Spontaneous symmetry breaking from anyon condensation

Abstract In a physical system undergoing a continuous quantum phase transition, spontaneous symmetry breaking occurs when certain symmetries of the Hamiltonian fail to be preserved in the ground state. In the traditional Landau theory, a symmetry group can break down to any subgroup. However, this n...

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Main Authors: Marcel Bischoff, Corey Jones, Yuan-Ming Lu, David Penneys
Format: Article
Language:English
Published: SpringerOpen 2019-02-01
Series:Journal of High Energy Physics
Subjects:
Online Access:http://link.springer.com/article/10.1007/JHEP02(2019)062
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spelling doaj-5848c7152029405eb234327a72c9f0ef2020-11-25T02:56:54ZengSpringerOpenJournal of High Energy Physics1029-84792019-02-012019214210.1007/JHEP02(2019)062Spontaneous symmetry breaking from anyon condensationMarcel Bischoff0Corey Jones1Yuan-Ming Lu2David Penneys3Department of Mathematics, Ohio UniversityDepartment of Mathematics, The Ohio State UniversityDepartment of Physics, The Ohio State UniversityDepartment of Mathematics, The Ohio State UniversityAbstract In a physical system undergoing a continuous quantum phase transition, spontaneous symmetry breaking occurs when certain symmetries of the Hamiltonian fail to be preserved in the ground state. In the traditional Landau theory, a symmetry group can break down to any subgroup. However, this no longer holds across a continuous phase transition driven by anyon condensation in symmetry enriched topological orders (SETOs). For a SETO described by a G-crossed braided extension C ⊆ C G × $$ \mathcal{C}\subseteq {\mathcal{C}}_G^{\times } $$ , we show that physical considerations require that a connected étale algebra A ∈ C $$ \mathcal{C} $$ admit a G-equivariant algebra structure for symmetry to be preserved under condensation of A. Given any categorical action G → EqBr( C $$ \mathcal{C} $$ ) such that g(A) ≅ A for all g ∈ G, we show there is a short exact sequence whose splittings correspond to G-equivariant algebra structures. The non-splitting of this sequence forces spontaneous symmetry breaking under condensation of A, while inequivalent splittings of the sequence correspond to different SETOs resulting from the anyon-condensation transition. Furthermore, we show that if symmetry is preserved, there is a canonically associated SETO of C A l o c $$ {\mathcal{C}}_A^{\mathrm{loc}} $$ , and gauging this symmetry commutes with anyon condensation.http://link.springer.com/article/10.1007/JHEP02(2019)062AnyonsSpontaneous Symmetry BreakingTopological Field TheoriesTopological States of Matter
collection DOAJ
language English
format Article
sources DOAJ
author Marcel Bischoff
Corey Jones
Yuan-Ming Lu
David Penneys
spellingShingle Marcel Bischoff
Corey Jones
Yuan-Ming Lu
David Penneys
Spontaneous symmetry breaking from anyon condensation
Journal of High Energy Physics
Anyons
Spontaneous Symmetry Breaking
Topological Field Theories
Topological States of Matter
author_facet Marcel Bischoff
Corey Jones
Yuan-Ming Lu
David Penneys
author_sort Marcel Bischoff
title Spontaneous symmetry breaking from anyon condensation
title_short Spontaneous symmetry breaking from anyon condensation
title_full Spontaneous symmetry breaking from anyon condensation
title_fullStr Spontaneous symmetry breaking from anyon condensation
title_full_unstemmed Spontaneous symmetry breaking from anyon condensation
title_sort spontaneous symmetry breaking from anyon condensation
publisher SpringerOpen
series Journal of High Energy Physics
issn 1029-8479
publishDate 2019-02-01
description Abstract In a physical system undergoing a continuous quantum phase transition, spontaneous symmetry breaking occurs when certain symmetries of the Hamiltonian fail to be preserved in the ground state. In the traditional Landau theory, a symmetry group can break down to any subgroup. However, this no longer holds across a continuous phase transition driven by anyon condensation in symmetry enriched topological orders (SETOs). For a SETO described by a G-crossed braided extension C ⊆ C G × $$ \mathcal{C}\subseteq {\mathcal{C}}_G^{\times } $$ , we show that physical considerations require that a connected étale algebra A ∈ C $$ \mathcal{C} $$ admit a G-equivariant algebra structure for symmetry to be preserved under condensation of A. Given any categorical action G → EqBr( C $$ \mathcal{C} $$ ) such that g(A) ≅ A for all g ∈ G, we show there is a short exact sequence whose splittings correspond to G-equivariant algebra structures. The non-splitting of this sequence forces spontaneous symmetry breaking under condensation of A, while inequivalent splittings of the sequence correspond to different SETOs resulting from the anyon-condensation transition. Furthermore, we show that if symmetry is preserved, there is a canonically associated SETO of C A l o c $$ {\mathcal{C}}_A^{\mathrm{loc}} $$ , and gauging this symmetry commutes with anyon condensation.
topic Anyons
Spontaneous Symmetry Breaking
Topological Field Theories
Topological States of Matter
url http://link.springer.com/article/10.1007/JHEP02(2019)062
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AT yuanminglu spontaneoussymmetrybreakingfromanyoncondensation
AT davidpenneys spontaneoussymmetrybreakingfromanyoncondensation
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