The description of relaxation by the methods of classical statistics and mechanics has a number of advantages, the chief one of which is obviously the opportunity of using in place of a large number of balance equations for individual levels a single transport equation for a distribution function over vibrational energy and, in a number of cases, the additional opportunity for more general and clearer consideration of the various factors characterizing intra- and intermolecular interactions. A version of the classical theory for vibrational relaxation during weak interaction of molecules with a gas is diffusion theory in which a Fokker-Planck diffusion equation serves as the transport equation. In particular, a detailed study of the influence of anharmonicity at various values of the adiabaticity parameter ξo on the kinetic characteristics of the process was carried out [2] within the limits of this theory on the basis of a solution of the diffusion equation from [1]; earlier [3], vibrational relaxation in a light inert-gas medium was considered in the diffusion approximation (for harmonic and anharmonic oscillators) which coresponds to relaxation for nonadiabatic interaction in a uniform temperature field (ξo → 0) as shown in [1]. The possibility of describing vibrational kinetics within the framework of diffusion theory involves two basic problems: 1) the possibility of approximating the transport equation for classical oscillators with a Fokker-Planck equation, and 2) the possibility of describing the relaxation of quantum oscillators by classical methods or the correspondence of classical and quantum theory of relaxation for weak interaction of molecules with a medium. The first of these problems is considered here.
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