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Gauge theories from principally extended disconnected gauge groups

Antoine Bourget, Alessandro Pini, Diego Rodriguez-Gomez

TL;DR

This work introduces principal extensions $\widetilde{G}=G\rtimes\Gamma$ as a principled way to gauge charge conjugation by enlarging the gauge group to a disconnected Lie group. Focusing on $\widetilde{\mathrm{SU}}(N)$, it develops the necessary group-theoretic machinery—representations, invariants, and Weyl integration formulas—and applies standard 4d $\mathcal{N}=2$ gauge-theory machinery to build SQCD-like theories with vector multiplets in the adjoint and real bifundamental-like hypermultiplets. A key result is that the Coulomb branch of $\widetilde{\mathrm{SU}}(N)$ is typically not freely generated (e.g., for $N\ge5$), as revealed by the Coulomb branch index and invariant theory, while the Higgs branch Hilbert series shows a modified global symmetry: $\mathrm{SO}(N_f)$ for even $N$ and $\mathrm{Sp}(\lfloor N_f/2\rfloor)$ for odd $N$. These findings highlight new IR structures, motivate extensions to quiver constructions and large-$N$ analyses, and suggest interesting avenues for string embeddings and class-$\mathcal{S}$ connections.

Abstract

We introduce gauge theories based on a class of disconnected gauge groups, called principal extensions. Although in this work we focus on 4d theories with N=2 SUSY, such construction is independent of spacetime dimensions and supersymmetry. These groups implement in a consistent way the discrete gauging of charge conjugation, for arbitrary rank. Focusing on the principal extension of SU(N), we explain how many of the exact methods for theories with 8 supercharges can be put into practice in that context. We then explore the physical consequences of having a disconnected gauge group: we find that the Coulomb branch is generically non-freely generated, and the global symmetry of the Higgs branch is modified in a non-trivial way.

Gauge theories from principally extended disconnected gauge groups

TL;DR

This work introduces principal extensions as a principled way to gauge charge conjugation by enlarging the gauge group to a disconnected Lie group. Focusing on , it develops the necessary group-theoretic machinery—representations, invariants, and Weyl integration formulas—and applies standard 4d gauge-theory machinery to build SQCD-like theories with vector multiplets in the adjoint and real bifundamental-like hypermultiplets. A key result is that the Coulomb branch of is typically not freely generated (e.g., for ), as revealed by the Coulomb branch index and invariant theory, while the Higgs branch Hilbert series shows a modified global symmetry: for even and for odd . These findings highlight new IR structures, motivate extensions to quiver constructions and large- analyses, and suggest interesting avenues for string embeddings and class- connections.

Abstract

We introduce gauge theories based on a class of disconnected gauge groups, called principal extensions. Although in this work we focus on 4d theories with N=2 SUSY, such construction is independent of spacetime dimensions and supersymmetry. These groups implement in a consistent way the discrete gauging of charge conjugation, for arbitrary rank. Focusing on the principal extension of SU(N), we explain how many of the exact methods for theories with 8 supercharges can be put into practice in that context. We then explore the physical consequences of having a disconnected gauge group: we find that the Coulomb branch is generically non-freely generated, and the global symmetry of the Higgs branch is modified in a non-trivial way.

Paper Structure

This paper contains 15 sections, 74 equations, 2 figures, 3 tables.

Figures (2)

  • Figure 1: Summary of the global symmetries of QCD with gauge group $\mathrm{SU}(N)$ and $\widetilde{\mathrm{SU}}(N)$ and $N_f$ flavors.
  • Figure 2: Dynkin diagram automorphisms.