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人工晶体学报 ›› 2022, Vol. 51 ›› Issue (9-10): 1785-1793.

• 研究论文 • 上一篇    下一篇

高密度闪烁体Nd∶GdTaO4和Nd∶LuTaO4发光跃迁强度计算

张庆礼1,2, 孙贵花1,2, 罗建乔1,2, 何異1,2,3, 陈迎迎1,2,3, 高进云1,2, 窦仁勤1,2, 刘文鹏1,2, 王小飞1,2, 丁守军2,4, 张德明1,2, 孙彧1,2   

  1. 1.中国科学院合肥物质科学研究院,安徽光学精密机械研究所,光子器件与材料安徽省重点实验室,合肥 230031;
    2.先进激光技术安徽省实验室,合肥 230037;
    3.中国科学技术大学,合肥 230026; 4.安徽工业大学数理科学与工程学院,马鞍山 243032
  • 收稿日期:2022-08-09 出版日期:2022-10-15 发布日期:2022-11-02
  • 作者简介:张庆礼(1973—),男,云南省人,博士,研究员。E-mail:zql@aiofm.ac.cn。张庆礼,云南省人,2001年毕业中国科技大学物理系,同年进入中国科学院安徽光学精密机械研究所工作,主要研究领域为人工晶体生长、发光物理等,兼任《人工晶体学报》编委、《量子电子学报》副主编、中国感光学会理事等。
  • 基金资助:
    国家自然科学基金(51172236,51802307);安徽省先进激光技术实验室开放项目(AHL20220ZR04,AHL2021KF07);安徽省重大科技专项(202203a05020002)

Optical Transition Intensity Calculation of High-Density Scintillator Nd∶GdTaO4 and Nd∶LuTaO4

ZHANG Qingli1,2, SUN Guihua1,2, LUO Jianqiao1,2, HE Yi1,2,3, CHEN Yingying1,2,3, GAO Jinyun1,2, DOU Renqin1,2, LIU Wenpeng1,2, WANG Xiaofei1,2, DING Shoujun2,4, ZHANG Deming1,2, SUN Yu1,2   

  1. 1. Anhui Provincial Key Laboratory of Photonic Devices and Materials, Anhui Institute of Optics and Fine Mechanics, Hefei Institutes of Physical Science, Chinese Academy of Sciences, Hefei 230031, China;
    2. Advanced Laser Technology Laboratory of Anhui Province, Hefei 230037, China;
    3. University of Science and Technology of China, Hefei 230026, China;
    4. School of Mathematics & Physics Ahut, Anhui University of Technology, Ma’anshan 243032, China
  • Received:2022-08-09 Online:2022-10-15 Published:2022-11-02

摘要: GdTaO4和LuTaO4是具有快发光衰减的新型重闪烁体。采用全谱拟合方法拟合了808 nm 激光二极管(LD)激发的M相Nd∶GdTaO4和M′相Nd∶LuTaO4的光致发光谱,给出了它们的跃迁强度参数Akt,p。在808 nm 激光激发下,GdTaO4中Nd3+离子4F3/2能级的上下两个晶场子能级的粒子布居数比例接近1,而在Nd∶LuTaO4中则为1.30、1.41,表明在808 nm激光激发下,Nd3+4F3/2两个晶场子能级间的无辐射弛豫速率与激发速率相近。通过给出的跃迁强度参数Akt,p计算了Judd-Ofelt跃迁强度参数Ωt,计算了Nd3+在GdTaO4、LuTaO4中的2P3/2跃迁几率,表明GdTaO4和LuTaO4中Nd3+的数百纳秒发光跃迁是由高的无辐射跃迁几率导致的快发光衰减。

关键词: 稀土钽酸盐, 重闪烁体, 跃迁强度, 发光, 无辐射跃迁, 布居数

Abstract: GdTaO4 and LuTaO4 are heavy scintillators with fast decay fluorescence. The photoluminsecence spectra of M phase Nd∶GdTaO4 and M′ phase Nd∶LuTaO4 excited by a laser diode (LD) of 808 nm were fitted with the full-profile fitting method, and the transition intensity parameters Akt,p were determined. Under the excitation of 808 nm LD laser, the population ratio between the upper and low crystal field energy levels of 4F3/2 for Nd3+ in GdTaO4 is near to 1, but in LuTaO4 is 1.30 and 1.41, which indicates that the relaxation rate between two crystal field energy levels is nearly equal to the excitation rate of LD. The Judd-Ofelt transition intensity parameters Ωt were calculated with Akt,p, and the transition probabilities from 2P3/2 of Nd3+ in GdTaO4 and LuTaO4 were computed, which indicates that the fast decay fluorescence of several hundred nanoseconds of Nd3+ in GdTaO4 and LuTaO4 is caused by the high nonradiative transition.

Key words: rare-earth tantalate, heavy scintillator, transition intensity, luminescence, nonradiative transition, population

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