Spontaneous symmetry breaking from anyon condensation
Open Access
- 12 February 2019
- journal article
- research article
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2019 (2) , 62
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 aG-crossed braided extension $$ \mathcal{C}\subseteq {\mathcal{C}}_G^{\times } $$ , we show that physical considerations require that a connected étale algebraA∈ $$ \mathcal{C} $$ admit aG-equivariant algebra structure for symmetry to be preserved under condensation ofA. Given any categorical actionG →EqBr( $$ \mathcal{C} $$ ) such thatg(A) ≅Afor allg∈G, we show there is a short exact sequence whose splittings correspond toG-equivariant algebra structures. The non-splitting of this sequence forces spontaneous symmetry breaking under condensation ofA, 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 $$ {\mathcal{C}}_A^{\mathrm{loc}} $$ , and gauging this symmetry commutes with anyon condensation.
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