Abstract

The 6D (2,0) theory has codimension-one symmetry defects associated to the outer-automorphism group of the underlying the simply-laced Lie algebra of ADE type. These symmetry defects give rise to twisted sectors of codimension-two defects that are either regular or irregular corresponding to simple or higher order poles of the Higgs field. In this paper, we perform a systematic study of twisted irregular codimension-two defects generalizing our earlier work in the untwisted case. In a class S setup, such twisted defects engineer 4D $\mathcal{N}=2$ superconformal field theories of the Argyres-Douglas type whose flavor symmetries are (subgroups of) nonsimply laced Lie groups. We propose formulas for the conformal and flavor central charges of these twisted theories, accompanied by nontrivial consistency checks. We also identify the 2D chiral algebra (vertex operator algebra) of a subclass of these theories and determine their Higgs branch moduli space from the associated variety of the chiral algebra.

Highlights

  • The six-dimensional (2,0) superconformal theories (SCFT) are mysterious quantum field theories that arise either as low energy descriptions of five branes in M-theory or in a decoupling limit of type-IIB string probing ADE singularities [1,2,3]

  • We review the general untwisted irregular defects, the resulting 4D N 1⁄4 2 SCFTs, as well as their physical data in Sec

  • We review the description of codimension-two Bogomol’nyi– Prasad–Sommerfield (BPS) defects in 6D (2,0) SCFTs in terms of the Higgs field and explain the class S construction of 4D N 1⁄4 2 SCFTs using the Hitchin system on a Riemann surface with defect insertions

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Summary

INTRODUCTION

The six-dimensional (2,0) superconformal theories (SCFT) are mysterious quantum field theories that arise either as low energy descriptions of five branes in M-theory or in a decoupling limit of type-IIB string probing ADE singularities [1,2,3]. A distinguished class of solutions to (1.1) and (1.2), known as the regular-semisimple type, gives rise to irregular codimension-two defects that are in one-to-one correspondence with three-fold quasihomogeneous isolated singularities of the compound Du Val (cDV) type (see Table III).. A distinguished class of solutions to (1.1) and (1.2), known as the regular-semisimple type, gives rise to irregular codimension-two defects that are in one-to-one correspondence with three-fold quasihomogeneous isolated singularities of the compound Du Val (cDV) type (see Table III).6 This connection between the two very different types of singularities is established by the observation that identical 4D N 1⁄4 2 SCFTs are engineered by (i) compactifying (2,0) SCFT on P1 with such a irregular defect inserted, and (ii) the decoupling limit of IIB string probing a cDV singularity.

BACKGROUND
TWISTED IRREGULAR DEFECTS
Classification of general twisted defects
Twisted irregular defects of regular semisimple type
A2N Class II ð3:18Þ
Physical parameters from the punctures
TWISTED THEORIES AND CENTRAL CHARGES
Classification of theories from twisted irregular defects
Flavor and conformal central charges
Twisted theories with Lagrangians
Twisted theories and non-Lagrangian conformal matter
VERTEX OPERATOR ALGEBRA OF TWISTED THEORIES
Admissible levels of the 2D current algebra
F4ða1Þ F4ða2Þ F4ða3Þ A 2 þ A1
CONCLUSION
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