Abstract

We study a class of 4-dimensional SU(N) chiral gauge theories with fermions in the 2-index symmetric and antisymmetric representations and classify their infrared phases. The choice N = 4ℤ corresponds to gauging the fermion number and makes the theory purely bosonic. We examine the most general background fields of the centers of the gauge, non-abelian flavor, and U(1)-axial groups that can be consistently activated, thereby determine the faithful global continuous and discrete symmetries of the theory. This allows us to identify new mixed 0-form/1-form ‘t Hooft anomalies on both spin and nonspin manifolds. If the theory confines, the absence of composite fermions implies that continuous symmetries must be broken down to anomaly-free subgroups. Anomalies associated with discrete symmetries can be saturated either by breaking the symmetry or by a symmetry-preserving topological quantum field theory (TQFT). The latter, however, is obstructed on spin manifold. The interplay between these features greatly restricts the possible infrared physics. We present two examples that demonstrate our approach. We argue that if the theory confines, the zoo of anomalies and TQFT obstruction greatly restrict the viable infrared condensates. We also discuss the possibility that some theories flow to a conformal fixed point.

Highlights

  • Part stems from the fact that putting these theories on a lattice and taking the continuum limit, hoping to learn about their infrared (IR) phases, is still far from being straightforward

  • Anomalies associated with discrete symmetries can be saturated either by breaking the symmetry or by a symmetrypreserving topological quantum field theory (TQFT)

  • We show that the IR phase is described by a non-linear sigma model associated with the symmetry breaking (SU(3) × U(1))/(Z4 × Z3) → SU(2) and domain walls from dχ

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Summary

Chiral gauge theories with 2-index fermions

We describe a class of chiral gauge theories whose fermion content consists of 2-index symmetric and 2-index anti-symmetric representations of the gauge group SU(N ). We discuss the global symmetries of the theory in detail and carefully identify the most general possible background fields that can be turned on. The latter will be used to identify the faithful global symmetry and will lead to an additional set of ‘t Hooft anomalies. This provides a refined probe of the theory and results in extra constraints on the allowed IR phases

The UV theory
Symmetries
Theory on spin manifolds
Theory on nonspin manifolds
Matching the anomalies in the IR
Absence of composite fermions
Unbroken discrete symmetry
Broken continuous symmetries: the Wess-Zumnio-Witten term
Broken discrete symmetries
Confinement with chiral symmetry breaking
Anomalies on spin manifold
CFU anomalies on nonspin manifold
Flow to an IR Conformal Field Theory
Vacuum condensates and IR phase
A The independent discrete symmetry
C Descending in the CFU background fluxes
D The 3-loop β-function and IR fixed points
Full Text
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