Open quantum system dynamics and the mean force Gibbs state
A. S. Trushechkin, M. Merkli, J. D. Cresser, J. Anders

TL;DR
This paper reviews recent advances in understanding how quantum systems at nanoscale interact with their environments, focusing on the steady states they reach and the role of the mean force Gibbs state in describing these equilibrium conditions.
Contribution
It provides a comprehensive overview of static and dynamic approaches to quantum thermodynamics, emphasizing the significance of the mean force Gibbs state and open quantum system methods.
Findings
Mean force Gibbs state generalizes the Gibbs state for strong system-environment coupling.
Dynamical models show convergence to the mean force Gibbs state under certain conditions.
Open problems remain in linking static and dynamical descriptions of quantum thermalization.
Abstract
The dynamical convergence of a system to the thermal distribution, or Gibbs state, is a standard assumption across all of the physical sciences. The Gibbs state is determined just by temperature and the system's energies alone. But at decreasing system sizes, i.e. for nanoscale and quantum systems, the interaction with their environments is not negligible. The question then arises: Is the system's steady state still the Gibbs state? And if not, how may the steady state depend on the interaction details? Here we provide an overview of recent progress on answering these questions. We expand on the state-of-the-art along two general avenues: First we take the static point-of-view which postulates the so-called mean force Gibbs state. This view is commonly adopted in the field of strong coupling thermodynamics, where modified laws of thermodynamics and non-equilibrium fluctuation relations…
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