2-Group Global Symmetries and Anomalies in Six-Dimensional Quantum Field Theories

TL;DR

This paper explores how higher-form symmetries and their anomalies in six-dimensional quantum field theories lead to the emergence of 2-group symmetries, with implications for classifying SCFTs and their anomalies.

Contribution

It demonstrates the presence of 2-group global symmetries in 6D theories due to mixed anomalies and provides an algorithm to compute 't Hooft anomalies for SCFTs from their tensor branch spectrum.

Findings

2-group symmetries arise from mixed anomalies in 6D theories.

SCFTs lack these anomalies, unlike little string theories.

The $a$-anomaly in all SCFTs with a tensor branch is positive.

Abstract

We examine six-dimensional quantum field theories through the lens of higher-form global symmetries. Every Yang-Mills gauge theory in six dimensions, with field strength $f^{(2)}$, naturally gives rise to a continuous 1-form global symmetry associated with the 2-form instanton current $J^{(2)} \sim * \text{Tr} \left( f^{(2)} \wedge f^{(2)}\right)$. We show that suitable mixed anomalies involving the gauge field $f^{(2)}$ and ordinary 0-form global symmetries, such as flavor or Poincar\'e symmetries, lead to continuous 2-group global symmetries, which allow two flavor currents or two stress tensors to fuse into the 2-form current $J^{(2)}$. We discuss several features of 2-group symmetry in six dimensions, many of which parallel the four-dimensional case. The majority of six-dimensional supersymmetric conformal field theories (SCFTs) and little string theories have infrared phases with non-abelian gauge fields. We show that the mixed anomalies leading to 2-group symmetries can be present in little string theories, but that they are necessarily absent in SCFTs. This allows us to establish a previously conjectured algorithm for computing the 't Hooft anomalies of most SCFTs from the spectrum of weakly-coupled massless particles on the tensor branch of these theories. We then apply this understanding to prove that the $a$-type Weyl anomaly of all SCFTs with a tensor branch must be positive, $a > 0$.