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This research advances the theoretical understanding of entanglement asymmetry in interacting quantum spin chains, specifically within the gapped phase where symmetry is spontaneously broken. By deriving a master formula that connects static susceptibility to form factors from sine-Gordon theory and validating it with density-matrix renormalization group simulations, the study provides new analytic tools for analyzing non-equilibrium properties of many-body systems.
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Entanglement asymmetry in the gapped XYZ spin-$\frac12$ chain

arXiv2 min de cititArticolul și perspectiva sunt în engleză.

arXiv:2607.25625v1 Announce Type: cross Abstract: The entanglement asymmetry measures how strongly a symmetry is broken inside a subsystem. Analytic results at equilibrium have so far covered free theories and, perturbatively, the critical XXZ chain. We compute the R\'enyi entanglement asymmetries of a large interval in the gapped, $U(1)$-breaking phase of the interacting XYZ chain. The calculation combines three ingredients. A charged-moment identity, which we prove for fermionic Gaussian and for injective matrix-product ground states, ties the asymmetry to the static susceptibility of the broken charge. A non-conservation sum rule then evaluates the susceptibility from sine-Gordon form factors, its two-kink and one-breather channels providing a lower bound on the universal amplitude. The Baxter--Johnson--Krinsky--McCoy solution supplies the kink mass for different couplings. Infinite-system density-matrix renormalization group simulations built on these masses reproduce the master formula.

Abstract:The entanglement asymmetry measures how strongly a symmetry is broken inside a subsystem. Analytic results at equilibrium have so far covered free theories and, perturbatively, the critical XXZ chain. We compute the Rényi entanglement asymmetries of a large interval in the gapped, $U(1)$-breaking phase of the interacting XYZ chain. The calculation combines three ingredients. A charged-moment identity, which we prove for fermionic Gaussian and for injective matrix-product ground states, ties the asymmetry to the static susceptibility of the broken charge. A non-conservation sum rule then evaluates the susceptibility from sine-Gordon form factors, its two-kink and one-breather channels providing a lower bound on the universal amplitude. The Baxter--Johnson--Krinsky--McCoy solution supplies the kink mass for different couplings. Infinite-system density-matrix renormalization group simulations built on these masses reproduce the master formula.

Statistical Mechanics (cond-mat.stat-mech); High Energy Physics - Theory (hep-th); Quantum Physics (quant-ph)

arXiv:2607.25625 [cond-mat.stat-mech]

(or arXiv:2607.25625v1 [cond-mat.stat-mech] for this version)

https://doi.org/10.48550/arXiv.2607.25625 Focus to learn more arXiv-issued DOI via DataCite (pending registration)

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