The emission switched from the λ = 3.3922 μ 5s'[1/2]01–4p'[3/2]2(3s2–3p4) line to the λ1 = 3.3912 μ 5s'[1/2]01–4p'[1/2]1(3s2-3p4) line in such a way as to maximize the power at the λ1 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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Balakin et al. (1975) studied this question.
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