首页> 外文会议>Optical Components and Materials IV; Proceedings of SPIE-The International Society for Optical Engineering; vol.6469 >Concentration dependence of the fluorescence decay profile in transition metal doped chalcogenide glass
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Concentration dependence of the fluorescence decay profile in transition metal doped chalcogenide glass

机译:过渡金属掺杂硫族化物玻璃中荧光衰减曲线的浓度依赖性

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In this paper we present the fluorescence decay profiles of vanadium and titanium doped gallium lanthanum sulphide (GLS) glass at various doping concentrations between 0.01 and 1% (molar). We demonstrate that below a critical doping concentration the fluorescence decay profile can be fitted with the stretched exponential function: exp[-(t/τ)~β], where τ is the fluorescence lifetime and (β is the stretch factor. At low concentrations the lifetime for vanadium and titanium doped GLS was 30 μs and 67 μs respectively. We validate the use of the stretched exponential model and discuss the possible microscopic phenomenon it arises from. We also demonstrate that above a critical doping concentration of around 0.1% (molar) the fluorescence decay profile can be fitted with the double exponential function: a~*exp-(t/τ_1)+ b~*exp-(t/τ_2), where τ_1and τ_2 are characteristic fast and slow components of the fluorescence decay profile, for vanadium the fast and slow components are 5 μs and 30 μs respectively and for titanium they are 15 μs and 67 μs respectively. We also show that the fluorescence lifetime of vanadium and titanium at low concentrations in the oxide rich host gallium lanthanum oxy-sulphide (GLSO) is 43 μs and 97 μs respectively, which is longer than that in GLS. From this we deduce that vanadium and titanium fluorescing ions preferentially substitute into high efficiency oxide sites until at a critical concentration they become saturated and low efficiency sulphide sites start to be filled.
机译:在本文中,我们介绍了在0.01和1%(摩尔)之间不同掺杂浓度下,钒和钛掺杂的镓镧镧硫化物(GLS)玻璃的荧光衰减曲线。我们证明,在临界掺杂浓度以下,荧光衰减曲线可以与拉伸的指数函数拟合:exp [-(t /τ)〜β],其中τ是荧光寿命,(β是拉伸因子。在低浓度下钒和钛掺杂的GLS的寿命分别为30μs和67μs。我们验证了拉伸指数模型的使用并讨论了由此产生的微观现象。我们还证明,高于临界掺杂浓度约0.1%(摩尔)荧光衰减轮廓可以拟合双指数函数:a〜* exp-(t /τ_1)+ b〜* exp-(t /τ_2),其中τ_1和τ_2是荧光衰减轮廓的特征快和慢分量钒的快速和慢速成分分别为5μs和30μs,钛的分别为15μs和67μs。我们还表明,在富氧化物的主体镓l中,低浓度时钒和钛的荧光寿命硫化亚锡(GLSO)分别为43μs和97μs,比GLS中的更长。由此我们可以得出结论,钒和钛发出的荧光离子优先取代成高效氧化物位点,直到在临界浓度下它们变为饱和并且低效硫化物位点开始被填充。

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