Reuse & Permissions

It is not necessary to obtain permission to reuse this article or its components as it is available under the terms of the Creative Commons Attribution 4.0 International license. This license permits unrestricted use, distribution, and reproduction in any medium, provided attribution to the author(s) and the published article's title, journal citation, and DOI are maintained. Please note that some figures may have been included with permission from other third parties. It is your responsibility to obtain the proper permission from the rights holder directly for these figures.

Export citation

Export citation

Choose format for download:

Download Citation
  • Open Access

Nonlinear effects in the black hole ringdown: Absorption-induced mode excitation

Laura Sberna1,*, Pablo Bosch2, William E. East3, Stephen R. Green1, and Luis Lehner3

  • 1Max Planck Institute for Gravitational Physics (Albert Einstein Institute), Am Mühlenberg 1, 14476 Potsdam, Germany
  • 2GRAPPA and Institute of High-Energy Physics, University of Amsterdam, Science Park 904, 1098 XH Amsterdam, Netherlands
  • 3Perimeter Institute, 31 Caroline Street North, N2L 2Y5 Ontario, Canada

  • *laura.sberna@aei.mpg.de

Phys. Rev. D 105, 064046 – Published 28 March, 2022

DOI: https://doi.org/10.1103/PhysRevD.105.064046

Abstract

Gravitational-wave observations of black hole ringdowns are commonly used to characterize binary merger remnants and to test general relativity. These analyses assume linear black hole perturbation theory, in particular that the ringdown can be described in terms of quasinormal modes even for times approaching the merger. Here we investigate a nonlinear effect during the ringdown, namely how a mode excited at early times can excite additional modes as it is absorbed by the black hole. This is a third-order secular effect: the change in the black hole mass causes a shift in the mode spectrum, so that the original mode is projected onto the new ones. Using nonlinear simulations, we study the ringdown of a spherically symmetric scalar field around an asymptotically anti–de Sitter black hole, and we find that this “absorption-induced mode excitation” is the dominant nonlinear effect. We show that this effect takes place well within the nonadiabatic regime, so we can analytically estimate it using a sudden mass-change approximation. Adapting our estimation technique to asymptotically flat Schwarzschild black holes, we expect absorption-induced mode excitation to play a role in the analysis and interpretation of current and future gravitational wave observations.

View figure in article

Physics Subject Headings (PhySH)

Article Text

References (62)

  1. W. Israel, Event horizons in static vacuum space-times, Phys. Rev. 164, 1776 (1967).
  2. W. Israel, Event horizons in static electrovac space-times, Commun. Math. Phys. 8, 245 (1968).
  3. B. Carter, Axisymmetric Black Hole Has Only Two Degrees of Freedom, Phys. Rev. Lett. 26, 331 (1971).
  4. R. Penrose, Gravitational collapse: The role of general relativity, Gen. Relativ. Gravit. 34, 1141 (2002).
  5. H.-P. Nollert, Topical review: Quasinormal modes: The characteristic ‘sound’ of black holes and neutron stars, Classical Quantum Gravity 16, R159 (1999).
  6. K. D. Kokkotas and B. G. Schmidt, Quasinormal modes of stars and black holes, Living Rev. Relativity 2, 2 (1999).
  7. E. Berti, V. Cardoso, and A. O. Starinets, Quasinormal modes of black holes and black branes, Classical Quantum Gravity 26, 163001 (2009).
  8. B. P. Abbott et al. (LIGO Scientific and Virgo Collaborations), Tests of General Relativity with GW150914, Phys. Rev. Lett. 116, 221101 (2016); Erratum, 121, 129902(E) (2018).
  9. R. Abbott et al. (LIGO Scientific, VIRGO and KAGRA Collaborations), Tests of general relativity with GWTC-3, arXiv:2112.06861.
  10. M. Isi, M. Giesler, W. M. Farr, M. A. Scheel, and S. A. Teukolsky, Testing the No-Hair Theorem with GW150914, Phys. Rev. Lett. 123, 111102 (2019).
  11. C. D. Capano, M. Cabero, J. Westerweck, J. Abedi, S. Kastha, A. H. Nitz, A. B. Nielsen, and B. Krishnan, Observation of a multimode quasi-normal spectrum from a perturbed black hole, arXiv:2105.05238.
  12. R. Cotesta, G. Carullo, E. Berti, and V. Cardoso, On the detection of ringdown overtones in GW150914, arXiv:2201.00822.
  13. E. Berti, V. Cardoso, and C. M. Will, On gravitational-wave spectroscopy of massive black holes with the space interferometer LISA, Phys. Rev. D 73, 064030 (2006).
  14. M. Maggiore et al., Science case for the Einstein telescope, J. Cosmol. Astropart. Phys. 03 (2020) 050.
  15. M. Bailes et al., Gravitational-wave physics and astronomy in the 2020s and 2030s, Nat. Rev. Phys. 3, 344 (2021).
  16. R. J. Gleiser, C. O. Nicasio, R. H. Price, and J. Pullin, Colliding Black Holes: How Far Can the Close Approximation Go?, Phys. Rev. Lett. 77, 4483 (1996).
  17. Y. Zlochower, R. Gomez, S. Husa, L. Lehner, and J. Winicour, Mode coupling in the nonlinear response of black holes, Phys. Rev. D 68, 084014 (2003).
  18. W. E. East, F. M. Ramazanoğlu, and F. Pretorius, Black hole superradiance in dynamical spacetime, Phys. Rev. D 89, 061503 (2014).
  19. H. Bantilan, F. Pretorius, and S. S. Gubser, Simulation of asymptotically AdS5 spacetimes with a generalized harmonic evolution scheme, Phys. Rev. D 85, 084038 (2012).
  20. J. L. Ripley, N. Loutrel, E. Giorgi, and F. Pretorius, Numerical computation of second order vacuum perturbations of Kerr black holes, Phys. Rev. D 103, 104018 (2021).
  21. S. R. Green, F. Carrasco, and L. Lehner, Holographic Path to the Turbulent Side of Gravity, Phys. Rev. X 4, 011001 (2014).
  22. A. Adams, P. M. Chesler, and H. Liu, Holographic Turbulence, Phys. Rev. Lett. 112, 151602 (2014).
  23. H. Yang, A. Zimmerman, and L. Lehner, Turbulent Black Holes, Phys. Rev. Lett. 114, 081101 (2015).
  24. E. Finch and C. J. Moore, Modeling the ringdown from precessing black hole binaries, Phys. Rev. D 103, 084048 (2021).
  25. X. Li, L. Sun, R. K. L. Lo, E. Payne, and Y. Chen, Angular emission patterns of remnant black holes, Phys. Rev. D 105, 024016 (2022).
  26. L. London, D. Shoemaker, and J. Healy, Modeling ringdown: Beyond the fundamental quasinormal modes, Phys. Rev. D 90, 124032 (2014); Erratum, 94, 069902 (2016).
  27. M. Giesler, M. Isi, M. A. Scheel, and S. Teukolsky, Black Hole Ringdown: The Importance of Overtones, Phys. Rev. X 9, 041060 (2019).
  28. G. B. Cook, Aspects of multimode Kerr ringdown fitting, Phys. Rev. D 102, 024027 (2020).
  29. A. Dhani and B. S. Sathyaprakash, Overtones, mirror modes, and mode-mixing in binary black hole mergers, arXiv:2107.14195.
  30. L. Magaña Zertuche et al., High precision ringdown modeling: Multimode fits and BMS frames, arXiv:2110.15922.
  31. M. Okounkova, Revisiting non-linearity in binary black hole mergers, arXiv:2004.00671.
  32. R. Shankar, Principles of Quantum Mechanics (Plenum, New York, 1980).
  33. S. A. Teukolsky and W. H. Press, Perturbations of a rotating black hole. III. Interaction of the hole with gravitational and electromagnetic radiation, Astrophys. J. 193, 443 (1974).
  34. S. R. Green, Orthogonality of Kerr quasinormal modes (2019), BIRS workshop on Time-like Boundaries in General Relativistic Evolution Problems.
  35. S. R. Green, S. Hollands, and P. Zimmerman (to be published).
  36. E. W. Leaver and S. Chandrasekhar, An analytic representation for the quasi-normal modes of kerr black holes, Proc. R. Soc. A 402, 285 (1985).
  37. W. Gautschi, Computational aspects of three-term recurrence relations, SIAM Rev. 9, 24 (1967).
  38. P. Bosch, S. R. Green, L. Lehner, and H. Roussille, Excited hairy black holes: Dynamical construction and level transitions, Phys. Rev. D 102, 044014 (2020).
  39. N. Andersson, Evolving test fieldsin a black hole geometry, Phys. Rev. D 55, 468 (1997).
  40. K. Glampedakis and N. Andersson, Quick and dirty methods for studying black hole resonances, Classical Quantum Gravity 20, 3441 (2003).
  41. E. Berti and V. Cardoso, Quasinormal ringing of kerr black holes: The excitation factors, Phys. Rev. D 74, 104020 (2006).
  42. E. W. Leaver, Spectral decomposition of the perturbation response of the schwarzschild geometry, Phys. Rev. D 34, 384 (1986).
  43. E. W. Leaver, Solutions to a generalized spheroidal wave equation: Teukolsky’s equations in general relativity, and the two-center problem in molecular quantum mechanics, J. Math. Phys. (N.Y.) 27, 1238 (1986).
  44. F. Carrasco, L. Lehner, R. C. Myers, O. Reula, and A. Singh, Turbulent flows for relativistic conformal fluids in 2+1 dimensions, Phys. Rev. D 86, 126006 (2012).
  45. N. Loutrel, J. L. Ripley, E. Giorgi, and F. Pretorius, Second order perturbations of Kerr black holes: Reconstruction of the metric, Phys. Rev. D 103, 104017 (2021).
  46. E. Poisson and M. Sasaki, Gravitational radiation from a particle in circular orbit around a black hole. 5: Black hole absorption and tail corrections, Phys. Rev. D 51, 5753 (1995).
  47. S. Bernuzzi, A. Nagar, and A. Zenginoglu, Horizon-absorption effects in coalescing black-hole binaries: An effective-one-body study of the non-spinning case, Phys. Rev. D 86, 104038 (2012).
  48. H. Tagoshi, S. Mano, and E. Takasugi, Post Newtonian expansion of gravitational waves from a particle in circular orbits around a rotating black hole: Effects of black hole absorption, Prog. Theor. Phys. 98, 829 (1997).
  49. R. Wald, General Relativity (University of Chicago Press, Chicago, 1984).
  50. C. W. Misner and D. H. Sharp, Relativistic equations for adiabatic, spherically symmetric gravitational collapse, Phys. Rev. 136, B571 (1964).
  51. M. E. Cahill and G. C. McVittie, Spherical symmetry and mass-energy in general relativity. I. General theory, J. Math. Phys. (N.Y.) 11, 1382 (1970).
  52. S. R. Dolan, Instability of the massive Klein-Gordon field on the Kerr spacetime, Phys. Rev. D 76, 084001 (2007).
  53. A. Buchel, L. Lehner, R. C. Myers, and A. van Niekerk, Quantum quenches of holographic plasmas, J. High Energy Phys. 05 (2013) 067.
  54. P. Bosch, S. R. Green, and L. Lehner, Nonlinear Evolution and Final Fate of Charged Anti-de Sitter Black Hole Superradiant Instability, Phys. Rev. Lett. 116, 141102 (2016).
  55. P. M. Chesler and L. G. Yaffe, Numerical solution of gravitational dynamics in asymptotically anti-de Sitter spacetimes, J. High Energy Phys. 07 (2014) 086.
  56. G. Calabrese, L. Lehner, D. Neilsen, J. Pullin, O. Reula, O. Sarbach, and M. Tiglio, Novel finite differencing techniques for numerical relativity: Application to black hole excision, Classical Quantum Gravity 20, L245 (2003).
  57. G. Calabrese, L. Lehner, O. Reula, O. Sarbach, and M. Tiglio, Summation by parts and dissipation for domains with excised regions, Classical Quantum Gravity 21, 5735 (2004).
  58. R. Arnowitt, S. Deser, and C. W. Misner, Dynamical structure and definition of energy in general relativity, Phys. Rev. J. Arch. 116, 1322 (1959).
  59. M. Campanelli and C. O. Lousto, The imposition of initial data in the Teukolsky equation.1. The nonrotating case, Phys. Rev. D 58, 024015 (1998).
  60. Z. Zhang, E. Berti, and V. Cardoso, Quasinormal ringing of kerr black holes. II. Excitation by particles falling radially with arbitrary energy, Phys. Rev. D 88, 044018 (2013).
  61. N. Oshita, On the ease of excitation of black hole ringing: Quantifying the importance of overtones by the excitation factors, Phys. Rev. D 104, 124032 (2021).
  62. Black Hole Perturbation Toolkit, http://bhptoolkit.org/.

Outline

Information

Sign In to Your Journals Account

Filter

Filter

Article Lookup

Enter a citation