Classical Integrability for Three-point Functions: Cognate Structure at Weak and Strong Couplings

TL;DR

This paper introduces a novel method for computing three-point functions in the SU(2) sector of $ ext{N}=4$ super Yang-Mills theory, unifying weak and strong coupling analyses through monodromy relations and analyticity arguments.

Contribution

It develops a universal approach using monodromy relations and analyticity to compute three-point functions at both weak and strong couplings, including new semi-classical formulas.

Findings

Derived compact semi-classical formulas for three-point functions at weak coupling.

Modified the strong coupling contour to align with weak coupling results.

Unified weak and strong coupling analyses through a new analyticity framework.

Abstract

In this paper, we develop a new method of computing three-point functions in the SU(2) sector of the $\mathcal{N}=4$ super Yang-Mills theory in the semi-classical regime at weak coupling, which closely parallels the strong coupling analysis. The structure threading two disparate regimes is the so-called monodromy relation, an identity connecting the three-point functions with and without the insertion of the monodromy matrix. We shall show that this relation can be put to use directly for the semi-classical regime, where the dynamics is governed by the classical Landau-Lifshitz sigma model. Specifically, it reduces the problem to a set of functional equations, which can be solved once the analyticity in the spectral parameter space is specified. To determine the analyticity, we develop a new universal logic applicable at both weak and strong couplings. As a result, compact semi-classical formulas are obtained for a general class of three-point functions at weak coupling including the ones whose semi-classical behaviors were not known before. In addition, the new analyticity argument applied to the strong coupling analysis leads to a modification of the integration contour, producing the results consistent with the recent hexagon bootstrap approach. This modification also makes the Frolov-Tseytlin limit perfectly agree with the weak coupling form.