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Highly Er^3 +/Yb^3+ Co-Doped Fluoroaluminate Glasses for Microchip Laser at 1.54μm
引用本文:张军杰,戴世勋,徐时清,汪国年,张丽艳,胡丽丽.Highly Er^3 +/Yb^3+ Co-Doped Fluoroaluminate Glasses for Microchip Laser at 1.54μm[J].中国稀土学报(英文版),2004,22(4):447-451.
作者姓名:张军杰  戴世勋  徐时清  汪国年  张丽艳  胡丽丽
作者单位:ShanghaiInstituteofOpticsandFineMechanics,ChineseAcademyofScience,Shanghai201800,China
基金项目:Projectsupportedbythe“Qimingxing”Project( 0 4QMX14 48)ofShanghaiMunicipalScienceandTechnologyCommissionand theNationalScienceFoundationofChina ( 60 2 0 70 0 6)andOpticalScienceandTechnologyofShanghai ( 0 2 2 2 610 46)
摘    要:A series of highly Er^3 /Yb^3 co-doped fluoroaluminate glasses were investigated in order to develop a microchip laser at 1.54μm under 980nm excitation. Measurements of absorption, emission and up-conversion spectra were performed to examine the effect of concentration quenching on spectroscopic properties. In the glasses with Er^3 concentrations below 10% (mol fraction), concentration quenching is low and the Er^3 /Yb^3 co-doped fluoroaluminate glasses gave stronger fluorescence of 1.54μm from the 4113/2→^4I15/2 transition than those of Er^3 singly-doped glasses. In the glass with Er^3 concentrations above 10%, concentration quenching of 1.54μm obviously occurs more than that of the Er^3 singly-doped samples because of the back energy-transfer from Er^3 to Yb^3 . To obtain the highest emission efficien-cy at 1.54μm, the optimum doping-concentration ratio of Er^3 /Yb^3 is found to be approximately 1 : 1 in mol fraction when the Er^3 concentration is less than 10%.

关 键 词:Er^3+  Yb^3+  微芯片激光器  激光振荡器  稀土元素  Fluoroaluminate玻璃
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