Generalized Chern-Pontryagin models

TL;DR

This paper introduces a new class of modified gravity models based on a function of the Ricci scalar and Chern-Pontryagin term, deriving field equations, solutions, and a scalar-tensor representation with two scalar fields.

Contribution

It formulates generalized four-dimensional Chern-Pontryagin models, derives their field equations, finds specific solutions, and presents a scalar-tensor form with two scalar fields, one dynamical and one non-dynamical.

Findings

First-order correction to frame-dragging effect due to parameter L

G"{o}del-type metrics remain unperturbed in the model

Scalar-tensor representation includes a dynamical scalar and a non-dynamical Chern-Simons scalar

Abstract

We formulate a new class of modified gravity models, that is, generalized four-dimensional Chern-Pontryagin models, whose action is characterized by an arbitrary function of the Ricci scalar $R$ and the Chern-Pontryagin topological term ${}^*RR$, i.e., $f(R, {}^*RR)$. Within this framework, we derive the gravitational field equations and solve them for a particular model, $f(R, {}^*RR)=R+\beta ({}^*RR)^2$, considering two ansatzes: the slowly rotating metric and first-order perturbations of G\"{o}del-type metrics. For the former, we find a first-order correction to the frame-dragging effect boosted by the parameter $L$, which characterizes the departures from general relativity results. For the latter, G\"{o}del-type metrics hold unperturbed. We conclude this paper by displaying that generalized four-dimensional Chern-Pontryagin models admit a scalar-tensor representation, whose explicit form presents two scalar fields: $\Phi$, a dynamical degree of freedom, while the second, $\vartheta$, a non-dynamical degree of freedom. In particular, the scalar field $\vartheta$ emerges coupled with the Chern-Pontryagin topological term ${}^*RR$, i.e., $\vartheta {}^*RR$, which is nothing more than Chern-Simons term.