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On the stability of KMS states in perturbative algebraic quantum field theories

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arxiv 1609.01124 v3 pith:RGROPMXX submitted 2016-09-05 math-ph hep-thmath.MP

On the stability of KMS states in perturbative algebraic quantum field theories

classification math-ph hep-thmath.MP
keywords equilibriumfreeperturbativestateadiabaticalgebraicanymorefield
verification ladder T0 review T1 audit T2 compute T3 formal T4 reserved
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We analyze the stability properties shown by KMS states for interacting massive scalar fields propagating over Minkowski spacetime, recently constructed in the framework of perturbative algebraic quantum field theories by Fredenhagen and Lindner \cite{FredenhagenLindner}. In particular, we prove the validity of the return to equilibrium property when the interaction Lagrangian has compact spatial support. Surprisingly, this does not hold anymore, if the adiabatic limit is considered, namely when the interaction Lagrangian is invariant under spatial translations. Consequently, an equilibrium state under the adiabatic limit for a perturbative interacting theory evolved with the free dynamics does not converge anymore to the free equilibrium state. Actually, we show that its ergodic mean converges to a non equilibrium steady state for the free theory.

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Cited by 3 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score.

  1. Kubo-Martin-Schwinger conditions for non-Hermitian systems

    quant-ph 2026-06 unverdicted novelty 7.0

    Positivity of the biorthogonal Gibbs functional characterizes quasi-Hermiticity for diagonalisable non-Hermitian operators with real spectra, and the resulting state satisfies the three analytic KMS conditions.

  2. Kubo-Martin-Schwinger conditions for non-Hermitian systems

    quant-ph 2026-06 unverdicted novelty 7.0

    For any diagonalisable non-Hermitian H with real spectrum, the biorthogonal Gibbs functional satisfies positivity of ω_bi(A†A) for all A if and only if H is quasi-Hermitian.

  3. Relative entropy for $\lambda \phi^4$ in the Rindler wedge

    hep-th 2026-07 accept novelty 6.5

    Relative entropy of vacuum vs coherent state for λφ⁴ in the Rindler wedge equals the classical interacting boost charge to O(λ) and obeys the Bekenstein bound.