Four-point functions of gravitons and conserved currents of CFT in momentum space: testing the nonlocal action with the TTJJ

TL;DR

This paper analyzes the four-point correlator involving gravitons and conserved currents in conformal field theory, comparing perturbative free field results with nonlocal anomaly induced actions to test their consistency and identify discrepancies.

Contribution

It provides a detailed perturbative computation of the TTJJ correlator and compares it with predictions from nonlocal anomaly actions, revealing differences in their anomaly parts and clarifying the correct form of the anomaly expansion.

Findings

Perturbative TTJJ correlator computed and analyzed.

Discrepancies found between perturbative results and nonlocal anomaly actions.

Correct form of the anomaly induced action expansion identified.

Abstract

We present an analysis of the perturbative realization of the $TTJJ$ correlator, with two stress energy tensors and two conserved currents, using free field theory realizations, integrating out conformal sectors in the quantum corrections. This allows defining, around flat space, an exact perturbative expansion of the complete anomaly effective action - up to 4-point functions - whose predictions can be compared against those of the anomaly induced action. The latter is a variational solution of the conformal anomaly constraint at $d=4$ in the form of a nonlocal Wess-Zumino action. The renormalization procedure and the degeneracies of the tensor structures of this correlator are discussed, valid for a generic conformal field theory, deriving its anomalous trace Ward identities (WIs). In this application, we also illustrate a general procedure that identifies the minimal number of tensorial structures and corresponding form factors for the $TTJJ$ and any $4$-point function. The result of the direct computation is compared against the expression of the same 4-point function derived from the nonlocal anomaly induced action. We show that the prediction for the anomalous part of the $TTJJ$ derived from such action, evaluated in two different conformal decompositions, the Riegert and Fradkin-Vilkovisky (FV) choices, differ from the anomaly part identified in the perturbative $TTJJ$, in the flat spacetime limit. The anomaly part of the correlator computed with the Riegert choice is affected by double poles, while the one computed with the FV choice does not satisfy the conservation WIs. We present the correct form of the expansion of the anomaly induced action at the second order in the metric perturbations around flat space that reproduces the perturbative result.