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Radiative and non-radiative transitions of excited Ti(3+) cations in sapphire

We have measured the fluorescence quantum efficiency in Ti(3+):sapphire single crystals between 150 K and 550 K. Using literature-given effective fluorescence lifetime temperature dependence, we show that the zero temperature radiative lifetime is (4.44 ± 0.04) μs, compared to the 3.85 μs of the flu...

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Detalles Bibliográficos
Autores principales: Shirakov, Avry, Burshtein, Zeev, Shimony, Yehoshua, Frumker, Eugene, Ishaaya, Amiel A.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group UK 2019
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6906470/
https://www.ncbi.nlm.nih.gov/pubmed/31827182
http://dx.doi.org/10.1038/s41598-019-55267-8
Descripción
Sumario:We have measured the fluorescence quantum efficiency in Ti(3+):sapphire single crystals between 150 K and 550 K. Using literature-given effective fluorescence lifetime temperature dependence, we show that the zero temperature radiative lifetime is (4.44 ± 0.04) μs, compared to the 3.85 μs of the fluorescence lifetime. Fluorescence lifetime thermal shortening resolves into two parallel effects: radiative lifetime shortening, and non-radiative transition rate enhancement. The first is due to thermally enhanced occupation of a ΔE = 1,700 cm(−1) higher (top) electronic state of the upper multiplet, exhibiting a transition oscillator strength of f = 0.62, compared to only 0.013 of the bottom electronic state of the same multiplet. The non-radiative rate relates to multi-phonon decay transitions stimulated by the thermal phonon occupation. Thermal enhancement of the configuration potential anharmonicity is also observed. An empiric expression for the figure-of-anharmonicity temperature dependence is given as [Formula: see text] (T) = [Formula: see text] (0)(1 + β exp(−ℏω(co) /k(B)T )), where [Formula: see text] (0) = 0.276, β = 5.2, ℏω(co) = 908 cm(−1), and k(B) is the Boltzmann constant.