Investigation of spectroscopy and the dual energy transfer mechanisms of Sm3+-doped telluroborate glasses

•Quenching effect of Sm3+ relates to energy transfer by dipole-dipole interaction.•Inokuti-Hirayama model is suitable for estimating energy transfer parameter.•Sm3+ concentration influences on energy transfer probability and lifetime value.•The luminescence intensity increases with increasing of tem...

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Published inOptical materials Vol. 55; pp. 62 - 67
Main Authors Van Do, Phan, Tuyen, Vu Phi, Quang, Vu Xuan, Hung, Le Xuan, Thanh, Luong Duy, Ngoc, Tran, Van Tam, Ngo, Huy, Bui The
Format Journal Article
LanguageEnglish
Published Elsevier B.V 01.05.2016
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Summary:•Quenching effect of Sm3+ relates to energy transfer by dipole-dipole interaction.•Inokuti-Hirayama model is suitable for estimating energy transfer parameter.•Sm3+ concentration influences on energy transfer probability and lifetime value.•The luminescence intensity increases with increasing of temperature.•The energy transfer between NBO-intrinsic defects and the Sm3+ ions. The absorption, luminescence, Raman spectra and lifetimes of Sm-doped alkali telluroborate glasses (TB glasses) TB:Sm3+ have been investigated. The dual energy transfers including energy transfer between Sm3+ - Sm3+ pairs and Sm3+ - non-bridging oxygen (NBO) intrinsic defects were investigated. The concentration quenching of luminescence intensity was explained by the non-radiative energy transfer between the Sm3+ ions through the cross-relaxation mechanism. The decay curves are single exponentials with low concentrations (lower 0.10mol%) and become non-exponentials at higher concentrations. The non-exponential decay curves are fitted to the Inokuti and Hirayama model to give the energy transfer parameters between Sm3+ ions. The dominant interaction mechanism for energy transfer process is dipole–dipole interaction. The energy transfer induced Sm3+ photoluminescence enhancement in tellurite glass was experimentally studied and confirmed.
ISSN:0925-3467
1873-1252
DOI:10.1016/j.optmat.2016.03.023