Stationary BTZ space-time in Ricci-Inverse and $f(\mathcal{R})$ gravity theories

TL;DR

This paper investigates stationary BTZ black hole solutions within Ricci-inverse and $f( ext{R})$ gravity theories, analyzing geodesics and modifications to the cosmological constant, thus extending understanding of lower-dimensional gravity models.

Contribution

It demonstrates the existence of stationary BTZ solutions in Ricci-inverse and $f( ext{R})$ gravity, providing explicit geodesic solutions and comparing them with general relativity results.

Findings

BTZ solutions are valid in Ricci-inverse and $f( ext{R})$ gravity theories.

Explicit geodesic solutions are derived in elementary functions.

Modified gravity theories alter the cosmological constant and geodesic structures.

Abstract

In this paper, we explore a stationary BTZ space-time within the framework of modified gravity theory, specifically focusing on Ricci-inverse gravity. It is important to clarify that ``Ricci-inverse" refers to the inverse of the Ricci tensor, not the Ricci scalar. We consider a general class of this gravity theory, where the function $f$ is defined by $f(\mathcal{R}, \mathcal{A}, A^{\mu\nu}\,A_{\mu\nu})$, with $\mathcal{R}$ and $\mathcal{A}$ representing the Ricci and anti-curvature scalars, respectively and $A^{\mu\nu}$ is the anti-curvature tensor. We demonstrate that stationary BTZ space-time is a valid solution in this gravity theory, wherein the cosmological constant undergoes modifications due to the coupling constants. Moreover, we study another modified gravity theory known as $f(\mathcal{R})$-gravity and analyze the stationary BTZ space-time. Subsequently, we fully integrate the geodesic equations for BTZ space-time constructed within the Ricci-Inverse gravity, expressing the solutions in terms of elementary functions and compared with the GR result. We classify different types of geodesics, including null and time-like geodesics, under three conditions: (i) nonzero mass and angular momentum, $M \neq 0, J\neq 0$, (ii) massless BTZ space-time, $M=0$ and $J=0$, and (iii) $M=-1, J=0$, that is $AdS_3$-type, and analyze the results in modified gravity theories and compare with the general relativity case.