Abstract

In order to obtain the SymTFT for a theory with an NN-ality extension of a discrete, Abelian group GG, one begins by considering a bulk GG-gauge theory, and then gauges an appropriate ZN\mathbb{Z}_N symmetry. This procedure involves three choices: the choice of a suitable bulk ZN\mathbb{Z}_N symmetry, of a fractionalization class, and of a discrete torsion. The first choice is, somewhat surprisingly, the most involved, and in this paper we discuss it in detail. In particular, we show that the choice of bulk ZN\mathbb{Z}_N symmetry determines all boundary FF-symbols with a single incoming NN-ality defect, and that any theory with an NN-ality symmetry is invariant under a certain twisted gauging given in terms of these FF-symbols. These FF-symbols can furthermore be input into the pentagon identities to obtain the other FF-symbols, up to freedoms related to the choices appearing in the second and third steps of bulk gauging. Although many of our results hold for general NN, we restrict ourselves in some places to the case of N=pN=p prime. In particular, for generic triality defects, we acquire explicit FF-symbols which are reminiscent of those in Tambara-Yamagami fusion categories.

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