简介概要

Highly Er3+/Yb3+ Co-Doped Fluoroaluminate Glasses for Microchip Laser at 1.54 μm

来源期刊:JOURNAL OF RARE EARTHS2004年第4期

论文作者:胡丽丽 汪国年 徐时清 张丽艳 张军杰 戴世勋

Key words:microchip laser; fluoroaluminate glasses; 1.54 μm; rare earths;

Abstract: A series of highly Er3+/Yb3+ co-doped fluoroaluminate glasses were investigated in order to develop a microchip laser at 1.54 μm under 980 nm 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 Er3+ concentrations below 10% (mol fraction), concentration quenching is low and the Er3+/Yb3+ co-doped fluoroaluminate glasses gave stronger fluorescence of 1.54 μm from the 4I13/2→ 4I15/2 transition than those of Er3+ singly-doped glasses. In the glass with Er3+ concentrations above 10%, concentration quenching of 1.54 μm obviously occurs more than that of the Er3+ singly-doped samples because of the back energy-transfer from Er3+ to Yb3+. To obtain the highest emission efficiency at 1.54 μm, the optimum in mol fraction when the Er3+ concentration is less than 10%.

详情信息展示

Highly Er3+/Yb3+ Co-Doped Fluoroaluminate Glasses for Microchip Laser at 1.54 μm

胡丽丽1,汪国年1,徐时清1,张丽艳1,张军杰1,戴世勋1

(1.Shanghai Institute of Optics and Fine Mechanics,Chinese Academy of Science,Shanghai 201800,China)

Abstract:A series of highly Er3+/Yb3+ co-doped fluoroaluminate glasses were investigated in order to develop a microchip laser at 1.54 μm under 980 nm 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 Er3+ concentrations below 10% (mol fraction), concentration quenching is low and the Er3+/Yb3+ co-doped fluoroaluminate glasses gave stronger fluorescence of 1.54 μm from the 4I13/2→ 4I15/2 transition than those of Er3+ singly-doped glasses. In the glass with Er3+ concentrations above 10%, concentration quenching of 1.54 μm obviously occurs more than that of the Er3+ singly-doped samples because of the back energy-transfer from Er3+ to Yb3+. To obtain the highest emission efficiency at 1.54 μm, the optimum in mol fraction when the Er3+ concentration is less than 10%.

Key words:microchip laser; fluoroaluminate glasses; 1.54 μm; rare earths;

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