Abstract
A method for the development of elements of nonequilibrium (ℏ, k) dynamics without the use of the Schrodinger equation is proposed. This method is based on the generalization of the Fokker-Planck and Hamilton-Jacoby equations by the successive account of the stochastic action of vacuum (quantum thermostat). It is shown that nonequilibrium wave functions in the presence of quantum-thermal diffusion in vacuum describe the approximation to the state of generalized thermal equilibrium both at zero and finite temperatures. They can be used as the basis for a universal description of transport processes.
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