Abstract

We study four-point functions of scalars, conserved currents, and stress tensors in a conformal field theory, generated by a local contact term in the bulk dual description, in two different causal configurations. The first of these is the standard Regge configuration in which the chaos bound applies. The second is the ‘causally scattering configuration’ in which the correlator develops a bulk point singularity. We find an expression for the coefficient of the bulk point singularity in terms of the bulk S matrix of the bulk dual metric, gauge fields and scalars, and use it to determine the Regge scaling of the correlator on the causally scattering sheet in terms of the Regge growth of this S matrix. We then demonstrate that the Regge scaling on this sheet is governed by the same power as in the standard Regge configuration, and so is constrained by the chaos bound, which turns out to be violated unless the bulk flat space S matrix grows no faster than s2 in the Regge limit. It follows that in the context of the AdS/CFT correspondence, the chaos bound applied to the boundary field theory implies that the S matrices of the dual bulk scalars, gauge fields, and gravitons obey the Classical Regge Growth (CRG) conjecture.

Highlights

  • It has recently been conjectured that the tree level S matrix of any ‘consistent’1 classical theory never grows faster with s than s2 in the Regge limit

  • We study four-point functions of scalars, conserved currents, and stress tensors in a conformal field theory, generated by a local contact term in the bulk dual description, in two different causal configurations

  • We find an expression for the coefficient of the bulk point singularity in terms of the bulk S matrix of the bulk dual metric, gauge fields and scalars, and use it to determine the Regge scaling of the correlator on the causally scattering sheet in terms of the Regge growth of this S matrix

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Summary

Introduction

It has recently been conjectured that the tree level S matrix of any ‘consistent’ classical theory never grows faster with s than s2 in the Regge limit. In this paper we demonstrate that the four-point function generated holographically by a local bulk contact term for scalars, gauge fields, or the metric necessarily violates the chaos bound whenever the flat space S matrix generated by the same contact term violates the CRG conjecture. As the insertion parameters θ and τ run over the range of study (2.2), the conformal cross ratios σ and ρ (or equivalently z and z -see around (2.6) for definitions) range over three different sheets in the complex cross ratio space corresponding to three distinct causal configurations (2.3) of the boundary points. Recall that the chaos bound theorem of [1] implies (see the appendix of that paper and section 6 for a brief review) that the correlator for a well behaved (unitary etc) boundary theory cannot grow faster than 1 σ in the small σ limit on the causally. The chaos bound applied to boundary correlators of a unitary theory implies that the bulk dual of that theory obeys the CRG conjecture

Insertion locations
Conformal cross ratios
Overlap between small τ and Regge
A path in cross ratio space
The same path on the complex cross ratio sheets
Summary of the trajectory in the complex plane
Intersections of boundary lightcones
Scaling limits of the two point function
Regge scaling
Small τ limit In the limit in which τ is taken to zero
Scaling with θ
Analyticity in a
Analyticity in the cross ratio e2ρ
Regge scaling of normalized correlators
Modulated propagators
Wave representation for propagators
Scalar φ4 correlator in AdS3
General scalar contact correlator in AdS3
Contact interactions involving gauge bosons and gravitons
The spin one propagator
Singularity in terms of scattering
Transforming to standard graviton polarizations
4.10 Regge scaling of normalized correlators
Inter relationship between the small θ and small a expansion
CRG conjecture from the chaos bound
Discussion and conclusions
Conformal cross ratios and intersection lightcones for four boundary points
Full Text
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