Abstract

We study 1/2 BPS Wilson loops in 3d $\mathcal{N}=4$ $U(N)$ Yang-Mills theory with one adjoint and $N_f$ fundamental hypermultiplets from the Fermi gas approach. By numerical fitting, we find the first few worldsheet instanton corrections to the Wilson loops with winding numbers 1, 2 and 3. We verify that our Fermi gas results are consistent with the matrix model results in the planar limit.

Highlights

  • Correctly reproduces the N 3/2 scaling of free energy expected from the holographically dual M-theory on AdS4 × S7/Zk [4]

  • We will study the vacuum expectation value (VEV) of 1/2 BPS Wilson loops in the Nf matrix model

  • We have studied the Wilson loops in the Nf matrix model from the Fermi gas approach

Read more

Summary

Review of Nf matrix model

The gauge kinetic term is irrelevant in IR and the S3 partition function of this theory is independent of the gauge coupling. This theory flows to a superconformal fixed point in the IR, which is conjectured to be holographically dual to M-theory on AdS4 × S7/ZNf. Using the supersymmetric localization, the S3 partition function is reduced to a finite dimensional integral [19], which is dubbed the Nf matrix model in [14]. In the large N limit, the integral (2.8) can be evaluated by the saddle point approximation, where the saddle point value μ∗ of the chemical potential is given by μ∗ ≈ Plugging this value μ∗ into the perturbative part of grand potential, we recover the N 3/2 behavior of free energy.

Wilson loops in Nf matrix model
Computation of trace
Odd winding number
Perturbative part
Instanton corrections
Fundamental representation
WKB expansion
Nf π sin πs
Planar solution of Nf matrix model
Planar resolvent
Planar free energy
Results of matrix model
Comparison with Fermi gas
Conclusions
Full Text
Paper version not known

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.