Abstract

We compute d-dimensional scalar six-point conformal blocks in the two possible topologies allowed by the operator product expansion. Our computation is a simple application of the embedding space operator product expansion formalism developed recently. Scalar six-point conformal blocks in the comb channel have been determined not long ago, and we present here the first explicit computation of the scalar six-point conformal blocks in the remaining inequivalent topology. For obvious reason, we dub the other topology the snowflake channel. The scalar conformal blocks, with scalar external and exchange operators, are presented as a power series expansion in the conformal cross-ratios, where the coefficients of the power series are given as a double sum of the hypergeometric type. In the comb channel, the double sum is expressible as a product of two 3F2-hypergeometric functions. In the snowflake channel, the double sum is expressible as a Kampé de Fériet function where both sums are intertwined and cannot be factorized. We check our results by verifying their consistency under symmetries and by taking several limits reducing to known results, mostly to scalar five-point conformal blocks in arbitrary spacetime dimensions.

Highlights

  • Conformal blocks are fixed by conformal invariance, they are notoriously difficult to compute in all generality

  • The scalar M -point conformal blocks in the so-called comb channel were presented in [43, 44]. They showed that the scalar M -point conformal blocks in the comb channel can be expressed as a power series expansion in the conformal cross-ratios with the coefficients containing a product of M − 4 3F2-hypergeometric functions

  • Completely determined by conformal invariance, higher-point conformal blocks are notoriously difficult to compute in all generality

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Summary

Scalar six-point conformal blocks

With the knowledge of the OPE and its explicit action on any function of conformal crossratios, one can in principle compute any correlation function starting from the known two-point functions or, for that matter, the only non-trivial one-point function With this technique, starting at five points and above, it is necessary to re-express the initial correlation function in terms of the conformal cross-ratios appropriate for the OPE differential operator, and rewrite the solution in terms of the most convenient conformal crossratios by re-summing as many superfluous sums as possible. This method is quite powerful, allowing the computation of conformal blocks in any channel.

M -point correlation functions from the OPE
Scalar M -point correlation functions
Scalar M -point correlation functions in the comb channel
Scalar six-point correlation functions in the snowflake channel
Sanity checks
Symmetry properties
OPE limit
Limit of unit operator
Discussion and conclusion
M -3 M -2 M -1 M
A Scalar five-point conformal blocks and the OPE
Proof of the equivalence
B Snowflake and the OPE
Proof of the snowflake
An alternative form
C Symmetry properties
Rotations of the triangle
Reflections of the triangle
Permutations of the dendrites
Full Text
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