How small can an over-spinning body be in general relativity?
arXiv:1406.6798 · doi:10.1103/PhysRevD.90.124079
Abstract
The angular momentum of the Kerr singularity should not be larger than a threshold value so that it is enclosed by an event horizon: The Kerr singularity with the angular momentum exceeding the threshold value is naked. This fact suggests that if the cosmic censorship exists in our Universe, an over-spinning body without releasing its angular momentum cannot collapse to spacetime singularities. A simple kinematical estimate of two particles approaching each other supports this expectation and suggests the existence of a minimum size of an over-spinning body. But this does not imply that the geometry near the naked singularity cannot appear. By analyzing initial data, i.e., a snapshot of a spinning body, we see that an over-spinning body may produce a geometry close to the Kerr naked singularity around itself at least as a transient configuration.
arXiv comment30 pages, 8 figures, the version published in PRD
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- Near- and sub-solar-mass naked singularities and black holes from transmutation of white dwarfs
- Timescale for trans-Planckian collisions in Kerr spacetime
- Scanning the parameter space of collapsing rotating thin shells
- Distinguishing Signature of Kerr-MOG Black Hole and Superspinar via Lense-Thirring Precession