Overtone generation in a supersonic chemical HF laser with an external cavity

V. P. Averjanov; O. B. Danilov; A. P. Zhevlakov; M. I. Ivanovskaja; D. O. Leschenko; S. A. Tulsky; A. A. Belajev; A. A. Belajev; V. G. Karelsky; V. G. Karelsky; P. G. Ljashedko; P. G. Ljashedko; J. P. Maksimov; J. P. Maksimov

Conference on Lasers and Electro-Optics
OSA Technical Digest (Optica Publishing Group, 1995),
paper CMJ7

Overtone generation in a supersonic chemical HF laser with an external cavity

V. P. Averjanov, O. B. Danilov, A. P. Zhevlakov, M. I. Ivanovskaja, D. O. Leschenko, S. A. Tulsky, A. A. Belajev, V. G. Karelsky, P. G. Ljashedko, and J. P. Maksimov

Conference on Lasers and Electro-Optics 1995

Baltimore, Maryland United States
21–26 May 1995
ISBN: 1-55752-400-9

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Infrared Gas Lasers (CMJ)

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V. P. Averjanov, O. B. Danilov, A. P. Zhevlakov, M. I. Ivanovskaja, D. O. Leschenko, S. A. Tulsky, A. A. Belajev, V. G. Karelsky, P. G. Ljashedko, and J. P. Maksimov, "Overtone generation in a supersonic chemical HF laser with an external cavity," in Conference on Lasers and Electro-Optics, T. Deutsch, J. Goldsmith, D. Killinger, and G. Valley, eds., Vol. 15 of OSA Technical Digest (Optica Publishing Group, 1995), paper CMJ7.

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Abstract

Usually, cavity mirrors are placed into the reactor chamber in overtone supersonic HF lasers. For suppression of fundamental-component generation, a three-or four-cavity mirror scheme with a broken axis is used. The reflection coefficient of these mirrors at λ = 2.6–3.0 μm is less by factor of 100 than at λ = 1.3–1.4 μm.

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