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This research establishes rapid mixing for quantum Gibbs samplers in one-dimensional non-commuting spin systems, significantly improving convergence bounds from linear to polylogarithmic scaling. By demonstrating that equilibration occurs via a two-stage process involving high-weight Pauli operators, the study refines our understanding of spectral gaps and dissipation rates in quantum thermalization.
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Spectral Analysis Beyond the Spectral Gap: Rapid Mixing of Quantum Gibbs Samplers in One Dimension

arXiv2 min read

arXiv:2610.05848v1 Announce Type: new Abstract: We prove rapid mixing of a quantum Gibbs sampler for general one-dimensional non-commuting local spin systems at every fixed positive temperature. In particular, for a system of $n$ sites, we show that the Kubo--Martin--Schwinger (KMS) detailed-balanced Gibbs sampler of~\cite{CKG2023} converges from any initial state to trace-norm error $\epsilon$ in time $O(\log^4(n)+\log(1/\epsilon))$. This improves the previous $O(n+\log(1/\epsilon))$ bound and establishes rapid mixing beyond high-temperature and weak-interaction regimes. Our proof explains why the slowest decay rate, captured by the spectral gap, can substantially underestimate the speed of equilibration. The key insight is that a state far from equilibrium must have a substantial component outside the span of low-weight Pauli operators, where stronger dissipation estimates apply. This yields two stages of relaxation: a double-exponential convergence from a bad initial state, followed by exponential convergence near equilibrium. We turn this mechanism into a framework for proving rapid mixing through spectral analysis beyond the gap. Our decay estimate is equivalent to exponential convergence in sandwiched R\'enyi-2 divergence. Together with the spectral gap, it also implies a modified logarithmic Sobolev inequality with rate $\Omega(\log^{-4}(n))$.

Abstract:We prove rapid mixing of a quantum Gibbs sampler for general one-dimensional non-commuting local spin systems at every fixed positive temperature. In particular, for a system of $n$ sites, we show that the Kubo--Martin--Schwinger (KMS) detailed-balanced Gibbs sampler of~\cite{CKG2023} converges from any initial state to trace-norm error $\epsilon$ in time $O(\log^4(n)+\log(1/\epsilon))$. This improves the previous $O(n+\log(1/\epsilon))$ bound and establishes rapid mixing beyond high-temperature and weak-interaction regimes. Our proof explains why the slowest decay rate, captured by the spectral gap, can substantially underestimate the speed of equilibration. The key insight is that a state far from equilibrium must have a substantial component outside the span of low-weight Pauli operators, where stronger dissipation estimates apply. This yields two stages of relaxation: a double-exponential convergence from a bad initial state, followed by exponential convergence near equilibrium. We turn this mechanism into a framework for proving rapid mixing through spectral analysis beyond the gap. Our decay estimate is equivalent to exponential convergence in sandwiched Rényi-2 divergence. Together with the spectral gap, it also implies a modified logarithmic Sobolev inequality with rate $\Omega(\log^{-4}(n))$.

arXiv:2610.05848 [quant-ph]

(or arXiv:2610.05848v1 [quant-ph] for this version)

https://doi.org/10.48550/arXiv.2610.05848 Focus to learn more arXiv-issued DOI via DataCite (pending registration)

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Full text under the publisher's open licence · 269 words

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