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This research introduces a two-parameter framework to characterize the continuous onset of Eigenstate Thermalization Hypothesis (ETH) violations, distinguishing between fading and trapped ergodicity mechanisms in disordered quantum spin chains. By demonstrating that observed thermalization breakdowns often stem from finite-size effects rather than complete system failure, this work refines theoretical models for understanding non-ergodic behavior in isolated many-body systems. Such insights are critical for advancing our grasp of quantum chaos and the stability limits required for fault-tolerant quantum computing architectures.
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Two-Parameter Ansatz for the Violation of Eigenstate Thermalization

arXiv2 min read

arXiv:2608.02744v1 Announce Type: cross Abstract: The eigenstate thermalization hypothesis (ETH) provides the prevailing framework for understanding quantum thermalization and ergodicity in isolated many-body systems. Yet, no general theory describes the continuous onset of ETH violation between the conventional ETH and its complete breakdown. Here, we introduce a two-parameter ansatz for the ETH violation that unifies and distinguishes two mechanisms: fading ergodicity and trapped ergodicity. While fading ergodicity captures the established route to ergodicity breaking, trapped ergodicity describes a distinct scenario in which ETH is violated in finite systems but restored in the thermodynamic limit. We test this framework in the spin-1/2 $J_1$-$J_2$ chains with on-site disorder and linear potential. In both cases, we find that the observed ETH violation is consistent with trapped ergodicity.

Abstract:The eigenstate thermalization hypothesis (ETH) provides the prevailing framework for understanding quantum thermalization and ergodicity in isolated many-body systems. Yet, no general theory describes the continuous onset of ETH violation between the conventional ETH and its complete breakdown. Here, we introduce a two-parameter ansatz for the ETH violation that unifies and distinguishes two mechanisms: fading ergodicity and trapped ergodicity. While fading ergodicity captures the established route to ergodicity breaking, trapped ergodicity describes a distinct scenario in which ETH is violated in finite systems but restored in the thermodynamic limit. We test this framework in the spin-1/2 $J_1$-$J_2$ chains with on-site disorder and linear potential. In both cases, we find that the observed ETH violation is consistent with trapped ergodicity.

Statistical Mechanics (cond-mat.stat-mech); Disordered Systems and Neural Networks (cond-mat.dis-nn); Quantum Physics (quant-ph)

arXiv:2608.02744 [cond-mat.stat-mech]

(or arXiv:2608.02744v1 [cond-mat.stat-mech] for this version)

https://doi.org/10.48550/arXiv.2608.02744 Focus to learn more arXiv-issued DOI via DataCite (pending registration)

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Full text under the publisher's open licence · 222 words

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