Switching of the emission wavelength of a helium-neon laser in the 3.39 μ region

The emission switched from the lambda$sub 0$=3.3922 $mu$ 5s'1/2$sup 0$$sub 1$--4p' 3/2$sub 2$(3s$sub 2$--3p$sub 4$) line to the lambda$sub 1$=3.3912 $mu$ 5s'1/2$sup 0$$sub 1$--4p'1/2$sub 1$(3s$sub 2$--3p$sub 2$) line in such a way as to maximize the power at the lambda$sub 1$ wav...

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Veröffentlicht in:Sov. J. Quant. Electron. (Engl. Transl.), v. 5, no. 2, pp. 230-231 v. 5, no. 2, pp. 230-231, 1975-02, Vol.5 (2), p.230-231
Hauptverfasser: Balakin, V A, Konovalov, I P, Ocheretyanyi, A I, Popov, A I, Protsenko, E D
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Sprache:eng
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Zusammenfassung:The emission switched from the lambda$sub 0$=3.3922 $mu$ 5s'1/2$sup 0$$sub 1$--4p' 3/2$sub 2$(3s$sub 2$--3p$sub 4$) line to the lambda$sub 1$=3.3912 $mu$ 5s'1/2$sup 0$$sub 1$--4p'1/2$sub 1$(3s$sub 2$--3p$sub 2$) line in such a way as to maximize the power at the lambda$sub 1$ wavelength. The absorption of both lines was determined in pure methane in the pressure range 0.05--1 atm and in methane-air mixtures at atmospheric pressure; a comparison was made of the gains of these lines in a helium-neon discharge.
ISSN:0049-1748
2169-530X
DOI:10.1070/QE1975v005n02ABEH010909