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This study reveals a fundamental dissociation between bulk and entanglement phase transitions in the Haldane phase, challenging long-standing interpretations of the momentum-resolved entanglement spectrum for XXZ ladders. By resolving distinct modes that cross at specific momenta, the research demonstrates how symmetry breaking can decouple topological edge excitations from physical bulk properties, signaling a breakdown of the Li–Haldane correspondence in certain regimes. These findings provide critical insights into quantum many-body systems where entanglement alone exhibits unique critical behavior incompatible with conventional one-dimensional Hamiltonian assumptions.
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Dissociation of bulk and entanglement phase transitions in the Haldane phase

arXiv3 min read

arXiv:2509.03588v2 Announce Type: cross Abstract: Quantum entanglement provides a sensitive probe of topological phases and strong correlations in quantum many-body systems. We revisit the momentum-resolved entanglement spectrum (ES) of the spin-$\frac12$ XXZ ladder in the Haldane phase, whose SU(2)-symmetric spectrum has for over fifteen years been interpreted as a single des Cloizeaux--Pearson mode. Using momentum-resolved entanglement spectroscopy based on exact diagonalization of ladders with up to 40 spins, we instead resolve two distinct modes crossing at $k=\pi/2$ and forming a sharp cusp rather than a single $\sin|k|$ branch, revising the SU(2)-symmetric ES. We then introduce explicit SU(2) symmetry breaking through an XXZ anisotropy. The ES undergoes a phase transition at the isotropic point, while the physical ladder remains in the Haldane phase until a distinct bulk transition at larger anisotropy, establishing a dissociation between bulk and entanglement phase transitions. Between the entanglement and bulk critical points, no gapless entanglement branch remains that can be interpreted as a Haldane-edge excitation, signalling breakdown of the Li--Haldane correspondence. In the easy-plane regime, the ES develops an Anderson tower of states, and the entanglement ground state exhibits long-ranged spin correlations on the finite chains studied, consistent with emergent U(1)-broken order and incompatible with conventional short-range one-dimensional Hamiltonians satisfying the assumptions underlying the Lieb--Schultz--Mattis and Mermin--Wagner--Hohenberg--Coleman theorems. Together, these results establish entanglement-only quantum criticality as a distinct manifestation of critical behaviour encoded in the entanglement description.

Abstract:Quantum entanglement provides a sensitive probe of topological phases and strong correlations in quantum many-body systems. We revisit the momentum-resolved entanglement spectrum (ES) of the spin-$\frac12$ XXZ ladder in the Haldane phase, whose SU(2)-symmetric spectrum has for over fifteen years been interpreted as a single des Cloizeaux--Pearson mode. Using momentum-resolved entanglement spectroscopy based on exact diagonalization of ladders with up to 40 spins, we instead resolve two distinct modes crossing at $k=\pi/2$ and forming a sharp cusp rather than a single $\sin|k|$ branch, revising the SU(2)-symmetric ES. We then introduce explicit SU(2) symmetry breaking through an XXZ anisotropy. The ES undergoes a phase transition at the isotropic point, while the physical ladder remains in the Haldane phase until a distinct bulk transition at larger anisotropy, establishing a dissociation between bulk and entanglement phase transitions. Between the entanglement and bulk critical points, no gapless entanglement branch remains that can be interpreted as a Haldane-edge excitation, signalling breakdown of the Li--Haldane correspondence. In the easy-plane regime, the ES develops an Anderson tower of states, and the entanglement ground state exhibits long-ranged spin correlations on the finite chains studied, consistent with emergent U(1)-broken order and incompatible with conventional short-range one-dimensional Hamiltonians satisfying the assumptions underlying the Lieb--Schultz--Mattis and Mermin--Wagner--Hohenberg--Coleman theorems. Together, these results establish entanglement-only quantum criticality as a distinct manifestation of critical behaviour encoded in the entanglement description.

Strongly Correlated Electrons (cond-mat.str-el); Quantum Physics (quant-ph)

arXiv:2509.03588 [cond-mat.str-el]

(or arXiv:2509.03588v2 [cond-mat.str-el] for this version)

https://doi.org/10.48550/arXiv.2509.03588 Focus to learn more arXiv-issued DOI via DataCite

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Full text under the publisher's open licence · 322 words

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