|
|
|
题名
|
作者
|
年代
|
出处
|
被引量
|
| 1 | Development of novel scintillator crystals显示文摘 | Martin Nikl Akira Yoshikawa Anna Vedda Tsuguo Fukuda | 2006 | Journal of Crystal Growth2006，，： | 1 |
| 2 | Growth and scintillation characteristics of CeF3, PrF3 and NdF3 single crystals 显示文摘 | Kiyoshi Shimamura Encarnacion G Villora Satoshi Nakakita Martin Nikl Noboru Ichinose | 2004 | Journal of Crystal Growth2004，264，13： | 1 |
| 3 | Develop- ment ofnovel scintillator crystals显示文摘 | Martin Nikl Akira Yoshikawa Anna Vedda | 2006 | Journal of CrystalGrowth2006，292，2： | 1 |
| 4 | Scintillation efficiency and X-ray imaging with the RE-Doped LuAG thin films grown by liquid phase epitaxy显示文摘 | Jan Tous Karel Blazek Miroslav Kucera Martin Nikl Jiri A. Mares | 2012 | Radiation Measurements2012，，4： | 1 |
| 5 | 热等静压烧结制备细晶粒 Ce,Y:SrHfO_(3) 闪烁陶瓷显示文摘Ce:SrHfO_(3)陶瓷因具有高密度和高有效原子序数,对高能射线具有很强的阻止能力。同时,Ce:SrHfO_(3)陶瓷还具有快衰减和高能量分辨率等优异的闪烁性能,引起了研究人员的广泛关注。由于传统的烧结方法难以实现非立方结构Ce:SrHfO_(3)陶瓷的透明化,本研究采用真空长时烧结和短时真空预烧结合热等静压烧结(Hot Isostatic Pressing,HIP)方法制备Ce,Y:SrHfO_(3)陶瓷。以金属氧化物和碳酸盐为原料,1200℃下煅烧8 h可以获得平均粒径为152 nm的纯相Ce,Y:SrHfO_(3)粉体。1800℃真空烧结20 h获得平均晶粒尺寸为28.6μm的不透明的Ce,Y:SrHfO_(3)陶瓷,而两步烧结法可以制备光学透过率良好的Ce,Y:SrHfO_(3)陶瓷。本研究详细分析了陶瓷致密化过程中微结构的演变,探究了预烧结温度对Ce,Y:SrHfO_(3)陶瓷密度、显微结构和光学透过率的影响。真空预烧(1500℃×2 h)结合HIP后处理(1800℃×3 h,200 MPa Ar)所获得的Ce,Y:SrHfO_(3)陶瓷在800 nm处的最高直线透过率为21.6%,平均晶粒尺寸仅为3.4μm。在X射线激发下,Ce,Y:SrHfO_(3)陶瓷在400 nm处产生Ce3+5d-4f发射峰,其XEL积分强度比商用锗酸铋(BGO)晶体高3.3倍,Ce,Y:SrHfO_(3)陶瓷在1μs门宽下的光产额约为3700 ph/MeV。良好的光学和闪烁性能可以拓宽Ce,Y:SrHfO_(3)陶瓷在闪烁探测领域的应用。 | 朱丹阳 钱康 陈肖朴 胡泽望 刘欣 李晓英 潘裕柏 MIHÓKOVÁEva NIKL Martin 李江 | 2021 | 无机材料学报2021，36，10： | 1 |
| 6 | Growth and scintillation properties of Yb-doped Lu 3 Al 5 O 12 crystals显示文摘 | Hiraku Ogino Akira Yoshikawa Jong-Ho Lee Martin Nikl Natalia Solovieva Tsuguo Fukuda | 2003 | Journal of Crystal Growth2003，，： | 1 |
| 7 | Growth and scintillation properties of Pr-doped Lu 3 Al 5 O 12 crystals显示文摘 | Hiraku Ogino Akira Yoshikawa Martin Nikl Aleksei Krasnikov Kei Kamada Tsuguo Fukuda | 2005 | Journal of Crystal Growth2005，，： | 1 |
| 8 | Scintillation properties of Gd 3 Al 2 Ga 3 O 12 :Ce 3+ single crystal scintillators显示文摘 | Ongsa Sakthong Weerapong Chewpraditkul Chalerm Wanarak Kei Kamada Akira Yoshikawa Petr Prusa Martin Nikl | 2014 | Nuclear Inst. and Methods in Physics Research, A2014，，： | 1 |
| 9 | Positron emission mammography using Pr:LuAG scintillator – Fusion of optical material study and systems engineering显示文摘 | Akira Yoshikawa Takayuki Yanagida Kei Kamada Yuui Yokota Jan Pejchal Akihiro Yamaji Yoshiyuki Usuki Seiichi Yamamoto Masayasu Miyake Kazuaki Kumagai Katsuhisa Sasaki T.R. dos Santos Mamoru Baba Masatoshi Ito Motohiro Takeda Noriaki Ohuchi Martin Nikl | 2010 | Optical Materials2010，，： | 1 |
| 10 | Compositional regulation of multi-component GYGAG:Ce scintillation ceramics:Self-sintering-aid effect and afterglow suppression显示文摘(Gd,Y,Ce)_(3)(Y_(x)Ga_(1−x))_(2)GaAl_(2)O_(12)(GYGAG:Ce)scintillation ceramics with different Y excess,where x=0.005−0.08,were fabricated by the solid-state reaction method.The effects of stoichiometry on the phase composition,optical quality,and microstructure of GYGAG:Ce ceramics were analyzed.GYGAG:Ce ceramics have a pure garnet phase and obtain good in-line transmittance when x<0.04,while more Y excess leads to the creation of the secondary phase.The change of x value influences the sintering behavior of the GYGAG:Ce ceramics:The excess of Y works as the self-sintering aid and significantly reduces the sintering temperature of ceramics.When x=0.01–0.04,the X-ray excited luminescence(XEL)spectra and light yields of GYGAG:Ce ceramics are similar.The fast scintillation decay time and afterglow intensity of GYGAG:Ce ceramics show a slight decrease with increasing x value.Finally,additional 50–500 ppm MgO and 100–500 ppm CaO were introduced to the GYGAG:Ce ceramic with x=0.04,and both were found to significantly increase the fast scintillation component and reduce the afterglow intensity by two orders of magnitude to 0.01%after X-ray cut-off. | Danyang Zhu Lexiang Wu Alena Beitlerova Romana Kucerkova Weerapong Chewpraditkul Martin Nikl Jiang Li | 2023 | Journal of Advanced Ceramics2023，12，10： | 0 |
| 11 | Ce掺杂浓度对Ce,Ca:Lu_(3)Al_(5)O_(12)陶瓷闪烁性能的影响显示文摘以共沉淀纳米粉体为原料,制备不同Ce掺杂浓度的x%(摩尔分数)Ce,0.15%Ca:Lu_(3)Al_(5)O_(12)(Ce,Ca:LuAG,x=0.1~0.5)闪烁陶瓷。在分析了Ce,Ca:Lu AG陶瓷的相组成和微观结构的基础上,研究了其闪烁特性与Ce浓度的关系,包括X射线激发发射光谱、光致发光衰减、闪烁衰减、光产额及快分量、余辉。当Ce浓度超过0.3%时,光致发光衰减的加速证实了浓度猝灭的发生。Ce,Ca:LuAG陶瓷的X射线激发发射强度和光产额在Ce浓度为0.3%时达到最大值。随着Ce浓度的增加,陶瓷的余辉水平逐渐降低。最后讨论了Ce,Ca:LuAG闪烁陶瓷的制备和性能优化的策略。 | 朱丹阳 蔡金伶 BEITLEROVA Alena KUCERKOVA Romana CHEWPRADITKUL Weerapong NIKL Martin 李江 | 2024 | 硅酸盐学报2024，52，3： | 0 |
| 12 | Development and prospects of garnet ceramic scintillators:A review显示文摘Garnet ceramic scintillators are a class of inorganic scintillation materials with excellent overall performance.The flexibility of cation substitution in different lattice positions leads to tunable and versatile properties and a wide range of applications.This paper starts with an overview of the development history of the inorganic scintillation materials,followed by a description of major preparation methods and characterization of garnet scintillation ceramics.Great progress obtained in recent years consisting in applying the band-gap and defect engineering strategies to the garnet scintillation ceramics is reviewed.Finally,the respective problems in the preparation and performance of multicomponent garnet single crystals and ceramics and the effective solutions are discussed.The garnet scintillation ceramics with the highest application potential are summarized,and the future development directions are proposed. | Danyang ZHU Martin NIKL Weerapong CHEWPRADITKUL Jiang LI | 2022 | Journal of Advanced Ceramics2022，11，12： | 0 |
您所在的机构暂未开通此部分的功能，请联系管理员