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This research investigates how entanglement entropy in non-Hermitian critical chains exhibits unique sensitivity to energy gaps near exceptional points, deviating from standard Calabrese-Cardy scaling. By mapping these systems onto de Sitter geometry via continuous multiscale entanglement renormalization, the study reveals a residual entropy term that persists even for sub-finite-size perturbations invisible in unitary models. These findings advance fundamental understanding of non-unitary quantum criticality and its geometric duals within theoretical physics frameworks.
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Beyond Calabrese-Cardy Scaling: Exceptional-Point Sensitivity from the de Sitter RT Surface

arXiv3 min read

arXiv:2607.21536v1 Announce Type: new Abstract: Entanglement entropy at one-dimensional criticality typically follows the Calabrese-Cardy scaling. In non-Hermitian critical chains near exceptional points, however, we show that the biorthogonal entropy of a finite system retains an additional sensitivity to a small energy gap \(\Delta\) even when \(\Delta < 1/L\). On top of the usual Calabrese-Cardy term, we find an interval-independent contribution \(S_{\rm res}=\log(\Delta L)\), visible as a vertical offset and detectable even for a one-site subsystem. This behavior has no Hermitian analogue: a sub-finite-size gap is effectively invisible to entanglement in unitary critical chains, whereas here the entropy continues to resolve such a gap through its dependence on \(\Delta L\). We interpret the result within the de Sitter geometry generated by non-unitary continuous multiscale entanglement renormalization: because the dS extremal surface reaches the IR endpoint, entanglement necessarily retains the endpoint contribution. On a finite ring, a regular circuit cannot terminate at a one-site product state and instead leaves an entangled two-site IR state. Computing the entanglement of the IR state recovers the same \(\log(\Delta L)\) term, identifying this additional long-range entanglement as the residual entropy left after finite-depth disentangling.

Abstract:Entanglement entropy at one-dimensional criticality typically follows the Calabrese-Cardy scaling. In non-Hermitian critical chains near exceptional points, however, we show that the biorthogonal entropy of a finite system retains an additional sensitivity to a small energy gap \(\Delta\) even when \(\Delta < 1/L\). On top of the usual Calabrese-Cardy term, we find an interval-independent contribution \(S_{\rm res}=\log(\Delta L)\), visible as a vertical offset and detectable even for a one-site subsystem. This behavior has no Hermitian analogue: a sub-finite-size gap is effectively invisible to entanglement in unitary critical chains, whereas here the entropy continues to resolve such a gap through its dependence on \(\Delta L\). We interpret the result within the de Sitter geometry generated by non-unitary continuous multiscale entanglement renormalization: because the dS extremal surface reaches the IR endpoint, entanglement necessarily retains the endpoint contribution. On a finite ring, a regular circuit cannot terminate at a one-site product state and instead leaves an entangled two-site IR state. Computing the entanglement of the IR state recovers the same \(\log(\Delta L)\) term, identifying this additional long-range entanglement as the residual entropy left after finite-depth disentangling.

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

arXiv:2607.21536 [quant-ph]

(or arXiv:2607.21536v1 [quant-ph] for this version)

https://doi.org/10.48550/arXiv.2607.21536 Focus to learn more arXiv-issued DOI via DataCite (pending registration)

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Full text under the publisher's open licence · 286 words

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