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Yb3+/Er3+共掺杂TeO2-WO3-ZnO玻璃的光谱性质
引用本文:李家成,李顺光,胡和方,干福熹.Yb3+/Er3+共掺杂TeO2-WO3-ZnO玻璃的光谱性质[J].发光学报,2004,25(5):495-500.
作者姓名:李家成  李顺光  胡和方  干福熹
作者单位:1. 中国科学院上海光学精密机械研究所, 上海 201800;2. 中国科学院上海光学精密机械研究所, 北京 100039
摘    要:制备了Yb3+/Er3+共掺杂的TeO2-WO3-ZnO玻璃,测量了Er3+在玻璃中的吸收光谱和970nmLD激发下的荧光光谱、荧光寿命和上转换光谱.计算了Yb3+/Er3+间的能量传递效率和Er3+离子1.5μm波段的吸收截面、发射截面,并研究了其荧光强度和上转换发光与Yb3+掺杂浓度间的关系.结果表明,Yb3+共掺杂可明显提高Er3+离子1.5μm发射的荧光强度,实验所得Yb3+离子的最佳掺杂浓度为Er3+离子浓度的3倍,在7.28×1020ions/cm3左右.Er3+离子1.5μm发射的荧光半峰全宽为67~72nm;上转换红、绿光均为双光子过程,随Yb3+掺杂浓度的增加,上转换红、绿光强度均增强.

关 键 词:Yb3+/Er3+共掺杂  碲钨酸盐玻璃  光谱性质  上转换发光
文章编号:1000-7032(2004)05-0495-06
收稿时间:2003-06-20
修稿时间:2003年6月20日

Spectroscopic Properties of Yb3 +/Er3 + -Codoped TeO2-WO3-ZnO Glasses
LI Jia-cheng.Spectroscopic Properties of Yb3 +/Er3 + -Codoped TeO2-WO3-ZnO Glasses[J].Chinese Journal of Luminescence,2004,25(5):495-500.
Authors:LI Jia-cheng
Institution:1. Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China;2. Graduate School of Chinese Academy of Sciences, Beijing 100039, China
Abstract:Tellurite glass has attracted considerable attention and development effort as a host for broad EDFA and EDWA.But the phonon energy of tellurite glass is relatively low as 770 cm-1,thus,the4I11/24I13/2 nonradiative decay is too slow to allow pumping at 980 nm.Tungsten-tellurite glass has higher phonon energy of 930 cm-1,which makes it possible pumping at 980 nm.The 1.5 μm emission bandwidth of Er3+ in tungsten-tellurite glass is also broad.The spectroscopic properties of Yb3+/Er3+-codoped TeO2-WO3-ZnO (TWZ) glasses were investigated,too. The Yb3+/Er3+-codoped TWZ glasses were prepared by traditional melting-quenching method.The absorption cross-section was calculated based on measured absorption spectra at room temperature.The emission cross-section was calculated by McCumber theory.The peak values of absorption cross-section and emission cross-section at 1.5 μm are 0.78 pm2 and 0.90 pm2,respectively.The 1.5 μm emission spectra,upconversion emission spectra and fluorescence lifetimes of Er3+,excited at 970 nm,were also measured.The dependence of Yb3+ doping concentration on the 1.5 μm emission and upconversion luminescence of Er3+ was studied.The calculated energy transfer efficiency from Yb3+ to Er3+ in Yb3+/Er3+-codoped TWZ glasses is about 65%.Yb3+-codoping can enhance the 1.5 μm emission intensity effectively.The optimum Yb3+ doping concentration is about 7.28×1020 ions/cm3,which is triple of the Er3+ doping concentration.The emission bandwidths of Er3+ at 1.5 μm in Yb3+/Er3+-codoped TWZ glasses are broad and the obtained full width at half maximum is between 67 nm and 72 nm.Three upconversion emission bands centered at about 533,547 and 668 nm,were observed.The three emission bands originate from the radiative transitions2H11/24I15/2,4S3/24I15/2 and4F9/24I15/2,respectively.The green and red upconversion emission are both double-photon process.With the increasing of Yb3+ doping concentration,the green and red upconversion emission intensity both increase.This can be ascribed to the increased energy transfer rate from Yb3+ to Er3+.
Keywords:Yb~(3+)/Er~(3+)-codoped  tungsten-tellurite glass  spectroscopic properties  upconversion emission
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