Abstract

We discuss scattering in a CFT via the conformal partial-wave analysis and the Regge limit. The focus of this paper is on understanding an OPE with Minkowski conformal blocks. Starting with a t-channel OPE, it leads to an expansion for an s-channel scattering amplitude in terms of t-channel exchanges. By contrasting with Euclidean conformal blocks we see a precise relationship between conformal blocks in the two limits without preforming an explicit analytic continuation. We discuss a generic feature for a CFT correlation function having singular $F^{(M)}(u,v)\sim {u}^{-\delta}\,$, $\delta>0$, in the limit $u \rightarrow 0$ and $v\rightarrow 1$. Here, $\delta=(\ell_{eff}-1)/2$, with $\ell_{eff}$ serving as an effective spin and it can be determined through an OPE. In particular, it is bounded from above, $\ell_{eff} \leq 2$, for all CFTs with a gravity dual, and it can be associated with string modes interpolating the graviton in AdS. This singularity is historically referred to as the Pomeron. This bound is nearly saturated by SYK-like effective $d=1$ CFT, and its stringy and thermal corrections have piqued current interests. Our analysis has been facilitated by dealing with Wightman functions. We provide a direct treatment in diagonalizing dynamical equations via harmonic analysis over physical scattering regions. As an example these methods are applied to the SYK model.

Highlights

  • Most current studies in conformal field theories (CFT) are carried out in the Euclidean limit

  • The emphasis will be on first developing a Mellin-like representation for the operator product expansion (OPE) sum so that it applies to the physical scattering region

  • In this paper we have focused on scattering in CFTs, for example off-shell photon-photon scattering, through an OPE with Minkowski conformal blocks

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Summary

INTRODUCTION

Most current studies in conformal field theories (CFT) are carried out in the Euclidean limit. This is true when using Euclidean conformal blocks (ECB) in exploiting the consequences of conformal invariance [1,2,3]. Recent interest in CFT in a Minkowski setting has increased to warrant a more systematic and direct treatment.. Recent interest in CFT in a Minkowski setting has increased to warrant a more systematic and direct treatment.1 Such an approach provides a framework where one can directly treat scattering problems, for example, inclusive and exclusive high energy near-forward scattering, among others. Many phenomenological applications to high energy physics at the LHC and HERA have been carried out with encouraging successes. In this paper we demonstrate a new method for directly computing Minkowski conformal blocks (MCB) as well as elucidating details about the Minkowski conformal block expansion relevant for arbitrary dimension

Overview
Outline
THE DLC LIMIT
Kinematics
Physical regions
Eikonal scattering
MINKOWSKI CONFORMAL BLOCKS
Definitions
Indicial analysis
Explicit construction of MCB
Symmetric treatment
Higher order expansion
MINKOWSKI OPE AND SCATTERING
Sommerfeld-Watson transform
Spectral curve
Scattering for SYK-like models
Kinematics of integral equation for ImΓ
Diagonalization
Identifying the leading intercept lÃ
Analyticity and corrections
DISCUSSION AND SUMMARY
Rindler coordinates for the DLC limit
Impact parameter representation and holography
Useful mathematical facts
Standard differential equation for conformal blocks
Comparison with analytically continued Euclidean conformal blocks
Direct computation
BFKL-DGLAP equation
Minkowski Green’s functions
Mellin-like representation and polynomial boundedness
Full Text
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