Abstract

The behavior of two lines P 1-0(11) and P 2-1(8) weakly absorbed by the atmosphere is experimentally investigated in the spectra of cw chemical multikilowatt HF lasers of five types that differ in size and construction scheme of the nozzle array. It is shown that the intensity of these lines can be controlled within certain limits by varying the gas-dynamic regime of the laser operation, the chemical composition of the active medium, the orientation of the optical axis of the cavity and the cavity feedback factor, and the construction of the nozzle array.

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