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Quantum mechanical evolution towards thermal equilibrium

3 Pith papers cite this work. Polarity classification is still indexing.

3 Pith papers citing it
abstract

The circumstances under which a system reaches thermal equilibrium, and how to derive this from basic dynamical laws, has been a major question from the very beginning of thermodynamics and statistical mechanics. Despite considerable progress, it remains an open problem. Motivated by this issue, we address the more general question of equilibration. We prove, with virtually full generality, that reaching equilibrium is a universal property of quantum systems: Almost any subsystem in interaction with a large enough bath will reach an equilibrium state and remain close to it for almost all times. We also prove several general results about other aspects of thermalisation besides equilibration, for example, that the equilibrium state does not depend on the detailed micro-state of the bath.

years

2026 2 2023 1

verdicts

UNVERDICTED 3

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representative citing papers

Grand-Canonical Typicality

quant-ph · 2026-01-06 · unverdicted · novelty 5.0

The paper establishes that typical states in a grand-canonical micro-canonical Hilbert subspace produce the grand-canonical density matrix and a GAP/Scrooge wave-function distribution for the subsystem.

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Showing 2 of 2 citing papers after filters.

  • Gauging Time Reversal Symmetry in Quantum Gravity: Arrow of Time from a Confinement--Deconfinement Transition physics.gen-ph · 2026-05-04 · unverdicted · none · ref 9 · internal anchor

    The emergence of the cosmological arrow of time is identified with a confinement-deconfinement transition in a Z2 lattice gauge theory on LQG spin networks, with the deconfined phase corresponding to a CZX-type SPT phase.

  • Grand-Canonical Typicality quant-ph · 2026-01-06 · unverdicted · none · ref 32 · internal anchor

    The paper establishes that typical states in a grand-canonical micro-canonical Hilbert subspace produce the grand-canonical density matrix and a GAP/Scrooge wave-function distribution for the subsystem.