Entanglement negativity and replica symmetry breaking in general holographic states

Abstract The entanglement negativity E $$ \mathcal{E} $$ (A : B) is a useful measure of quantum entanglement in bipartite mixed states. In random tensor networks (RTNs), which are related to fixed-area states, it was found in ref. [1] that the dominant saddles computing the even Rényi negativity E 2...

Full description

Saved in:
Bibliographic Details
Main Authors: Xi Dong, Jonah Kudler-Flam, Pratik Rath
Format: Article
Language:English
Published: SpringerOpen 2025-01-01
Series:Journal of High Energy Physics
Subjects:
Online Access:https://doi.org/10.1007/JHEP01(2025)022
Tags: Add Tag
No Tags, Be the first to tag this record!
_version_ 1832595076003397632
author Xi Dong
Jonah Kudler-Flam
Pratik Rath
author_facet Xi Dong
Jonah Kudler-Flam
Pratik Rath
author_sort Xi Dong
collection DOAJ
description Abstract The entanglement negativity E $$ \mathcal{E} $$ (A : B) is a useful measure of quantum entanglement in bipartite mixed states. In random tensor networks (RTNs), which are related to fixed-area states, it was found in ref. [1] that the dominant saddles computing the even Rényi negativity E 2 k $$ {\mathcal{E}}^{(2k)} $$ generically break the ℤ 2k replica symmetry. This calls into question previous calculations of holographic negativity using 2D CFT techniques that assumed ℤ 2k replica symmetry and proposed that the negativity was related to the entanglement wedge cross section. In this paper, we resolve this issue by showing that in general holographic states, the saddles computing E 2 k $$ {\mathcal{E}}^{(2k)} $$ indeed break the ℤ 2k replica symmetry. Our argument involves an identity relating E 2 k $$ {\mathcal{E}}^{(2k)} $$ to the k-th Rényi entropy on subregion AB ∗ in the doubled state ρ AB A A ∗ BB ∗ $$ {\left.|{\rho}_{AB}\right\rangle}_{A{A}^{\ast }{BB}^{\ast }} $$ , from which we see that the ℤ 2k replica symmetry is broken down to ℤ k . For k < 1, which includes the case of E $$ \mathcal{E} $$ (A : B) at k = 1/2, we use a modified cosmic brane proposal to derive a new holographic prescription for E 2 k $$ {\mathcal{E}}^{(2k)} $$ and show that it is given by a new saddle with multiple cosmic branes anchored to subregions A and B in the original state. Using our prescription, we reproduce known results for the PSSY model and show that our saddle dominates over previously proposed CFT calculations near k = 1. Moreover, we argue that the ℤ 2k symmetric configurations previously proposed are not gravitational saddles, unlike our proposal. Finally, we contrast holographic calculations with those arising from RTNs with non-maximally entangled links, demonstrating that the qualitative form of backreaction in such RTNs is different from that in gravity.
format Article
id doaj-art-d1c7e28c852f4deda05d9022f5b60891
institution Kabale University
issn 1029-8479
language English
publishDate 2025-01-01
publisher SpringerOpen
record_format Article
series Journal of High Energy Physics
spelling doaj-art-d1c7e28c852f4deda05d9022f5b608912025-01-19T12:07:02ZengSpringerOpenJournal of High Energy Physics1029-84792025-01-012025114110.1007/JHEP01(2025)022Entanglement negativity and replica symmetry breaking in general holographic statesXi Dong0Jonah Kudler-Flam1Pratik Rath2Department of Physics, University of CaliforniaSchool of Natural Sciences, Institute for Advanced StudyCenter for Theoretical Physics and Department of Physics, University of CaliforniaAbstract The entanglement negativity E $$ \mathcal{E} $$ (A : B) is a useful measure of quantum entanglement in bipartite mixed states. In random tensor networks (RTNs), which are related to fixed-area states, it was found in ref. [1] that the dominant saddles computing the even Rényi negativity E 2 k $$ {\mathcal{E}}^{(2k)} $$ generically break the ℤ 2k replica symmetry. This calls into question previous calculations of holographic negativity using 2D CFT techniques that assumed ℤ 2k replica symmetry and proposed that the negativity was related to the entanglement wedge cross section. In this paper, we resolve this issue by showing that in general holographic states, the saddles computing E 2 k $$ {\mathcal{E}}^{(2k)} $$ indeed break the ℤ 2k replica symmetry. Our argument involves an identity relating E 2 k $$ {\mathcal{E}}^{(2k)} $$ to the k-th Rényi entropy on subregion AB ∗ in the doubled state ρ AB A A ∗ BB ∗ $$ {\left.|{\rho}_{AB}\right\rangle}_{A{A}^{\ast }{BB}^{\ast }} $$ , from which we see that the ℤ 2k replica symmetry is broken down to ℤ k . For k < 1, which includes the case of E $$ \mathcal{E} $$ (A : B) at k = 1/2, we use a modified cosmic brane proposal to derive a new holographic prescription for E 2 k $$ {\mathcal{E}}^{(2k)} $$ and show that it is given by a new saddle with multiple cosmic branes anchored to subregions A and B in the original state. Using our prescription, we reproduce known results for the PSSY model and show that our saddle dominates over previously proposed CFT calculations near k = 1. Moreover, we argue that the ℤ 2k symmetric configurations previously proposed are not gravitational saddles, unlike our proposal. Finally, we contrast holographic calculations with those arising from RTNs with non-maximally entangled links, demonstrating that the qualitative form of backreaction in such RTNs is different from that in gravity.https://doi.org/10.1007/JHEP01(2025)022AdS-CFT CorrespondenceGauge-Gravity Correspondence
spellingShingle Xi Dong
Jonah Kudler-Flam
Pratik Rath
Entanglement negativity and replica symmetry breaking in general holographic states
Journal of High Energy Physics
AdS-CFT Correspondence
Gauge-Gravity Correspondence
title Entanglement negativity and replica symmetry breaking in general holographic states
title_full Entanglement negativity and replica symmetry breaking in general holographic states
title_fullStr Entanglement negativity and replica symmetry breaking in general holographic states
title_full_unstemmed Entanglement negativity and replica symmetry breaking in general holographic states
title_short Entanglement negativity and replica symmetry breaking in general holographic states
title_sort entanglement negativity and replica symmetry breaking in general holographic states
topic AdS-CFT Correspondence
Gauge-Gravity Correspondence
url https://doi.org/10.1007/JHEP01(2025)022
work_keys_str_mv AT xidong entanglementnegativityandreplicasymmetrybreakingingeneralholographicstates
AT jonahkudlerflam entanglementnegativityandreplicasymmetrybreakingingeneralholographicstates
AT pratikrath entanglementnegativityandreplicasymmetrybreakingingeneralholographicstates