On the Brauer groups of symmetries of abelian Dijkgraaf-Witten theories
Jürgen Fuchs, Jan Priel, Christoph Schweigert, Alessandro Valentino
TL;DR
The work identifies and realizes the full Brauer-Picard group of symmetries for abelian Dijkgraaf–Witten theories by embedding the abstract Brauer–Picard data into gauge-theoretic surface defects. It shows that the symmetry group is generated by Aut$(A)$ (kinematical), B-fields (dynamical), and partial electric–magnetic dualities, and that each symmetry is encoded by a defect whose transmission functor acts on bulk Wilson lines via a braided auto-equivalence of ${ m D}(A) ext{-mod}$, i.e. by an element of ${ m O}_q(Aigoplus A^*)$. A central tool is the transmission functor, arising from cylinders with defects, which provides a concrete field-theoretic realization of the bijection between invertible bimodule categories and braided auto-equivalences of the center. The paper also proves that these generators suffice to generate ${ m O}_q(Aigoplus A^*)$, thereby classifying all symmetries of the bulk theory in terms of concrete gauge-theoretic data and clarifying the action on bulk Wilson lines. $
Abstract
Symmetries of three-dimensional topological field theories are naturally defined in terms of invertible topological surface defects. Symmetry groups are thus Brauer-Picard groups. We present a gauge theoretic realization of all symmetries of abelian Dijkgraaf-Witten theories. The symmetry group for a Dijkgraaf-Witten theory with gauge group a finite abelian group $A$, and with vanishing 3-cocycle, is generated by group automorphisms of $A$, by automorphisms of the trivial Chern-Simons 2-gerbe on the stack of $A$-bundles, and by partial e-m dualities. We show that transmission functors naturally extracted from extended topological field theories with surface defects give a physical realization of the bijection between invertible bimodule categories of a fusion category and braided auto-equivalences of its Drinfeld center. The latter provides the labels for bulk Wilson lines; it follows that a symmetry is completely characterized by its action on bulk Wilson lines.
