Search arXiv⌕ Search

arXiv · 1805.00293

Black-hole Spectroscopy by Making Full Use of Gravitational-Wave Modeling

Abstract

The Kerr nature of a compact-object-coalescence remnant can be unveiled by observing multiple quasi-normal modes (QNMs) in the post-merger signal. Current methods to achieve this goal rely on matching the data with a superposition of exponentially damped sinusoids with amplitudes fitted to numerical-relativity (NR) simulations of binary black-hole (BBH) mergers. These models presume the ability to correctly estimate the time at which the gravitational-wave (GW) signal starts to be dominated by the QNMs of a perturbed BH. Here we show that this difficulty can be overcome by using multipolar inspiral-merger-ringdown waveforms, calibrated to NR simulations, as already developed within the effective-one-body formalism (EOBNR). We build a parameterized (nonspinning) EOBNR waveform model in which the QNM complex frequencies are free parameters (pEOBNR), and use Bayesian analysis to study its effectiveness in measuring QNMs in GW150914, and in synthetic GW signals of BBHs injected in Gaussian noise. We find that using the pEOBNR model gives, in general, stronger constraints compared to the ones obtained when using a sum of damped sinusoids and using Bayesian model selection, we also show that the pEOBNR model can successfully be employed to find evidence for deviations from General Relativity in the ringdown signal. Since the pEOBNR model properly includes time and phase shifts among QNMs, it is also well suited to consistently combine information from several observations --- e.g., we find on the order of $\sim 30$ GW150914-like BBH events would be needed for Advanced LIGO and Virgo at design sensitivity to measure the fundamental frequencies of both the $(2,2)$ and $(3,3)$ modes, and the decay time of the $(2,2)$ mode with an accuracy of $\lesssim 5\%$ at the $2\mbox{-}σ$ level, thus allowing to test the BH's no-hair conjecture.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

Richard Brito, Alessandra Buonanno, Vivien Raymond. 2018-10-22. Black-hole Spectroscopy by Making Full Use of Gravitational-Wave Modeling. https://doi.org/10.1103/physrevd.98.084038

Cite the original work for its findings. Save a collection to share your selection of sources.

KEEP EXPLORING

Related papers

An upper bound on the minimum orbital period of black holes

Previous research has focused on establishing lower bounds on the minimum orbital period of black holes. In this work, we explore the complementary question of whether an upper bound exists for the minimum orbital period of black holes. We investigate the minimum orbital periods of three types of black holes: Schwarzschild, Reissner-Nordström and Kerr-Newman black holes. We find that the minimum orbital period of these black holes is bounded by an upper limit $T_{min} \leqslant 6\sqrt{3}πM$, where $M$ is the black hole mass. Our results suggest that this upper bound on the minimum orbital period may be a general property in black hole spacetimes.

gr-qc↗

Bounds on the minimum orbital period in the background of 5-dimensional charged black holes

In this paper, we study the upper and lower bounds on the minimum orbital period of 5-dimensional charged black holes. Our results indicate that the upper bound of the minimum orbital period corresponds to non-charged black holes, while the lower bound is achieved in the case of maximally charged black holes. We further establish precise analytical expressions for the upper and lower bounds of the minimum orbital period. Our findings provide valuable insights into 5-dimensional charged black holes and help constrain theoretical gravity models.

gr-qc↗

Analysis of minimum orbital periods around d-dimensional charged black holes

This paper investigates the bounds on the minimum orbital period for test objects around d-dimensional charged black holes in asymptotically flat spacetimes. We derive the exact critical radius and the minimum orbital period. We then prove analytically that the minimum orbital period decreases strictly as the charge of the black hole increases. Thus, the upper limit is reached for an uncharged black hole, while the lower limit is attained for a maximally charged one, and the two bounds take the closed form $\frac{2π(d-2)}{d-3}[(d-2)M]^{\frac{1}{d-3}}\leqslant T_{min} \leqslant 2π\sqrt{\frac{d-1}{d-3}}\,[(d-1)M]^{\frac{1}{d-3}}$. Since the minimum period equals $2π$ times the shadow radius, the upper bound is equivalently a universal upper bound on the shadow radius. These results improve our understanding of dynamics around d-dimensional black holes and impose constraints on candidate gravity theories.

gr-qc↗