Symmetry enriched string-nets: Exactly solvable models for SET phases
Chris Heinrich, Fiona Burnell, Lukasz Fidkowski, Michael Levin
TL;DR
The paper develops symmetry-enriched string-net models to realize 2D bosonic SET phases with finite onsite symmetry $G$ using commuting-projector Hamiltonians. It hinges on a two-step gauging/ungauging procedure: first realize the gauged SET phase with a string-net model and then ungauge to obtain a $G$-symmetric model whose gauged theory matches the original string-net data, thereby realizing all braided $G$-crossed extensions of a given topological order. The construction is anchored in the Drinfeld center and $G$-extensions, and is demonstrated through multiple explicit examples, including the toric code with $e ightleftharpoons m$ symmetry, bosonic $ ext{Z}_2$ SPT, and non-Abelian doubles like $S_3$ and $A_4$, showing the framework captures both symmetry actions and anyon permutations. This provides a powerful, algorithmic path to realize, classify, and study SET phases in 2D and offers a foundation for exploring broader symmetry groups and higher dimensions. The work underscores the feasibility of physically realizing rich SET orders and paves the way for systematic construction of models with targeted symmetry actions on anyons.
Abstract
We construct exactly solvable models for a wide class of symmetry enriched topological (SET) phases. Our construction applies to 2D bosonic SET phases with finite unitary onsite symmetry group $G$ and we conjecture that our models realize every phase in this class that can be described by a commuting projector Hamiltonian. Our models are designed so that they have a special property: if we couple them to a dynamical lattice gauge field with gauge group $G$, the resulting gauge theories are equivalent to modified string-net models. This property is what allows us to analyze our models in generality. As an example, we present a model for a phase with the same anyon excitations as the toric code and with a $\mathbb{Z}_2$ symmetry which exchanges the $e$ and $m$ type anyons. We further illustrate our construction with a number of additional examples.
