Making use of the thermo field dynamics (TFD) we formulate a calculabl
e method for time-dependent nonequilibrium systems in a time represent
ation (t-representation) rather than in the k0-Fourier representation.
The corrected one-body propagator in the t-representation has the for
m of B-1 (diagonal matrix) B (B being a thermal Bogoliubov matrix). Th
e number parameter in B here is the observed number (the Heisenberg nu
mber) with a fluctuation. With the usual definition of the on-shell se
lf-energy a self-consistent renormalization condition leads to a kinet
ic equation for the number parameter. This equation turns out to be th
e Boltzmann equation, from which the entropy law follows.