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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Bibliographic Details
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
Description
Summary: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.
ISSN:1029-8479