“…The excitation process into a continuum can be described by the following system of the generalized kinetic equations 2–4, 6, 8: where z n are the populations of the laser‐excited states with energy E n ; W n,n ±1 is the rate of the radiative transitions; W n,n ±1 = σ n,n ±1 I ( t ), where σ n,n ±1 are the cross‐sections of the radiative transitions up and down, I ( t ) is the laser radiation intensity (photon · cm −2 · s −1 ); k VT n,n ±1 are the constants of rate of the V‐T relaxation; d n is the monomolecular decay rate; Θ( n‐N min ) is the Heaviside function as an additional multiplier in the diffusion coefficient D ( R ) n 3 , which “freezes” the stochastic processes in the area of the low‐lying states according to the well‐known Chirikov's criterion 10. The key difference between our model and other theoretical models is in an explicit accounting for effect of the stochastic diffusion in the quasicontinuum.…”