Abstract

We develop a new technique for computing a class of four-point correlation functions of heavy half-BPS operators in planar mathcal{N} = 4 SYM theory which admit factorization into a product of two octagon form factors with an arbitrary bridge length. We show that the octagon can be expressed as the Fredholm determinant of the integrable Bessel operator and demonstrate that this representation is very efficient in finding the octagons both at weak and strong coupling. At weak coupling, in the limit when the four half-BPS operators become null separated in a sequential manner, the octagon obeys the Toda lattice equations and can be found in a closed form. At strong coupling, we exploit the strong Szegő limit theorem to derive the leading asymptotic behavior of the octagon and, then, apply the method of differential equations to determine the remaining subleading terms of the strong coupling expansion to any order in the inverse coupling. To achieve this goal, we generalize results available in the literature for the asymptotic behavior of the determinant of the Bessel operator. As a byproduct of our analysis, we formulate a Szegő-Akhiezer-Kac formula for the determinant of the Bessel operator with a Fisher-Hartwig singularity and develop a systematic approach to account for subleading power suppressed contributions.

Highlights

  • This paper is devoted to the study of four-point correlation functions of half-BPS singletrace operators in four-dimensional maximally supersymmetric Yang-Mills theory (N = 4 SYM)

  • We develop a new technique for computing a class of four-point correlation functions of heavy half-BPS operators in planar N = 4 SYM theory which admit factorization into a product of two octagon form factors with an arbitrary bridge length

  • We show that the octagon can be expressed as the Fredholm determinant of the integrable Bessel operator and demonstrate that this representation is very efficient in finding the octagons both at weak and strong coupling

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Summary

Introduction

It was recently recognized that difficulties at weak and strong coupling can be alleviated by a judicial choice of the half-BPS operators [2] The latter are built from K scalar fields (with K ≥ 2) each carrying one unit of the R-charge. Their four-point correlation function at Born level (zero coupling constant) is given by the product of free scalar propagators stretched between the four operators in a pairwise manner (see the leftmost panel in figure 1). Choosing the half-BPS operators appropriately and taking their R-charge K to be arbitrarily large, one can ensure that the four bridges connecting the four operators in a sequential manner have a large length O(K) whereas the length of the remaining two stays finite

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