Abstract

We study in general spacetime dimension the symmetry of the theory obtained by gauging a non-anomalous finite normal Abelian subgroup AA of a ΓΓ-symmetric theory. Depending on how anomalous ΓΓ is, we find that the symmetry of the gauged theory can be i) a direct product of G=Γ/AG=Γ/A and a higher-form symmetry A^\hat A with a mixed anomaly, where A^\hat A is the Pontryagin dual of AA; ii) an extension of the ordinary symmetry group GG by the higher-form symmetry A^\hat A; iii) or even more esoteric types of symmetries which are no longer groups. We also discuss the relations to the effect called the H3(G,A^)H^3(G,\hat A) symmetry localization obstruction in the condensed-matter theory and to some of the constructions in the works of Kapustin-Thorngren and Wang-Wen-Witten.

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