Toward Null State Equations in $d>2$

TL;DR

This paper extends the understanding of heavy-light scalar correlators in large central charge CFTs from two to higher dimensions, deriving new differential equations that match known holographic and bootstrap results.

Contribution

It introduces a new class of differential equations governing near-lightcone correlators in four-dimensional CFTs with large central charge, generalizing the 2D BPZ equation.

Findings

Derived a new PDE $x^3 u_{xxxy}+u=0$ for 4D CFT correlators.

Showed solutions reproduce known holographic and bootstrap results.

Extended the framework to cases with $ ext{dim}=-2,-3$.

Abstract

In two-dimensional CFTs with a large central charge, the level-two BPZ equation governs the heavy-light scalar four-point correlator when the light probe scalar has dimension $h= - {1\over 2}$; the corresponding linear ordinary differential equation can be recast into a schematic form $x^2 u_{xx}+u=0$. In this paper, we make an observation that in a class of four-dimensional CFTs with a large central charge, the heavy-light scalar correlator in the near-lightcone limit obeys a similar equation, $x^3 u_{xxxy}+u=0$, when the light scalar has dimension $\Delta=-1$. We focus on the multi-stress tensor sector of the theory and also discuss the corresponding equations for the cases with $\Delta = -2, -3$. The solutions to these linear partial differential equations in higher dimensions are shown, after a suitable change of variables, to reproduce the near-lightcone correlators previously obtained via holography and the conformal bootstrap.