Abstract

We describe general methods for determining higher-form symmetry groups of known 5d and 6d superconformal field theories (SCFTs), and 6d little string theories (LSTs). The 6d theories can be described as supersymmetric gauge theories in 6d which include both ordinary non-abelian 1-form gauge fields and also abelian 2-form gauge fields. Similarly, the 5d theories can also be often described as supersymmetric non-abelian gauge theories in 5d. Naively, the 1-form symmetry of these 6d and 5d theories is captured by those elements of the center of ordinary gauge group which leave the matter content of the gauge theory invariant. However, an interesting subtlety is presented by the fact that some massive BPS excitations, which includes the BPS instantons, are charged under the center of the gauge group, thus resulting in a further reduction of the 1-form symmetry. We use the geometric construction of these theories in M/F-theory to determine the charges of these BPS excitations under the center. We also provide an independent algorithm for the determination of 1-form symmetry for 5d theories that admit a generalized toric construction (i.e. a 5-brane web construction). The 2-form symmetry group of 6d theories, on the other hand, is captured by those elements of the center of the abelian 2-form gauge group that leave all the massive BPS string excitations invariant, which is much more straightforward to compute as it is encoded in the Green-Schwarz coupling associated to the 6d theory.

Highlights

  • We describe general methods for determining higher-form symmetry groups of known 5d and 6d superconformal field theories (SCFTs), and 6d little string theories (LSTs)

  • We provide an independent algorithm for the determination of 1-form symmetry for 5d theories that admit a generalized toric construction (i.e. a 5-brane web construction)

  • In 5d recent progress has been made in mapping out and furthering the classification of SCFTs using the M-theory realization on canonical singularities [8,9,10,11,12,13,14,15,16,17,18,19,20,21,22,23,24,25]

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Summary

Higher-form symmetries of 6d SCFTs and LSTs

This section is devoted to the study of higher-form symmetries in supersymmetric 6d theories. The theory on the tensor branch carries massive BPS string excitations in one-to-one correspondence with a special basis for these tensor multiplets These strings are charged under the 2-form gauge fields living in the tensor multiplets. See [21] for more details on this notation in the context of 6d SCFTs. If we forget about the BPS strings for a moment, there is a U(1) 2-form symmetry associated to each tensor multiplet i under which the “Wilson surface” for the 2-form gauge field living within the tensor multiplet i has charge 1. The structure of 6d LSTs is similar to that of 6d SCFTs, the crucial difference being that the matrix Ωij is only positive semi-definite for 6d LSTs. Naively, one might expect that the 2-form symmetry group for an LST would be captured by the quotient lattice.

Examples
Relative nature of 6d SCFTs and LSTs
F Λ2 Λ3 S2 F S F Λ2 Λ3 FSCFSCF
Untwisted case
Twisted case
Geometric analysis
Brane-web and GTP analysis
Full Text
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