Abstract

Persistent phosphor as a kind of light-emitting material can store excitation energy in the so-called traps, and then persistently release the energy in the form of light emission after the end of excitation. This emission is called persistent luminescence. Much attention has been paid to optimizing the emission performance of persistent phosphors, including emission wavelength and persistent time. However, research on the excitation for charging persistent phosphors is relatively lacking. To acquire the persistent luminescence effectively, the traps need to be filled typically by ionizing irradiation. That is, high-energy light (such as ultraviolet light) is a general requirement for charging the persistent phosphors. Taking into account the fact that low-energy illumination (e.g. visible or infrared light) is much more suitable and less harmful than ultraviolet light for some practical applications, taking advantage of the low-energy light excitation is therefore an urgent issue to be solved in the persistent luminescence area. Several low-energy excitation approaches have been reported, in which up-conversion charging (UCC) is a promising candidate for charging phosphors using low-energy excitation light sources. The definition of UCC is as follows: UCC is a non-linear excitation for storage phosphors, in which the traps are typically filled via a two-step ionization mechanism. Prior research on the UCC has focused primarily on the demonstration of two-step ionization and the associated trapping properties. Recently, researchers have realized that the excitation light may release some trapped electrons while filling the traps (i.e. excitation-light stimulated detrapping). Competition between the trapping and detrapping during the UCC has been roughly described on the assumption that the illumination dose is in a certain range and the effect of ambient-temperature stimulated detrapping is negligible. Despite the initial progress, the exact effect of detrapping on the UCC process needs to be further explored. Here we demonstrate the effect of detrapping on UCC dynamics by a rate equation approach. Accordingly, taking LaMgGa<sub>11</sub>O<sub>19</sub>:Mn<sup>2+</sup> phosphor illuminated by a 450 nm laser for example, we measure its thermoluminescence. Our measurements reveal that the competition between the trapping and detrapping depends both on illumination power and on illumination duration. The experimental results are consistent well with the theoretical predictions, thereby offering a new insight into the understanding of UCC. In addition, the experimental demonstration on the LaMgGa<sub>11</sub>O<sub>19</sub>:Mn<sup>2+</sup> phosphor allows us to explore the generality of the present UCC model. Accordingly, we expect some existing phosphors can now be revisited.

Highlights

  • The straight line is a quadratic fit of the data

  • The straight line is a fit of the data

  • 本文以 450 nm 激光激发的 LaMgGa11O19:Mn2+ 材料为例, 通过分析速率方 程, 讨论了陷阱的光辐照填充与激发光激励排空之间的竞争

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Summary

Introduction

在此基础上 , 选 择 450 nm 激光激发的 LaMgGa11O19:Mn2+ 长余辉材料体系为模板, 分析了激发光剂量与材料热 释光强度的函数关系, 揭示了光辐照陷阱填充与光排空之间的动力学竞 争. 每次谱学测试之前, 样品内部的余辉陷阱需经退火排空 (420 °C 马弗炉中退火 15 min). 图 2 (a) LaMgGa11O19:Mn2+ 材料的上转换充能余辉发射谱; (b) 上转换充能及伴随的余 辉发射路径示意图 Fig. 2. (a) Up-conversion charging induced persistent luminescence (UCC-PersL) emission spectra of LaMgGa11O19:Mn2+; (b) Schematic representation of the UCC-PersL process. 例如, 如果每次测试中固定了辐照时长 t, 在小功率范围内辐照样品 (P·t 的数值很小), N-P 函数关系依然可用方程 (6) 拟合.

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