Abstract

We study the vacuum moduli spaces of 3d $$ \mathcal{N}=2 $$ supersymmetric quantum field theories by applying the formalism developed in our previous paper [1]. The 3d theories can be realized by branes in type IIB string theory, which in a decoupling limit reduce to 4d $$ \mathcal{N}=4 $$ super-Yang-Mills theory on an interval with BPS defects inserted. The moduli space of a given 3d theory is obtained by solving a generalization of Nahm’s equations with appropriate boundary/junction conditions, along with help from the S-duality of type IIB string theory. Our classical computations reproduce many known results about the quantum-corrected moduli spaces of 3d theories, e.g. U(N c ) theories with N f flavors with mass and FI parameters turned on. In particular, our methods give first-principles derivations of several results in the literature, including the s-rule, quantum splitting of classical Coulomb branches, the lifting of the Coulomb branch by non-Abelian instantons, quantum merging of Coulomb and Higgs branches, and phase transitions from re-ordering 5-branes.

Highlights

  • String theory enjoys many deep connections with quantum field theory

  • We study the vacuum moduli spaces of 3d N = 2 supersymmetric quantum field theories by applying the formalism developed in our previous paper [1]

  • By combining the expectations based on ζr → 0 limit of columns (a) and (d), we infer the structure of the undeformed moduli space as intersections of a three dimensional Higgs branch and two Coulomb branches illustrated at the bottom of figure 14

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Summary

Introduction

String theory enjoys many deep connections with quantum field theory. For example, the solitonic objects of string theory such as D-branes support gauge fields living on the brane worldvolume. In [1], we performed a study of interface conditions for N = 4 super-Yang-Mills theory, and explicitly constructed UV Lagrangians for such defect systems. These defect systems realize 3d N = 2 field theories in the IR, and can be constructed from type IIB brane configurations with D3-branes (which support the 4d N = 4 theory) suspended between 5-brane defects. This happens when the gauge symmetry is completely broken In this Sduality frame, our classical computation gives the quantum-corrected moduli space.

Moduli space from generalized Nahm equations
Bulk BPS equations
Gauge symmetry breaking and X9
GC quotient and stability
Example: the conifold
Nahm pole
Constraints from the s-rule
Real mass and FI deformations
Complex mass deformation
D5—1D3—NS5—1D3—NS5 —1D3—D5
D5—1D3—NS5 —1D3—NS5—1D3—D5
Vortices and skyrmions in defect theories
Analysis in the electric theory
Analysis in the S-dual
Real mass deformations
Discussion

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