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This paper provides a rigorous analytical derivation for the late-time volume-law scaling of Local Operator Entanglement in chaotic many-body systems, bridging numerical observations with theoretical frameworks like the Eigenstate Thermalization Hypothesis. By validating these findings against simulations of the 1D mixed-field Ising model, the work clarifies the fundamental limits of quantum chaos indicators without relying solely on empirical data.
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A derivation of the late-time volume law for local operator entanglement

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arXiv:2603.25387v2 Announce Type: replace Abstract: Local Operator Entanglement (LOE) has emerged an indicator of quantum chaos in many-body systems. Numerical studies have shown that, in chaotic systems, LOE grows linearly in time and displays a volume-law behavior at late times, scaling proportionally with the number of local degrees of freedom. Despite extensive numerical evidence, complemented by analytical studies in integrable systems, a fully analytical understanding of the emergence of the volume law remains incomplete. In this paper, we contribute toward this goal by deriving a late-time expression for LOE in chaotic systems that exhibits volume-law scaling. Our derivation proceeds by expressing the late-time LOE in the Liouville eigenstate basis and relies on three main assumptions: a higher-order non-resonance condition for the Hamiltonian eigenenergies, the Eigenstate Thermalization Hypothesis (ETH) ansatz for the matrix elements of the initial local operator, and the replacement of Hamiltonian eigenstates with random states in the final expression for LOE. Under these assumptions, we obtain an explicit formula displaying volume-law scaling. Finally, we complement our analytical derivation with numerical simulations of the 1D mixed-field Ising model, testing the resulting formula and exploring the regime of validity of our assumptions.

Abstract:Local Operator Entanglement (LOE) has emerged an indicator of quantum chaos in many-body systems. Numerical studies have shown that, in chaotic systems, LOE grows linearly in time and displays a volume-law behavior at late times, scaling proportionally with the number of local degrees of freedom. Despite extensive numerical evidence, complemented by analytical studies in integrable systems, a fully analytical understanding of the emergence of the volume law remains incomplete. In this paper, we contribute toward this goal by deriving a late-time expression for LOE in chaotic systems that exhibits volume-law scaling. Our derivation proceeds by expressing the late-time LOE in the Liouville eigenstate basis and relies on three main assumptions: a higher-order non-resonance condition for the Hamiltonian eigenenergies, the Eigenstate Thermalization Hypothesis (ETH) ansatz for the matrix elements of the initial local operator, and the replacement of Hamiltonian eigenstates with random states in the final expression for LOE. Under these assumptions, we obtain an explicit formula displaying volume-law scaling. Finally, we complement our analytical derivation with numerical simulations of the 1D mixed-field Ising model, testing the resulting formula and exploring the regime of validity of our assumptions.

Quantum Physics (quant-ph); Other Condensed Matter (cond-mat.other)

arXiv:2603.25387 [quant-ph]

(or arXiv:2603.25387v2 [quant-ph] for this version)

https://doi.org/10.48550/arXiv.2603.25387 Focus to learn more arXiv-issued DOI via DataCite

J. Phys. A: Math. Theor. 59, 335301 (2026)

https://doi.org/10.1088/1751-8121/ae8f8a Focus to learn more DOI(s) linking to related resources

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