Optical Spectra and Gain Properties of Ho3+/Pr3+ Co-doped LiYF4 Crystal

The LiYF4 single crystals singly doped Ho3+ and co-doped Ho3+, Pr3+ ions were grown by a modified Bridgman method. The Judd-Ofelt strength parameters (Ω2, Ω4, Ω6) of No3+ were calculated according to the absorption spectra and the Judd-Ofelt theory, by which the radiative transition probabilities (A...

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Published inJournal of materials science & technology Vol. 30; no. 9; pp. 910 - 916
Main Authors Peng, Jiangtao, Xia, Haiping, Wang, Peiyuan, Hu, Haoyang, Tang, Lei, Zhang, Yuepin, Jiang, Haochuan, Chen, Baojiu
Format Journal Article
LanguageEnglish
Published Elsevier Ltd 01.09.2014
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Summary:The LiYF4 single crystals singly doped Ho3+ and co-doped Ho3+, Pr3+ ions were grown by a modified Bridgman method. The Judd-Ofelt strength parameters (Ω2, Ω4, Ω6) of No3+ were calculated according to the absorption spectra and the Judd-Ofelt theory, by which the radiative transition probabilities (A), fluorescence branching ratios (β) and radiative lifetime (τ rad) were obtained. The radiative lifetimes of 5/6 and 5/7 levels in Ho3+ (1 mol%):LiYF4 are 10.89 and 20.19 ms, respectively, while 9.77 and 18.50 ms in Ho3+/pr3+ doped crystals. Hence, the τ rad of 5/7 level decreases significantly by introduction of Pr3+ into Ho3+:LiYF4 crystal which is beneficial to the emission of 2.9 μm. The maximum emission cross section of Ho3+:LiYF4 crystal located at 2.05 μm calculated by McCumber theory is 0.51 ×10-20 cm2 which is compared with other crystals. The maximum emission cross section at 2948 nm in Ho3+/pr3+ co-doped LiYF4 crystal obtained by Fuchtbauer- Ladenburg theory is 0.68 × 10-20 cm2, and is larger than the value of 0.53 × 10-20 cm2 in Ho3+ singly doped LiYF4 crystal. Based on the absorption and emission cross section spectra, the gain cross section spectra were calculated. In the Ho3- ions singly doped LiYF4 crystal, the gain cross sections for 2.05 μm infrared emission becomes positive once the population inversion level reaches 30%. It means that the pump threshold for obtaining 2.05 μm laser is probably lower which is an advantage for Ho3+-doped LiYF4 2.05 μm infrared lasers. The calculated gain cross section for 2.9 μm mid-infrared emission does not become positive until the population inversion level reaches 40% in Ho3+/pr3+:LiYF4 crystal, but 50% in Ho3+ singly doped LiYF4 crystal, indicating that a low pumping threshold is achieved for the H03+:5/6 → 5/7 laser operation with the introduction of Pr3+ ions. It was also demonstrated that Pr3+ ion can deplete rapidly the lower laser Ho3+:5/7 level and has influence on the Ho3+:5/6 level. The Ho3+/pr3+:LiYF4 crystal may be a potential media for 2.9 μm mid-infrared laser.
Bibliography:21-1315/TG
The LiYF4 single crystals singly doped Ho3+ and co-doped Ho3+, Pr3+ ions were grown by a modified Bridgman method. The Judd-Ofelt strength parameters (Ω2, Ω4, Ω6) of No3+ were calculated according to the absorption spectra and the Judd-Ofelt theory, by which the radiative transition probabilities (A), fluorescence branching ratios (β) and radiative lifetime (τ rad) were obtained. The radiative lifetimes of 5/6 and 5/7 levels in Ho3+ (1 mol%):LiYF4 are 10.89 and 20.19 ms, respectively, while 9.77 and 18.50 ms in Ho3+/pr3+ doped crystals. Hence, the τ rad of 5/7 level decreases significantly by introduction of Pr3+ into Ho3+:LiYF4 crystal which is beneficial to the emission of 2.9 μm. The maximum emission cross section of Ho3+:LiYF4 crystal located at 2.05 μm calculated by McCumber theory is 0.51 ×10-20 cm2 which is compared with other crystals. The maximum emission cross section at 2948 nm in Ho3+/pr3+ co-doped LiYF4 crystal obtained by Fuchtbauer- Ladenburg theory is 0.68 × 10-20 cm2, and is larger than the value of 0.53 × 10-20 cm2 in Ho3+ singly doped LiYF4 crystal. Based on the absorption and emission cross section spectra, the gain cross section spectra were calculated. In the Ho3- ions singly doped LiYF4 crystal, the gain cross sections for 2.05 μm infrared emission becomes positive once the population inversion level reaches 30%. It means that the pump threshold for obtaining 2.05 μm laser is probably lower which is an advantage for Ho3+-doped LiYF4 2.05 μm infrared lasers. The calculated gain cross section for 2.9 μm mid-infrared emission does not become positive until the population inversion level reaches 40% in Ho3+/pr3+:LiYF4 crystal, but 50% in Ho3+ singly doped LiYF4 crystal, indicating that a low pumping threshold is achieved for the H03+:5/6 → 5/7 laser operation with the introduction of Pr3+ ions. It was also demonstrated that Pr3+ ion can deplete rapidly the lower laser Ho3+:5/7 level and has influence on the Ho3+:5/6 level. The Ho3+/pr3+:LiYF4 crystal may be a potential media for 2.9 μm mid-infrared laser.
LiYF4 crystal; 2.9 μm; Ho3/pr3+; Optical spectra; Gain cross section
ISSN:1005-0302
1941-1162
DOI:10.1016/j.jmst.2013.09.014