Interface contributions to topological entanglement in abelian Chern-Simons theory

Abstract We study the entanglement entropy between (possibly distinct) topological phases across an interface using an Abelian Chern-Simons description with topological boundary conditions (TBCs) at the interface. From a microscopic point of view, these TBCs correspond to turning on particular gappi...

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Main Authors: Jackson R. Fliss, Xueda Wen, Onkar Parrikar, Chang-Tse Hsieh, Bo Han, Taylor L. Hughes, Robert G. Leigh
Format: Article
Language:English
Published: SpringerOpen 2017-09-01
Series:Journal of High Energy Physics
Subjects:
Online Access:http://link.springer.com/article/10.1007/JHEP09(2017)056
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spelling doaj-916fe1eafc484c21b9ddf0f8f254a7dc2020-11-24T22:49:52ZengSpringerOpenJournal of High Energy Physics1029-84792017-09-012017913410.1007/JHEP09(2017)056Interface contributions to topological entanglement in abelian Chern-Simons theoryJackson R. Fliss0Xueda Wen1Onkar Parrikar2Chang-Tse Hsieh3Bo Han4Taylor L. Hughes5Robert G. Leigh6Department of Physics, University of IllinoisDepartment of Physics, University of IllinoisDavid Rittenhouse Laboratory, University of PennsylvaniaDepartment of Physics, University of IllinoisDepartment of Physics, University of IllinoisDepartment of Physics, University of IllinoisDepartment of Physics, University of IllinoisAbstract We study the entanglement entropy between (possibly distinct) topological phases across an interface using an Abelian Chern-Simons description with topological boundary conditions (TBCs) at the interface. From a microscopic point of view, these TBCs correspond to turning on particular gapping interactions between the edge modes across the interface. However, in studying entanglement in the continuum Chern-Simons description, we must confront the problem of non-factorization of the Hilbert space, which is a standard property of gauge theories. We carefully define the entanglement entropy by using an extended Hilbert space construction directly in the continuum theory. We show how a given TBC isolates a corresponding gauge invariant state in the extended Hilbert space, and hence compute the resulting entanglement entropy. We find that the sub-leading correction to the area law remains universal, but depends on the choice of topological boundary conditions. This agrees with the microscopic calculation of [1]. Additionally, we provide a replica path integral calculation for the entropy. In the case when the topological phases across the interface are taken to be identical, our construction gives a novel explanation of the equivalence between the left-right entanglement of (1+1)d Ishibashi states and the spatial entanglement of (2+1)d topological phases.http://link.springer.com/article/10.1007/JHEP09(2017)056Chern-Simons TheoriesTopological Field TheoriesGauge SymmetryTopological States of Matter
collection DOAJ
language English
format Article
sources DOAJ
author Jackson R. Fliss
Xueda Wen
Onkar Parrikar
Chang-Tse Hsieh
Bo Han
Taylor L. Hughes
Robert G. Leigh
spellingShingle Jackson R. Fliss
Xueda Wen
Onkar Parrikar
Chang-Tse Hsieh
Bo Han
Taylor L. Hughes
Robert G. Leigh
Interface contributions to topological entanglement in abelian Chern-Simons theory
Journal of High Energy Physics
Chern-Simons Theories
Topological Field Theories
Gauge Symmetry
Topological States of Matter
author_facet Jackson R. Fliss
Xueda Wen
Onkar Parrikar
Chang-Tse Hsieh
Bo Han
Taylor L. Hughes
Robert G. Leigh
author_sort Jackson R. Fliss
title Interface contributions to topological entanglement in abelian Chern-Simons theory
title_short Interface contributions to topological entanglement in abelian Chern-Simons theory
title_full Interface contributions to topological entanglement in abelian Chern-Simons theory
title_fullStr Interface contributions to topological entanglement in abelian Chern-Simons theory
title_full_unstemmed Interface contributions to topological entanglement in abelian Chern-Simons theory
title_sort interface contributions to topological entanglement in abelian chern-simons theory
publisher SpringerOpen
series Journal of High Energy Physics
issn 1029-8479
publishDate 2017-09-01
description Abstract We study the entanglement entropy between (possibly distinct) topological phases across an interface using an Abelian Chern-Simons description with topological boundary conditions (TBCs) at the interface. From a microscopic point of view, these TBCs correspond to turning on particular gapping interactions between the edge modes across the interface. However, in studying entanglement in the continuum Chern-Simons description, we must confront the problem of non-factorization of the Hilbert space, which is a standard property of gauge theories. We carefully define the entanglement entropy by using an extended Hilbert space construction directly in the continuum theory. We show how a given TBC isolates a corresponding gauge invariant state in the extended Hilbert space, and hence compute the resulting entanglement entropy. We find that the sub-leading correction to the area law remains universal, but depends on the choice of topological boundary conditions. This agrees with the microscopic calculation of [1]. Additionally, we provide a replica path integral calculation for the entropy. In the case when the topological phases across the interface are taken to be identical, our construction gives a novel explanation of the equivalence between the left-right entanglement of (1+1)d Ishibashi states and the spatial entanglement of (2+1)d topological phases.
topic Chern-Simons Theories
Topological Field Theories
Gauge Symmetry
Topological States of Matter
url http://link.springer.com/article/10.1007/JHEP09(2017)056
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