2021
DOI: 10.48550/arxiv.2109.09757
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On the ease of excitation of black hole ringing: Quantifying the importance of overtones by the excitation factors

Naritaka Oshita
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Cited by 6 publications
(9 citation statements)
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“…The first three overtones have comparable excitation amplitudes, with the latter growing slightly with n. Indeed, their excitation factors, the measure of their intrinsic excitability, grow with n peaking around n = 4 to 6 for nonextremal black holes, as recently shown in Ref. [60].…”
Section: Numerical Estimatessupporting
confidence: 65%
See 1 more Smart Citation
“…The first three overtones have comparable excitation amplitudes, with the latter growing slightly with n. Indeed, their excitation factors, the measure of their intrinsic excitability, grow with n peaking around n = 4 to 6 for nonextremal black holes, as recently shown in Ref. [60].…”
Section: Numerical Estimatessupporting
confidence: 65%
“…The excitation factors of a Schwarzschild black hole can also be computed from the asymptotic expansion of the solutions of the Teukolsky equation, see for instance Refs. [59,60].…”
Section: A Qnm Horizon Flux and Area Evolutionmentioning
confidence: 99%
“…Regarding future directions, it would be interesting to obtain the corrections to the overtone frequencies, as they seem to be relevant for the ringdown signal [71,72]. Also, even though the QNMs at leading order in the spin have already been computed for Einstein-dilaton-Gauss-Bonnet theory [56] and for dynamical Chern-Simons gravity [57,58], it remains important to generalize those results to the more general scalar-tensor theory presented in [34] so that one has a complete catalogue of QNMs in EFT extensions of GR.…”
Section: Discussionmentioning
confidence: 99%
“…It has long been known that including overtones improves the agreement between ringdown-only fits and the complete gravitational waveforms from perturbed BHs. This was first shown by direct integration of the perturbation equations sourced by infalling particles or collapsing matter [29][30][31][32] and then, more rigorously, using Green's function techniques [33][34][35][36][37]. Overtones were shown to improve agreement with numerical simulations of collapse [38], head-on collisions [39] and quasicircular mergers [26] leading to BH formation, and their omission leads to significant biases in mass and spin estimates [40,41].…”
Section: Introductionmentioning
confidence: 99%
“…[43] showed that including overtones up to n = 7 in the ringdown model improves the agreement with numerical relativity simulations for all times beyond the time t peak where |h 2 + + h 2 × | has a maximum, claiming that this observation "implies that the spacetime is well described as a linearly perturbed BH with a fixed mass and spin as early as the peak." Their study's insistence on an intrinsically linear physical description spurred a sequence of additional investigations, both on the modeling and on the observational side [37,[44][45][46][47][48][49][50][51][52]. If higher overtones can indeed be measured by starting at the peak, the larger ringdown signal-to-noise ratio (SNR) would open the door to more precise tests of GR.…”
Section: Introductionmentioning
confidence: 99%