Abstract

We study the action of S-duality on half-BPS Wilson loop operators in 5d mathcal{N}=1 theories. The duality is the statement that different massive deformations of a single 5d SCFT are described by different gauge theories, or equivalently that the SCFT points in parameter space of two gauge theories coincide. The pairs of dual theories that we study are realized by brane webs in type IIB string theory that are S-dual to each other. We focus on SU(2) SQCD theories with Nf ≤ 4 flavors, which are self-dual, and on SU(3) SQCD theories, which are dual to SU(2)2 quiver theories. From string theory engineering we predict that Wilson loops are mapped to dual Wilson loops under S-duality. We confirm the predictions with exact computations of Wilson loop VEVs, which we extract from the 5d half-index in the presence of auxiliary loop operators (also known as higher qq-characters) sourced by D3 branes placed in the brane webs. A special role is played by Wilson loops in tensor products of the (anti)fundamental representation, which provide a natural basis to express the S-duality action. The exact computations also reveal the presence of additional multiplicative factors in the duality map, in the form of background Wilson loops.

Highlights

  • Introduction and summary of resultsFive-dimensional SCFTs deformed by relevant operators often admit a low energy description in terms of 5d N = 1 SYM gauge theories with matter

  • We study the action of S-duality on half-BPS Wilson loop operators in 5d N = 1 theories

  • The duality is the statement that different massive deformations of a single 5d SCFT are described by different gauge theories, or equivalently that the SCFT points in parameter space of two gauge theories coincide

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Summary

Introduction and summary of results

With background Wilson loops Y1, Y2 which are given, for instance in the duality relating the SU(3) Nf = 2 to the SU(2) × SU(2) quiver without fundamental hypermultiplet These results are based on exact computations up to 2 or 3-instanton corrections and for the Wilson loops in the lowest rank representations, namely with n = 1, 2 (sometimes n = 3) and n1 + n2 ≤ 2, which is as far as we could reasonably go technically The remaining appendices contain details about the ADHM instanton computations (appendix A) and some exact results which were too voluminous to fit in the main text (appendix C)

Branes and loops
Brane setup
Half-BPS loop operators
S-duality
Half-index computations from residues
S-duality of Wilson loops
Generalization
A ADHM formulae
Single gauge node case
Linear quiver case
C Results
Full Text
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