Weak cosmic censorship conjecture in the pure Lovelock gravity
Sanjar Shaymatov, Naresh Dadhich

TL;DR
This paper investigates the weak cosmic censorship conjecture in pure Lovelock gravity, showing that rotating black holes in dimensions greater than a certain threshold always obey WCCC, with implications for black hole formation in higher dimensions.
Contribution
It establishes a dimensional threshold in pure Lovelock gravity beyond which rotating black holes always obey WCCC, extending previous results from Einstein gravity.
Findings
Pure Lovelock rotating black holes obey WCCC in dimensions > 4N+1.
In higher dimensions, gravity becomes repulsive, preventing overspinning.
The threshold depends on the degree N of the Lovelock polynomial.
Abstract
It is well known that a rotating black hole in four dimension could be overspun by linear order test particle accretion which however always gets overturned when non-linear perturbations are included. It turns out that in the Einstein gravity, repulsion due to rotation dominates over attraction due to mass in dimensions, , and consequently black hole cannot be overspun even for linear order accretion. For the pure Lovelock rotating black hole, this dimensional threshold is where is degree of single th order term in the Lovelock polynomial in the action. Thus the pure Lovelock rotating black holes always obey the weak cosmic censorship conjecture (WCCC) in all dimensions greater than . Since overall gravity being repulsive beyond this dimensional threshold, how is rotating black hole then formed there?
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Taxonomy
TopicsBlack Holes and Theoretical Physics · Cosmology and Gravitation Theories · Astrophysical Phenomena and Observations
