Abstract:Thermodynamic equilibrium properties of a macroscopic system emerge from an interaction with a thermal bath. In the weak coupling regime, the description of thermodynamic states turns possible to describe the system in terms of its time-independent intensive and extensive variables. However, this is not an obvious task in both the classical and quantum cases when either dealing with finite systems described by a few degrees of freedom when the statistical fluctuations play an important role, i.e., not in the t… Show more
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