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首页> 外文期刊>Nuclear Instruments & Methods in Physics Research. B, Beam Interactions with Materials and Atoms >Mathematical formulation of T_(max)-T_(stop) method for LM-OSL and its experimental validation on α-Al_2O_3:C
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Mathematical formulation of T_(max)-T_(stop) method for LM-OSL and its experimental validation on α-Al_2O_3:C

机译:LM-OSL的T_(max)-T_(stop)方法的数学公式及其在α-Al_2O_3:C上的实验验证

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摘要

A mathematical formulation and its experimental validation on α-Al_2O_3:C for evaluating the number of OSL components has been described. The method consists of various partial bleaching steps of LM-OSL curve and as a result, the peak position (T_(max)) of the resultant curve shifts if the system contains multiple components. However, for single component system the peak position of the resultant curve doesn't change on partial bleaching for a phosphor obeying first order kinetics. The method has been theoretically formulated for single and multiple component system with different order of kinetics and validated experimentally on the commercial α-Al_2O_3:C OSL phosphor. The slope of the curve between shift in T_(max) and bleaching time gives the number of the OSL components and measure of their closeness in terms of photoionization cross-section. Based on this result, the photoionization cross-section of the two embedded peaks in the LM-OSL curve of α-Al_2O_3:C were found to be 1.51 × 10~(-18) cm~2 and 5.02 × 10~(-19) cm~2 using CW-OSL and NL-OSL method.
机译:描述了一种数学公式及其在α-Al_2O_3:C上用于评估OSL组分数量的实验验证。该方法由LM-OSL曲线的各个部分漂白步骤组成,因此,如果系统包含多个组件,则所得曲线的峰值位置(T_(max))会移动。但是,对于单组分系统,对于遵循一级动力学的荧光粉,部分漂白后所得曲线的峰值位置不会改变。该方法已从理论上为具有不同动力学顺序的单组分和多组分系统制定,并在商用α-Al_2O_3:C OSL荧光粉上进行了实验验证。 T_(max)的偏移和漂白时间之间的曲线斜率给出了OSL组分的数量,并以光电离截面的形式测量了它们的紧密度。基于该结果,发现α-Al_2O_3:C的LM-OSL曲线中两个嵌入峰的光电离截面分别为1.51×10〜(-18)cm〜2和5.02×10〜(-19使用CW-OSL和NL-OSL方法测量)cm〜2。

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