Abstract:We present a thorough observational investigation of the heuristic quantised ringdown model presented by Foit and Kleban (2019 Class. Quantum Grav.
36 035006). This model is based on the Bekenstein–Mukhanov conjecture, stating that the area of a black hole (BH) horizon is an integer multiple of the Planck area
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“…One of the tools to test the Kerr geometry is BH spectroscopy [24-26], now a thriving field [27][28][29][30][31][32][33][34]. If a compact binary merger leads to the formation of a rotating BH, as predicted in GR, the spacetime should asymptote to the Kerr metric through a relaxation process during which it can be described as a perturbation of the Kerr metric.…”
Section: Introductionmentioning
confidence: 99%
“…The simplicity of BHs (whether isolated or in binaries) implies that they are ideal laboratories to probe the limitations of GR, as long as environmental effects or astrophysical uncertainties can be ignored. In this Letter we ask an important question: is it really possible to ignore environmental effects?One of the tools to test the Kerr geometry is BH spectroscopy [24-26], now a thriving field [27][28][29][30][31][32][33][34]. If a compact binary merger leads to the formation of a rotating BH, as predicted in GR, the spacetime should asymptote to the Kerr metric through a relaxation process during which it can be described as a perturbation of the Kerr metric.…”
Recent work applying the notion of pseudospectrum to gravitational physics showed that the quasinormal mode spectrum of black holes is unstable, with the possible exception of the longest-lived (fundamental) mode. The fundamental mode dominates the expected signal in gravitational wave astronomy, and there is no reason why it should have privileged status. We compute the quasinormal mode spectrum of two model problems where the Schwarzschild potential is perturbed by a small "bump" consisting of either a Pöschl-Teller potential or a Gaussian, and we show that the fundamental mode is destabilized under generic perturbations. We present phase diagrams and study a simple double-barrier toy problem to clarify the conditions under which the spectral instability occurs.
Introduction.The advent of gravitational-wave (GW) astronomy [1, 2] and of very long baseline interferometry [3,4] opened exciting new windows to the invisible Universe. Black holes (BHs) play a unique role in the endeavor to test our understanding of general relativity (GR) and in the search for new physics [5][6][7][8][9][10][11].According to the singularity theorems [12,13], classical GR must fail in BH interiors. Quantum mechanics in BH spacetimes also leads to puzzling consequences, such as the information paradox [14][15][16]. It is tempting to conjecture that a theory of quantum gravity will resolve these issues, but the scale and nature of quantum gravity corrections to BH spacetimes is unknown. Uniqueness results in vacuum GR imply that BHs are the simplest macroscopic objects in the Universe [17], and BHs do not "polarize" in binary systems [18][19][20][21][22][23]. The simplicity of BHs (whether isolated or in binaries) implies that they are ideal laboratories to probe the limitations of GR, as long as environmental effects or astrophysical uncertainties can be ignored. In this Letter we ask an important question: is it really possible to ignore environmental effects?One of the tools to test the Kerr geometry is BH spectroscopy [24-26], now a thriving field [27][28][29][30][31][32][33][34]. If a compact binary merger leads to the formation of a rotating BH, as predicted in GR, the spacetime should asymptote to the Kerr metric through a relaxation process during which it can be described as a perturbation of the Kerr metric. The late-time GW signal (the "ringdown") is a superposition of damped exponentials with complex frequencies known as the quasinormal modes (QNMs), which can be computed within perturbation theory as poles of the associated Green's function [35][36][37]. The residues corresponding to these poles in the complex frequency plane dictate the amplitude of the response. To model a ringdown signal using Kerr QNM frequencies in vacuum, we should take into account the surrounding matter (even if it can be considered as a small perturbation). This is the
“…One of the tools to test the Kerr geometry is BH spectroscopy [24-26], now a thriving field [27][28][29][30][31][32][33][34]. If a compact binary merger leads to the formation of a rotating BH, as predicted in GR, the spacetime should asymptote to the Kerr metric through a relaxation process during which it can be described as a perturbation of the Kerr metric.…”
Section: Introductionmentioning
confidence: 99%
“…The simplicity of BHs (whether isolated or in binaries) implies that they are ideal laboratories to probe the limitations of GR, as long as environmental effects or astrophysical uncertainties can be ignored. In this Letter we ask an important question: is it really possible to ignore environmental effects?One of the tools to test the Kerr geometry is BH spectroscopy [24-26], now a thriving field [27][28][29][30][31][32][33][34]. If a compact binary merger leads to the formation of a rotating BH, as predicted in GR, the spacetime should asymptote to the Kerr metric through a relaxation process during which it can be described as a perturbation of the Kerr metric.…”
Recent work applying the notion of pseudospectrum to gravitational physics showed that the quasinormal mode spectrum of black holes is unstable, with the possible exception of the longest-lived (fundamental) mode. The fundamental mode dominates the expected signal in gravitational wave astronomy, and there is no reason why it should have privileged status. We compute the quasinormal mode spectrum of two model problems where the Schwarzschild potential is perturbed by a small "bump" consisting of either a Pöschl-Teller potential or a Gaussian, and we show that the fundamental mode is destabilized under generic perturbations. We present phase diagrams and study a simple double-barrier toy problem to clarify the conditions under which the spectral instability occurs.
Introduction.The advent of gravitational-wave (GW) astronomy [1, 2] and of very long baseline interferometry [3,4] opened exciting new windows to the invisible Universe. Black holes (BHs) play a unique role in the endeavor to test our understanding of general relativity (GR) and in the search for new physics [5][6][7][8][9][10][11].According to the singularity theorems [12,13], classical GR must fail in BH interiors. Quantum mechanics in BH spacetimes also leads to puzzling consequences, such as the information paradox [14][15][16]. It is tempting to conjecture that a theory of quantum gravity will resolve these issues, but the scale and nature of quantum gravity corrections to BH spacetimes is unknown. Uniqueness results in vacuum GR imply that BHs are the simplest macroscopic objects in the Universe [17], and BHs do not "polarize" in binary systems [18][19][20][21][22][23]. The simplicity of BHs (whether isolated or in binaries) implies that they are ideal laboratories to probe the limitations of GR, as long as environmental effects or astrophysical uncertainties can be ignored. In this Letter we ask an important question: is it really possible to ignore environmental effects?One of the tools to test the Kerr geometry is BH spectroscopy [24-26], now a thriving field [27][28][29][30][31][32][33][34]. If a compact binary merger leads to the formation of a rotating BH, as predicted in GR, the spacetime should asymptote to the Kerr metric through a relaxation process during which it can be described as a perturbation of the Kerr metric. The late-time GW signal (the "ringdown") is a superposition of damped exponentials with complex frequencies known as the quasinormal modes (QNMs), which can be computed within perturbation theory as poles of the associated Green's function [35][36][37]. The residues corresponding to these poles in the complex frequency plane dictate the amplitude of the response. To model a ringdown signal using Kerr QNM frequencies in vacuum, we should take into account the surrounding matter (even if it can be considered as a small perturbation). This is the
“…Moreover, it has been employed to explore possible signatures [86][87][88] of the area quantisation on the BH ringdown emission in Ref. [89] and to obtain bounds [84] on a possible new physics length scale entering QNM spectra, in a linearized perturbative scheme [90].…”
We calculate the quasi-normal mode complex frequencies of the Kerr-Newman black hole with arbitrary values of spin and charge, for the modes typically dominant during a binary black hole coalescence, ( , m, n) = {(2, 2, 0), (2, 2, 1), (3, 3, 0)}. Building analytical fits of the black hole spectrum, we construct a template to model the post-merger phase of a binary black hole coalescence in the presence of a remnant U (1) charge. Aside from astrophysical electric charge, our template can accommodate extensions of the Standard Model, such as a dark photon. Applying the model to LIGO-Virgo detections, we find that we are unable to distinguish between the charged and uncharged hypotheses from a purely post-merger analysis of the current events. However, restricting the mass and spin to values compatible with the analysis of the full signal, we obtain a 90th percentile bound q < 0.33 on the black hole charge-to-mass ratio, for the most favorable case of GW150914. Under similar assumptions, by simulating a typical loud signal observed by the LIGO-Virgo network at its design sensitivity, we assess that this model can provide a robust measurement of the charge-to-mass ratio only for values q 0.5; here we also assume that the mode amplitudes are similar to the uncharged case in creating our simulated signal. Lower values, down to q ∼ 0.3, could instead be detected when evaluating the consistency of the pre-merger and post-merger emission.
“…One of the very intriguing questions in fundamental physics is how gravity behaves in the quantum regime. Since GWs bring information from the very close vicinity of BHs, it is expected that GWs may shed some light on this mystery [35][36][37][38][39][40][41]. The idea behind such expectations follows from the fact that the Planck scale physics may affect the tidal Love numbers of the compact objects [11,12].…”
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