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 TT appears in the OPE O(x)O(0)\mathcal{O}(x) \mathcal{O}(0), then the large spin ℓ\ell Fock space states [TT⋯T]ℓ[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 ⟨OOOO⟩\langle \mathcal{O} \mathcal{O} \mathcal{O} \mathcal{O} \rangle correlator build the classical `TT 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 TT exchange in the 4-pt correlator of O\mathcal{O}. Our results should be useful for systematizing 1/ℓ1/\ell perturbation theory in general CFTs and simplifying the computation of large spin OPE coefficients. As examples we obtain the leading log⁡ℓ\log \ell dependence of Fock space conformal block coefficients, and we directly compute the OPE coefficients of the simplest `triple-trace' operators.

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