Abstract

We propose an interesting BPS/CFT correspondence playground: the correlation function of two intersecting half-BPS surface defects in four-dimensional mathcal{N} = 2 supersymmetric SU(N) gauge theory with 2N fundamental hypermultiplets. We show it satisfies a difference equation, the fractional quantum T-Q relation. Its Fourier transform is the 5-point conformal block of the {hat{mathfrak{sl}}}_N current algebra with one of the vertex operators corresponding to the N-dimensional {mathfrak{sl}}_N representation, which we demonstrate with the help of the Knizhnik-Zamolodchikov equation. We also identify the correlator with a state of the {XXX}_{{mathfrak{sl}}_2} spin chain of N Heisenberg-Weyl modules over Y ( {mathfrak{sl}}_2 ). We discuss the associated quantum Lax operators, and connections to isomonodromic deformations.

Highlights

  • Distinct realms of theoretical physics find themselves connected through supersymmetric field theories

  • We propose an interesting BPS/CFT correspondence playground: the correlation function of two intersecting half-BPS surface defects in four-dimensional N = 2 supersymmetric SU(N ) gauge theory with 2N fundamental hypermultiplets

  • We show that the insertion of a vortex-string type surface defect transverse to the regular monodromy defect on the BPS side amounts to the insertion of the N -dimensional representation of slN on the CFT side

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Summary

Introduction

Distinct realms of theoretical physics find themselves connected through supersymmetric field theories. As the additional evidence for the BPS/CFT correspondence, the fractional quantum T-Q equation is the Fourier transform of the KZ equations for the 4-point conformal block with additional insertion of a degenerate field It is an extension of the statement that the vacuum expectation value of the regular orbifold surface defect in the SU(N ) gauge theory with 2N fundamental hypermultiplets obeys the KZ equation obeyed by the 4-point slN conformal block [43].

Surface defects from folded branes
The bulk gauge theory
Introducing surface defects from folded branes: the Q-observables
Bulk theory with just one qq-character
Bulk theory with the surface defect Q-observable and the qq-character
Intersecting surface defects from branes on orbifold
Orbifold surface defect as the disorder operator
Construction of the surface defect via an orbifold
Vacuum expectation value of the surface defect observable
Folded branes on orbifold and fractional Q-observables
Fractional qq-characters
With fractional Q-observables
Quantum T-Q equations as Dyson-Schwinger equations
Quantum T-Q equations
Fractional quantum T-Q equations
The vortex string defect
Fourier transform to vortex string defect
On the intersection of surface defects
Knizhnik-Zamolodchikov equations
Some representations of slN
Degenerate 5-point correlation function
Knizhnik-Zamolodchikov equations from the T-Q equations
The y-component
The q-component
XXXsl2 spin chain
Construction of Lax operators
Transfer matrix and higher rank qq-characters
Similarity with the spin chain transfer matrix
Discussion
Full Text
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