Abstract

Classical field configurations such as the Coulomb potential and Schwarzschild solution are built from the t-channel exchange of many light degrees of freedom. We study the CFT analog of this phenomenon, which we term the `eikonalization' of conformal blocks. We show that when an operator $T$ appears in the OPE $\mathcal{O}(x) \mathcal{O}(0)$, then the large spin $\ell$ Fock space states $[TT \cdots T]_{\ell}$ also appear in this OPE with a computable coefficient. The sum over the exchange of these Fock space states in an $\langle \mathcal{O} \mathcal{O} \mathcal{O} \mathcal{O} \rangle$ correlator build the classical `$T$ field' in the dual AdS description. In some limits the sum of all Fock space exchanges can be represented as the exponential of a single $T$ exchange in the 4-pt correlator of $\mathcal{O}$. Our results should be useful for systematizing $1/\ell$ perturbation theory in general CFTs and simplifying the computation of large spin OPE coefficients. As examples we obtain the leading $\log \ell$ dependence of Fock space conformal block coefficients, and we directly compute the OPE coefficients of the simplest `triple-trace' operators.

Highlights

  • Introduction and summaryThe correlation functions of local operators in Conformal Field Theories (CFTs) must satisfy fundamental consistency conditions encoding conformal symmetry and quantum mechanical unitarity

  • We show that when an operator T appears in the operator product expansion (OPE) O(x)O(0), the large spin Fock space states [T T · · · T ] appear in this OPE with a computable coefficient

  • The non-universal behavior of the [T T ]n, OPE coefficients dictates the existence of other operators in the O1(x)O2(0) OPE

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Summary

Introduction and summary

The correlation functions of local operators in Conformal Field Theories (CFTs) must satisfy fundamental consistency conditions encoding conformal symmetry and quantum mechanical unitarity. These results hold in the limit → ∞ with the external dimensions ∆i fixed, which has the AdS interpretation of the exchange of well-separated light mediators between two objects with fixed energy. The universal contributions to exchanged conformal blocks that we derive here arise instead from the approximate Fock space structure of CFT operators at large spin We refer to this behavior as the ‘eikonalization’ of conformal blocks because of its exponentiated structure at large ∆i, suggesting a similar interpretation in terms of classical background fields in AdS.

CFT spectra from the bottom up
Review of cluster decomposition and double-trace operators
Anomalous dimensions from minimal twist operators
Semi-classical Virasoro blocks and eikonalization
Eikonalization at large spin
Exponentiation of large spin operators and AdS field theory
Explicit construction of large- ‘multi-trace’ modes
Large spin OPE coefficients from a boostrap analysis
Exchange of Oi in the lightcone OPE limit
OPE limits and direct extraction of large spin operators
Conformal blocks in their cross-channel OPE limit
Existence of the OPE and boundedness of Mellin amplitudes
Universality of large spin OPE coefficients and a theorem of Darboux
Future directions
A Lightcone formulation of correlation functions
Lightcone subgroup and four-point functions
Conformal blocks and lightcone OPE limit
B Scalar conformal blocks at small u
C Details of Mellin asymptotics
Exponentiation of currents
Virasoro blocks and graviton mixing
Full Text
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