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首页> 外文期刊>Journal of Physics. Condensed Matter >Origin of broad NIR photoluminescence in bismuthate glass and Bi-doped glasses at room temperature
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Origin of broad NIR photoluminescence in bismuthate glass and Bi-doped glasses at room temperature

机译:铋酸盐玻璃和双掺杂玻璃在室温下广泛的NIR光致发光的起源

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摘要

Bi-doped glasses with broadband photoluminescence in the near-infrared (NIR) spectral range are presently receiving significant consideration for potential applications in telecommunications, widely tunable fiber lasers and spectral converters. However, the origin of NIR emission remains disputed. Here, we report on NIR absorption and emission properties of bismuthate glass and their dependence on the melting temperature. Results clarify that NIR emission occurs from the same centers as it does in Bi-doped glasses. The dependence of absorption and NIR emission of bismuthate glasses on the melting temperature is interpreted as thermal dissociation of Bi_2O_3 into elementary Bi. Darkening of bismuthate glass melted at 1300 __ is due to the agglomeration of Bi atoms. The presence of Bi nanoparticles is confirmed by transmission electron microscopy, high-resolution energy dispersive x-ray spectroscopy and element distribution mapping. By adding antimony oxide as an oxidation agent to the glass, NIR emission centers can be eliminated and Bi~(3+) is formed. By comparing with atomic spectral data, absorption bands at__320 ,__500 , 700 , 800 and 1000 nm observed in Bi-doped glasses are assigned to Bi~0 transitions ~4S_(3/2)_ú ~2P_(3/2), ~4S_(3/2) _ú~2P_(1/2), ~4S_(3/2)_ú~2D_(5/2), ~4S_(3/2)_ú~2D_(3/2)(2) and ~4S_(3/2)_ú~2D_(3/2)(1), respectively, and broadband NIR emission is assigned to the transition ~2D_(3/2)(1)_ú~4S_(3/2).
机译:目前,在电信,可广泛调谐的光纤激光器和光谱转换器中的潜在应用中,具有近红外(NIR)光谱范围的宽带光致发​​光的双掺杂玻璃正在受到广泛的考虑。但是,近红外发射的起源仍存在争议。在这里,我们报道了铋酸盐玻璃的近红外吸收和发射特性及其对熔融温度的依赖性。结果表明,NIR发射发生在与Bi掺杂玻璃相同的中心。铋酸盐玻璃的吸收和NIR发射与熔融温度的相关性被解释为Bi_2O_3热解离为基本Bi。在1300℃熔化的铋酸盐玻璃变黑是由于Bi原子的团聚。通过透射电子显微镜,高分辨率能量色散X射线光谱法和元素分布图确认了Bi纳米粒子的存在。通过向玻璃中添加氧化锑作为氧化剂,可以消除NIR发射中心并形成Bi〜(3+)。通过与原子光谱数据比较,将在Bi掺杂玻璃中观察到的在__320,__ 500,700,800和800 nm处的吸收带分配给Bi〜0跃迁〜4S_(3/2)_ú〜2P_(3/2),〜4S_ (3/2)_ú〜2P_(1/2),〜4S_(3/2)_ú〜2D_(5/2),〜4S_(3/2)_ú〜2D_(3/2)(2)和〜分别将4S_(3/2)_ú〜2D_(3/2)(1)和宽带NIR发射分配给过渡〜2D_(3/2)(1)_ú〜4S_(3/2)。

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