We present a method that computes Wilson loops in ABJM theory, highlighting new relations and resolving discrepancies with numerical data.
A bstract We present a new technique for computing supersymmetric Wilson loops in the ABJM theory via supersymmetric localization, valid for arbitrary values of the rank of the gauge group N and the Chern-Simons level k . The approach relies on an operator representation of the Wilson loops within the Fermi gas formalism in terms of the resolvent of a certain integral operator previously encountered in the computation of the ABJM partition function on the round three-sphere. By deriving a set of nontrivial relations for this resolvent, we obtain exact expressions for the generating functions of Wilson loops in terms of the partition function. For large k , these expressions reproduce the weak-coupling expansion of the Wilson loops, and in the large- N limit at fixed k they match previously obtained high-precision numerical results. This analysis also resolves the longstanding discrepancy between numerical data and the semiclassical expression for the 1/6 BPS Wilson loop.
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Boldis et al. (2026) studied this question.
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