Abstract

We study momentum space dispersion formulas in general QFTs and their applications for CFT correlation functions. We show, using two independent methods, that QFT dispersion formulas can be written in terms of causal commutators. The first derivation uses analyticity properties of retarded correlators in momentum space. The second derivation uses the largest time equation and the defining properties of the time-ordered product. At four points we show that the momentum space QFT dispersion formula depends on the same causal double-commutators as the CFT dispersion formula. At n-points, the QFT dispersion formula depends on a sum of nested advanced commutators. For CFT four-point functions, we show that the momentum space dispersion formula is equivalent to the CFT dispersion formula, up to possible semi-local terms. We also show that the Polyakov-Regge expansions associated to the momentum space and CFT dispersion formulas are related by a Fourier transform. In the process, we prove that the momentum space conformal blocks of the causal double-commutator are equal to cut Witten diagrams. Finally, by combining the momentum space dispersion formulas with the AdS Cutkosky rules, we find a complete, bulk unitarity method for AdS/CFT correlators in momentum space.

Highlights

  • In the past decade, there has been a resurgence of interest in studying quantum field theory (QFT) and quantum gravity with bootstrap methods

  • We study momentum space dispersion formulas in general QFTs and their applications for conformal field theories (CFTs) correlation functions

  • At four points we show that the momentum space QFT dispersion formula depends on the same causal double-commutators as the CFT dispersion formula

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Summary

Introduction

There has been a resurgence of interest in studying quantum field theory (QFT) and quantum gravity with bootstrap methods. The conformal bootstrap uses unitarity, causality, and locality to derive rigorous bounds on the space of conformal field theories (CFTs) [1, 2]. Lorentzian methods have played a central role in the analytic conformal bootstrap, including the discovery of the large-spin expansion [3,4,5,6], the Lorentzian inversion formula [7], and the conformal dispersion formula [8]. S-matrix dispersion formulas are derived by leveraging the analyticity properties of scattering amplitudes [9, 59, 61, 62]. To derive a dispersion formula, we first express the amplitude in terms of a contour integral,

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