Abstract

Conformal blocks are the fundamental, theory-independent building blocks in any CFT, so it is important to understand their holographic representation in the context of AdS/CFT. We describe how to systematically extract the holographic objects which compute higher-point global (scalar) conformal blocks in arbitrary spacetime dimensions, extending the result for the four-point block, known in the literature as a geodesic Witten diagram, to five- and six-point blocks. The main new tools which allow us to obtain such representations are various higher-point propagator identities, which can be interpreted as generalizations of the well-known flat space star-triangle identity, and which compute integrals over products of three bulk-to-bulk and/or bulk-to-boundary propagators in negatively curved spacetime. Using the holographic representation of the higher-point conformal blocks and higher-point propagator identities, we develop geodesic diagram techniques to obtain the explicit direct-channel conformal block decomposition of a broad class of higher-point AdS diagrams in a scalar effective bulk theory, with closed-form expressions for the decomposition coefficients. These methods require only certain elementary manipulations and no bulk integration, and furthermore provide quite trivially a simple algebraic origin of the logarithmic singularities of higher-point tree-level AdS diagrams. We also provide a more compact repackaging in terms of the spectral decomposition of the same diagrams, as well as an independent discussion on the closely related but computationally simpler framework over p-adics which admits comparable statements for all previously mentioned results.

Highlights

  • Into a combination of two- and three-point functions, which are fixed entirely by conformal invariance, up to an overall constant for the three-point function given by the OPE coefficient

  • In this paper we presented new results establishing the holographic duals of global scalar conformal blocks for the five-point block (equations (2.18)–(2.19)), and the six-point block in the OPE channel (equations (2.22)–(2.23)) in p-adic AdS/CFT, and the six-point block in the OPE channel in conventional AdSd+1/CFTd (equations (4.15)–(4.17)), following the techniques introduced in ref. [70] where the dual of the global five-point block in conventional AdSd+1/CFTd was obtained

  • In contrast with the four-point block, whose holographic dual is a single tree-level four-point AdS exchange diagram except with all AdS integrations replaced with geodesic integrals, the precise holographic representations for higher-point blocks turn out to be more complicated for a number of reasons

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Summary

A p-adicetude

We will be focusing on the computationally simpler setup of p-adic AdS/CFT. One of the practical benefits of the p-adic AdS/CFT setup of refs. The putative dual conformal field theory lives on the boundary of the Bruhat-Tits tree described by the projective line over the p-adic numbers (or some appropriate extension of p-adic numbers).

Propagator identities on the Bruhat-Tits tree
Holographic duals of five- and six-point conformal blocks
Conformal block decomposition of bulk diagrams
Logarithmic singularities
Propagator identities in AdS
Propagator identities involving two propagators
Holographic dual of the six-point block in the OPE channel
OPE limit
Eigenfunction of conformal Casimirs
Conformal block decomposition via geodesic diagrams
Five-point exchange diagrams
Six-point diagrams
Algebraic origin of logarithmic singularities
Spectral decomposition of AdS diagrams
Discussion
A Spectral decomposition: four-point examples
Propagator identities
Hypergeometric identities
Full Text
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