Charged black holes: Wave equations for gravitational and electromagnetic perturbations
arXiv:gr-qc/0211036 · doi:10.1086/344572
Abstract
A pair of wave equations for the electromagnetic and gravitational perturbations of the charged Kerr black hole are derived. The perturbed Einstein-Maxwell equations in a new gauge are employed in the derivation. The wave equations refer to the perturbed Maxwell spinor and to the shear of a principal null direction of the Weyl curvature. The whole construction rests on the tripod of three distinct derivatives of the first curvature of a principal null direction.
arXiv comment12 pages, to appear in Ap.J
References in corpus (7)
- Rapid X-ray flaring from the direction of the supermassive black hole at the Galactic Centre
- Analytic Solutions of the Teukolsky Equation and their Low Frequency Expansions
- 'Stable' QPOs and Black Hole Properties from Diskoseismology
- Analytic Solutions of the Teukolsky Equation and their Properties
- On the interpretation of the burst structure of GRBs
- Computing radiation from Kerr black holes: Generalization of the Sasaki-Nakamura equation
- Teukolsky Master Equation: De Rham wave equation for the gravitational and electromagnetic fields in vacuum
Cited by in corpus (5)
- Quasinormal modes of Kerr-Newman black holes: coupling of electromagnetic and gravitational perturbations
- Direct Measurements of Black Hole Charge with Future Astrometrical Missions
- Constraining the electric charges of some astronomical bodies in Reissner-Nordstrom spacetimes and generic r^-2-type power-law potentials from orbital motions
- Effect of charge on negative-phase-velocity propagation of electromagnetic waves in the ergosphere of a rotating black hole
- Principal null directions of perturbed black holes