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Er3+/Yb3+共掺碲钨酸盐玻璃的热稳定性和1.5μm波段的光谱性质
引用本文:沈祥,聂秋华,徐铁峰,戴世勋,王训四.Er3+/Yb3+共掺碲钨酸盐玻璃的热稳定性和1.5μm波段的光谱性质[J].发光学报,2006,27(1):36-40.
作者姓名:沈祥  聂秋华  徐铁峰  戴世勋  王训四
作者单位:宁波大学, 信息科学与工程学院, 浙江, 宁波, 315211
基金项目:中国科学院资助项目;浙江省自然科学基金;浙江省科技厅资助项目;宁波大学校科研和教改项目
摘    要:制备了Er3+/Yb3+共掺的碲钨酸盐玻璃样品,TeO2-WO3-RmOn(RmOn=PbO,BaO,La2O3,Bi2O3),研究了样品的热稳定性和1.5μm波段的光谱性质。碲酸盐中引入WO3的目的是为提高基质的声子能量,使Er3+离子4I13/24I15/2的多声子弛豫速率增加,从而提高4I13/2能级上的Er3+离子数,这对提高1.5μm处的荧光强度有利,另外加入WO3也能提高碲酸盐玻璃的抗析晶能力。测试了样品的FT-IR光谱,发现碲钨酸盐玻璃样品中存在着TeO4、TeO3、WO4和WO6结构体。周围环境的不对称性导致Er3+在1.5μm处的光谱有非均匀的展宽和大的受激发射截面。Er3+在70TeO2-20WO3-10Bi2O3玻璃中4I13/24I15/2能级发射的荧光半峰全宽(FWHM)为77nm,应用McCumber理论计算的受激发射截面(σpeak)为1.03×10-20cm2。其FWHM×σpeak乘积远大于掺Er3+的铋酸盐、磷酸盐、碲酸盐和硅酸盐玻璃,说明碲钨酸盐玻璃是一种制备宽带光纤放大器优良基质材料。

关 键 词:光谱性质  Er3+/Yb3+共掺杂  碲钨酸盐玻璃  热稳定性
文章编号:1000-7032(2006)01-0036-05
收稿时间:2004-08-24
修稿时间:2004-08-242004-11-15

Er3+/Yb3+ Codoped Tungsten-tellurite Glasses: the Thermal Stability and Spectral Properties at 1.5 μm Band
SHEN Xiang,NIE Qiu-hua,XU Tie-feng,DAI Shi-xun,WANG Xun-si.Er3+/Yb3+ Codoped Tungsten-tellurite Glasses: the Thermal Stability and Spectral Properties at 1.5 μm Band[J].Chinese Journal of Luminescence,2006,27(1):36-40.
Authors:SHEN Xiang  NIE Qiu-hua  XU Tie-feng  DAI Shi-xun  WANG Xun-si
Institution:Faculty of Information Science and Engineering, Ningbo University, Ningbo 315211, China
Abstract:Er3+/Yb3+ codoped tungsten-tellurite (WT) glasses, TeO2-WO3-RmOn (RmOn =PbO, BaO, La2O3, Bi2O3), were prepared and investigated. WO3 has been introduced in the tellurite glasses due to the following two reasons: The first one is to increase the phonon energy and the multi-phonon relaxation rate of the Er3+:4I11/2→4I13/2 transition, which benefits the population inversion between the 4I13/2 and 4I15/2 level of Er3+. The second is to enhance the thermal stability against crystallization. The structural studies were done through FT-IR spectral analysis and revealed that these glasses contain TeO4, TeO3, WO4 and WO6 units as the local structures. The asymmetry of Er3+ sites results in inhomogeneous broadening of spectra and large emission cross-section at 1.5 μm band. The fluorescence full width at half maximum FWHM=77 nm, and the peak of the emission cross-section σpeak =1.03×10-20 cm2, are manifested in 70TeO2-20WO3-10Bi2O3 glass. The gain bandwidth properties, FWHM×σepeak, of Er3+ in WT glasses have advantages over those of bismuthate, phosphate, tellurite and silicate glasses, indicating the WT glasses are promising host materials for 1.5 μm broadband amplification.
Keywords:spectral properties  Er~(3 ) /Yb~(3 ) codoped  tungsten-tellurite glass  thermal stability
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