A maximally rotating Kerr black hole is said to be extremal. In this paper we introduce the corresponding restrictions for isolated and dynamical horizons. These reduce to the standard notions for Kerr but in general do not require the horizon to be either stationary or rotationally symmetric. We consider physical implications and applications of these results. In particular we introduce a parameter e which characterizes how close a horizon is to extremality and should be calculable in numerical simulations
AbstractExtremal rotating cohomogeneity-1 black holes in Einstein–Maxwell theory feature two branche...
We prove that for sub-extremal axisymmetric and stationary black holes with arbitrary surrounding ma...
Rapidly rotating black hole (BH) solutions in theories beyond general relativity (GR) play a key rol...
The spin angular momentum S of an isolated Kerr black hole is bounded by the surface area A of its a...
The spin angular momentum S of an isolated Kerr black hole is bounded by the surface area A of its a...
The fact that one must evaluate the near-extremal and near-horizon limits of Kerr spacetime in a spe...
The spin angular momentum S of an isolated Kerr black hole is bounded by the surface area A of its a...
We show that the horizon instability of the extremal Kerr black hole is associated with a singular b...
We analytically study the linear response of a near-extremal Kerr black hole to external scalar, ele...
This Brief presents in a self-contained, non-technical and illustrative fashion the state-of-the-art...
We show that extremal Kerr black holes are sensitive probes of new physics. Stringy or quantum corre...
© 2015 American Physical Society. We consider generic rotating axially symmetric "dirty" (surrounded...
© 2015 American Physical Society. We consider generic rotating axially symmetric "dirty" (surrounded...
© 2015 American Physical Society. We consider generic rotating axially symmetric "dirty" (surrounded...
The rotating regular Hayward’s spacetime, apart from mass (M) and angular momentum (a), has an addit...
AbstractExtremal rotating cohomogeneity-1 black holes in Einstein–Maxwell theory feature two branche...
We prove that for sub-extremal axisymmetric and stationary black holes with arbitrary surrounding ma...
Rapidly rotating black hole (BH) solutions in theories beyond general relativity (GR) play a key rol...
The spin angular momentum S of an isolated Kerr black hole is bounded by the surface area A of its a...
The spin angular momentum S of an isolated Kerr black hole is bounded by the surface area A of its a...
The fact that one must evaluate the near-extremal and near-horizon limits of Kerr spacetime in a spe...
The spin angular momentum S of an isolated Kerr black hole is bounded by the surface area A of its a...
We show that the horizon instability of the extremal Kerr black hole is associated with a singular b...
We analytically study the linear response of a near-extremal Kerr black hole to external scalar, ele...
This Brief presents in a self-contained, non-technical and illustrative fashion the state-of-the-art...
We show that extremal Kerr black holes are sensitive probes of new physics. Stringy or quantum corre...
© 2015 American Physical Society. We consider generic rotating axially symmetric "dirty" (surrounded...
© 2015 American Physical Society. We consider generic rotating axially symmetric "dirty" (surrounded...
© 2015 American Physical Society. We consider generic rotating axially symmetric "dirty" (surrounded...
The rotating regular Hayward’s spacetime, apart from mass (M) and angular momentum (a), has an addit...
AbstractExtremal rotating cohomogeneity-1 black holes in Einstein–Maxwell theory feature two branche...
We prove that for sub-extremal axisymmetric and stationary black holes with arbitrary surrounding ma...
Rapidly rotating black hole (BH) solutions in theories beyond general relativity (GR) play a key rol...