Abstract
In this paper we use the spinor-helicity formalism to calculate 3-point functions involving scalar operators and spin-s conserved currents in general 3d CFTs. In spinor-helicity variables we notice that the parity-even and the parity-odd parts of a correlator are related. Upon converting spinor-helicity answers to momentum space, we show that correlators involving spin-s currents can be expressed in terms of some simple conformally invariant conserved structures. This in particular allows us to understand and separate out contact terms systematically, especially for the parity-odd case. We also reproduce some of the correlators using weight-shifting operators.
Highlights
The study of CFT correlation functions in momentum space was initiated systematically in [1, 2]
In appendix B we describe in detail our terminology of homogeneous and non-homogeneous contributions to a correlator and discuss how they differ from the usual splitting of a correlation function into transverse and longitudinal pieces
We will convert these expressions into the momentum space and see that the non-homogeneous contribution to the parity-odd correlator becomes a contact term
Summary
The study of CFT correlation functions in momentum space was initiated systematically in [1, 2]. Our goal in this paper is to study 3-point correlators of scalar operators and conserved spin-s currents in d = 3 CFTs in spinor-helicity variables as well as in momentum space. In [2], parity-even 3-point momentum space correlators involving scalar operator and conserved currents up to spin-2 (stress tensor) were computed by solving the conformal Ward identities (CWI). These correlators were later obtained using weight-shifting operators in [11, 12]. Upon converting spinor-helicity answers to momentum space, we see that the results for correlators involving spin-s currents can be expressed in terms of some simple conformally invariant conserved structures.
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