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The structural and luminescence properties of strontium borotellurite glass doped with europium and dysprosium

机译:掺and和的硼酸锶锶玻璃的结构和发光性能

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摘要

A series of strontium borotellurite glasses with the general formula xSrO·(100-x)[0.5B2O3·0.5TeO2], (15 = x = 35 mol%) have been prepared. In addition, glass samples with the composition 20SrO·40B2O3·40TeO2 and 30SrO·35B2O3·35TeO2 doped with Europium, Eu3+ and Dysprosium, Dy3+, (1 mol% each) were also prepared. All the glass samples were prepared using melt quenching method, followed by annealing process at 400 oC for 6 hours. The structural property of the glass samples was characterized using X-ray diffractometer (XRD) and Fourier transform infrared spectrometer and the luminescence property using fluorescence spectrometer. The XRD diffraction patterns showed the amorphous phase of the glass sample. Infrared spectra reveals that increased of strontium in borotellurite glass significantly promote conversion of [BO3] to [BO4] and [TeO4] to [TeO3] in the structural units. This conversion indicated some disintegration of boroxol rings into network structures while strontium acted as network modifier. The emission spectra line of undoped and doped glasses is in the visible range. The emission spectra line of undoped glass at 513 nm originated from the glass host. The emission spectra lines from Eu3+ doped glass are due to transition of Eu3+ ion at 5D0?7F0 (580 nm), 5D0?7F1 (593 nm), 5D0?7F2 (613 nm) and 5D0?7F3 (652 nm). Meanwhile the emission spectra lines from Dy3+ doped glass are due to transition from 4F9/2?6H15/2 (483 nm), 4F9/2?6H13/2 (578 nm) and 4F9/2?6H11/2 (660 nm). The emission spectra lines from Eu3+ and Dy3+ doped glass are shown at 483 nm, 513 nm, 578 nm, 613 nm and 660 nm. The results revealed that the emission intensity of Eu3+ and Dy3+ doped glass are dependent on host composition. Furthermore, the luminescence decay curve for Eu3+ doped glass showed multi-exponential decay with lifetimes for 20SBT:1Eu3+ glass are 1 ns and 22 ns, while for 30SBT:1Eu3+ glass, the lifetimes are 1 ns and 18 ns.
机译:制备了一系列通式为xSrO·(100-x)[0.5B2O3·0.5TeO2](15 = x = 35 mol%)的锶硼铁酸盐玻璃。另外,还制备了掺有Euro,Eu3 +和Dy,Dy3 +(各自为1摩尔%)的组成为20SrO·40B2O3·40TeO2和30SrO·35B2O3·35TeO2的玻璃样品。使用熔融淬火方法制备所有玻璃样品,然后在400 oC下退火6小时。使用X射线衍射仪(XRD)和傅立叶变换红外光谱仪表征玻璃样品的结构性能,并使用荧光光谱仪表征玻璃的发光性能。 XRD衍射图显示玻璃样品的非晶相。红外光谱表明,硼碲石玻璃中锶的增加显着促进了结构单元中[BO3]向[BO4]和[TeO4]向[TeO3]的转化。这种转化表明,硼酸环有些分解成网络结构,而锶用作网络改性剂。未掺杂和掺杂的玻璃的发射光谱线在可见范围内。未掺杂玻璃在513 nm处的发射光谱线起源于玻璃主体。 Eu3 +掺杂玻璃的发射光谱线是由于Eu3 +离子在5D0?7F0(580 nm),5D0?7F1(593 nm),5D0?7F2(613 nm)和5D0?7F3(652 nm)的跃迁引起的。同时,来自Dy3 +掺杂玻璃的发射光谱线是由于从4F9 / 2→6H15 / 2(483 nm),4F9 / 2→6H13 / 2(578 nm)和4F9 / 2→6H11 / 2(660 nm)跃迁引起的。掺杂Eu3 +和Dy3 +的玻璃的发射光谱线显示为483 nm,513 nm,578 nm,613 nm和660 nm。结果表明,掺杂Eu3 +和Dy3 +的玻璃的发射强度取决于基质组成。此外,Eu3 +掺杂玻璃的发光衰减曲线显示出多指数衰减,其中20SBT:1Eu3 +玻璃的寿命为1 ns和22 ns,而30SBT:1Eu3 +玻璃的寿命为1 ns和18 ns。

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    Uning Royston;

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  • 年度 2014
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