Your browser doesn't support javascript.
loading
Multimode Quasinormal Spectrum from a Perturbed Black Hole.
Capano, Collin D; Cabero, Miriam; Westerweck, Julian; Abedi, Jahed; Kastha, Shilpa; Nitz, Alexander H; Wang, Yi-Fan; Nielsen, Alex B; Krishnan, Badri.
Affiliation
  • Capano CD; Max-Planck-Institut für Gravitationsphysik (Albert-Einstein-Institut), Callinstraße 38, 30167 Hannover, Germany.
  • Cabero M; Leibniz Universität Hannover, 30167 Hannover, Germany.
  • Westerweck J; Department of Physics, University of Massachusetts, Dartmouth, Massachusetts 02747, USA.
  • Abedi J; Department of Physics and Astronomy, The University of British Columbia, Vancouver BC V6T 1Z4, Canada.
  • Kastha S; Max-Planck-Institut für Gravitationsphysik (Albert-Einstein-Institut), Callinstraße 38, 30167 Hannover, Germany.
  • Nitz AH; Leibniz Universität Hannover, 30167 Hannover, Germany.
  • Wang YF; Max-Planck-Institut für Gravitationsphysik (Albert-Einstein-Institut), Callinstraße 38, 30167 Hannover, Germany.
  • Nielsen AB; Leibniz Universität Hannover, 30167 Hannover, Germany.
  • Krishnan B; Department of Mathematics and Physics, University of Stavanger, NO-4036 Stavanger, Norway.
Phys Rev Lett ; 131(22): 221402, 2023 Dec 01.
Article in En | MEDLINE | ID: mdl-38101361
ABSTRACT
When two black holes merge, the late stage of gravitational wave emission is a superposition of exponentially damped sinusoids. According to the black hole no-hair theorem, this ringdown spectrum depends only on the mass and angular momentum of the final black hole. An observation of more than one ringdown mode can test this fundamental prediction of general relativity. Here, we provide strong observational evidence for a multimode black hole ringdown spectrum using the gravitational wave event GW190521, with a maximum Bayes factor of 56±1 (1σ uncertainty) preferring two fundamental modes over one. The dominant mode is the ℓ=m=2 harmonic, and the subdominant mode corresponds to the ℓ=m=3 harmonic. The amplitude of this mode relative to the dominant harmonic is estimated to be A_{330}/A_{220}=0.2_{-0.1}^{+0.2}. We estimate the redshifted mass and dimensionless spin of the final black hole as 330_{-40}^{+30}M_{⊙} and 0.86_{-0.11}^{+0.06}, respectively. We find that the final black hole is consistent with the no-hair theorem and constrain the fractional deviation from general relativity of the subdominant mode's frequency to be -0.01_{-0.09}^{+0.08}.

Full text: 1 Collection: 01-internacional Database: MEDLINE Language: En Journal: Phys Rev Lett Year: 2023 Document type: Article Affiliation country: Germany Country of publication: United States

Full text: 1 Collection: 01-internacional Database: MEDLINE Language: En Journal: Phys Rev Lett Year: 2023 Document type: Article Affiliation country: Germany Country of publication: United States