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首页> 外文期刊>RSC Advances >Nanosized (Y1?xGdx)2O2S:Tb3+ particles: synthesis, photoluminescence, cathodoluminescence studies and a model for energy transfer in establishing the roles of Tb3+ and Gd3+
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Nanosized (Y1?xGdx)2O2S:Tb3+ particles: synthesis, photoluminescence, cathodoluminescence studies and a model for energy transfer in establishing the roles of Tb3+ and Gd3+

机译:纳米(Y1?XGDX)2O2s:Tb3 +颗粒:合成,光致发光,阴极发光研究和能量转移模型,用于建立TB3 +和GD3 +的作用

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Herein we describe the synthesis and spectral analysis of nanosized (Y _(1? x ) Gd _( x ) ) _(2) O _(2) S:Tb ~(3+) phosphors between x = 0 and x = 1 with 0.1 and 2 mol% Tb ~(3+) . The concentration of Gd ~(3+) was varied in steps of 0.1 (mole ratio Gd ~(3+) ). X-ray diffraction analyses confirmed the purity and composition of the phosphor materials. The photoluminescence spectra of the series of phosphors with 0.1 mol% Tb ~(3+) showed a colour change of the fluorescence light from blue to green when x was increased from 0 to 1, whereas the samples of the series with 2 mol% Tb ~(3+) yielded essentially green light. These phenomena could be explained in terms of energy transfer from the Tb ~(3+ 5) D _(3) -level at 26?316 cm ~(?1) to the CT-minimum of (Y _(1? x ) Gd _( x ) ) _(2) O _(2) S:Tb ~(3+) for the series with 0.1 mol% Tb ~(3+) , while for the series with 2 mol% Tb ~(3+) cross relaxation between the ~(5) D _(3) , ~(7) F _( J ) and ~(5) D _(4) levels of Tb ~(3+) caused additional depopulation of the ~(5) D _(3) -level at low Gd ~(3+) concentrations. Cathodoluminescence spectra recorded at temperatures between ?170 °C and 20 °C confirmed the proposed energy flow and enabled the evaluation of the energy barrier for this energy flow. By modelling the energy flow we were able to show that the concentration of Gd ~(3+) is critical in controlling the change in colour of the (Y _(1? x ) Gd _( x ) ) _(2) O _(2) S:Tb ~(3+) for the series with 0.1 mol% and that the presence of just over x = 0.1 of Gd ~(3+) is enough to switch to the energy transfer route present in the x = 1.0 parent phosphor. In addition the charge transfer band of (Y _(1? x ) Gd _( x ) ) _(2) O _(2) S:Tb ~(3+) showed a red shift of about 6 nm upon increasing x from 0 to 1. This red shift has been described in terms of an electrostatic model that enabled a calculation of the rearrangement of the electrons during the charge transfer.
机译:在此,我们描述了纳米化的合成和光谱分析(Y _(1?x)gd _(x))_(2)o _(2)s:tb〜(3+)荧光体x = 0和x = 1之间0.1和2mol%Tb〜(3+)。 Gd〜(3+)的浓度以0.1的步骤变化(摩尔比Gd〜(3+))。 X射线衍射分析证实了磷光体材料的纯度和组成。当X从0到1增加时,具有0.1mol%Tb〜(3+)的荧光体的一系列荧光粉的光致发光光谱显示出从蓝色到绿色的荧光的颜色变化,而X系列的样品为2摩尔%TB 〜(3+)产生基本绿灯。这些现象可以在从TB〜(3+ 5)D _(3) - 在26Ω·316cm〜(α1)处的能量转移到(y_(1≤x)的ct-minum gd _(x))_(2)o _(2)S:Tb〜(3+)的系列,0.1mol%Tb〜(3+),同时为2 mol%Tb〜(3+ )〜(5)d _(3),〜(7)f _(j)和〜(5)d _(4)水平的Tb〜(3+)之间的交叉弛豫导致〜(5 )D _(3) - 低Gd〜(3+)浓度的玻璃。在Δ170℃和20°C之间的温度下记录的阴极发光光谱确认了所提出的能量流,并使能该能量流动的能量屏障进行评估。通过建模能量流,我们能够表明GD〜(3+)的浓度在控制(Y _(1≤x)Gd _(x))_(2)O _的颜色变化方面是至关重要的(2)S:TB〜(3+)对于0.1摩尔%的系列,并且刚刚x = 0.1的Gd〜(3+)的存在足以切换到x = 1.0中存在的能量转移路线亲本磷光体。此外,(Y _(1≤x)gd _(x))_(2)o _(2)s:tb〜(3+)在增加x时显示为约6nm的红色偏移0至1。已经根据静电模型描述了这种红色移位,该静电模型能够在电荷转移期间能够计算电子的重新排列。

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