Abstract

We analyze the parity-odd correlators langle JJOrangle _{odd},langle JJTrangle _{odd},langle TTOrangle _{odd} and langle TTTrangle _{odd} in momentum space, constrained by conformal Ward identities, extending our former investigation of the parity-odd chiral anomaly vertex. We investigate how the presence of parity-odd trace anomalies affect such correlators. Motivations for this study come from holography, early universe cosmology and from a recent debate on the chiral trace anomaly of a Weyl fermion. In the current CFT analysis, O can be either a scalar or a pseudoscalar operator and it can be identified with the trace of the stress–energy tensor. We find that the langle JJOrangle _{odd} and langle TTOrangle _{odd} can be different from zero in a CFT. This occurs when the conformal dimension of the scalar operator is Delta _3=4, as in the case of O=T^{mu }_{mu }. Moreover, if we assume the existence of parity-odd trace anomalies, the conformal langle JJTrangle _{odd} and langle TTTrangle _{odd} are nonzero. In particular, in the case of langle JJTrangle _{odd} the transverse–traceless component is constrained to vanish, and the correlator is determined only by the trace part with the anomaly pole.

Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call