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首页> 外文期刊>Chinese physics >Up-conversion luminescence research of Er(0.5):ZBLAN material for volumetric display application when excited by 1520 nm laser
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Up-conversion luminescence research of Er(0.5):ZBLAN material for volumetric display application when excited by 1520 nm laser

机译:Er(0.5):ZBLAN材料在1520 nm激光激发下的上转换发光研究

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摘要

The up-conversion luminescence of the ZBLAN fluoride glass Er(0.5):ZBLAN, when excited by a 1520 nm semiconductor laser, is studied in this paper. The absorption and common-fluorescence spectra are also measured in order to understand the up-conversion clearly. It is found that there are seven strong up-conversion luminescence lines (406.97~m, 410.42nm), (521.97~m, 527.56 nm), (542.38~m, 549.27 nm), (654.27~m, 665.70 nm), 801.57~m nm, 819.46 nm, and 840.00 nm, which can be recognized as the fluorescence transitions of (~2G~4F~2H)_(9/2) → ~4I_(15/2) ~2H_(11/2) → ~4I_(15/2), ~4S_(3/2) → ~4I_(15/2), ~4F_(9/2) → ~4I_(15/2) ~4I_(9/2) → ~4I_(15/2) (~2G~4F~2H)_(9/2) → ~4I_(9/2), and ~4S_(3/2) → ~4I_(13/2) respectively. Meanwhile, the small up-conversion fluorescence lines 379.20nm, 453.10nm and 490.60nm are the transitions of ~4G_(11/2) → ~4I_(15/2), ~4F_(5/2) → ~4I_(15/2) and ~4F_(7/2) → ~4I_(15/2) respectively. It is interesting that the slopes of log F―logP curves, the double-logarithmic variation of up-conversion luminescence intensity F with laser power P, are different from each other for these observed up-conversion luminescence, this being valuable for the volumetric display. Comprehensive discussions find that the ~4G_(11/2) → ~4I_(15/2), (~2G~4F~2H)_(9/2) → ~4I_(15/2), (~2H_(11/2) → ~4I_(15/2), ~4S_(3/2) → ~4I_(15/2), ~4F_(9/2) → ~4I_(15/2)), and ~4I_(9/2) → ~4I_(15/2) up-conversion luminescences are five-photon, four-photon, three-photon, and two-photon up-conversion luminescences respectively. It is found also that the absorption from ground-state ~4I_(15/2) level to ~4I_(13/2) level is very large, which is beneficial to the sequential energy transfer up-conversion to occur.
机译:本文研究了由1520 nm半导体激光器激发的ZBLAN氟化物玻璃Er(0.5):ZBLAN的上转换发光。为了清楚地了解上转换,还测量了吸收光谱和共荧光光谱。发现有7条强上转换发光线(406.97〜m,410.42nm),(521.97〜m,527.56 nm),(542.38〜m,549.27 nm),(654.27〜m,665.70 nm),801.57 〜m nm,819.46 nm和840.00 nm,可以识别为(〜2G〜4F〜2H)_(9/2)→〜4I_(15/2)〜2H_(11/2)→的荧光跃迁〜4I_(15/2),〜4S_(3/2)→〜4I_(15/2),〜4F_(9/2)→〜4I_(15/2)〜4I_(9/2)→〜4I_( 15/2)(〜2G〜4F〜2H)_(9/2)→〜4I_(9/2)和〜4S_(3/2)→〜4I_(13/2)。同时,小的向上转换荧光线379.20nm,453.10nm和490.60nm是〜4G_(11/2)→〜4I_(15/2),〜4F_(5/2)→〜4I_(15 / 2)和〜4F_(7/2)→〜4I_(15/2)。有趣的是,log F-logP曲线的斜率,即上转换发光强度F与激光功率P的双对数变化,对于这些观察到的上转换发光是互不相同的,这对于体积显示是有价值的。综合讨论发现〜4G_(11/2)→〜4I_(15/2),(〜2G〜4F〜2H)_(9/2)→〜4I_(15/2),(〜2H_(11 / 2)→〜4I_(15/2),〜4S_(3/2)→〜4I_(15/2),〜4F_(9/2)→〜4I_(15/2))和〜4I_(9 / 2)→〜4I_(15/2)上转换发光分别是五光子,四光子,三光子和两光子上转换发光。还发现从基态〜4I_(15/2)能级到〜4I_(13/2)能级的吸收非常大,这有利于发生顺序的能量转移上转换。

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