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 |
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Hauptverfasser: | , , , , |
Format: | Artikel |
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. |
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ISSN: | 0049-1748 2169-530X |
DOI: | 10.1070/QE1975v005n02ABEH010909 |