCC) for medical imaging and MeV gamma-ray astronomy. The ETCC consists of a gaseous Time Projection Chamber (μ-TPC) and pixel scintillator arrays. To improve the detection efficiency, we have optimized the gas mixture in the μ-TPC and operated the ETCC at high pressure. Basic characteristics such as the gas gain, drift velocity, energy resolution, and position resolution of the μ-TPC were examined, and using this optimization, both the efficiency and the angular resolution of the ETCC were measured. We achieved a steady gas gain of ∼20,000 in Ar/CF<inf>4</inf>/isoC<inf>4</inf>H<inf>10</inf> (54:40:6) at 1.4 atm. The diffusion constant in Ar/CF<inf>4</inf>/isoC<inf>4</inf>H<inf>10</inf> (54:40:6) at 1.4 atm was ∼2 times better than in Ar/C<inf>2</inf>H <inf>6</inf> (90:10) at 1 atm. The efficiency in Ar/CF<inf>4</inf>/isoC <inf>4</inf>H<inf>10</inf> (54:40:6) at 1.4 atm was also ∼2 times higher than in Ar/C<inf>2</inf>H<inf>6</inf> (90:10) at 1 atm. © 2010 Elsevier B.V. All rights reserved.

    DOI: 10.1016/j.nima.2010.06.305

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  576. Development of the tracking Compton/pair-creation camera based on a gaseous TPC and a scintillation camera

    Ueno, K; Tanimori, T; Kubo, H; Miuchi, K; Kabuki, S; Iwaki, S; Higashi, N; Parker, JD; Kurosawa, S; Takahashi, M; Sawano, T; Taniue, K; Nakamura, K; Toyokawa, H; Takada, A; Nishimura, H; Hattori, K

    NUCLEAR INSTRUMENTS & METHODS IN PHYSICS RESEARCH SECTION A-ACCELERATORS SPECTROMETERS DETECTORS AND ASSOCIATED EQUIPMENT   Vol. 628 ( 1 ) page: 158 - 161   2011.2

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    Publisher:Nuclear Instruments and Methods in Physics Research Section A Accelerators Spectrometers Detectors and Associated Equipment  

    We have evaluated the possibility of the Electron-Tracking Compton Camera (ETCC) to simultaneously operate as a pair-creation camera. The ETCC consists of a gaseous micro-time projection chamber (micro-TPC) and a scintillation camera. Several prototypes of the camera were developed and their performance was studied. Because the micro-TPC can detect a large number of hit points along one charged particle track, has a good position resolution of about 0.2 mm, and uses the filling gas as the scattering material, the influence of multiple scattering is small. This makes the micro-TPC well-suited to detecting pair-creation events. We have examined the performance of a camera of size 10×10×15 cm<sup>3</sup>, using the pair-creation mode in the energy range of 10100 MeV. Using this camera, we performed a proof-of-principle experiment with laser inverse Compton gamma rays at the National Institute of Advanced Industrial Science and Technology (AIST), and we succeeded in tracking electronpositron pairs and in reconstructing 10 and 20 MeV gamma rays. In this paper, we report the fundamental performance of the gamma-ray camera with pair-creation mode. © 2010 Elsevier B.V. All rights reserved.

    DOI: 10.1016/j.nima.2010.06.307

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  577. IMPACT OF REDUCTION IN GVHD-RELATED MORTALITY FOR RECENT IMPROVEMENT OF NON-RELAPSE MORTALITY AFTER ALLOGENEIC HEMATOPOIETIC CELL TRANSPLANTATION Open Access

    Kurosawa, S; Yakushijin, K; Yamaguchi, T; Atsuta, Y; Nagamura-Inoue, T; Akiyama, H; Taniguchi, S; Miyamura, K; Takahashi, S; Eto, T; Morishima, Y; Sakamaki, H; Fukuda, T

    BIOLOGY OF BLOOD AND MARROW TRANSPLANTATION   Vol. 17 ( 2 ) page: S288 - S289   2011.2

  578. 6LiF-SrxCa1-xF2 doped with Ce and Eu eutectic scintillator for neutron detection

    Yanagida T., Fukuda K., Fujimoto Y., Kawaguchi N., Yamazaki A., Watanabe K., Futami Y., Pejchal J., Kurosawa S., Yokota Y., Yoshikawa A.

    IEEE Nuclear Science Symposium Conference Record     page: 1594 - 1597   2011

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    Publisher:IEEE Nuclear Science Symposium Conference Record  

    Eu<sup>2+</sup> 0.05, 0.1, and 0.2% activated LiF-SrF<inf>2</inf> eutectic scintillators were fabricated by the Bridgman method using <sup>6</sup>Li enriched (95%) raw material. In α-ray induced radio luminescence spectra, Eu<sup>2+</sup> doped eutectic scintillators showed intense emission peak at 430 nm due to an emission from Eu<sup>2+</sup> 5d-4f transition of Eu:SrF <inf>2</inf> layers. When <sup>252</sup>Cf neutrons were irradiated, they exhibited almost the same light yields of 5000-7000 ph/n with a typical decay times of several hundreds ns. © 2011 IEEE.

    DOI: 10.1109/NSSMIC.2011.6154639

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  579. <SUP>6</SUP>LiF-Sr<sub>x</sub>Ca<sub>1-x</sub>F<sub>2</sub> doped with Ce and Eu eutectic scintillator for neutron detection

    Yanagida, T; Fukuda, K; Fujimoto, Y; Kawaguchi, N; Yamazaki, A; Watanabe, K; Futami, Y; Pejchal, J; Kurosawa, S; Yokota, Y; Yoshikawa, A

    2011 IEEE NUCLEAR SCIENCE SYMPOSIUM AND MEDICAL IMAGING CONFERENCE (NSS/MIC)     page: 1594 - 1597   2011

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  580. Clinical Characteristics of Young-Onset and Medical Treatment-Requiring Hypertension Identified By Targeted Screening in University Health Check-Up

    Endo, Y; Serizawa, F; Kato, T; Toyama, H; Ejima, Y; Sato, A; Kurosawa, S; Hasegawa, Y; Hida, W; Matsubara, M

    CLINICAL AND EXPERIMENTAL HYPERTENSION   Vol. 33 ( 8 ) page: 552 - 557   2011

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    Language:English   Publisher:Clinical and Experimental Hypertension  

    Based on targeted screening for hypertension at a university health check-up, we previously reported a high incidence of white-coat hypertension and estimated prevalence of hypertension requiring medical treatments (HT) as around 0.1% in young population aged less than 30. In spite of such low prevalence, continuous screening for seven consecutive years (20032009) increased the number of HT students to 20 (19 males and 1 female). We presently assessed the clinical characteristics of these HTs. Renovascular hypertension was found in the only female HT and aortic valve regurgitation in two HTs. Resting 17 HTs were diagnosed as having essential hypertension (EH). A father and/or a mother had EH in 16 out of 17 EHs, and blood pressure (BP) at home was slightly elevated (135145 mm Hg in systolic) except three obese EHs (body mass index more than 30) who demonstrated more than 160 mm Hg in systolic. Plasma aldosterone-renin ratio (ARR) of EHs did not differ from that of normal controls, and Pearson correlation coefficient (R) between ARR and systolic BP (SBP) was -0.2. Its partial correlation coefficient, however, was statistically significant (R = -0.55, P = .026) after correcting for body mass index, which was significantly correlated with both SBP (P = .006, after correcting for ARR) and ARR (P = .004, after correcting for SBP). In conclusion, most of young-onset HTs are male EHs, and aortic valve regurgitation should be carefully checked. Excess plasma renin activity would be one of additional characteristics of young-onset EH to male gender, genetic background, and increased body mass. © Informa Healthcare USA, Inc.

    DOI: 10.3109/10641963.2011.577482

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    PubMed

  581. Dopant segregation in Czochralski grown rare-earth-ion doped 6LiCaAlF6 single crystal for thermal neutron detection

    Kawaguchi N., Yanagida T., Fujimoto Y., Yamazaki A., Watanabe K., Fukuda K., Kurosawa S., Futami Y., Yokota Y., Yoshikawa A.

    IEEE Nuclear Science Symposium Conference Record     page: 1591 - 1593   2011

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    Publisher:IEEE Nuclear Science Symposium Conference Record  

    Dopant segregation in Ce doped <sup>6</sup>LiCaAlF<inf>6</inf> single crystal was researched by evaluating a position dependence of light yields in the crystal. Ce doped <sup>6</sup>LiCaAlF<inf>6</inf> single crystal was grown by Czochralski technique and several parts of the crystal were cut from grown crystal and polished. Position dependence of radioluminescence spectra and pulse height spectra were investigated. © 2011 IEEE.

    DOI: 10.1109/NSSMIC.2011.6154638

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  582. Dopant Segregation in Czochralski Grown Rare-Earth-Ion Doped <SUP>6</SUP>LiCaAlF<sub>6</sub> Single Crystal for Thermal Neutron Detection

    Kawaguchi, N; Yanagida, T; Fujimoto, Y; Yamazaki, A; Watanabe, K; Fukuda, K; Kurosawa, S; Futami, Y; Yokota, Y; Yoshikawa, A

    2011 IEEE NUCLEAR SCIENCE SYMPOSIUM AND MEDICAL IMAGING CONFERENCE (NSS/MIC)     page: 1591 - 1593   2011

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  583. Light output uniformity of Czochralski grown rare-earth-ion doped 6LiCaAlF6 single crystal for thermal neutron detection

    Kawaguchi N., Yanagida T., Fujimoto Y., Yamazaki A., Watanabe K., Fukuda K., Kajimoto S., Fukumura H., Kurosawa S., Futami Y., Yokota Y., Yoshikawa A.

    IEEE Nuclear Science Symposium Conference Record     page: 4869 - 4871   2011

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    Publisher:IEEE Nuclear Science Symposium Conference Record  

    Light output uniformity of Ce doped <sup>6</sup>LiCaAlF<inf>6</inf> single crystal was researched. Ce doped <sup>6</sup>LiCaAlF<inf>6</inf> single crystal was grown by Czochralski technique and several parts of the crystal were cut from grown crystal and polished. Position dependence of radioluminescence spectra and pulse height spectra were investigated. © 2011 IEEE.

    DOI: 10.1109/NSSMIC.2011.6152487

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  584. Light Output Uniformity of Czochralski Grown Rare-Earth-Ion Doped <SUP>6</SUP>LiCaAlF<sub>6</sub> Single Crystal for Thermal Neutron Detection

    Kawaguchi, N; Yanagida, T; Fujimoto, Y; Yamazaki, A; Watanabe, K; Fukuda, K; Kajimoto, S; Fukumura, H; Kurosawa, S; Futami, Y; Yokota, Y; Yoshikawa, A

    2011 IEEE NUCLEAR SCIENCE SYMPOSIUM AND MEDICAL IMAGING CONFERENCE (NSS/MIC)     page: 4869 - 4871   2011

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  585. Neutron Imaging Detector Based on the μPIC Micro-Pixel Gaseous Chamber

    Parker, JD; Harada, M; Hattori, K; Iwaki, S; Kabuki, S; Kishimoto, Y; Kubo, H; Kurosawa, S; Miuchi, K; Nishimura, H; Oku, T; Sawano, T; Shinohara, T; Suzuki, J; Tanimori, T; Ueno, K

    2011 IEEE NUCLEAR SCIENCE SYMPOSIUM AND MEDICAL IMAGING CONFERENCE (NSS/MIC)     page: 393 - 399   2011

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  586. Neutron imaging detector based on the μpIC micro-pixel gaseous chamber

    Parker J.D., Harada M., Hattori K., Iwaki S., Kabuki S., Kishimoto Y., Kubo H., Kurosawa S., Miuchi K., Nishimura H., Oku T., Sawano T., Shinohara T., Suzuki J.I., Tanimori T., Ueno K.

    IEEE Nuclear Science Symposium Conference Record     page: 393 - 399   2011

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    Publisher:IEEE Nuclear Science Symposium Conference Record  

    A neutron imaging detector employing the micro-pixel gaseous chamber (μPIC) and an FPGA (Field Programmable Gate Array)-based data acquisition system has been developed for applications in small-angle neutron scattering (SANS) and neutron radiography at high-intensity, pulsed neutron sources. A small amount of <sup>3</sup>He added to the gas mixture is used as the neutron absorber, with a detection efficiency for thermal neutrons of up to 30%. Our FPGA program permits the simultaneous measurement of the track length and energy deposition for the resulting proton-triton tracks, allowing the separation of the proton and triton for improved position resolution. The detector features a spatial resolution of less than 120 μm, a time resolution of ∼1 μs, and an effective gamma sensitivity of less than 10<sup>-9</sup>. We report preliminary results from a third test experiment performed in February 2011 at the NOBORU beam line at the J-PARC spallation neutron source. We will also discuss ongoing efforts to optimize the gas mixture for improved position resolution and planned upgrades to the data acquisition system. © 2011 IEEE.

    DOI: 10.1109/NSSMIC.2011.6154525

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  587. Simulation Study for the Higher Sensitivity of an Electron-Tracking Compton Camera at over 1 MeV

    Takada, A; Tanimori, T; Kubo, H; Miuchi, K; Kabuki, S; Parker, JD; Kishimoto, Y; Mizumoto, T; Ueno, K; Kurosawa, S; Iwaki, S; Sawano, T; Taniue, K; Nakamura, K; Higashi, N; Matsuoka, Y; Komura, S; Sato, Y

    2011 IEEE NUCLEAR SCIENCE SYMPOSIUM AND MEDICAL IMAGING CONFERENCE (NSS/MIC)     page: 1215 - 1221   2011

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  588. SMILE: A balloon-borne sub-MeV/MeV gamma-ray Compton Camera using an Electron-Tracking gaseous TPC and a scintillation camera

    Sawano T., Hattori K., Higashi N., Iwaki I., Kabuki S., Kishimoto Y., Kubo H., Kurosawa S., Matsuoka Y., Miuchi K., Nakamura K., Nishimura H., Parker J., Takada A., Takahashi M., Tanimori T., Taniue K., Ueno K.

    Proceedings of the 32nd International Cosmic Ray Conference Icrc 2011   Vol. 9   page: 183 - 186   2011

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    Publisher:Proceedings of the 32nd International Cosmic Ray Conference Icrc 2011  

    We have been developing an Electron-Tracking Compton Camera (ETCC) as a next generation MeV gammaray detector, consisting of a gaseous electron tracker which measures the three-dimensional track and the energy of the Compton-recoil electron, and pixel scintillation arrays which measure the absorption point and the energy of the scattered gamma ray. As the first step toward a future all-sky survey with a planned sensitivity of one order magnitude higher than COMPTEL, we successfully observed the diffuse cosmic and atmospheric gamma rays at balloon altitudes with a small ETCC in the Sub-MeV gamma-ray Imaging Loaded-on-balloon Experiment I (SMILE-I). Building on the success of the SMILE-I ETCC, we are developing a large size ETCC for the next flight to observe celestial objects in the sub-MeV/MeV region. This larger detector is expected to achieve a sensitivity comparable to COMPTEL.

    DOI: 10.7529/ICRC2011/V09/1120

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  589. SMILE-II: OBSERVATION OF CELESTIAL AND ATMOSPHEREIC MEV GAMMA RAYS USING A BALLOON-BORNE WIDE FIELDS OF VIEW ELECTRON-TRACKING COMPTON CAMERA

    Takada, A; Tanimori, T; Kubo, H; Miuchi, K; Kabuki, S; Parker, JD; Kishimoto, Y; Mizumoto, T; Ueno, K; Kurosawa, S; Iwaki, S; Sawano, T; Taniue, K; Nakamura, K; Higashi, N; Matsuoka, Y; Komura, S; Sato, Y; Arvelius, S; Turunen, E

    20TH ESA SYMPOSIUM ON EUROPEAN ROCKET AND BALLOON PROGRAMMES AND RELATED RESEARCH   Vol. 700   page: 567 - 571   2011

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  590. Simulation study for the higher sensitivity of an electron-tracking compton camera at over 1 MeV

    Takada A., Tanimori T., Kubo H., Miuchi K., Kabuki S., Parker J.D., Kishimoto Y., Mizumoto T., Ueno K., Kurosawa S., Iwaki S., Sawano T., Taniue K., Nakamura K., Higashi N., Matsuoka Y., Komura S., Sato Y.

    IEEE Nuclear Science Symposium Conference Record     page: 1215 - 1221   2011

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    Publisher:IEEE Nuclear Science Symposium Conference Record  

    We have developed an Electron-Tracking Compton Camera (ETCC) as a next-generation MeV gamma-ray telescope. Our detector consists of a gaseous electron tracker as a Compton-scattering target and a position sensitive scintillation camera as a scattered gamma ray absorber. We launched a small size (10 cm cubic) ETCC loaded on a balloon in 2006, and obtained the fluxes of diffuse cosmic and atmospheric gamma rays in the energy range between 125 keV and 1:25 MeV. However, for MeV gamma-ray astronomy, we need to detect the photons at higher energy, thus we must improve the sensitivity of the ETCC in the higher energy range above 1 MeV. For this purpose, we investigate an electron absorber, which is placed between the electron tracker and the photo-absorber. Using Geant4 simulation, we confirmed that the detection energy range is shifted to the range of 0:35-5:0 MeV for the new configuration of the ETCC. © 2011 IEEE.

    DOI: 10.1109/NSSMIC.2011.6154605

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  591. Imaging study of a phantom and small animal with a two-head electron-tracking Compton gamma-ray camera Open Access

    Kabuki S., Kimura H., Amano H., Nakamoto Y., Kubo H., Miuchi K., Kurosawa S., Kawashima H., Ueda M., Ogawa K., Togashi K., Saji H., Tanimori T., Okada T., Takahashi M.

    IEEE Nuclear Science Symposium Conference Record     page: 2844 - 2847   2010.12

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    Publisher:IEEE Nuclear Science Symposium Conference Record  

    We have developed an electron-tracking Compton camera (ETCC) for new medical imaging device. Conventional gamma camera, PET and SPECT, have the problem of energy limitation. This problem is one of the major problems for this study. However, our ETCC has a wide energy dynamic range (200-1300 keV). Also ETCC have the wide field of view because ETCC does not need a collimator and does not need to catch two gamma rays which produced by the annihilation process. In this paper, we show the results of imaging result of the 3-D which have imaged only one direction using one head camera. And we have developed the two-head ETCC. Two-head ETCC have a good efficiency and spatial resolution. © 2010 IEEE.

    DOI: 10.1109/NSSMIC.2010.5874313

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  592. Performance of a neutron imaging detector based on the μpIC micro-pixel gaseous chamber

    Parker J.D., Harada M., Hattori K., Iwaki S., Kabuki S., Kishimoto Y., Kubo H., Kurosawa S., Miuchi K., Nishimura H., Oku T., Sawano T., Shinohara T., Suzuki J.I., Tanimori T., Ueno K.

    IEEE Nuclear Science Symposium Conference Record     page: 291 - 297   2010.12

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    Publisher:IEEE Nuclear Science Symposium Conference Record  

    A new detector employing a time projection chamber built on the micro-pixel gaseous chamber (PIC) and an FPGA (Field Programmable Gate Array)-based data acquisition system has been developed as a thermal-neutron imaging detector for small-angle neutron scattering (SANS) and neutron radiography. A small amount of <sup>3</sup>He added to the gas mixture is used as the neutron absorber, giving a detection efficiency for thermal neutrons of up to 30%. An improved FPGA program permits the simultaneous measurement of the track length and energy deposition for the resulting proton-triton pairs, allowing the separation of the proton and triton for improved position resolution. Here we report the preliminary results of several test experiments performed at the NOBORU beam line at the J-PARC Spallation Neutron Source in November 2009 and June 2010. During these experiments, we observed time-averaged data rates up to 4.5 MHz, and with a time resolution on the order of 1 s per neutron event, we were able to cleanly separate the individual neutron pulses and determine neutron energy by time-of-flight. Using images of cadmium test charts, the position resolution of our detector was estimated as 315 15m (preliminary). We also successfully observed resonance absorption in various metals, SANS diffraction from spherical SiO<inf>2</inf> nanoparticles, and Bragg edge transmission of a welded steel plate. © 2010 IEEE.

    DOI: 10.1109/NSSMIC.2010.5873767

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  593. Changes In Incidence and Causes of Non-Relapse Mortality (NRM) After Allogeneic Hematopoietic Cell Transplantation (allo-HCT): Are Transplants Improving?

    Kurosawa, S; Yakushijin, K; Yamaguchi, T; Atsuta, Y; Nagamura-Inoue, T; Akiyama, H; Taniguchi, S; Miyamura, K; Takahashi, S; Eto, T; Morishima, Y; Sakamaki, H; Fukuda, T

    BLOOD   Vol. 116 ( 21 ) page: 397 - 397   2010.11

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  594. Development of an 8 x 8 array of LaBr<sub>3</sub>(Ce) scintillator pixels for a gaseous Compton gamma-ray camera

    Kurosawa, S; Kubo, H; Hattori, K; Ida, C; Iwaki, S; Kabuki, S; Kubo, A; Kunieda, E; Miuchi, K; Nakahara, T; Nishimura, H; Parker, JD; Takada, A; Takahashi, M; Tanimori, T; Ueno, K

    NUCLEAR INSTRUMENTS & METHODS IN PHYSICS RESEARCH SECTION A-ACCELERATORS SPECTROMETERS DETECTORS AND ASSOCIATED EQUIPMENT   Vol. 623 ( 1 ) page: 249 - 251   2010.11

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    Publisher:Nuclear Instruments and Methods in Physics Research Section A Accelerators Spectrometers Detectors and Associated Equipment  

    We have developed LaBr<inf>3</inf>(Ce) pixel scintillator arrays for an electron-tracking Compton camera (ETCC) that consists of a gaseous time projection chamber (TPC) and the scintillators. The TPC measures the three-dimensional track and energy of a Compton recoil electron, while the scintillators measure the energy and position of the scattered gamma ray. Therefore, the ETCC is able to reconstruct Compton scattering event by event. We adopted LaBr<inf>3</inf>(Ce) scintillators because the angular resolution of the ETCC depends on the energy resolution of the scintillators, and LaBr <inf>3</inf>(Ce) has an FWHM energy resolution of about 3% at 662 keV using a single-anode photomultiplier tube (PMT). We have developed an 8×8 array of LaBr<inf>3</inf>(Ce) scintillator pixels with a pixel size of 5.8×5.8×15.0 mm<sup>3</sup>, which has an FWHM energy resolution of 5.8±0.9% at 662 keV when coupled to a multi-anode PMT (Hamamatsu H8500). The ETCC with the LaBr<inf>3</inf>(Ce) arrays has an FWHM angular resolution of 4.2±0.3° at 662 keV. © 2010 Elsevier B.V. All rights reserved.

    DOI: 10.1016/j.nima.2010.02.211

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  595. Electron-tracking Compton gamma-ray camera for small animal and phantom imaging

    Kabuki, S; Kimura, H; Amano, H; Nakamoto, Y; Kubo, H; Miuchi, K; Kurosawa, S; Takahashi, M; Kawashima, H; Ueda, M; Okada, T; Kubo, A; Kunieda, E; Nakahara, T; Kohara, R; Miyazaki, O; Nakazawa, T; Shirahata, T; Yamamoto, E; Ogawa, K; Togashi, K; Saji, H; Tanimori, T

    NUCLEAR INSTRUMENTS & METHODS IN PHYSICS RESEARCH SECTION A-ACCELERATORS SPECTROMETERS DETECTORS AND ASSOCIATED EQUIPMENT   Vol. 623 ( 1 ) page: 606 - 607   2010.11

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    Publisher:Nuclear Instruments and Methods in Physics Research Section A Accelerators Spectrometers Detectors and Associated Equipment  

    We have developed an electron-tracking Compton camera (ETCC) for medical use. Our ETCC has a wide energy dynamic range (2001300 keV) and wide field of view (3 sr), and thus has potential for advanced medical use. To evaluate the ETCC, we imaged the head (brain) and bladder of mice that had been administered with F-18-FDG. We also imaged the head and thyroid gland of mice using double tracers of F-18-FDG and I-131 ions. © 2010 Elsevier B.V. All rights reserved.

    DOI: 10.1016/j.nima.2010.03.085

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  596. First underground results with NEWAGE-0.3a direction-sensitive dark matter detector Open Access

    Miuchi, K; Nishimura, H; Hattori, K; Higashi, N; Ida, C; Iwaki, S; Kabuki, S; Kubo, H; Kurosawa, S; Nakamura, K; Parker, J; Sawano, T; Takahashi, M; Tanimori, T; Taniue, K; Ueno, K; Sekiya, H; Takeda, A; Tsuchiya, K; Takada, A

    PHYSICS LETTERS B   Vol. 686 ( 1 ) page: 11 - 17   2010.3

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    Publisher:Physics Letters Section B Nuclear Elementary Particle and High Energy Physics  

    A direction-sensitive dark matter search experiment at Kamioka underground laboratory with the NEWAGE-0.3a detector was performed. The NEWAGE-0.3a detector is a gaseous micro-time-projection chamber filled with CF<inf>4</inf> gas at 152 Torr. The fiducial volume and target mass are 20 × 25 × 31 cm<sup>3</sup> and 0.0115 kg, respectively. With an exposure of 0.524 kg days, improved spin-dependent weakly interacting massive particle (WIMP)-proton cross section limits by a direction-sensitive method were achieved including a new record of 5400 pb for 150 GeV/ c<sup>2</sup> WIMPs. We studied the remaining background and found that ambient γ-rays contributed about one-fifth of the remaining background and radioactive contaminants inside the gas chamber contributed the rest. © 2010 Elsevier B.V. All rights reserved.

    DOI: 10.1016/j.physletb.2010.02.028

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  597. Result and Prospect for Balloon-Borne Experiments of Sub-MeV and MeV Gamma-ray Astronomy using an Electron-Tracking Compton Camera

    Tanimori T., Kubo H., Kurosawa S., Ida C., Iwaki S., Miuchi K., Mizuta E., Nagayoshi T., Nishimura H., Hattori K., Nonaka N., Kabuki S., Okada Y., Orito R., Takada A., Takahashi M., Ueno K.

    JAXA research and development report   Vol. 9   page: 19 - 30   2010.3

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    Language:Japanese   Publisher:Japan Aerospace Exploration Agency  

    We developed the Electron-Tracking Compton Camera (ETCC) with reconstructing the track of a recoil electron in Compton process for both sub-MeV and MeV gamma rays to explore MeV gamma-ray astronomy in space. By adding the direction of a recoil electron to Compton reconstruction method, the direction of the incident gamma ray is determined for each individual photon. Also, an angle between the recoil electron and scattered gamma ray is powerful for the kinematical background-rejection. Since MeV gamma-ray astronomy has suffered from huge background so far, this new method is expected to increase the sensitivity. In the simulation, a 50 cm cubic ETCC would provide about 10 times better sensitivity than that of COMPTEL for one year observation in space. As a first step, we observed diffuse cosmic and atmospheric gamma rays at balloon altitudes with an ETCC consisting of the 10 cm cubic Time Projection Chamber (μ-TPC) and the GSO crystal pixel arrays surrounding the μ-TPC (SMILE-I). This instrument was launched on 1st September, 2006 from the Sanriku Balloon Center, and we successfully carried out about 3-hour observation time at an altitude of 32-35 km, and consequently obtained the both gamma-ray spectra between 0.1 and 1 MeV. In addition, this result indicates that the expected detection sensitivity of a future SMILE experiment between 150 keV and 20 MeV would provide a ten times better sensitivity than those of other missions at around 1 MeV. For the next balloon-borne experiment, we are developing a larger ETCC for detecting sub-MeV gamma rays from celestial point sources such as Crab and Cygnus X-1 during a few hours observation.

    CiNii Research

  598. THE CASE FOR A DIRECTIONAL DARK MATTER DETECTOR AND THE STATUS OF CURRENT EXPERIMENTAL EFFORTS Open Access

    Ahlen, S; Afshordi, N; Battat, JBR; Billard, J; Bozorgnia, N; Burgos, S; Caldwell, T; Carmona, JM; Cebrian, S; Colas, P; Dafni, T; Daw, E; Dujmic, D; Dushkin, A; Fedus, W; Ferrer, E; Finkbeiner, D; Fisher, PH; Forbes, J; Fusayasu, T; Galan, J; Gamble, T; Ghag, C; Giomataris, I; Gold, M; Gomez, H; Gomez, ME; Gondolo, P; Green, A; Grignon, C; Guillaudin, O; Hagemann, C; Hattori, K; Henderson, S; Higashi, N; Ida, C; Iguaz, FJ; Inglis, A; Irastorza, IG; Iwaki, S; Kaboth, A; Kabuki, S; Kadyk, J; Kallivayalil, N; Kubo, H; Kurosawa, S; Kudryavtsev, VA; Lamy, T; Lanza, R; Lawson, TB; Lee, A; Lee, ER; Lin, T; Loomba, D; Lopez, J; Luzon, G; Manobu, T; Martoff, J; Mayet, F; McCluskey, B; Miller, E; Miuchi, K; Monroe, J; Morgan, B; Muna, D; Murphy, AS; Naka, T; Nakamura, K; Nakamura, M; Nakano, T; Nicklin, GG; Nishimura, H; Niwa, K; Paling, SM; Parker, J; Petkov, A; Pipe, M; Pushkin, K; Robinson, M; Rodriguez, A; Rodriguez-Quintero, J; Sahin, T; Sanderson, R; Sanghi, N; Santos, D; Sato, O; Sawano, T; Sciolla, G; Sekiya, H; Slatyer, TR; Snowden-Ifft, DP; Spooner, NJC; Sugiyama, A; Takada, A; Takahashi, M; Takeda, A; Tanimori, T; Taniue, K; Tomas, A; Tomita, H; Tsuchiya, K; Turk, J; Tziaferi, E; Ueno, K; Vahsen, S; Vanderspek, R; Vergados, J; Villar, JA; Wellenstein, H; Wolfe, I; Yamamoto, RK; Yegoryan, H

    INTERNATIONAL JOURNAL OF MODERN PHYSICS A   Vol. 25 ( 1 ) page: 1 - 51   2010.1

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    Publisher:International Journal of Modern Physics A  

    We present the case for a dark matter detector with directional sensitivity. This document was developed at the 2009 CYGNUS workshop on directional dark matter detection, and contains contributions from theorists and experimental groups in the field. We describe the need for a dark matter detector with directional sensitivity; each directional dark matter experiment presents their project's status; and we close with a feasibility study for scaling up to a one ton directional detector, which would cost around $150M. © World Scientific Publishing Company.

    DOI: 10.1142/S0217751X10048172

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  599. Balloon-borne sub-MeV/MeV gamma-ray observation using a Compton camera with a gaseous TPC and scintillation camera

    Kurosawa, S; Kubo, H; Hattori, K; Ida, C; Iwaki, S; Higashi, N; Kabuki, S; Kishimoto, Y; Miuchi, K; Nakamura, K; Nishimura, H; Parker, JD; Sawano, T; Takada, A; Takahashi, M; Tanimori, T; Taniue, K; Ueno, K

    SPACE TELESCOPES AND INSTRUMENTATION 2010: ULTRAVIOLET TO GAMMA RAY   Vol. 7732   2010

  600. Imaging Study of a Phantom and Small Animal with a Two-Head Electron-Tracking Compton Gamma-Ray Camera

    Kabuki, S; Kimura, H; Amano, H; Nakamoto, Y; Kubo, H; Miuchi, K; Kurosawa, S; Takahashi, M; Kawashima, H; Ueda, M; Okada, T; Ogawa, K; Togashi, K; Saji, H; Tanimori, T

    2010 IEEE NUCLEAR SCIENCE SYMPOSIUM CONFERENCE RECORD (NSS/MIC)     page: 2844 - 2847   2010

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  601. Performance of a Neutron Imaging Detector Based on the μPIC Micro-Pixel Gaseous Chamber

    Parker, JD; Harada, M; Hattori, K; Iwaki, S; Kabuki, S; Kishimoto, Y; Kubo, H; Kurosawa, S; Miuchi, K; Nishimura, H; Oku, T; Sawano, T; Shinohara, T; Suzuki, J; Tanimori, T; Ueno, K

    2010 IEEE NUCLEAR SCIENCE SYMPOSIUM CONFERENCE RECORD (NSS/MIC)     page: 291 - 297   2010

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  602. A novel position-sensitive radiation detector using a gaseous photomultiplier and a UV scintillator

    Kurosawa S., Kubo H., Tanimori T., Taniue K., Sekiya H., Yoshikawa A., Yanagida T., Yokota Y., Fukuda K., Ishizu S., Kawaguchi N., Suyama T.

    Proceedings of Science     2009.12

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    Publisher:Proceedings of Science  

    We developed a novel position-sensitive radiation detector that consists of an ultraviolet (UV) imaging gas photomultiplier and a UV scintillator. The former consists of a micro pixel gaseous chamber (μ-PIC), two gas electron multipliers (GEMs), and a semitransparent CsI photocathode of diameter 34 mm deposited on a MgF<inf>2</inf> window. It was coupled to a LaF<inf>3</inf>(Nd) scintillator that emits UV light. We successfully conducted photon counting and imaging using this detector along with an alpha particle source.

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  603. Performance of 8 x 8 Pixel LaBr<sub>3</sub>:Ce and Gd<sub>2</sub>SiO<sub>5</sub>:Ce Scintillator Arrays Coupled to a 64-Channel Multi-Anode PMT

    Kurosawa, S; Kubo, H; Hattori, K; Ida, C; Iwaki, S; Kabuki, S; Miuchi, K; Nishimura, H; Okada, Y; Parker, JD; Takada, A; Takahashi, M; Tanimori, T; Ueno, K; Yanagida, Y

    IEEE TRANSACTIONS ON NUCLEAR SCIENCE   Vol. 56 ( 6 ) page: 3779 - 3788   2009.12

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    Publisher:IEEE Transactions on Nuclear Science  

    We have developed a LaBr<inf>3</inf> :Ce scintillator array consisting of 8 × 8 pixels with a size of 5.8 mm × 5.8 mm × 15.0 mm, which serves as an absorber of scattered gamma rays with energies from 0.1 to 1 MeV in a Compton camera. The pixels were cut from two pieces of LaBr<inf>3</inf> :Ce crystal with a diameter of 38 mm and a length of 38 mm with full width at half-maximum (FWHM) energy resolutions of 4.1 ± 0.1 % and 3.0 ± 0.1 % at 356 and 662 keV, respectively, measured with a single anode photomultiplier tube (PMT). The crystal had the following volumetric uniformities: light outputs with a difference of 0.5% (standard deviation: SD) and energy resolutions with that of 2% (SD) at 356 keV. In contrast, for each pixel in the array, the average and SD FWHM energy resolutions over 64 pixels, measured with a single-anode PMT and a collimator, were 5.8 ± 0.9% at 356 keV. The array was then coupled to a 64-channel multi-anode PMT (Hamamatsu H8500), the anode pitch of which was the same as the LaBr :Ce pixel pitch of 6.1 mm. When the 64 anodes were read out from four channels in a resistor chain by the charge division method, the FWHM energy resolution of all 64 pixels was 7.0 ± 0.5 % at 662 keV, whereas that of the inner6 × 6 pixels was 5.8±0.4% at 662 keV. In addition, we measured a Gd<inf>2</inf>SiO <inf>5</inf> :Ce (GSO:Ce) scintillator array consisting of 8×8 pixels with a size of 5.9 mm × 5.9 mm × 13.0 mm to compare its performance with that of the LaBr<inf>3</inf> :Ce array. The FWHM energy resolution of all 64 GSO:Ce pixels was 10.8 ± 0.3% at 662 keV. With these energy resolutions, FWHM angular resolutions of the Compton camera using the LaBr<inf>3</inf> :Ce and GSO:Ce arrays are expected to be 4.6° and 5.3°, respectively, at 662 keV. © 2009 IEEE.

    DOI: 10.1109/TNS.2009.2034657

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  604. Developments of a large area VUV sensitive gas PMT with GEM/μPIC Open Access

    Sekiya, H; Ida, C; Kubo, H; Kurosawa, S; Tanimori, T; Yoshikawa, A; Yanagida, T; Yokota, Y; Fukuda, K; Ishizu, S; Kawaguchi, N; Suyama, T

    JOURNAL OF INSTRUMENTATION   Vol. 4 ( 11 )   2009.11

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    A new large area UV photon detector with micro pattern gaseous detectors is developed and evaluated. A semitransparent CsI photocathode deposited on a MgF<inf>2</inf> window was combined with 10cm × 10cm GEM and μPIC. Using Ar+C<inf>2</inf>H<inf>6</inf> (10%) gas, we achieved the gas gain of more than 10<sup>5</sup> which is enough to detect single photoelectron. We, then, irradiated vacuum UV photons (VUV, around 172nm) from the newly developed LaF<inf>3</inf>(Nd) scintillator to the detector and the single photoelectrons were successfully detected. We also demonstrated the imaging capability of the detector with μPIC readout systems. © 2009 IOP Publishing Ltd and SISSA.

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  605. Cesarean section and primary pulmonary hypertension: the role of intravenous dexmedetomidine

    Toyama, H; Wagatsuma, T; Ejima, Y; Matsubara, M; Kurosawa, S

    INTERNATIONAL JOURNAL OF OBSTETRIC ANESTHESIA   Vol. 18 ( 3 ) page: 262 - 267   2009.7

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    Primary pulmonary hypertension is a fatal disease that frequently becomes evident in pregnancy. The management of pregnant women with primary pulmonary hypertension poses a number of difficult problems, especially where regional anesthesia is considered to be contraindicated. A 30-year-old woman who developed primary pulmonary hypertension at 23 weeks of pregnancy was transferred to our hospital. Systolic pulmonary artery pressure and plasma brain natriuretic peptide levels were markedly elevated. Nitric oxide inhalation and prostacyclin prevented the progression of cardiac failure and reduced both plasma brain natriuretic peptide and pulmonary artery pressure. Cesarean section was performed at 32 weeks under general anesthesia. A combination of nitric oxide, prostacyclin, nitroglycerin, and dobutamine were administered during surgery. Intravenous dexmedetomidine was specifically used during emergence and recovery from anesthesia. This provided effective pain relief and hemodynamic stability. Throughout the clinical course, brain natriuretic peptide levels was monitored and used as an indicator of cardiac failure. © 2008 Elsevier Ltd. All rights reserved.

    DOI: 10.1016/j.ijoa.2008.08.001

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  606. A Dynamic Anomaly Detection Scheme for AODV-Based Mobile Ad Hoc Networks

    Nakayama, H; Kurosawa, S; Jamalipour, A; Nemoto, Y; Kato, N

    IEEE TRANSACTIONS ON VEHICULAR TECHNOLOGY   Vol. 58 ( 5 ) page: 2471 - 2481   2009.6

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    Mobile ad hoc networks (MANETs) are usually formed without any major infrastructure. As a result, they are relatively vulnerable to malicious network attacks, and therefore, security is a more significant issue than infrastructure-based wireless networks. In MANETs, it is difficult to identify malicious hosts as the topology of the network dynamically changes. A malicious host can easily interrupt a route for which it is one of the forming nodes in the communication path. In the literature, there are several proposals to detect such malicious hosts inside the network. In those methods, a baseline profile, which is defined as per static training data, is usually used to verify the identity and the topology of the network, thus preventing any malicious host from joining the network. Since the topology of a MANET dynamically changes, the mere use of a static baseline profile is not efficient. In this paper, we propose a new anomaly-detection scheme based on a dynamic learning process that allows the training data to be updated at particular time intervals. Our dynamic learning process involves calculating the projection distances based on multidimensional statistics using weighted coefficients and a forgetting curve. We use the network simulator 2 (ns-2) system to conduct the MANET simulations and consider scenarios for detecting five types of attacks. The simulation results involving two different networks in size show the effectiveness of the proposed techniques. © 2009 IEEE.

    DOI: 10.1109/TVT.2008.2010049

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  607. Tracking performance of the NEWAGE-0.3a direction-sensitive dark matter detector

    Nishimura, H; Miuchi, K; Hattori, K; Iwaki, S; Ida, C; Kabuki, S; Kubo, H; Kurosawa, S; Sekiya, H; Takada, A; Takahashi, M; Takeda, A; Tanimori, T; Tsuchiya, K; Ueno, K

    ASTROPARTICLE PHYSICS   Vol. 31 ( 3 ) page: 185 - 191   2009.4

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    NEWAGE-0.3a is a prototype direction-sensitive dark matter search detector. We measured its response to electron tracks and nuclear tracks while focusing on the tracking performances in an underground laboratory. It showed a gamma-ray rejection power of 8.1 ± 1.9 × 10<sup>-6</sup> at 100 keV α.e.(alpha-equivalent) and an energy resolutions of 45% at 6 MeV α.e. The absolute nuclear efficiency was 80% at 100 keV α.e. and the nuclear directional-dependent efficiency was also measured. The three-dimensional angular resolution for the nuclear track was 46 ± 3° in the energy range from 100 keV α.e. to 400 keV α.e. © 2009 Elsevier B.V. All rights reserved.

    DOI: 10.1016/j.astropartphys.2008.12.011

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  608. A Direction-Sensitive Dark Matter Search Experiment (NEWAGE)

    Nishimura, H; Ida, KHC; Iwaki, S; Kabuki, S; Kubo, H; Kurosawa, S; Miuchi, K; Takada, A; Tanimori, T; Ueno, K

    JOURNAL OF THE PHYSICAL SOCIETY OF JAPAN   Vol. 78   page: 218 - 220   2009.1

  609. The Observation of Diffuse Cosmic and Atmospheric Gamma Rays with an Electron-Tracking Compton Camera Loaded on a Balloon Open Access

    Takada, A; Kubo, H; Nishimura, H; Ueno, K; Tanimori, T; Miuchi, K; Tsuchiya, K; Kabuki, S; Hattori, K; Kurosawa, S; Ida, C; Iwaki, S; Nonaka, N; Mizuta, E

    JOURNAL OF THE PHYSICAL SOCIETY OF JAPAN   Vol. 78   page: 161 - 164   2009.1

  610. Functionally important structural elements of the cyanobacterial clock-related protein Pex

    Kurosawa, S; Murakami, R; Onai, K; Morishita, M; Hasegawa, D; Iwase, R; Uzumaki, T; Hayashi, F; Kitajima-Ihara, T; Sakata, S; Murakami, M; Kouyama, T; Ishiura, M

    GENES TO CELLS   Vol. 14 ( 1 ) page: 1 - 16   2009.1

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    Pex, a clock-related protein involved in the input pathway of the cyanobacterial circadian clock system, suppresses the expression of clock gene kaiA and lengthens the circadian period. Here, we determined the crystal structure of Anabaena Pex (Ana Pex; Anabaena sp. strain PCC 7120) and Synechococcus Pex (Syn Pex; S ynechococcus sp. strain PCC 7942). Pex is a homodimer that forms a winged-helix structure. Using the DNase I protection and electrophoresis mobility shift assays on a Synechococcus kaiA upstream region, we identified a minimal 25-bp sequence that contained an imperfectly inverted repeat sequence as the Pex-binding sequence. Based on crystal structure, we predicted the amino acid residues essential for Pex's DNA-binding activity and examined the effects of various Ala-substitutions in the α3 helix and wing region of Pex on in vitro DNA-binding activity and in vivo rhythm functions. Mutant Ana Pex proteins carrying a substitution in the wing region displayed no specific DNA-binding activity, whereas those carrying a substitution in the α3 helix did display specific binding activity. But the latter were less thermostable than wild-type Ana Pex and their in vitro functions were defective. We concluded that Pex binds a kaiA upstream DNA sequence via its wing region and that its α3 helix is probably important to its stability. © Journal compilation © 2009 by the Molecular Biology Society of Japan/Blackwell Publishing Ltd.

    DOI: 10.1111/j.1365-2443.2008.01245.x

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  611. Compton Imaging Camera Using an Electron-Tracking Gaseous TPC and a Scintillation Camera

    Ueno, K; Hattori, K; Ida, C; Iwaki, S; Kabuki, S; Kubo, H; Kurosawa, S; Miuchi, K; Nishimura, H; Okada, Y; Takada, A; Takahashi, M; Tanimori, T; Tsuchiya, K

    2008 IEEE NUCLEAR SCIENCE SYMPOSIUM AND MEDICAL IMAGING CONFERENCE (2008 NSS/MIC), VOLS 1-9     page: 2745 - +   2009

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  612. Development of a Neutron Imaging Detector Based on the μPIC Micro-Pixel Gaseous Chamber

    Parker, JD; Hattori, K; Ida, C; Iwaki, S; Kabuki, S; Kubo, H; Kurosawa, S; Miuchi, K; Nishimura, H; Takahashi, M; Tanimori, T; Ueno, K

    2009 IEEE NUCLEAR SCIENCE SYMPOSIUM CONFERENCE RECORD, VOLS 1-5     page: 1107 - 1112   2009

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    A new detector employing the micro-pixel gaseous chamber (μPIC) is currently being developed as a thermal neutron imaging detector for applications in small angle neutron scattering (SANS), neutron radiography, and radioactive material detection. Neutron detection is achieved through the <sup>3</sup>He(n, p)<sup>3</sup>H absorption reaction by adding <sup>3</sup>He to the usual Argon-Ethane gas mixture. The μPIC, with a pixel pitch of 400 microns, is coupled with an FPGA-based data acquisition system with a 100 MHz internal clock. This combined system has excellent spatial (< 1mm) and time (10 ns) resolutions and is capable of handling counting rates greater than 5 MHz. These qualities make it well suited to SANS measurements at pulsed neutron sources. Here, we report the performance of a new dedicated μPIC-based neutron imaging detector system along with the results of a test experiment at a small Tandem accelerator-based neutron source currently under development at Kyoto University. This new detector features a 10 x 10 x 5 cm<sup>3</sup> active volume and operates at gas pressures up to 2 atm. With this design, we expect a neutron detection efficiency of ∼30% for a gas mixture containing 30% <sup>3</sup>He at a total pressure of 2 atm. Additionally, an improved FPGA encoder program allows the simultaneous measurement of the track length and energy deposition, allowing a finer position resolution and strong rejection of the gamma-ray and fast neutron backgrounds. ©2009 IEEE.

    DOI: 10.1109/NSSMIC.2009.5402419

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  613. Development of Electron Tacking Compton Camera based on Micro Pixel Gas Detector and its Application for Medical Imaging

    Tanimori, FT; Amano, H; Hattori, K; Ida, C; Iwaki, S; Kabuki, S; Kawashima, H; Kimura, H; Kohara, R; Kubo, A; Kubo, H; Kunieda, E; Kurosawa, S; Miuchi, K; Miyazaki, O; Nakazawa, T; Nakahara, T; Nakamoto, Y; Nishimura, H; Ogawa, K; Okada, T; Okada, Y; Shirahata, T; Saji, H; Takada, A; Togashi, K; Tsuchiya, K; Ueda, M; Ueno, K; Yamamoto, E

    2008 IEEE NUCLEAR SCIENCE SYMPOSIUM AND MEDICAL IMAGING CONFERENCE (2008 NSS/MIC), VOLS 1-9     page: 5530 - +   2009

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  614. DIRECTION-SENSITIVE DARK MATTER SEARCH-NEWAGE

    Miuchi, K; Nishimura, H; Hattori, K; Ida, C; Iwaki, S; Kabuki, S; Kubo, H; Kurosawa, S; Takada, A; Tanimori, T; Ueno, K

    CRAL-IPNL: DARK ENERGY AND DARK MATTER: OBSERVATIONS, EXPERIMENTS AND THEORIES   Vol. 36   page: 243 - +   2009

  615. Endothelial Progenitor Cells Are Not Mobilized in COPD Patients by Thoracic Surgery.

    Takahashi, T; Suzuki, S; Kurosawa, S; Kato, M; Kubo, H

    AMERICAN JOURNAL OF RESPIRATORY AND CRITICAL CARE MEDICINE   Vol. 179   2009

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  616. Imaging Reagents Study for Nuclear Medicine Using an Electron-Tracking Compton Gamma-Ray Camera

    Kabuki, S; Kimura, H; Amano, H; Nakamoto, Y; Kubo, H; Miuchi, K; Kurosawa, S; Takahashi, M; Kawashima, H; Ueda, M; Okada, T; Ogawa, K; Togashi, K; Saji, H; Tanimori, T

    2009 IEEE NUCLEAR SCIENCE SYMPOSIUM CONFERENCE RECORD, VOLS 1-5     page: 2813 - +   2009

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    We have developed an electron-tracking Compton camera (ETCC) for new imaging reagents study. Energy limitation of gamma camera is major problem for this study. However, our ETCC has a wide energy dynamic range (200-1300 keV). In this paper, we show the results of imaging reagent study as follows: (1) F-18-FDG (511 keV) and I-131-MIBG (364 keV) simultaneous imaging for double clinical tracer imaging, (2) Zn-65-porphyrin (1116 keV) imaging for high energy gamma-ray imaging and, (3) middle size animal imaging (rabbit). Also we studied the improvement for the camera system. ©2009 IEEE.

    DOI: 10.1109/NSSMIC.2009.5401649

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  617. Low-power Wide-dynamic-range Readout System for a 64-channel Multi-anode PMT of a Scintillation Gamma Camera

    Kubo, H; Hattori, K; Ida, C; Iwaki, S; Kabuki, S; Kubo, S; Kurosawa, S; Miuchi, K; Nishimura, H; Okada, Y; Takada, A; Takahashi, M; Tanimori, T; Tsuchiya, K; Ueno, K

    2008 IEEE NUCLEAR SCIENCE SYMPOSIUM AND MEDICAL IMAGING CONFERENCE (2008 NSS/MIC), VOLS 1-9     page: 456 - +   2009

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  618. Simultaneous imaging of multi nuclides using the Electron tracking Compton Gamma-Ray Camera based on small animal and phantom experiments

    Kabuki, S; Kubo, H; Miuchi, K; Kurosawa, S; Kimura, H; Kohara, R; Miyazaki, O; Nakazawa, T; Shirahata, T; Yamamoto, E; Kubo, A; Kunieda, E; Nakahara, T; Amano, H; Kawashima, H; Ueda, M; Okada, T; Nakamoto, Y; Ogawa, K; Togashi, K; Saji, H; Tanimori, T

    2008 IEEE NUCLEAR SCIENCE SYMPOSIUM AND MEDICAL IMAGING CONFERENCE (2008 NSS/MIC), VOLS 1-9     page: 3212 - +   2009

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  619. Study on the Use of Electron-Tracking Compton Gamma-Ray Camera to Monitor the Therapeutic Proton Dose Distribution in Real Time

    Kabuki, S; Ueno, K; Kurosawa, S; Iwaki, S; Kubo, H; Miuchi, K; Fujii, Y; Kim, D; Kim, J; Kohara, R; Miyazaki, O; Sakae, T; Shirahata, T; Takayanagi, T; Terunuma, T; Tsukahara, Y; Yamamoto, E; Yasuoka, K; Tanimori, T

    2009 IEEE NUCLEAR SCIENCE SYMPOSIUM CONFERENCE RECORD, VOLS 1-5     page: 2437 - +   2009

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    Radiation therapy with proton and heavy-ion beams has been better established lately and the patient throughput is increasing. Although the therapy beam is controlled with high accuracy, it is difficult to know the location of distal dose falloff in the body. If real-time monitoring of the location is realized, the treatment quality would be improved. We have developed an electrontracking Compton camera (ETCC) for real-time monitoring on the proton therapy. Our ETCC has a wide energy dynamic range of 200-1300 keV and a wide field of view. Therefore, ETCC has a potential as a quality assurance tool for proton therapy. We simulated and conducted an experiment with a 155 MeV proton beam and a water phantom. We succeeded in imaging a Bragg peak with prompt gamma rays. ©2009 IEEE.

    DOI: 10.1109/NSSMIC.2009.5402130

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  620. Advanced compton camera system for nuclear medicine: Prototype system study

    Kohara R., Shirahata T., Nakazawa T., Miyazaki O., Kabuki S., Kurosawa S., Miuchi K., Kubo H., Tanimori T., Nakahara T., Kunieda E., Kubo A., Fujii H.

    IEEE Nuclear Science Symposium Conference Record     page: 3906 - 3908   2008.12

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    A gamma-ray imager called Compton camera is expected as a new medical instrument for nuclear medicine. It has several advantages over the conventional techniques such as positron emission tomography and single photon emission tomography. Especially, the Compton camera can expand the range of diagnosis and therapy because various gamma-ray energies can be measured without changing system configuration. Many studies have been made on the Compton camera, however, its medical application is still challenging because in clinical environments it is very difficult to image targets due to large background activities. We will establish the imaging techniques and demonstrate the imaging capabilities of the advanced Compton camera. We constructed the prototype system with the gaseous chamber and the scintillation counter. We performed phantom experiments with a <sup>131</sup>I gamma-ray source, assuming clinical environments. We evaluated the contrast resolution and found the limitations on the concentration ratio and the magnitude of statistics for imaging hotspots in the large background activity. We performed the Compton tomography in the only three-direction scan and obtained an axial image. We also demonstrated the fusion image with X-ray CT for clinical application. ©2008 IEEE.

    DOI: 10.1109/NSSMIC.2008.4774137

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  621. Compton imaging camera using an electron-tracking gaseous tpc and a scintillation camera

    Ueno K., Hattori K., Ida C., Iwaki S., Kabuki S., Kubo H., Kurosawa S., Miuchi K., Nishimura H., Okada Y., Takada A., Takahashi M., Tanimori T., Tsuchiya K.

    IEEE Nuclear Science Symposium Conference Record     page: 3470 - 3474   2008.12

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    We are developing an Electron-Tracking Compton imaging Camera (ETCC) based on a gaseous Time Projection Chamber (TPC) and a scintillation camera. The ETCC detects the energy and the direction of the incident gamma ray using the information of the recoil electron and the scattered gamma ray. We have developed the ETCC with a detection volume of 23 × 28 × 30 cm <sup>3</sup> which consists of the 23 × 28 × 30 cm<sup>3</sup> gaseous TPC and 30 × 30 cm<sup>2</sup> GSO(Ce) scintillation camera. And we obtained the gamma-ray image and investigated the performances of the ETCC. The Angular Resolution Measure (ARM) and the Scatter Plane Deviation (SPD) are 6.1 degree and 64.5 degree (HWHM) at 662keV, respectively, and the energy resolution is 18.0%(FWHM) at 662keV. ©2008 IEEE.

    DOI: 10.1109/NSSMIC.2008.4775084

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  622. It is possible to classify non-erosive reflux disease (NERD) patients into endoscopically normal groups and minimal change groups by subjective symptoms and responsiveness to rabeprazole - A report from a study with Japanese patients

    Kusano M., Shirai N., Yamaguchi K., Hongo M., Chiba T., Kinoshita Y., Ohara S., Hoshihara Y., Kurosawa S., Watanabe Y., Furuta T., Joh T., Higuchi K., Fujiwara Y., Habu Y., Miwa H., Haruma K., Manabe N., Adachi K., Shimatani T., Ito M., Fujimoto K.

    Digestive Diseases and Sciences   Vol. 53 ( 12 ) page: 3082 - 3094   2008.12

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    The hypothesis that non-erosive reflux disease (NERD) patients comprise various subgroups is gaining popularity. This study was conducted to investigate the possibility of categorizing NERD patients according to symptom types and response to acid-suppressive drug rabeprazole (RPZ) 10 mg/day. NERD patients were classified as grade N (endoscopically normal), M (minimal change), or erosive GERD, and answered a 51-item, yes-or-no questionnaire pre and post-treatment. Compared to erosive GERD, clear differences existed in pretreatment prevalence of symptoms and responsiveness to RPZ in grades N and M; the results suggested stomachaches (especially at night) were significant symptoms in grade N and dysmotility-like symptoms like bloated stomach were significant in grade M while gastroesophageal reflux symptoms were significant in erosive GERD. Clinical significance of classifying NERD was indicated from different symptoms and responsiveness to PPI. © 2008 Springer Science+Business Media, LLC.

    DOI: 10.1007/s10620-008-0290-2

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  623. Low-power Wide-dynamic-range readout system for a 64-channel multi-anode PMT of a scintillation gamma camera

    Kubo H., Hattori K., Ida C., Iwaki S., Kabuki S., Kubo S., Kurosawa S., Miuchi K., Nishimura H., Okada Y., Takada A., Takahashi M., Tanimori T., Tsuchiya K., Ueno K.

    IEEE Nuclear Science Symposium Conference Record     page: 1181 - 1185   2008.12

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    We have developed a low-power wide-dynamicrange readout system for a 64-channel multi-anode photomultiplier (PMT) of a scintillation gamma camera. Each anode is individually read with the system that contains discrete devices of amplifiers, comparators, sample-hold ADCs, and FPGAs. The size of the system which is designed for a twodimensional array of Hamamatsu flat panel PMT 88500 is 5×5×14 cm<sup>3</sup>. The input dynamic range is variable by replacing the feedback capacitor of the preamplifier (e.g., 700 pC and 4000 pC for GSO(Ce) and LaBr3(Ce) crystals, respectively). The serialized ADC data are sent to a VME sequence module. The total power consumption is 1.6 W per 64 channels. With this system we have developed a gamma camera using an 8×8 array of GSO(Ce) pixels with a pixel size of 6×6×13 mm<sup>3</sup> coupled to an H8500, and btained flood-field irradiation images at energies from 30 keV to 1.3 MeV. The energy resolution was 10.8±0.4% (FWHM) at 662 keV. In addition, we used the readout system for an 8×8 array of LaBr <inf>3</inf>(Ce) pixels with a pixel size of 6×6×15 mm<sup>3</sup> and obtained a flood-field irradiation image at 662 keV. © 2008 IEEE.

    DOI: 10.1109/NSSMIC.2008.4774613

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  624. Simultaneous imaging of multi nuclides using the electron tracking compton gamma-ray.camera based on small animal and phantom experiments

    Kabuki S., Kubo H., Miuchi K., Kurosawa S., Kimura H., Kohara R., Miyazaki O., Nakazawa T., Shirahata T., Yamamoto E., Kubo A., Kunieda E., Nakahara T., Amano H., Kawashima H., Ueda M., Okada T., Nakamoto Y., Ogawa K., Togashi K., Saji H., Tanimori T., Hattori K., Nagayoshi T., Nishimura H., Sekiya H., Takada A., Ueno K.

    IEEE Nuclear Science Symposium Conference Record     page: 3937 - 3941   2008.12

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    Compton Camera has a potential for nuclear medicine. Because energy dynamic range and field of view is wide. Electron Tracking Compton Camera (ETCC) which we have developed consists of two letectors micro Time Projection Chamber (llTPC) and Pixel Scintillator Array (PSA). We have developed two type of ETCC small and large, and we have evaluated these cameras and .have imaged phantom and small animal. ©2008 IEEE.

    DOI: 10.1109/NSSMIC.2008.4774145

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  625. Sepsis is characterized by the increases in percentages of circulating CD4<SUP>+</SUP>CD25<SUP>+</SUP> regulatory T cells and plasma levels of soluble CD25 Open Access

    Saito, K; Wagatsuma, T; Toyama, H; Ejima, Y; Hoshi, K; Shibusawa, M; Kato, M; Kurosawa, S

    TOHOKU JOURNAL OF EXPERIMENTAL MEDICINE   Vol. 216 ( 1 ) page: 61 - 68   2008.9

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    The function of immune system is to protect hosts from invading microorganisms by destroying infected cells while minimizing damage to tissues. Among immune cells, CD4<sup>+</sup>CD25<sup>+</sup> regulatory T cells (Treg cells) control immune responses by limiting infectious processes. However, it remains unclear whether Treg cells are induced in systemic inflammatory response syndrome (SIRS) or infectious SIRS (i.e. sepsis). SIRS and sepsis arc associated with stressful inflammatory conditions. We therefore measured CD25<sup>+</sup> T cells and circulating CD4<sup>+</sup> T cells, along with plasma levels of CD25, interleukin (IL)-6, and IL-10, in 20 septic patients (64 ± 11 years), 16 SIRS patients (59 ± 16 years), and control subjects: 13 elderly (60 ± 16 years) and 14 young volunteers (28 ± 3 years). Septic patients (23.3 ± 11.8%, p < 0.01) showed significantly higher percentages of CD25<sup>+</sup> cells among CD44<sup>T</sup> cells (i.e. Treg cells) than did either young (10.6 ± 3.7%) or elderly volunteers (11.1 ± 3.8%). The percentages of Treg cells in septic patients were higher than those in SIRS patients (12.4 ± 6.9%, p < 0.01). Moreover, plasma levels of soluble CD25 were significantly higher in septic patients, compared to the levels in SIRS patients or volunteers (p < 0.01). No significant difference in plasma levels of IL-6 or IL-10 was found between septic patients and SIRS patients. Thus, sepsis is associated with the increased percentages of Treg cells and elevated plasma level of soluble CD25. The elevation of these parameters might be a useful marker of infections in SIRS. © 2008 Tohoku University Medical Press.

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  626. Anesthetics, immune cells, and immune responses Open Access

    Kurosawa, S; Kato, M

    JOURNAL OF ANESTHESIA   Vol. 22 ( 3 ) page: 263 - 277   2008.8

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    General anesthesia accompanied by surgical stress is considered to suppress immunity, presumably by directly affecting the immune system or activating the hypothalamic-pituitary-adrenal axis and the sympathetic nervous system. Along with stress such as surgery, blood transfusion, hypothermia, hyperglycemia, and postoperative pain, anesthetics per se are associated with suppressed immunity during perioperative periods because every anesthetic has direct suppressive effects on cellular and neurohumoral immunity through influencing the functions of immunocompetent cells and inflammatory mediator gene expression and secretion. Particularly in cancer patients, immunosuppression attributable to anesthetics, such as the dysfunction of natural killer cells and lymphocytes, may accelerate the growth and metastases of residual malignant cells, thereby worsening prognoses. Alternatively, the anti-inflammatory effects of anesthetics may be beneficial in distinct situations involving ischemia and reperfusion injury or the systemic inflammatory response syndrome (SIRS). Clinical anesthesiologists should select anesthetics and choose anesthetic methods with careful consideration of the clinical situation and the immune status of critically ill patients, in regard to long-term mortality, morbidity, and the optimal prognosis. © Japanese Society of Anesthesiologists 2008.

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  627. Performance of the gamma-ray camera based on GSO(Ce) scintillator array and PSPMT with the ASIC readout system

    Ueno, K; Hattori, K; Ida, C; Iwaki, S; Kabuki, S; Kubo, H; Kurosawa, S; Miuchi, K; Nagayoshi, T; Nishimura, H; Orito, R; Takada, A; Tanimori, T

    NUCLEAR INSTRUMENTS & METHODS IN PHYSICS RESEARCH SECTION A-ACCELERATORS SPECTROMETERS DETECTORS AND ASSOCIATED EQUIPMENT   Vol. 591 ( 1 ) page: 268 - 271   2008.6

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    We have studied the performance of a readout system with ASIC chips for a gamma-ray camera based on a 64-channel multi-anode PSPMT (Hamamatsu flat-panel H8500) coupled to a GSO(Ce) scintillator array. The GSO array consists of 8×8 pixels of 6×6×13 mm<sup>3</sup> with the same pixel pitch as the anode of the H8500. This camera is intended to serve as an absorber of an electron tracking Compton gamma-ray camera that measures gamma rays up to ∼1 MeV. Because we need a readout system with low power consumption for a balloon-borne experiment, we adopted a 32-channel ASIC chip, IDEAS VA32_HDR11, which has one of the widest dynamic range among commercial chips. However, in the case of using a GSO(Ce) crystal and the H8500, the dynamic range of VA32_HDR11 is narrow, and therefore the H8500 has to be operated with a low gain of about 10<sup>5</sup>. If the H8500 is operated with a low gain, the camera has a narrow incident-energy dynamic range from 100 to 700 keV, and a bad energy resolution of 13.0% (FWHM) at 662 keV. We have therefore developed an attenuator board in order to operate the H8500 with the typical gain of 10<sup>6</sup>, which can measure up to ∼1 MeV gamma ray. The board makes the variation of the anode gain uniform and widens the dynamic range of the H8500. The system using the new attenuator board has a good uniformity of min:max∼1:1.6, an incident-energy dynamic range from 30 to 900 keV, a position resolution of less than 6 mm, and a typical energy resolution of 10.6% (FWHM) at 662 keV with a low power consumption of about 1.7 W/64ch. Crown Copyright © 2008.

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  628. Characteristics of young-onset white coat hypertension identified by targeted screening for hypertension at a university health check-up Open Access

    Toyama, H; Hasegawa, Y; Ejima, Y; Kurosawa, S; Sanada, S; Hatano, R; Hida, W; Matsubara, M

    HYPERTENSION RESEARCH   Vol. 31 ( 6 ) page: 1063 - 1068   2008.6

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    Previously we estimated the prevalence of essential hypertension (EH) as around 0.1% and suggested that male gender, obesity, and strong genetic background (hypertension in parents) were risk factors for EH in a young population aged less than 30 based on targeted screening for hypertension at a university health check-up. This study also revealed a high incidence of white coat hypertension (WCH) in university students, and thus, we continued this screening for four consecutive years, and examined the prognosis and clinical characteristics of young-onset WCH. Three occasions of casual blood pressure (BP) measurement and additional home BP measurement revealed 72 WCH and 15 EH students (all males) during the 4-year study period. None of the WCH students had elevated home BP to the level of hypertension during their stay at university, and 26 out of 38 WCH students participating screening in the following years showed normal casual BP. Although WCH students showed a significantly higher pulse rate than controls, WCH could not be fully differentiated from EH either by pulse rate or by correlation between casual BP value and pulse rate. These findings indicate the requirement of longer follow-up after graduation to determine the prognosis of young-onset WCH, though EH and WCH In the young population share the same risk factors and, possibly, autonomic nervous system dysfunction. Since diagnosis of WCH has limited importance for university students, screening of EH following a general health check-up would elevate the clinical validity of casual BP measurement at the university.

    DOI: 10.1291/hypres.31.1063

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  629. Electrochemical determination of L-lactate using phenylboronic acid monolayer-modified electrodes

    Takahashi, S; Kurosawa, S; Anzai, JI

    ELECTROANALYSIS   Vol. 20 ( 7 ) page: 816 - 818   2008.4

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    The surface of a gold (Au) disk electrode was modified with a self-assembled monomolecular layer of dithiobis(4-butylamino-m-phenylboronic acid) (DTBA-PBA) to prepare L-lactate-sensitive electrodes. The DTBA-PBA-modified electrodes exhibited an attenuated cyclic voltammogram (CV) for the Fe(CN)<inf>6</inf><sup>3-</sup> ion in the presence of L-lactate, as a result of the formation of phenylboronate ester of L-lactate accompanied with the addition of OH<sup>-</sup> ion to the boron atom. In other words, the negatively charged DTBA-PBA monolayer blocked the electrode surface from the access of the Fe(CN)<inf>6</inf><sup>3-/4-</sup> ions. Thus, the DTBA-PBA monolayer-modified Au electrode can be used for determining l-lactate on the basis of the change in redox current of Fe(CN)<inf>6</inf><sup>3-/4-</sup> ions. The calibration graph useful for determining 1 - 30 mM L-lactate was obtained. © 2008 Wiley-VCH Verlag GmbH & Co. KGaA.

    DOI: 10.1002/elan.200704097

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  630. NEWAGE Open Access

    Nishimura H., Hattori K., Ida C., Iwaki S., Kabuki S., Kubo H., Kurosawa S., Miuchi K., Sekiya H., Takada A., Takeda A., Tanimori T., Ueno K.

    Journal of Physics Conference Series   Vol. 120 ( Part 4 )   2008.1

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    We developed a three-dimensional gaseous tracking device, and performed a direction-sensitive dark matter search in a surface laboratory. By using 150 Torr carbon-tetrafluoride (CF<inf>4gas</inf>), we obtained a sky map drawn with the recoil directions of the carbon and fluorine nuclei, and set the first limit on the spin-dependent WIMP (Weakly Interacting Massive Particles)proton cross section by a direction-sensitive method.

    DOI: 10.1088/1742-6596/120/4/042025

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  631. Development of an electron-tracking Compton camera based on a gaseous TPC and a scintillation camera for a balloon-borne experiment

    Ueno, K; Tanimori, T; Kubo, H; Miuchi, K; Kabuki, S; Takada, A; Nishimura, H; Hattori, K; Kurosawa, S; Ida, C; Iwaki, S

    SPACE TELESCOPES AND INSTRUMENTATION 2008: ULTRAVIOLET TO GAMMA RAY, PTS 1 AND 2   Vol. 7011   2008

  632. Detecting blackhole attack on AODV-based mobile Ad Hoc networks by dynamic learning method

    Kurosawa S., Nakayama H., Kato N., Jamalipour A., Nemoto Y.

    International Journal of Network Security   Vol. 5 ( 3 ) page: 338 - 346   2007.12

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    This paper analyzes the blackhole attack which is one of the possible attacks in ad hoc networks. In a blackhole attack, a malicious node impersonates a destination node by sending a spoofed route reply packet to a source node that initiates a route discovery. By doing this, the malicious node can deprive the traffic from the source node. In order to prevent this kind of attack, it is crucial to detect the abnormality occurs during the attack. In conventional schemes, anomaly detection is achieved by defining the normal state from static training data. However, in mobile ad hoc networks where the network topology dynamically changes, such static training method could not be used efficiently. In this paper, we propose an anomaly detection scheme using dynamic training method in which the training data is updated at regular time intervals. The simulation results show the effectiveness of our scheme compared with conventional scheme.

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  633. Performance of the gamma-ray camera based on scintillator array and PSPMT with an ASIC readout system

    Ueno K., Hattori K., Ida C., Iwaki S., Kabuki S., Kubo H., Kurosawa S., Miuchi K., Nishimura H., Takada A., Tanimori T., Sekiya H.

    Proceedings of Science     2007.12

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    We have studied the performance of a readout system with ASIC chips for our gamma camera based on 64 channels multi-anode PSPMT(Hamamatsu flat-panel H8500) coupled to a GSO(Ce) scintillator array. The GSO array consists of 8×8 pixels of 6×6×13mm<sup>3</sup> with the same pixel pitch as the anode of H8500. This camera is intended for an absorber of an Electron Tracking Compton gamma-ray camera which measures up to about 1 MeV gamma-ray. We need a readout system with low power consumption in order to make a camera which has 64×108 readout channels for a balloon-borne experiment. We adopted the ASIC chip, IDEAS VA32-HDR11, with low power consumption of 1.3 W/64 ch and dynamic range of ∼-35 pC, which is one of chips with widest range among commercial ones. However, we have to operate the H8500 with the low gain of about 10<sup>5</sup> because it only measures up to about 100 keV gamma-ray with the typical gain of about 10<sup>6</sup>, and we developed an attenuator board in order to operate the H8500 with the typical gain. The attenuator board has 64 singular resistors adjusted to the anode gain and uniforms variation of the anode gain of the H8500, min:max∼1:2.3, before inputs to ASIC chips. Using the board, The H8500 was able to operate with the gain of about 10<sup>6</sup> and the output signals from that board had a good uniformity of min:max∼1:1.2. The system with the new attenuator board has the incident energy dynamic range of 30 to 900keV, the position resolution of less than 6mm, and a typical energy resolution of about 11.7%(FWHM) at 662keV. © Copyright owned by the author(s).

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  634. [Pharmacodynamics and pharmacokinetics of remifentanil: overview and comparison with other opioids].

    Kato M, Satoh D, Okada Y, Sugiyama K, Toda N, Kurosawa S

    Masui. The Japanese journal of anesthesiology   Vol. 56 ( 11 ) page: 1281 - 6   2007.11

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  635. Pharmacodynamics and pharmacokinetics of remifentanil: Overview and comparison with other opioids

    Kato M., Satoh D., Okada Y., Sugiyama K., Toda N., Kurosawa S.

    Japanese Journal of Anesthesiology   Vol. 56 ( 11 ) page: 1281 - 1286   2007.11

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    In this review, the authors tried to summarize the characteristics and main differences of remifentanil with other opioids, and to overview its pharmacodynamics and pharmacokinetics. Clearance and volume of distribution of remifentnail are extremely different from other conventional opioids. In addition, the context-sensitive half time of remifentanil is almost stable (about 3 minutes) even if the continuous infusion of remifentanil lasts for longer than 10 hours. As remifentanil is metabolized by a non-specific esterase, excretion of remifentnil is predictable in basically all patients undergoing general anesthesia and surgery. Therefore, remifentanil is considered to be an optimal opioid as an analgesic combined either with inhalational anesthetics or intravenous hypnotics in balanced general anesthesia.

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  636. Gamma-ray imaging with a large micro-TPC and a scintillation camera

    Hattori, K; Kabuki, S; Kubo, H; Kurosawa, S; Miuchi, K; Nagayoshi, T; Nishimura, H; Okada, Y; Orito, R; Sekiya, H; Takada, A; Takeda, A; Tanimori, T; Ueno, K

    NUCLEAR INSTRUMENTS & METHODS IN PHYSICS RESEARCH SECTION A-ACCELERATORS SPECTROMETERS DETECTORS AND ASSOCIATED EQUIPMENT   Vol. 581 ( 1-2 ) page: 517 - 521   2007.10

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    Publisher:Nuclear Instruments and Methods in Physics Research Section A Accelerators Spectrometers Detectors and Associated Equipment  

    We report on the development of a large Compton camera with the full reconstruction of the Compton process based on a prototype. This camera consists of two kinds of detectors. One is a gaseous time projection chamber (micro-TPC) for measuring the energy and the track of a Compton recoil electron. The micro-TPC is based on a μ-PIC and a GEM, which are micro-pattern gas detectors (MPGDs). The size of the micro-TPC was 10 cm × 10 cm × 8 cm in the case of the prototype, and we enlarged it to 23 cm × 28 cm × 15 cm. The other detector part is a NaI (Tl) Anger camera for measuring the scattered gamma-ray. With these informations, we can completely reconstruct a Compton event, and determine the direction of the incident gamma-ray, event by event. We succeeded in reconstructing events of incident 662 keV gamma-rays. The measured angular resolutions of the "angular resolution measure" (ARM) and the "scatter plane deviation" (SPD) were 9 . 3<sup>{ring operator}</sup> and 158<sup>{ring operator}</sup> (FWHM), respectively. © 2007 Elsevier B.V. All rights reserved.

    DOI: 10.1016/j.nima.2007.08.039

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  637. Direction-sensitive dark matter search results in a surface laboratory Open Access

    Miuchi, K; Hattori, K; Kabuki, S; Kubo, H; Kurosawa, S; Nishimura, H; Okada, Y; Takada, A; Tanimori, T; Tsuchiya, K; Ueno, K; Sekiya, H; Takeda, A

    PHYSICS LETTERS B   Vol. 654 ( 3-4 ) page: 58 - 64   2007.10

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    Publisher:Physics Letters Section B Nuclear Elementary Particle and High Energy Physics  

    We developed a three-dimensional gaseous tracking device and performed a direction-sensitive dark matter search in a surface laboratory. By using 150 Torr carbon-tetrafluoride (CF<inf>4</inf>) gas, we obtained a sky map drawn with the recoil directions of the carbon and fluorine nuclei, and set the first limit on the spin-dependent WIMP (Weakly Interacting Massive Particles)-proton cross section by a direction-sensitive method. Thus, we showed that a WIMP-search experiment with a gaseous tracking device can actually set limits. Furthermore, we demonstrated that this method will potentially play a certain role in revealing the nature of dark matter when a low-background large-volume detector is developed. © 2007 Elsevier B.V. All rights reserved.

    DOI: 10.1016/j.physletb.2007.08.042

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  638. Efficacy of rabeprazole on heartburn symptom resolution in patients with non-erosive and erosive gastro-oesophageal reflux disease: A multicenter study from Japan

    Miwa H., Sasaki M., Furuta T., Koike T., Habu Y., Ito M., Fujiwara Y., Wada T., Nagahara A., Hongo M., Chiba T., Kinoshita Y., Ohara S., Kusano M., Hoshihara Y., Kurosawa S., Watanabe Y., Joh T., Higuchi K., Haruma K., Manabe N., Adachi K., Shimatani T., Fujimoto K.

    Alimentary Pharmacology and Therapeutics   Vol. 26 ( 1 ) page: 69 - 77   2007.7

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    Background: Few studies have compared the efficacy of proton pump inhibitors in resolving the symptoms of non-erosive reflux disease (NERD) and of erosive gastro-oesophageal reflux disease (GERD) in Japan. Aim: To investigate and compare the efficacy of 4-week course of rabeprazole 10 mg/day on symptom resolution in NERD and erosive GERD in Japan. Methods: The modified Los Angeles classification was used to grade endoscopically GERD in patients with heartburn (Grades N and M: NERD, Grades A and B: mild reflux oesophagitis (RO), and Grades C and D: severe RO). Rabeprazole 10 mg/day was administered for 4 weeks to 180 patients who kept symptom diaries. Results: Complete relief of the symptoms was achieved in 35.8% of the NERD group and 55.4% of the erosive GERD group (mild RO: 51.1% and severe RO: 77.8%). Rabeprazole was significantly more effective in erosive GERD than in NERD patients. Among the NERD subgroups (Grades N and M), no difference in symptom improvement was observed. Conclusions: Four-week, rabeprazole 10 mg/day acid suppression therapy was effective in resolving symptoms in Japanese GERD patients. This therapy was more effective in erosive GERD than in NERD patients, and in those with severe RO than in those with mild RO. © 2007 The Authors.

    DOI: 10.1111/j.1365-2036.2007.03350.x

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  639. Performance of a time-projection chamber with a large-area micro-pixel-chamber readout Open Access

    Miuchi, K; Hattori, K; Kabuki, S; Kubo, H; Kurosawa, S; Nishimura, H; Takada, A; Tsuchiya, K; Okada, Y; Tanimori, T; Ueno, K

    NUCLEAR INSTRUMENTS & METHODS IN PHYSICS RESEARCH SECTION A-ACCELERATORS SPECTROMETERS DETECTORS AND ASSOCIATED EQUIPMENT   Vol. 576 ( 1 ) page: 43 - 46   2007.6

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    Publisher:Nuclear Instruments and Methods in Physics Research Section A Accelerators Spectrometers Detectors and Associated Equipment  

    A micro-time-projection chamber (micro-TPC) with a detection volume of 23×28×31 cm<sup>3</sup> was developed, and its fundamental performance was examined. The micro-TPC consists of a micro-pixel chamber with a detection area of 31×31 cm<sup>2</sup> as a two-dimensional imaging device and a gas electron multiplier (GEM) with an effective area of 23×28 cm<sup>2</sup> as a pre-gas-multiplier. The micro-TPC was operated at a gas gain of 50,000, and energy resolutions and spatial resolutions were measured. © 2007 Elsevier B.V. All rights reserved.

    DOI: 10.1016/j.nima.2007.01.117

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  640. Validity of endoscopic classification of nonerosive reflux disease

    Joh T., Miwa H., Higuchi K., Shimatani T., Manabe N., Adachi K., Wada T., Sasaki M., Fujiwara Y., Hongo M., Chiba T., Kinoshita Y., Ohara S., Kusano M., Hoshihara Y., Kurosawa S., Watanabe Y., Furuta T., Habu Y., Haruma K., Ito M., Fujimoto K.

    Journal of Gastroenterology   Vol. 42 ( 6 ) page: 444 - 449   2007.6

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    Background: Minimal changes, such as erythema without sharp demarcation or whitish turbidity of the lower esophageal mucosa, have recently been used for endoscopic classification of nonerosive reflux disease (NERD) in Japan. This study examined the usefulness of such changes in characterizing the pathophysiology of NERD. Methods: Physicians specializing in esophageal endoscopy performed endoscopy on 115 patients with NERD. Based on the presence or absence of minimal changes, patients were categorized as displaying NERD with minimal changes (grade M, n = 49) or with no minimal changes or mucosal breaks (grade N, n = 66). Clinical features, quality of life (QOL) scores, and ambulatory 24-h esophageal pH values were compared between groups. Ambulatory 24-h esophageal pH values were monitored in 31 patients (14 grade M and 17 grade N patients) who gave consent out of 115 patients. Results: In ambulatory 24-h esophageal pH monitoring, 57.1% (8/14) of grade M patients had pH < 4 more than 4% of the time (abnormal acid reflux) compared with 11.8% (2/17) in the grade N group, a significant difference (P = 0.018). QOL scores did not differ significantly between grades and were significantly lower in both groups compared with the general Japanese population. No significant differences were observed in patient background between the grade M and grade N groups. Conclusions: Frequency of abnormal acid reflux with NERD is higher in patients with minimal changes than in patients without such changes. Minimal changes are most likely attributable to gastric acid reflux. © Springer-Verlag Tokyo 2007.

    DOI: 10.1007/s00535-007-2022-3

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  641. Antibody immobilization to phospholipid polymer layer on gold substrate of quartz crystal microbalance immunosensor.

    Park J, Kurosawa S, Takai M, Ishihara K

    Colloids and surfaces. B, Biointerfaces   Vol. 55 ( 2 ) page: 164 - 72   2007.4

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    DOI: 10.1016/j.colsurfb.2006.11.032

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  642. [Anesthetic management in two infants undergoing hemilaminectomy for giant mediastinal neuroblastoma].

    Toda N, Murakami N, Ando T, Kokubo M, Kurosawa S, Kato M

    Masui. The Japanese journal of anesthesiology   Vol. 56 ( 2 ) page: 158 - 62   2007.2

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  643. Anesthetic management in two infants undergoing hemilaminectomy for giant mediastinal neuroblastoma

    Toda N., Murakami N., Ando T., Kokubo M., Kurosawa S., Kato M.

    Japanese Journal of Anesthesiology   Vol. 56 ( 2 ) page: 158 - 162   2007.2

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    We report the anesthetic management in two infants who were a three-month-old boy (case 1) and a two-month-old girl (case 2), undergoing hemilaminectomy for giant mediastinal neuroblastoma. Neuroblastoma invades into the intrathecal space in a rare occasion, resulting in paraplegia, which requires emergent operation to save the spinal cord. Mediastinal neuroblastoma also possesses significant respiratory and cardiovascular risks due to the close anatomic relationship with vital organs. In the present report, we show that preoperative computed tomography (CT) scan and/or echo-cardiography revealed tracheal deviation in case 1 and mass compression of the left atrium in case 2. Therefore, the patients with mediastinal masses should be carefully evaluated before subjecting them to anesthesia. Especially, there is a possibility that the masses which do not appear to compress the airway and cardiovascular systems develop the airway obstruction and cardiovascular collapse after induction of general anesthesia. In fact, before induction of general anesthesia in the case 2, trial of the prone positioning which was scheduled for the hemilaminectomy, resulted in bradycardia and hypotension, presumably due to the compression of the left atrium. In summary, the authors here discussed the preoperative evaluation and anesthetic management for giant mediastinal neuroblastoma in infants.

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  644. An Electron-Tracking Compton imaging Camera based on a gaseous TPC and a scintillation camera

    Ueno, K; Hattori, K; Kabuki, S; Kubo, H; Kurosawa, S; Miuchi, K; Nagayoshi, T; Nishimura, H; Okada, Y; Orito, R; Takada, A; Tanimori, T; Tsuchiya, K

    2007 IEEE NUCLEAR SCIENCE SYMPOSIUM CONFERENCE RECORD, VOLS 1-11   Vol. 3   page: 1960 - +   2007

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    We are developing an Electron-Tracking Compton imaging Camera (ETCC) based on a gaseous Time Projection Chamber (TPC) and a scintillation camera. The ETCC detects the energy and the direction of the incident gamma ray using the information of the recoil electron and the scattered gamma ray. We have developed the ETCC with a detection volume of 23 × 28 × 15 cm <sup>3</sup> which consists of the 23 × 28 × 15 cm<sup>3</sup> gaseous TPC and 30 × 30 cm<sup>2</sup> GSO(Ce) scintillation camera. And we obtained the gamma-ray image and investigated the performances of the ETCC. The Angular Resolution Measure (ARM) and the Scatter Plane Diviation (SPD) are 6.1 degree and 64.5 degree (HWHM) at 662keV, respectively, and the energy resolution is 18.0%(FWHM) at 662keV. © 2007 IEEE.

    DOI: 10.1109/NSSMIC.2007.4436538

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  645. Detector performance of the newage experiment Open Access

    Miuchi K., Hattori K., Kabuki S., Kubo H., Kurosawa S., Nishimura H., Okada Y., Takada A., Tanimori T., Tsuchiya K., Ueno K., Sekiya H., Takeda A.

    Proceedings of the 6th International Workshop on the Identification of Dark Matter Idm 2006     page: 308 - 313   2007

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    Publisher:Proceedings of the 6th International Workshop on the Identification of Dark Matter Idm 2006  

    NEWAGE(NEw generation WIMP search with an Advanced Gaseous tracking device Experiment) project is a direction-sensitive dark matter search experiment with a gaseous micro time-projection-chamber(μ-TPC).W e report on the performance of the μ-TPC with a detection volume of 23 x 28 x 30 cm<sup>3</sup> operated with a carbon-tetrafluoride (CF<inf>4</inf>) of 0.2 bar.

    DOI: 10.1142/9789812770288_0042

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  646. Development of a gamma camera based on an 8x8 array of LaBr<sub>3</sub>(Ce) scintillator pixels coupled to a 64-channel multi-anode PMT

    Kubo, H; Hattori, K; Ida, C; Iwaki, S; Kabuki, S; Kurosawa, S; Miuchi, K; Nagayoshi, T; Nishimura, H; Okada, Y; Orito, R; Takada, A; Tanimori, T; Tsuchiya, K; Ueno, K

    2007 IEEE NUCLEAR SCIENCE SYMPOSIUM CONFERENCE RECORD, VOLS 1-11   Vol. 6   page: 4569 - +   2007

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    We have developed a gamma camera based on an array of LaBr<inf>3</inf>(Ce) scintillator pixels coupled to a multi-anode photomultiplier tube (MAPMT). It consisted of an 8×8 array of LaBr3(Ce) pixels with a size of 5.8×5.8×15 mm<sup>3</sup> and a 64-channel MAPMT (Hamamatsu flat-panel H8500) with an effective area of 49×49 mm<sup>2</sup>. The pixels of the LaBr<inf>3</inf>(Ce) array were made from two LaBr<inf>3</inf>(Ce) monolithic crystals with a diameter of 38 mm and a height of 38 mm, which had energy resolutions of 4.33+0.02 % at 356 keV and 3.25±0.01 % at 662 keV. They were assembled into the array with a reflector between pixels, and sealed hermetically by our own technique. The pitch of the LaBr<inf>3</inf>(Ce) pixels, 6.1 mm, was determined to be the same as that of the anodes. The thickness of pixels was 15 mm to have moderate detection efficiency for sub-MeV/MeV gamma rays. We evaluated the performance as follows. At first, in order to remove the effect of the gain variance among anodes of the MAPMT, the array was coupled to a single-anode PMT, and collimated gamma rays from isotopes were irradiated to one pixel in the array. The energy resolutions (FWHM) were 5.4 (average) ±1.0 (RMS) % at 356 keV and 4.5±1.0 % at 662 keV. Next, in order to obtain a gamma-ray image of 64 pixels by readout of only four channels, we used a resistor-chain readout system in the charge division method. In flood field irradiation of gamma rays, each pixel was clearly resolved. The energy resolutions (FWHM) of 64 pixels were 8.6±1.0 % at 356 keV and 5.8±0.9 % at 662 keV. The averages were represented by (5.8±0.7) (E/662 keV)<sup>-0.52±0.02</sup> % at energies from 122 keV to 835 keV. © 2007 IEEE.

    DOI: 10.1109/NSSMIC.2007.4437127

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  647. Diagnostic approach of using an electron tracking compton gamma-ray camera based on small animal and phantom experiments

    Kabuki, S; Hattori, K; Kawashima, H; Kimura, H; Kohara, R; Kubo, A; Kubo, H; Kurosawa, S; Kunieda, E; Miuchi, K; Miyazaki, O; Nagayoshi, T; Nakahara, T; Nakamoto, Y; Nakazawa, T; Nishimura, H; Ogawa, K; Okada, T; Okada, Y; Orito, R; Saji, H; Sekiya, H; Shirahata, T; Takada, A; Tanimori, T; Togashi, K; Ueda, M; Ueno, K; Yamamoto, E

    2007 IEEE NUCLEAR SCIENCE SYMPOSIUM CONFERENCE RECORD, VOLS 1-11   Vol. 5   page: 3395 - +   2007

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    A conventional Compton camera reconstructs initial gamma-rays direction as circle. A Compton gamma-ray camera which we have developed can detect electron tracks. So our camera can reconstruct the initial gamma-rays as arc. It makes getting the low noise of image. In this paper, we report the results of three version of electron tracking camera. One is 10 × 10 × 10 cm <sup>3</sup> Time Projection Chamber (TPC) as a scatter detector and 15 × 15 cm<sup>2</sup> GSO pixel scintillator array (PSA) as an absorber. Second is a 10 × 10 × 10 cm<sup>3</sup> TPC and a 10 × 10 cm<sup>2</sup> LaBr<inf>3</inf> PSA. The energy resolution of LaBr<inf>3</inf> scintillator is about 2 times better than GSO scintillator. Third is a 30 × 30 × 15 cm<sup>3</sup> TPC and a 30 × 30 cm<sup>2</sup> GSO pixel PSA. The efficiency of this system is better than 10 cm<sup>3</sup> cube Compton gammra-ray camera. © 2007 IEEE.

    DOI: 10.1109/NSSMIC.2007.4436859

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  648. Observation of diffuse gamma-ray with electron-tracking compton imaging camera loaded on balloon

    Takada, A; Tanimori, T; Kubo, H; Miuchi, K; Tsuchiya, K; Kabuki, S; Nishimura, H; Hattori, K; Ueno, K; Kurosawa, S; Nonaka, N; Mizuta, E; Orito, R; Nagayoshi, T

    2007 IEEE NUCLEAR SCIENCE SYMPOSIUM CONFERENCE RECORD, VOLS 1-11   Vol. 4   page: 2558 - +   2007

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    We have developed an Electron Tracking Compton Camera (ETCC) as an MeV gamma-ray telescope in the next generation. Our detector consists of a gaseous time projection chamber and a position sensitive scintillation camera. In order to evaluate the performance of this detector, we constructed a flight model detector as a balloon experiment for the observation of diffuse cosmic gamma rays and atmospheric gamma rays. The balloon launched on September 1 in 2006. The balloon reached to 35 km at altitude, and the level flight continued during 4.0 hours. We succeeded in the detection of about 200 downward gamma rays in the energy range of 100 keV - 1 MeV during the 3.5 hours level flight (live time 3.0 hours). The detected photon number was consistent to the simulated one. Also, we measured the dependence of the gamma-ray flux on the zenith angle between 0° and 90°. Here we report on the detailed performance of the ETCC in this flight. © 2007 IEEE.

    DOI: 10.1109/NSSMIC.2007.4436672

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  649. Erratum to "Preparation of long-lifetime gas recognition films by plasma polymerization technique" [Sens. Actuators B 108 (1-2) (2005) 558-563] (DOI:10.1016/j.snb.2004.12.086)

    Kurosawa S., Miura H., Takahashi H., Park J., Aizawa H., Noda K., Yamada K., Hirata M.

    Sensors and Actuators B Chemical   Vol. 115 ( 1 )   2006.5

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    DOI: 10.1016/j.snb.2005.06.004

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  650. [Perioperative changes in the circulatory blood volumes in patients undergoing the abdominal aortic aneurysm repair].

    Yamamoto Y, Hoshi K, Ito J, Ito Y, Kurosawa S, Kato M

    Masui. The Japanese journal of anesthesiology   Vol. 55 ( 2 ) page: 164 - 8   2006.2

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  651. Perioperative changes in the circulatory blood volumes in patients undergoing the abdominal aortic aneurysm repair

    Yamamoto Y., Hoshi K., Ito J., Ito Y., Kurosawa S., Kato M.

    Japanese Journal of Anesthesiology   Vol. 55 ( 2 ) page: 164 - 168   2006.2

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    Publisher:Japanese Journal of Anesthesiology  

    Background: The effect of the intraoperative volume load on the circulating blood volume is unclear. Therefore, we investigated the changes of the perioperative blood volume in patients undergoing major surgery. Methods: In 16 patients undergoing abdominal aortic aneurysm repair, we measured the circulating blood volume (BV · kg<sup>-1</sup>) with the pulse dye-densitometry method (DDG analyzer) before operation, just after operation, on the first postoperative day (IPOD) and 2POD. Anesthesia was maintained with general anesthesia and epidural analgesia. The volume of infusion depended on empiric judgment by an anesthesiologist. Results: Mean anesthesia time was 390 minutes, the mean volume of infusion 4225 ml, transfusion 1329 g, blood loss 1567 g, urine output 729 ml, and mean water balance +3287ml. The mean body weight (BW) was 59.2 ± 13.7 (before), 60.2 ± 14.4 (just after), 60.5 ± 14.3 (IPOD), and 60.3 ± 14.3 (2POD) kg, respectively. The mean BV · kg<sup>-1</sup> was 78.0 ± 19.0 (before), 65.6 ± 13.4 (just after), 70.4 ± 15.7 (IPOD), and 76.5 ± 18.2 (2POD) ml · kg<sup>-1</sup>, respectively. The mean BW after operation increased significantly from the value before surgery. However, the mean BV · kg<sup>-1</sup> decreased significantly. There was a significant correlation between the intraoperative increase in BW and intraanesthetic water balance (Y = -2.91 + 0.071X; R = 0.66, P = 0.0412), but there was no significant correlation between the change in BV · kg<sup>-1</sup> and intraanesthetic water balance. Conclusions: Intraoperative water balance influenced a change of BW significantly, but did not affect BV · kg<sup>-1</sup>.

    Scopus

  652. Measurement of Interaction Forces between Montmorillonite Particles in NaCl Solutions using a Colloidal Probe Atomic Force Microscopy Open Access

    Kurosawa S., Mizukami M., Sato H., Kurihara K., Nozawa J., Tsutimoto K.

    Transactions of the Atomic Energy Society of Japan   Vol. 5 ( 3 ) page: 251 - 256   2006.1

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    Publisher:Transactions of the Atomic Energy Society of Japan  

    DOI: 10.3327/taesj2002.5.251

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  653. Balloon-Borne Sub-MeV Gamma-ray Imager Using Electron Tracking Gaseous TPC and Scintillation Camera

    Kubo, H; Hattori, K; Kabuki, S; Kurosawa, S; Miuchi, K; Nagayoshi, T; Nishimura, H; Okada, Y; Orito, R; Sekiya, H; Takada, A; Tanimori, T; Ueno, K

    2006 IEEE NUCLEAR SCIENCE SYMPOSIUM CONFERENCE RECORD, VOL 1-6   Vol. 1   page: 406 - 410   2006

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    Publisher:IEEE Nuclear Science Symposium Conference Record  

    A balloon-borne sub-MeV gamma-ray imaging detector for astrophysics has been developed. It measures a three dimensional track of a Compton-recoil electron and determines the incident direction of each photon in a reduced arc projected on the sky. Our developed detector consists of two parts: One is a gaseous time projection chamber (μ-TPC) with a size of 10×10×14 cm<sup>3</sup> with a micro pixel chamber (μ-PIC) readout, which measures both the three dimensional track and the energy of the Compton recoil electron. The other is a position-sensitive scintillation camera enclosing the μ-TPC, which consists of arrays of pixellated GSO(Ce) scintillators coupled to multianodes PMTs and measures both the direction and the energy of the scattered gamma ray. By the full reconstruction of incident gamma rays from these measurements, we have successfully obtained gamma-ray images in the 0.1-0.9 MeV range. The angular resolutions (FWHM) were 8.5° and 120° for single photon with 662 keV for an angular resolution measure and a scatter plane deviation, respectively. The detector had no collimator, and the field of view was 1 sr. In order to measure both the cosmic and the atmospheric gamma-ray background in the sub-MeV region, a balloon equipped with this detector was launched from JAXA/ISAS Sanriku Balloon Center in Japan on September 1, 2006, and flew for 7 hours with the highest altitude of 35 km. Based on the detector, a larger detector with the μ-TPC with a size of 30×30×30 cm <sup>3</sup> is being developed in order to observe celestial objects in the sub-MeV region. © 2006 IEEE.

    DOI: 10.1109/NSSMIC.2006.356185

    Web of Science

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  654. Development of a Electron Tracking Compton Gamma-Ray Camera Using a Gas Micro-Tracking Device for Nuclear Medicine

    Kabuki, S; Hattori, K; Kawashima, H; Kimura, H; Kohara, R; Kubo, A; Kubo, H; Kurosawa, S; Kunieda, E; Miyazaki, O; Nagayoshi, T; Nakahara, T; Nakazawa, T; Nishimura, H; Ogawa, K; Okada, Y; Orito, R; Saji, H; Sekiya, H; Shirahata, T; Takada, A; Tanimori, T; Ueda, M; Ueno, K; Yamamoto, E

    2006 IEEE NUCLEAR SCIENCE SYMPOSIUM CONFERENCE RECORD, VOL 1-6   Vol. 5   page: 2971 - 2975   2006

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    Publisher:IEEE Nuclear Science Symposium Conference Record  

    The Electron Tracking Compton Gamma-Ray Camera is consisted of two detectors which are a scatter detector and absorb detector. The scatter detector is a Time Projection Chamber which spatial resolution is 0.4 mm and energy resolution is 25% at 22 keV. This system can take the recoiled electron track and energy. The absorb detector which catches the position and energy of a scattered gamma-ray. This detector is consisted of GSO scintillator and multianode photomultiplier tube. A position resolution is 6 mm and the energy resolution is 11% at 662 keV. A spatial resolution of this whole system is 3 cm at 10cm distance from detector and the efficiency is 10<sup>-5</sup> sec <sup>-1</sup> cm<sup>-2</sup>. And, we report the various kinds of images. © 2006 IEEE.

    DOI: 10.1109/NSSMIC.2006.356499

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  655. A self-adaptive intrusion detection method for AODV-based mobile ad hoc networks

    Kurosawa S., Nakayama H., Kato N., Jamalipour A., Nomoto Y.

    2nd IEEE International Conference on Mobile Ad Hoc and Sensor Systems Mass 2005   Vol. 2005   page: 773 - 780   2005.12

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    Publisher:2nd IEEE International Conference on Mobile Ad Hoc and Sensor Systems Mass 2005  

    Mobile ad hoc networks (MANET) are usually formed without any major infrastructure. As a result, they are relatively vulnerable to malicious network attacks and therefore the security is a more significant issue than in infrastructure-type wireless networks. In these networks, it is difficult to identify malicious hosts, as the topology of the network changes dynamically. A malicious host can easily interrupt a route for which the malicious host is one of the forming nodes in the communication path. In the literature, there are several proposals to detect such malicious host inside the network. In those methods usually a baseline profile is defined in accordance to static training data and then they are used to verify the identity and the topology of the network, thus avoiding any malicious host to be joined in the network. Since the topology of a MANET is dynamically changing, use of a static profile is not efficient. In this paper, we propose a new intrusion detection scheme based on a learning process, so that the training data can be updated at particular time intervals. The simulation results show the effectiveness of the proposed technique compared to conventional schemes. © 2005 IEEE.

    DOI: 10.1109/MAHSS.2005.1542870

    Scopus

  656. Sivelestat, a neutrophil elastase inhibitor, reduces mortality rate of critically ill patients Open Access

    Hoshi, K; Kurosawa, S; Kato, M; Andoh, K; Satoh, D; Kaise, A

    TOHOKU JOURNAL OF EXPERIMENTAL MEDICINE   Vol. 207 ( 2 ) page: 143 - 148   2005.10

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    Language:English   Publisher:Tohoku Journal of Experimental Medicine  

    Many studies have suggested that neutrophil elastase (NE) may contribute to multiple organ failure (MOF) and acute injury of lung endothelial cells. It is therefore conceivable that NE inhibitors may improve the outcome of MOF patients. A synthetic NE inhibitor, sivelestat, which was developed and released in Japan, inhibited inflammatory reactions in various animal models. We examined the medical records of patients requiring more than two days of respiratory care in four intensive care units to investigate whether sivelestat contributed to improvement of their conditions. A total of 110 patients were divided into two groups (sivelestat treated group of 57 patients and untreated group of 53 patients). The conditions and age of the patients were similar in both groups. Sivelestat (0.2 mg/kg/hr) was administered continuously for 14 days beginning on the day of the intensive care unit (ICU) admission or for less than 14 days until discharge from the ICU. Hospital mortality differed significantly between the two groups (treated: 19% and untreated: 40%, p < 0.05). The severity of acute lung injury is defined by the ratio of arterial oxygen partial pressure (PaO2)/fraction concentration of oxygen in the inspired air (FiO2). When the PaO2/FiO<inf>2</inf> ratio is more than 200 mmHg, the morbidity is lower. In patients with PaO2/FiO2 ratio more than 200 mmHg, the hospital mortality was 33.3% (7/21) in the untreated group and 6.0% (1/18) in the treated group (p = 0.0236). We conclude that administration of sivelestat reduces mortality of critically ill patients. © 2005 Tohoku University Medical Press.

    DOI: 10.1620/tjem.207.143

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    PubMed

  657. [Anesthetic management for two cases of living related small bowel transplantation].

    Adachi K, Murakami N, Sasaki S, Kurosawa S, Horinouchi T, Kato M

    Masui. The Japanese journal of anesthesiology   Vol. 54 ( 8 ) page: 893 - 7   2005.8

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    Language:Japanese  

    PubMed

  658. Anesthetic management for two cases of living related small bowel transplantation

    Adachi K., Murakami N., Sasaki S., Kurosawa S., Horinouchi T., Kato M.

    Japanese Journal of Anesthesiology   Vol. 54 ( 8 ) page: 893 - 897   2005.8

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    Publisher:Japanese Journal of Anesthesiology  

    Isolated small bowel transplantation allows patients with irreversible small bowel failure to be weaned from total parenteral nutrition (TPN). We reported the first two cases of anesthesia for living related donor small bowel transplantation in our hospital. They had required long-term TPN. This resulted in thrombosis of the major blood vessels which critically restricted vascular access available for TPN, leading to a life-threatening condition for the patients. In patients with known difficult vascular access, performing a magnetic resonance imaging before surgery to evaluate patency of central veins seems reasonable, as well as inserting a central catheter before the surgical procedure. Graft reperfusion may cause hemodynamic instability due to changes in potassium, acid-base status as the preservative solution is flushed out of the implant. Hemodynamic, respiratory parameters and urinary output were well preserved throughout the procedure. Besides, a transitory increase in potassium following graft revascularization and biochemical changes were small. Anesthetic management requires comprehensive preoperative assessment and sufficient management without interfering with intestinal function, optimizing splanchnic perfusion to ensure implant viability.

    Scopus

  659. Preparation of long-lifetime gas recognition films by plasma polymerization technique

    Kurosawa S., Miura H., Takahashi H., Park J., Aizawa H., Noda K., Yamada K., Hirata M.

    Sensors and Actuators B Chemical   Vol. 108 ( 1-2 SPEC. ISS. ) page: 558 - 563   2005.7

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    Publisher:Sensors and Actuators B Chemical  

    Gas sorption and desorption properties of plasma-polymerized acrylic acid film (PPAAF) and cast poly(acrylic acid) film (CPAAF) were determined by QCM technique. The gas sorption properties of PPAAF are almost the same as those of CPAAF. PPAAF showed an excellent stability in repeated usage of the gas sorption and desorption cycles. © 2005 Elsevier B.V. All rights reserved.

    DOI: 10.1016/j.snb.2004.12.086

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  660. Enzyme-based glucose fuel cell using Vitamin K<sub>3</sub>-immobilized polymer as an electron mediator Open Access

    Sato, F; Togo, M; Islam, MK; Matsue, T; Kosuge, J; Fukasaku, N; Kurosawa, S; Nishizawa, M

    ELECTROCHEMISTRY COMMUNICATIONS   Vol. 7 ( 7 ) page: 643 - 647   2005.7

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    Publisher:Electrochemistry Communications  

    To create an enzyme-based biological fuel cell generating electricity from glucose and O<inf>2</inf>, we modified a glassy carbon electrode with a bi-layer polymer membrane, the inner layer containing diaphorase (Dp) and the outer, glucose dehydrogenase (GDH, an NAD<sup>+</sup>-dependent enzyme). The Dp membrane was formed from a newly synthesized 2-methyl-1,4-naphthoquinone (Vitamin K<inf>3</inf>; VK<inf>3</inf>)-based polymer. This polymer showed reversible redox activity at a potential close to that of free VK<inf>3</inf> (-0.25 V vs. Ag/AgCl sat. KCl), and served as an electron mediator of Dp for the electrocatalytic oxidation of NADH to NAD<sup>+</sup>. The addition of Ketjenblack into the Dp/VK<inf>3</inf> film enhanced the generation of NAD <sup>+</sup>. The outer GDH membrane oxidized glucose continuously using NAD<sup>+</sup> generated at the inner Dp film. To construct the glucose/O <inf>2</inf> biological fuel cell, we coupled the enzyme-modified anode with a polydimethylsiloxane-coated Pt cathode. The cell's open circuit voltage was 0.62 V and its maximum power density was 14.5 μW/cm<sup>2</sup> at 0.36 V in an air-saturated phosphate buffered saline solution (pH 7.0) at 37 °C containing 0.5 mM NADH and 10 mM glucose. Although its performance deteriorated to ca. 4 μW/cm<sup>2</sup> over 4 days, the cell subsequently maintained this power density for more than 2 weeks. © 2005 Elsevier B.V. All rights reserved.

    DOI: 10.1016/j.elecom.2005.04.015

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Books 2

  1. Research of Efficient and Fast Scintillator Garnet Crystals: The Role of Ce4+ in Ce3+, Mg2+-Co-Doped Gd3Al2Ga3O12 from Spectroscopic and XANES Characterizations

    Boulon G., Guyot Y., Guzik M., Dantelle G., Testemale D., Kurosawa S., Kamada K., Yoshikawa A.

    NATO Science for Peace and Security Series B Physics and Biophysics  2022 

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    In this lecture, two main goals have been shown: first, the state-of-art of the inorganic scintillator materials used for many important applications and, secondly, the illustration of the dynamics of this field by giving spectroscopic and scintillation properties of the most advanced oxide scintillator Ce<sup>3+</sup>, Mg<sup>2+</sup>-co-doped Gd<inf>3</inf>Al<inf>2</inf>Ga<inf>3</inf>O<inf>12</inf> (GAGG) garnet host, grown by using both the micro-pulling-down (μ-PD) and the Czochralski methods at the Tohoku University, Sendai. The adopted strategy for optimization of garnet scintillator composition in both, the defect engineering and band gap engineering of this research program gives us the opportunity to discuss on the role of Ce<sup>4+</sup> ion which has always been a challenge for Ce<sup>3+</sup>-doped luminescent crystals. By analogy with the approach used for commercial Ce<sup>3+</sup>, Mg<sup>2+</sup>-co-doped-doped orthosilicates as Lu<inf>2</inf>SiO<inf>5</inf> (LSO) and (Lu<inf>1−x</inf>Y<inf>x</inf>)<inf>2</inf>SiO<inf>5</inf> (LYSO), we confirm the creation of stable Ce<sup>4+</sup> oxidation state and we evaluate the Ce<sup>3+</sup>/Ce<sup>4+</sup> ratio of concentrations in Ce<sup>3+</sup>, Mg<sup>2+</sup>-co-doped Gd<inf>3</inf>Al<inf>2</inf>Ga<inf>3</inf>O<inf>12</inf> (GAGG) garnet by XANES spectroscopy analysed at the Ce L<inf>III</inf> threshold of the European Synchrotron Radiation Facility (ESRF) in Grenoble.

    DOI: 10.1007/978-94-024-2138-5_12

    Scopus

  2. Transparent High-Density Oxide Ceramics Prepared by Spark Plasma Sintering

    Goto T., Ito A., Yoshikawa A., Kurosawa S., Pejchal J.

    Nanocomposite Ceramic and Thin Film Scintillators  2016.1  ( ISBN:9789814745222, 9789814745239

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Presentations 3

  1. SMILE-72: Development of Gas TPC Towards Increased Sensitivity and Stability

    Abe M., Yoshioka R., Tanimori T., Takemura T., Yoshikawa K., Nakamura Y., Takada A., Ikeda T., Tahara K., Tsukamoto H., Kobayashi K., Mizumura Y., Sawano T., Nakamori T., Iiyama H., Kurosawa S., Miuchi K., Mori M., Hamaguchi K., Sawano T., Oka T., Kushida J.

    Meeting Abstracts of the Physical Society of Japan  2024  The Physical Society of Japan

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  2. SMILE-3へ向けたガスTPC部の開発

    塚本 博丈, 高田 淳史, 出口 颯馬, 佐藤 太陽, 池田 智法, 谷森 達, 阿部 光, 中森 健之, 吉岡 龍, 飯山 陽輝, 八重樫 大, 水村 好貴, 澤野 達哉, 坂田 望祥, 宗像 勇輔, 岡本 奏歩, 岡 知彦, 森 正樹, 櫛田 淳子, 黒澤 俊介, 濱口 健二, 身内 賢太朗

    大気球シンポジウム: 2024年度  2024.10  宇宙航空研究開発機構宇宙科学研究所 (JAXA)(ISAS)

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    Language:Japanese  

    レポート番号: isas24-sbs-027

    CiNii Research

  3. Exploring the Origin of Galactic Diffuse MeV Gamma Rays with SMILE-3

    MIZUMURA Yoshitaka, TAKADA Atsushi, TSUKAMOTO Hirotake, ABE Mitsuru, DEGUCHI Soma, SATO Taiyo, NAKAMORI Takeshi, IKEDA Tomonori, YAEGASHI Dai, SAWANO Tatsuya, SAKATA Misaki, OKAMOTO Kanaho, OKA Tomohiko, IIYAMA Haruki, KUSHIDA Junko, MORI Masaki, KUROSAWA Shunsuke, MUNAKATA Yusuke, HAMAGUCHI Kenji, MIUCHI Kentaro, TANIMORI Toru, YOSHIOKA Ryo

    Balloon Symposium: 2024  2024.10 

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    Language:Japanese  

    CiNii Research

KAKENHI (Grants-in-Aid for Scientific Research) 2

  1. Improvement of scintillation properties of new type scintillator crystals with gadolinium ions based on electronic structure analysis

    Grant number:26420673  2014.4 - 2018.3

    Grants-in-Aid for Scientific Research  Grant-in-Aid for Scientific Research (C)

    Kitaura Mamoru

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    Authorship:Coinvestigator(s) 

    We have investigated the origin of shallow electron traps in Ce:GAGG crystals by using various spectroscopy techniques, in order to improve scintillation properties of this material. It turned out that shallow electron traps are composed of Gd2+ ions adjacent to oxygen vacancies. The Gd2+ ions are antisite defects occupying B sites in the garnet lattice. The first-principles calculations revealed antisite Gd2+ ions are introduced due to cation deficiency at the B sites. The reduction of cation deficiency is the best way to improve scintillation properties of Ce:GAGG crystals. To do so, it was found that Mg2+ codoping is useful.

  2. 広視野MeVガンマ線カメラを用いた長期気球実験による銀河面探査

    Grant number:08J00940  2008 - 2010

    科学研究費助成事業  特別研究員奨励費

    黒澤 俊介

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    Authorship:Principal investigator 

    Grant amount:\1800000 ( Direct Cost: \1800000 )

    宇宙において放射されるガンマ線の多くはシンクロトロン放射など連続ガンマ線であるが、今までに撮像観測されてきた例はX線やTeVガンマ線など他の波長域に比べて少ない。ラインガンマ線の場合にはそのエネルギーのみを解析で使用するのでガンマ線バックグラウンドなどの除去が比較的容易であるが、連続ガンマ線の場合は難しく、イメージングが難しい。ここで、電子飛跡型コンプトンカメラは検出器内でコンプトン散乱を起こさせ、そこで生じる反跳電子および散乱ガンマ線の(3次元)方向とエネルギーを測定できるので、既存のカメラよりもバックグラウンドを抑えることができる。そこで電子飛跡型コンプトンカメラを開発し、連続ガンマ線のイメージング実証実験を行った。本実験は大阪大学核物理センターにおいて140MeVの陽子線ビームを使用して、水をターゲットにして、生じるガンマ線の撮像を行った。エネルギー帯を463-559keVおよび800-2000keVに分けて再構成したイメージでは、前者のほうが広がったイメージになった。これは511keV(電子陽電子対消滅線)の発生分布がブラッグピークと対応していないために生じるもので、一方後者は即発ガンマ線などが由来となっているガンマ線でブラッグピーク位置をトレースし、このイメージ分布はシミュレーションとも矛盾がなかった。この結果から、今までラインガンマ線のみしか行われてこなかったわれわれのカメラのイメージングについて、連続ガンマ線に対するイメージング能力も実証された。これによって、銀河面をはじめ多くの連続ガンマ線放射天体の位置同定といった撮像を行えることが期待できる。なお本実験において、コンプトンカメラのエネルギー測定範囲を今までの1.3MeVから2MeVまで上げることに成功した。