Cargando…
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...
Autores principales: | , , , , |
---|---|
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 |
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. |
---|