Zero Mass limit of Kerr-MOG Black Hole Equals Wormhole
arXiv:2412.08844 · doi:10.1103/PhysRevD.111.064013
Abstract
It has been argued in existing literature that the zero mass limit of Kerr spacetime corresponds to either flat Minkowski spacetime or a wormhole exhibiting a locally flat geometry. In this study, we examine that the zero mass limit of the Kerr-MOG black hole is equivalent to a wormhole. Moreover, we derive the Kerr-Schild form of the Kerr-MOG black hole through specific coordinate transformations. We further investigate the physical and topological characteristics of the Kerr-MOG black hole within the framework of modified gravity. Our analysis also includes a discussion of the wormhole using cylindrical coordinates, which comprises two distinct coordinate patches. Furthermore, we extend our analysis to the Kerr-Newman black hole and show that the \emph{zero mass limit of the Kerr-Newman black hole does not yield a wormhole}. However, if we impose an additional criterion such that \emph{both the mass parameter and the charge parameters are equal to zero}, then the Kerr-Newman black hole will be a wormhole.
Accepted for publication in PRD
References in corpus (9)
- Black Holes in Modified Gravity (MOG)
- The Kerr Metric
- Modified Gravity Black Holes and their Observable Shadows
- Incidences between points and lines on a two-dimensional variety
- The Bullet Cluster 1E0657-558 evidence shows Modified Gravity in the absence of Dark Matter
- Rotational Velocity Curves in the Milky Way as a Test of Modified Gravity
- Schwarzschild and Kerr Solutions of Einstein's Field Equation -- an introduction
- Zero mass limit of Kerr spacetime is a wormhole
- Ring wormholes via duality rotations