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Effect of network modifiers on spectroscopic properties of Sm3+ ions doped gallium silicate glasses

In this work, the glass 42AO-7Nb2O5-21Ga2O3–29SiO2-1Sm2O3(A = Ca,Sr,Ba) are prepared by the conventional melt quenching technique. The effects of modifiers on the glass network structure and luminescence properties were investigated by XRD, Raman spectroscopy, spectrophotometry, and J-O theory, resp...

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Bibliographic Details
Published in:Optical materials 2024-06, Vol.152, p.115445, Article 115445
Main Authors: Hong, Zhi, Lin, Zikang, Yue, Haodong, Luo, Xin, Hou, HaiLan, Lai, Fengqin, Wang, Wei, You, Weixiong, Huang, Jianhui
Format: Article
Language:English
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Summary:In this work, the glass 42AO-7Nb2O5-21Ga2O3–29SiO2-1Sm2O3(A = Ca,Sr,Ba) are prepared by the conventional melt quenching technique. The effects of modifiers on the glass network structure and luminescence properties were investigated by XRD, Raman spectroscopy, spectrophotometry, and J-O theory, respectively. The J-O intensity parameters which were calculated though the absorption spectra were used to evaluate the laser parameters such as the radiative excursion probability of Sm3+ ions in different samples at each energy level, the emission cross section, the radiative lifetime, and the optical gain parameter. When BaO is used as a network modifier, the emission cross section is maximized at the 4G5/2 → 6H7/2 transition, with σem = 9.47 × 10−22 cm2. The experiments results reveal that altering the network modifier can effectively improves the laser emission performance of the samples, and the Sm3+ ions doped gallium silicate glasses has prospective applications in solid state orange lasers. [Display omitted] •A novel glass 42AO-7Nb2O5-21Ga2O3–29SiO2-1Sm2O3(A = Ca,Sr,Ba) was prepared.•The influence of network modifier's cation radius on the wave number of Raman peak is small, but the peak intensity increases with the increase of cation radius.•Sm3+ ions doped gallium silicate glasses has prospective applications in solid state orange lasers.
ISSN:0925-3467
1873-1252
DOI:10.1016/j.optmat.2024.115445