Highly Entangled Stationary States from Strong Symmetries

We find that the presence of strong non-Abelian symmetries can lead to highly entangled stationary states even for unital quantum channels. We derive exact expressions for the bipartite logarithmic negativity, Rényi negativities, and operator space entanglement for stationary states restricted to on...

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الحاوية / القاعدة:Physical Review X
المؤلفون الرئيسيون: Yahui Li, Frank Pollmann, Nicholas Read, Pablo Sala
التنسيق: مقال
اللغة:الإنجليزية
منشور في: American Physical Society 2025-03-01
الوصول للمادة أونلاين:http://doi.org/10.1103/PhysRevX.15.011068
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author Yahui Li
Frank Pollmann
Nicholas Read
Pablo Sala
author_facet Yahui Li
Frank Pollmann
Nicholas Read
Pablo Sala
author_sort Yahui Li
collection DOAJ
container_title Physical Review X
description We find that the presence of strong non-Abelian symmetries can lead to highly entangled stationary states even for unital quantum channels. We derive exact expressions for the bipartite logarithmic negativity, Rényi negativities, and operator space entanglement for stationary states restricted to one symmetric subspace, with focus on the trivial subspace. We prove that these apply to open quantum evolutions whose commutants, characterizing all strongly conserved quantities, correspond to either the universal enveloping algebra of a Lie algebra or the Read-Saleur commutants. The latter provides an example of quantum fragmentation, whose dimension is exponentially large in system size. We find a general upper bound for all these quantities given by the logarithm of the dimension of the commutant on the smaller bipartition of the chain. As Abelian examples, we show that strong U(1) symmetries and classical fragmentation lead to separable stationary states in any symmetric subspace. In contrast, for non-Abelian SU(N) symmetries, both logarithmic and Rényi negativities scale logarithmically with system size. Finally, we prove that, while Rényi negativities with n>2 scale logarithmically with system size, the logarithmic negativity (as well as generalized Rényi negativities with n<2) exhibits a volume-law scaling for the Read-Saleur commutants. Our derivations rely on the commutant possessing a Hopf algebra structure in the limit of infinitely large systems and, hence, also apply to finite groups and quantum groups.
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spelling doaj-art-0a034d8ea37d4f3cbd5009aba612d6132025-08-20T01:43:03ZengAmerican Physical SocietyPhysical Review X2160-33082025-03-0115101106810.1103/PhysRevX.15.011068Highly Entangled Stationary States from Strong SymmetriesYahui LiFrank PollmannNicholas ReadPablo SalaWe find that the presence of strong non-Abelian symmetries can lead to highly entangled stationary states even for unital quantum channels. We derive exact expressions for the bipartite logarithmic negativity, Rényi negativities, and operator space entanglement for stationary states restricted to one symmetric subspace, with focus on the trivial subspace. We prove that these apply to open quantum evolutions whose commutants, characterizing all strongly conserved quantities, correspond to either the universal enveloping algebra of a Lie algebra or the Read-Saleur commutants. The latter provides an example of quantum fragmentation, whose dimension is exponentially large in system size. We find a general upper bound for all these quantities given by the logarithm of the dimension of the commutant on the smaller bipartition of the chain. As Abelian examples, we show that strong U(1) symmetries and classical fragmentation lead to separable stationary states in any symmetric subspace. In contrast, for non-Abelian SU(N) symmetries, both logarithmic and Rényi negativities scale logarithmically with system size. Finally, we prove that, while Rényi negativities with n>2 scale logarithmically with system size, the logarithmic negativity (as well as generalized Rényi negativities with n<2) exhibits a volume-law scaling for the Read-Saleur commutants. Our derivations rely on the commutant possessing a Hopf algebra structure in the limit of infinitely large systems and, hence, also apply to finite groups and quantum groups.http://doi.org/10.1103/PhysRevX.15.011068
spellingShingle Yahui Li
Frank Pollmann
Nicholas Read
Pablo Sala
Highly Entangled Stationary States from Strong Symmetries
title Highly Entangled Stationary States from Strong Symmetries
title_full Highly Entangled Stationary States from Strong Symmetries
title_fullStr Highly Entangled Stationary States from Strong Symmetries
title_full_unstemmed Highly Entangled Stationary States from Strong Symmetries
title_short Highly Entangled Stationary States from Strong Symmetries
title_sort highly entangled stationary states from strong symmetries
url http://doi.org/10.1103/PhysRevX.15.011068
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