Abstract
In Chap. 17 we have considered the route of a system into its global equilibrium state due to the coupling to an environment - the way from a nonequilibrium initial state into the stationary global equilibrium state. In fact, this relaxation process may even look like an exponential decay described by a rate equation, i.e., a statistical behavior for the considered system, while system and environment follow a Schrödinger equation. This is the key-feature of the Schrödinger dynamics of bipartite systems, by which the problem of time reversal invariance of microscopic equations and irreversibility can be overcome.
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Gemmer, J., Michel, M., Mahler, G. 19 Heat Conduction. In: Quantum Thermodynamics. Lecture Notes in Physics, vol 657. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-540-44513-5_19
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DOI: https://doi.org/10.1007/978-3-540-44513-5_19
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