Higher Form Symmetries TFT in 6d

TL;DR

This paper derives the symmetry topological field theory (TFT) for 6d (1,0) theories with 2-form and 1-form symmetries, revealing their mixing into a 3-group structure and exploring implications for anomalies and holography.

Contribution

It provides the first derivation of the symmetry TFT for 6d (1,0) theories with rank 1 tensor multiplet, including the mixing of higher-form symmetries and their holographic realization.

Findings

Derived the symmetry TFT for 6d (1,0) theories with a tensor multiplet.

Identified a 3-group structure mixing 1-form and 2-form symmetries.

Confirmed mixed anomalies via 5d Coulomb branch analysis.

Abstract

Symmetries and anomalies of a $d$-dimensional quantum field theory are often encoded in a $(d+1)$-dimensional topological action, called symmetry topological field theory (TFT). We derive the symmetry TFT for the 2-form and 1-form symmetries of 6d $(1,0)$ field theories, focusing on theories with a single tensor multiplet (rank 1). We implement this by coupling the low-energy tensor branch action to the background fields for the higher-form symmetries and by looking at the symmetry transformation rules on dynamical and background fields. These transformation rules also imply a mixing of the higher-form symmetries in a 3-group structure. For some specific and related higher rank cases, we also derive the symmetry TFT from the holographic dual IIA supergravity solutions. The symmetry TFT action contains a coupling between the 2-form symmetry and the 1-form symmetry backgrounds, which leads to a mixed anomaly between the 1-form symmetries of the 5d KK-theory obtained by circle compactification. We confirm this by a pure 5d analysis provided by the 5d effective low-energy Coulomb branch Lagrangian coupled to background fields. We also derive the symmetry TFT for 5d $SU(p)$ supersymmetric gauge theories with Chern-Simons level $q$ and for 5d theories without non-abelian gauge theory description at low-energy. Finally, we discuss the fate of the 2-form and 1-form symmetry of rank 1 6d field theories when coupled to gravity.