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作 者:夏海平[1] 林琼斐[1] 王金浩[1] 张约品[1] 杨钢锋[2] 张勤远[2]
机构地区:[1]宁波大学光电子功能材料重点实验室,宁波315211 [2]华南理工大学光通信材料研究所,特种功能材料教育部重点实验室,广州510640
出 处:《武汉理工大学学报》2007年第E01期264-268,共5页Journal of Wuhan University of Technology
基 金:浙江省自然科学基金(Y406220)和宁波市博士基金(2005A610010,2005610023)
摘 要:用高温熔融法制备了不同Tm^3+浓度掺杂的65GeO2—12AlF3—8Li2O-10BaF2—5La2O3-xTm2O3(x=0.5mol%,1.0mol%,2.0mol%,4.0mol%,6.0mol%)玻璃。从吸收光谱特性出发,根据Judd—Ofelt理论,计算得到了Tm^3+离子的J—O强度参数(Ω2,Ω4,Ω6)及Tm^3+离子各激发能级的自发跃迁几率、荧光分支比以及辐射寿命等光谱参量。在808nm波长的激发下,研究了不同Tm^3+掺杂浓度下玻璃在~1.47μm与~1.8μm处的荧光特性,在掺杂浓度约达到.1.0mol%时,在1.8μm处的荧光强度达最大,然后随着掺杂浓度的增大,其荧光强度反而降低。作者从Tm^3+的交叉驰豫与浓度猝灭效应解释了这一荧光强度变化的过程。Glasses with the compositions of 65GeO2-12AlF3-8Li2O-10BaF2-5La2O3 doped with different Tm^3+ concentration (0.5,1.0,2.0,4.0,6.0 mol % ) were fabricated by conventional melting method. According to the absorption spectra and the Judd-Ofelt theory, the J-O strength parameters(Ω2, Ω4,Ω6) were calculated, by which the radiative transition probabilities, branching ratios and radiative lifetimes were obtained. The infrared emission spectra (with 808nm LD excitation) at -- 1.47 μm and --1.8 μm of various concentration Tm^3+ -doped glasses were studied. The emission intensity at ~ 1.8 μm reaches to the maximum when the Tm^3+ -doping concentration is near to be 1.0 mol% and then decreases at higher concentration. The mechanism of the change of the fluorescence intensity was explained from the cross-relaxation effect and the concentration quenching of Tm^3+ effect.
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