Abstract

We consider the 6d (2, 0) theory on a fibration by genus g curves, and dimensionally reduce along the fiber to 4d theories with duality defects. This generalizes class S theories, for which the fibration is trivial. The non-trivial fibration in the present setup implies that the gauge couplings of the 4d theory, which are encoded in the complex structures of the curve, vary and can undergo S-duality transformations. These monodromies occur around 2d loci in space-time, the duality defects, above which the fiber is singular. The key role that the fibration plays here motivates refering to this setup as theories of class F. In the simplest instance this gives rise to 4d mathcal{N}=4 Super-Yang-Mills with space-time dependent coupling that undergoes SL(2, ℤ) monodromies. We determine the anomaly polynomial for these theories by pushing forward the anomaly polynomial of the 6d (2, 0) theory along the fiber. This gives rise to corrections to the anomaly polynomials of 4d mathcal{N}=4 SYM and theories of class S. For the torus case, this analysis is complemented with a field theoretic derivation of a U(1) anomaly in 4d mathcal{N}=4 SYM. The corresponding anomaly polynomial is tested against known expressions of anomalies for wrapped D3-branes with varying coupling, which are known field theoretically and from holography. Extensions of the construction to 4d mathcal{N}=0 and 1, and 2d theories with varying coupling, are also discussed.

Highlights

  • Theories of class S are 4d N = 2 supersymmetric theories, defined by dimensional reduction with a topological twist of the 6d (2, 0) superconformal field theory (SCFT) on a curve Cg,n of genus g with n punctures [1]

  • The theories we will study are a generalization of class S to fibrations and will be referred to as2 theories of class F : they are obtained by reducing the M5-brane theory on a curve C, which varies over the 4d space-time, allowing for monodromies in duality symmetries of the 4d theory, which are elements of the mapping class group MCGg

  • In this paper we extend this result to include a non-trivial R-symmetry bundle, and to include U(1)3 anomalies, and in addition we study the contribution to the U(1) anomalies, not just of the bulk N = 4 gauginos, and those from the degrees of freedom living on the duality defects when τ varies holomorphically along M4

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Summary

Introduction

To provide more depth to this proposal, let us discuss class F in the case of C = T 2 in some more detail This theory has an intrinsically 4d description in terms of 4d N = 4 SYM, with space-time dependent τ and with duality defects of complex codimension one, around which τ undergoes SL(2, Z) monodromies. We derive these contributions from duality defects by a careful analysis of the pushforward of I8 for singular elliptic fibrations: the Kodaira singularity type determines the flavor symmetries.

F is for fiber
Elliptic fibrations
Modular anomaly revisited
Anomaly polynomial of class F from 6d
Class F with torus-fibers
Class F with torus-fibers: duality defects
Σ in CY3: strings in 6d
Σ in CY4: strings in 4d
Σ in K3: strings in 8d
Extensions
Non-supersymmetric setup: self-dual tensor and 4d Maxwell theory
Conclusions and outlook
A Characteristic classes and anomaly polynomials
Summary of chararacteristic classes
Integration of anomaly polynomials
Full Text
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