An extension of the scheme of non-equilibrium thermodynamics developed prev
iously is given for quantum mechanical systems. A master equation for the d
ensity matrix of the system follows from this scheme. Onsager relations are
given and derived. Application to a spin system gives the Bloch equations.
The application to a one-dimensional damped harmonic oscillator results in
equations, which enable us to calculate the usual Green functions. For the
last case we derive, as a new alternative, quantum mechanical Langevin equ
ations. A new element, compared to the classical Langevin equations, is a r
andom velocity. The correlation of the random velocity with the random forc
e then results from the zero point motion of the oscillator. The applicatio
n of mesoscopic non-equilibrium thermodynamics to these wellknown problems
illustrates the usefullness of this method. (C) 2001 Elsevier Science B.V.
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