Abstract

We study the consistency of the cubic couplings of a (partially-)massless spinning field to two scalars in (d + 1)-dimensional de Sitter space. Gauge invariance of observables with external (partially)-massless spinning fields translates into Ward-Takahashi identities on the boundary. Using the Mellin-Barnes representation for boundary correlators in momentum space, we give a systematic study of Ward-Takahashi identities for tree-level 3- and 4-point processes involving a single external (partially-)massless field of arbitrary integer spin-J. 3-point Ward-Takahashi identities constrain the mass of the scalar fields to which a (partially-)massless spin-J field can couple. 4-point Ward-Takahashi identities then constrain the corresponding cubic couplings. For massless spinning fields, we show that Weinberg’s flat space results carry over to (d+1)-dimensional de Sitter space: for spins J = 1, 2 gauge-invariance implies charge-conservation and the equivalence principle while, assuming locality, higher-spins J > 2 cannot couple consistently to scalar matter. This result also applies to anti-de Sitter space. For partially-massless fields, restricting for simplicity to those of depth-2, we show that there is no consistent coupling to scalar matter in local theories. Along the way we also give a detailed account of how contact amplitudes with and without derivatives are represented in the Mellin-Barnes representation. Various new explicit expressions for 3- and 4-point functions involving (partially-)massless fields and conformally coupled scalars in dS4 are given.

Highlights

  • Recent years have seen a renewed interested in the challenge to extend the successes of the Bootstrap and the AdS/CFT paradigm to more general backgrounds, in particular those that are closer to real world

  • We study the consistency of the cubic couplings of amassless spinning field to two scalars in (d + 1)-dimensional de Sitter space

  • Using the Mellin-Barnes representation for boundary correlators in momentum space, we give a systematic study of Ward-Takahashi identities for tree-level 3- and 4-point processes involving a single externalmassless field of arbitrary integer spin-J. 3-point Ward-Takahashi identities constrain the mass of the scalar fields to which amassless spin-J field can couple. 4-point Ward-Takahashi identities constrain the corresponding cubic couplings

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Summary

Three-point functions

In this case the Mellin-Barnes representation is not required to describe the correlator completely and the integrals can be lifted to give explicit closed form expressions for the three-point function of a (partially)massless field and two conformally coupled scalars. For a (most-likely) incomplete list see refs. [9, 10, 15, 16, 21, 24, 45, 48,49,50,51,52,53,54,55,56,57]

Mellin-Barnes representation
Weight shifting operators
Ward-Takahashi identities
Massless fields
Partially-massless fields
On improvement terms
Special case: conformally coupled scalars
Four-point functions
Exchanges
On bulk quartic contact terms
Coupling massless spinning fields to scalar matter
Coupling partially-massless spinning fields to scalar matter
A Helicity projection operators
B Mellin-Barnes representation of 3pt functions with a spin-J operator
C Bulk quartic contact terms from improvements
Full Text
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