Abstract

In three dimensional ${\cal N}=4$ Chern-Simons-matter theories two independent fermionic Wilson loop operators can be defined, which preserve half of the supersymmetry charges and are cohomologically equivalent at classical level. We compute their three-loop expectation value in a convenient color sector and prove that the degeneracy is uplifted by quantum corrections. We expand the matrix model prediction in the same regime and by comparison we conclude that the quantum 1/2 BPS Wilson loop is the average of the two operators. We provide an all-loop argument to support this claim at any order. As a by-product, we identify the localization result at three loops as a correction to the framing factor induced by matter interactions. Finally, we comment on the quantum properties of the non-1/2 BPS Wilson loop operator defined as the difference of the two fermionic ones.

Highlights

  • The expectation value of 1/4 BPS operators can be computed via a matrix model average, which in turn allows for the exact computation of the 1/2 BPS circular Wilson loops if the aforementioned cohomological relation survives at quantum level

  • In this paper we have identified the correct linear combination of fermionic Wilson loops that corresponds to the quantum 1/2 BPS operator in N = 4 CS-matter theories associated to necklace quivers

  • The expectation value of 1/2 BPS Wilson loops in N = 4 CS-matter theories can be exactly evaluated through localization procedure and reduced to a matrix integral

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Summary

Cohomological equivalence

As proved in [2, 3], the classical fermionic 1/2 BPS loops are both cohomologically equivalent to the 1/4 BPS bosonic operator given in eq (2.4). If at a given order in perturbation theory we find Wψ1 = Wψ2 , comparison with the localization prediction (2.13) will provide a non-trivial equation that uniquely fixes the relative coefficient between Wψ1 and Wψ2, so leading to the correct quantum BPS fermionic operator. With this motivation in mind, we will go through the perturbative evaluation of Wψ1 and Wψ2 searching for potential differences, and match it with the weak coupling expansion of the matrix model result for W1+/4

All-loop relation between Wψ1 and Wψ2
Range-three result at three loops
Removing framing
Quantum uplift of cohomological equivalence
Discussion
A Conventions and Feynman rules
B Useful identities on the unit circle
C Parity and reality of a generic WL diagram
E Cancellation of gauge dependent terms
G Trigonometric integrations
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