Abstract

In a recent letter we suggested a natural generalization of the flat-space spinor-helicity formalism in four dimensions to anti-de Sitter space. In the present paper we give some technical details that were left implicit previously. For lower-spin fields we also derive potentials associated with the previously found plane-wave solutions for field strengths. We then employ these potentials to evaluate some three-point amplitudes. This analysis illustrates a typical computation of an amplitude without internal lines in our formalism.

Highlights

  • In a recent letter we suggested a natural generalization of the flat-space spinorhelicity formalism in four dimensions to anti-de Sitter space

  • In a recent letter [52] we suggested a natural spinor-helicity formalism in AdS4 and made first steps in developing it

  • In the present paper we proposed the AdS counterpart of the flat spinor-helicity representation for the potentials

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Summary

Introduction

In recent years significant progress was achieved in amplitudes’ computations as well as in understanding of various hidden structures underlying them. The analysis further complicates for spinning fields due to proliferation of tensor indices This begs the question: is there any natural generalization of the spinor-helicity formalism to AdS space, which allows to deal with amplitudes of massless fields as efficiently as in flat space?. Additional motivation to address this question is related to higher-spin theories It was discovered recently [11, 34] that the spinor-helicity formalism allows to construct additional consistent cubic amplitudes compared to those available within the framework that employs Lorentz tensors. Unlike amplitudes we computed previously, for which essential simplification occurred due to conformal invariance of the associated vertices or due to the possibility to express them in terms of field strengths, in the present paper we deal with the cases, in which no such simplifications occur These examples, illustrate a genuine computation of a three-point amplitude using the spinor-helicity formalism in AdS4. The paper has a number of appendices, in which we collect our notations and present various technical results

Spinor-helicity representation in flat space
Plane-wave solutions
Amplitudes from space-time integrals
Amplitudes from symmetries
Massless representations in AdS4
AdS4 geometry
Plane waves for field strengths
Plane waves for potentials
Spin 1
Fixing an ansatz
Solving for potentials
Spin 2
Higher-spin potentials
Scattering amplitudes from space-time integrals
Simple examples
Genuine three-point amplitudes
Spin 0 − 12 − 32 amplitude
Spin 0 − 0 − 2 amplitude
Three-point amplitudes from symmetries
Helicity-changing operators
10 Conclusion and outlook
A Notations and conventions
B AdS4 and spinors
C Details on spin 32 potential
D Details on spin 2 potential
E Details on amplitudes from symmetries
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