光致发光
闪烁
微秒
发光
分析化学(期刊)
兴奋剂
量子产额
材料科学
产量(工程)
离子
激发态
Crystal(编程语言)
光电子学
化学
冶金
原子物理学
光学
物理
程序设计语言
计算机科学
量子力学
荧光
探测器
色谱法
作者
Tao Wu,Zhehao Hua,Gao Tang,Huiyun Ban,Hua Cai,Jifeng Han,Hui Liu,Shan Liu,S. Qian,Laishun Qin,Jing Ren,X. Sun,Xin‐Yuan Sun,Yufeng Wen,Yao Zhu
摘要
Abstract Ce 3+ ‐doped 20Gd 2 O 3 –20Al 2 O 3 –60SiO 2 (GAS: x Ce 3+ ) glasses ( x = 0.3, 0.7, 1.1, 1.5, 1.9 mol%) with Si 3 N 4 as a reducing agent were prepared. The density of the glasses is around 4.2 g/cm 3 . With the increase in the Ce 3+ concentration, both the photoluminescence (PL) and PL excitation peaks of GAS: x Ce 3+ glasses show a redshift because the 4f–5d energy levels of Ce 3+ ions are narrowed. PL quantum yield and PL decay time of GAS: x Ce 3+ glasses are 28.32–50.59% and 43–64 ns, respectively. In addition, they both first increases and then decreases with the Ce 3+ concentration increasing, reached the maximum when x = 1.1 mol%. The integrated X‐ray excited luminescence (XEL) intensity of the GAS:1.1Ce 3+ glass is 23.86% of that of Bi 4 Ge 3 O 12 (BGO) crystal, and the light yield reaches 1200 ph/MeV with an energy resolution of 22.98% at 662 keV when exposed to γ‐rays. The PL and XEL thermal activation energies of GAS: x Ce 3+ glasses are independent of Ce 3+ ions concentration. Scintillating decay time of the glasses exhibits two components consisting of nanosecond and microsecond levels, and the scintillating decay time gradually decreases with the Ce 3+ concentration increasing. The difference between PL and scintillating decay time is discussed regarding the different luminescent mechanisms.
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