2-Group Symmetries of 3-dimensional Defect TQFTs and Their Gauging

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Hauptverfasser: Carqueville, Nils, Haake, Benjamin
Format: Preprint
Veröffentlicht: 2025
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author Carqueville, Nils
Haake, Benjamin
author_facet Carqueville, Nils
Haake, Benjamin
contents A large class of symmetries of topological quantum field theories is naturally described by functors into higher categories of topological defects. Here we study 2-group symmetries of 3-dimensional TQFTs. We explain that these symmetries can be gauged to produce new TQFTs iff certain defects satisfy the axioms of orbifold data. In the special case of Reshetikhin-Turaev theories coming from $G$-crossed braided fusion categories $\mathcal C^\times_G$, we show that there are 0- and 1-form symmetries which have no obstructions to gauging. We prove that gauging the 0-form $G$-symmetry on the neutral component $\mathcal C_e$ of $\mathcal C^\times_G$ produces its equivariantisation $(\mathcal C^\times_G)^G$, which in turn features a generalised symmetry whose gauging recovers $\mathcal C_e$. If $G$ is commutative, the latter symmetry reduces to a 1-form symmetry involving the Pontryagin dual group.
format Preprint
id arxiv_https___arxiv_org_abs_2506_08178
institution arXiv
publishDate 2025
record_format arxiv
spellingShingle 2-Group Symmetries of 3-dimensional Defect TQFTs and Their Gauging
Carqueville, Nils
Haake, Benjamin
Quantum Algebra
High Energy Physics - Theory
Mathematical Physics
A large class of symmetries of topological quantum field theories is naturally described by functors into higher categories of topological defects. Here we study 2-group symmetries of 3-dimensional TQFTs. We explain that these symmetries can be gauged to produce new TQFTs iff certain defects satisfy the axioms of orbifold data. In the special case of Reshetikhin-Turaev theories coming from $G$-crossed braided fusion categories $\mathcal C^\times_G$, we show that there are 0- and 1-form symmetries which have no obstructions to gauging. We prove that gauging the 0-form $G$-symmetry on the neutral component $\mathcal C_e$ of $\mathcal C^\times_G$ produces its equivariantisation $(\mathcal C^\times_G)^G$, which in turn features a generalised symmetry whose gauging recovers $\mathcal C_e$. If $G$ is commutative, the latter symmetry reduces to a 1-form symmetry involving the Pontryagin dual group.
title 2-Group Symmetries of 3-dimensional Defect TQFTs and Their Gauging
topic Quantum Algebra
High Energy Physics - Theory
Mathematical Physics
url https://arxiv.org/abs/2506.08178