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This research establishes the Gibbs state in quantum statistical mechanics as the unique solution derived purely from dynamical stability, eliminating the need for the traditional "zeroth law of thermodynamics." By demonstrating that an environment of harmonic oscillators suffices to isolate these states, the work provides a more rigorous foundation for thermal equilibrium without relying on heuristic or typicality-based arguments. This theoretical advancement strengthens the mathematical underpinnings essential for developing robust quantum simulation algorithms and understanding open quantum systems.
Gibbs state postulate from dynamical stability
arXiv:2512.13451v2 Announce Type: replace-cross Abstract: Gibbs states play a central role in quantum statistical mechanics as the standard description of thermal equilibrium. Traditionally, their use is justified either by a heuristic, a posteriori reasoning, or by derivations based on notions of typicality or passivity. In this work, we show that Gibbs states are completely characterized by assuming dynamical stability of the system itself and of the system in weak contact with an arbitrary environment. This builds on and strengthens a result by Frigerio, Gorini, and Verri (1986), who derived Gibbs states from dynamical stability using an additional assumption that they referred to as the "zeroth law of thermodynamics", as it concerns a nested dynamical stability of a triple of systems. We prove that this "zeroth law" is redundant and that an environment consisting solely of harmonic oscillators is sufficient to single out Gibbs states as the only dynamically stable states.
Abstract:Gibbs states play a central role in quantum statistical mechanics as the standard description of thermal equilibrium. Traditionally, their use is justified either by a heuristic, a posteriori reasoning, or by derivations based on notions of typicality or passivity. In this work, we show that Gibbs states are completely characterized by assuming dynamical stability of the system itself and of the system in weak contact with an arbitrary environment. This builds on and strengthens a result by Frigerio, Gorini, and Verri (1986), who derived Gibbs states from dynamical stability using an additional assumption that they referred to as the "zeroth law of thermodynamics", as it concerns a nested dynamical stability of a triple of systems. We prove that this "zeroth law" is redundant and that an environment consisting solely of harmonic oscillators is sufficient to single out Gibbs states as the only dynamically stable states.
Mathematical Physics (math-ph); Statistical Mechanics (cond-mat.stat-mech); Quantum Physics (quant-ph)
arXiv:2512.13451 [math-ph]
(or arXiv:2512.13451v2 [math-ph] for this version)
https://doi.org/10.48550/arXiv.2512.13451 Focus to learn more arXiv-issued DOI via DataCite
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