1994
DOI: 10.1070/qe1994v024n04abeh000088
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Characteristics of the changes in the refractive index due to interaction of a radiation pulse with an inverted medium

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Cited by 5 publications
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“…Thus, we can ignore the variation in the parameters in the longitudinal direction compared to their variation across the beam and consider an optically thin gas layer. In this case, the variation in the hydrodynamic quantities and concentrations of the components is determined by the hierarchy of the characteristic times of various macro and microtransfer processes [14,15]. For a reactive gas in vibrational nonequilibrium, these are the times of the following processes: induced transitions (τ I ); the energy relaxation of vibrationally excited states (τ VT ); the radiation-pulse duration (τ p ); the chemical reaction resulting in formation of the component determining the igniting mechanism of the mixture (τ ch i,q ); the propagation of acoustic vibrations across the beam (τ a ), the multicomponent (τ D,i ) and thermal diffusion of the ith component (τ T,i ); the vibrational thermal diffusion (τ V D,i ); heat conduction (τ λ ); vibrational thermal conduction of the jth oscillator (τ V,j ); convection due to viscosity (τ c ); the state transition of the medium due to the striction force (τ F ).…”
Section: Formulation Of the Problem And Basic Assumptionsmentioning
confidence: 99%
“…Thus, we can ignore the variation in the parameters in the longitudinal direction compared to their variation across the beam and consider an optically thin gas layer. In this case, the variation in the hydrodynamic quantities and concentrations of the components is determined by the hierarchy of the characteristic times of various macro and microtransfer processes [14,15]. For a reactive gas in vibrational nonequilibrium, these are the times of the following processes: induced transitions (τ I ); the energy relaxation of vibrationally excited states (τ VT ); the radiation-pulse duration (τ p ); the chemical reaction resulting in formation of the component determining the igniting mechanism of the mixture (τ ch i,q ); the propagation of acoustic vibrations across the beam (τ a ), the multicomponent (τ D,i ) and thermal diffusion of the ith component (τ T,i ); the vibrational thermal diffusion (τ V D,i ); heat conduction (τ λ ); vibrational thermal conduction of the jth oscillator (τ V,j ); convection due to viscosity (τ c ); the state transition of the medium due to the striction force (τ F ).…”
Section: Formulation Of the Problem And Basic Assumptionsmentioning
confidence: 99%
“…This is due to the contribution of nuclear motion and the effect of an electric field on the vibrational wave function [14][15][16]. This can lead to a change in the refractive index of molecular gas [17][18][19] and self-focusing of an intense laser beam in a gaseous medium [20][21][22].…”
Section: Introductionmentioning
confidence: 99%
“…Thus, we can ignore the variation in the parameters in the longitudinal direction compared to their variation across the beam and consider an optically thin gas layer. In this case, the variation in the hydrodynamic quantities and concentrations of the components is determined by the hierarchy of the characteristic times of various macro-and micro-transfer processes [23,24].…”
Section: Formulation Of the Problem And Governing Equationsmentioning
confidence: 99%