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It is well known that resonance absorption of radiation by a gas can lead to excitation of molecular internal degrees of freedom, and this determines, to a significant degree, the nonlinear response of the medium. Hydrodynamic effects have been analyzed primarily within the model of a nonviscous thermally nonconducting gas, neglecting the influence of diffusion and heat conduction, which in a vibrationally nonequilibrium gas depends significantly on the degree of excitation and can significantly influence the behavior of the concentrations of the mixture components even over times shorter than the characteristic times of these processes [8]. The imaginary part is associated with the absorption coefficient tq, and the real part is associated with the index of refraction n. A change of n in the beam channel causes the light rays to be deflected from the initial direction and determines, to a significant degree, the character of laser propagation in a nonlinear medium [1].
It is well known that resonance absorption of radiation by a gas can lead to excitation of molecular internal degrees of freedom, and this determines, to a significant degree, the nonlinear response of the medium. Hydrodynamic effects have been analyzed primarily within the model of a nonviscous thermally nonconducting gas, neglecting the influence of diffusion and heat conduction, which in a vibrationally nonequilibrium gas depends significantly on the degree of excitation and can significantly influence the behavior of the concentrations of the mixture components even over times shorter than the characteristic times of these processes [8]. The imaginary part is associated with the absorption coefficient tq, and the real part is associated with the index of refraction n. A change of n in the beam channel causes the light rays to be deflected from the initial direction and determines, to a significant degree, the character of laser propagation in a nonlinear medium [1].