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Y3+掺杂Ce:Li6Lu(BO3)3闪烁体的发光性能研究
引用本文:孙丹丹,潘尚可,任国浩,吴云涛,商珊珊,张国庆.Y3+掺杂Ce:Li6Lu(BO3)3闪烁体的发光性能研究[J].无机材料学报,2013,28(9):987-991.
作者姓名:孙丹丹  潘尚可  任国浩  吴云涛  商珊珊  张国庆
作者单位:(1. 中国科学院 上海硅酸盐研究所, 上海201800; 2. 中国计量学院 材料科学与工科学院, 杭州310018; 3. 中国地质大学 地球科学学院,武汉430074)
基金项目:国家自然科学基金(51272263)
摘    要:针对Ce:Li6Lu(BO3)3晶体有效原子序数(Zeff)高的问题, 采用低原子序数的Y3+离子部分置换晶体中的Lu3+离子。通过固相合成法制备了Ce:Li6Lu1-xYx(BO3)3(0≤x≤1)固溶体。X射线粉末衍射(XRD)分析表明, 该系列固溶体结构与Li6Gd(BO3)3晶体相同, 空间群为P21/c。其X射线激发发射(XSL)的发光强度随着Y3+的含量增加而降低, 当x=0.5时, 固溶体的有效原子序数与Li6Gd(BO3)3闪烁体相当, 但XSL发光强度是其1.4倍。Ce:Li6Lu0.5Y0.5(BO3)3的XSL光谱和PL光谱都在400 nm附近出现Ce3+离子的特征峰, 可拟合出361和419 nm两个发光分量, 分别对应于Ce3+离子的激发态电子的5d12F5/25d12F7/2能级跃迁。Ce:Li6Lu0.5Y0.5(BO3)3固溶体的衰减时间比Ce:Li6Lu(BO3)3略长, 为19.6 ns。当x=0.50~0.70时, Ce:Li6Lu1-xYx(BO3)3(0≤x≤1)闪烁体比较适合作为中子探测材料。

关 键 词:固相合成  Ce:Li6Lu1-xYx(BO3)3  X射线激发发射谱  PL光谱  衰减时间  
收稿时间:2012-12-06
修稿时间:2013-01-21

Luminescence Properties of High Y3+-doped Ce:Li6Lu(BO3)3 Scintillators
SUN Dan-Dan,PAN Shang-Ke,REN Guo-Hao,WU Yun-Tao,SHANG Shan-Shan,ZHANG Guo-Qing.Luminescence Properties of High Y3+-doped Ce:Li6Lu(BO3)3 Scintillators[J].Journal of Inorganic Materials,2013,28(9):987-991.
Authors:SUN Dan-Dan  PAN Shang-Ke  REN Guo-Hao  WU Yun-Tao  SHANG Shan-Shan  ZHANG Guo-Qing
Affiliation:(1. Shanghai Institute of Ceramics, Chinese Academy of Sciences, Shanghai 201800, China; 2. College of Materials Science and Engineering, China Jiliang University, Hangzhou 310018, China; 3. Faculty of Earth Sciences, China University of Gesciences, Wuhan 430074, China)
Abstract:To decrease the high effective atomic number (Zeff) of Ce:Li6Lu(BO3)3 crystal, Y3+, which has a lower atomic number, is introduced to substitute Lu3+. The Ce:Li6Lu1-xYx(BO3)3(0≤x≤1) solid solutions were prepared by the solid-state synthesis method. Based on the X-ray powder diffraction (XRD) analysis, Ce: Li6Lu1-xYx(BO3)3 (0≤x≤1) solid solutions and Li6Gd(BO3)3 crystal have the similar XRD patterns and belong to the space group P21/c. The luminescence intensity of X-ray stimulated luminescence (XSL) spectrum of Ce:Li6Lu1-xYx(BO3) (0≤x≤1) decreases with the increasing of the content of Y3+. In the case of x=0.5, the Zeff of Ce:Li6Lu0.5Y0.5(BO3)3 is similar to that of Ce:Li6Gd(BO3)3, while the luminescence intensity of Ce:Li6Lu0.5Y0.5(BO3)3 is as much as 1.4 times of Ce:Li6Gd(BO3)3. The XSL and PL spectra of Ce:Li6Lu0.5Y0.5(BO3)3 indicate that the emission band around 400?nm can be fitted into two peaks, 391 nm and 419 nm, which correspond to the electronic transition from 5d energy level to 2F5/2 and 2F7/2 of Ce3+ ions, respectively. The decaying time of Ce:Li6Lu0.5Y0.5(BO3)3 is about 19.6 ns. When x=0.50-0.70, Ce:Li6Lu1-xYx(BO3)3(0≤x≤1) is suitable for using as neutron detection material.
Keywords:solid-state synthesis  Ce:Li6Lu1-xYx(BO3)3  X-ray stimulated luminescence spectrum  PL spectrum  decay time  
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