Generating functions and large-charge expansion of integrated correlators in N=4 supersymmetric Yang-Mills theory
Abstract
We recently proved that, when integrating out spacetime dependence with a certain measure, four-point correlators O2O2O(i)p O(j)p in SU(N) N=4 super Yang-Mills are governed by a universal Laplace-difference equation. Here O(i)p is a superconformal primary with charge p and degeneracy i. These observables, called integrated correlators, are modular functions of coupling τ. The Laplace-difference equation relates integrated correlators of different charges recursively. In this paper, we introduce generating functions for the integrated correlators that sum over the charge. By utilising the Laplace-difference equation, we determine the generating functions given initial data. We show that the transseries of the integrated correlators in the large-p (large-charge) expansion consists of three parts: 1) is independent of τ as a power series in 1/p, plus an additional (p) term if i=j; 2) is a power series in 1/p, with coefficients given by a sum of the non-holomorphic Eisenstein series; 3) is a sum of exponentially decayed modular functions in the large-p limit, which can be viewed as a generalisation of the non-holomorphic Eisenstein series. When i=j, there is an additional modular function that is independent of p and is determined by the integrated correlator with p=2. The Laplace-difference equation was obtained with a reorganisation of the operators that means the large-charge limit is taken in a particular way here. From the SL(2,Z)-invariant results, we also determine the generalised 't Hooft genus expansion and associated large-p non-perturbative corrections of the integrated correlators by introducing λ = pg2YM. The generating functions have subtle differences between even and odd N with important consequences in resurgence.
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