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Effect of dopants on laser-induced damage threshold of ZnGeP2 N. N. Yudin, M. M. Zinoviev, V. S. Kuznetsov [et al.]

Contributor(s): Yudin, Nikolay N | Zinoviev, Mikhail M | Kuznetsov, Vladimir S | Slyunko, Elena S | Podzyvalov, Sergey N | Voevodin, Vladimir I | Lysenko, Alexey | Kalsin, Andrey | Shaimerdenova, Leyla K | Baalbaki, Houssain A | Kalygina, Vera MMaterial type: ArticleArticleContent type: Текст Media type: электронный Subject(s): монокристаллы | порог лазерного повреждения | структураGenre/Form: статьи в журналах Online resources: Click here to access online In: Crystals Vol. 13, № 3. P. 440 (1-9)Abstract: The effect of doping Mg, Se, and Ca by diffusion into ZnGeP2 on the optical damage threshold at a wavelength of 2.1 μm has been studied. It has been shown that diffusion-doping with Mg and Se leads to an increase in the laser-induced damage threshold (LIDT) of a single crystal (monocrystal), ZnGeP2; upon annealing at a temperature of 750 °C, the damage threshold of samples doped with Mg and Se increases by 31% and 21% from 2.2 ± 0.1 J/cm2 to 2.9 ± 0.1 and 2.7 ± 0.1 J/cm2, respectively. When ZnGeP2 is doped with Ca, the opposite trend is observed. It has been suggested that the changes in the LIDT depending on the introduced impurity by diffusion can be explained by the creation of additional energy dissipation channels due to the processes of radiative and fast non-radiative relaxation through impurity energy levels, which further requires experimental confirmation.
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The effect of doping Mg, Se, and Ca by diffusion into ZnGeP2 on the optical damage threshold at a wavelength of 2.1 μm has been studied. It has been shown that diffusion-doping with Mg and Se leads to an increase in the laser-induced damage threshold (LIDT) of a single crystal (monocrystal), ZnGeP2; upon annealing at a temperature of 750 °C, the damage threshold of samples doped with Mg and Se increases by 31% and 21% from 2.2 ± 0.1 J/cm2 to 2.9 ± 0.1 and 2.7 ± 0.1 J/cm2, respectively. When ZnGeP2 is doped with Ca, the opposite trend is observed. It has been suggested that the changes in the LIDT depending on the introduced impurity by diffusion can be explained by the creation of additional energy dissipation channels due to the processes of radiative and fast non-radiative relaxation through impurity energy levels, which further requires experimental confirmation.

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