2008/10/27 by Shahar Hod · 3 citations
Physics and Astronomy · #Astrophysical Phenomena and Observations #Black Holes and Theoretical Physics #Cosmology and Gravitation Theories #astro-ph #gr-qc #hep-th #quant-ph
paper · pdf · doi:10.1103/physrevd.78.084035
published as Phys.Rev.D78:084035,2008 · 5 pages
openalex publication_date 2008/10/27 · arxiv created 2008/11/24 · arxiv updated 2009/12/01 · openalex created_date 2025/10/10 · openalex updated_date 2026/07/28
We study analytically the relaxation phase of perturbed, rapidly rotating black holes. In particular, we derive a simple formula for the fundamental quasinormal resonances of near-extremal Kerr black holes. The formula is expressed in terms of the black hole physical parameters: \ensuremathω=m\ensuremathΩ\ensuremath-i2\ensuremathπTBH(n+(1)/(2)), where TBH and \ensuremathΩ are the temperature and angular velocity of the black hole, and m is the azimuthal harmonic index of a corotating equatorial mode. This formula implies that the relaxation period \ensuremathτ\ensuremath∼1/\ensuremath\mathfrakI\ensuremathω of the black hole becomes extremely long as the extremal limit TBH\ensuremath→0 is approached. The analytically derived formula is shown to agree with direct numerical computations of the black hole resonances. We use our results to demonstrate analytically the fact that near-extremal Kerr black holes saturate the recently proposed universal relaxation bound.