Published October 15, 2021 | Version Published + Submitted
Journal Article Open

Universal features of gravitational waves emitted by superkick binary black hole systems

  • 1. ROR icon California Institute of Technology
  • 2. ROR icon Cornell University

Abstract

We use numerical relativity to study the merger and ringdown stages of "superkick" binary black hole systems (those with equal mass and antiparallel spins). We find a universal way to describe the mass and current quadrupole gravitational waves emitted by these systems during the merger and ringdown stage: (i) The time evolutions of these waves are insensitive to the progenitor's parameters (spins) after being normalized by their own peak values. (ii) The peak values, which encode all the spin information of the progenitor, can be consistently fitted to formulas inspired by post-Newtonian theory. We find that the universal evolution of the mass quadrupole wave can be accurately modeled by the so-called Backwards One-Body (BOB) model. However, the BOB model, in its present form, leads to a lower waveform match and a significant parameter-estimation bias for the current quadrupole wave. We also decompose the ringdown signal into seven overtones, and study the dependence of mode amplitudes on the progenitor's parameters. Such dependence is found to be insensitive to the overtone index (up to a scaling factor). Finally, we use the Fisher matrix technique to investigate how the ringdown waveform can be at least as important for parameter estimation as the inspiral stage. Assuming the Cosmic Explorer, we find the contribution of ringdown portion dominates as the total mass exceeds ∼250 M_⊙. For massive binary black hole (BBH) systems, the accuracy of parameter measurement is improved by incorporating the information of ringdown—the ringdown sector gives rise to a different parameter correlation from inspiral stage; hence, the overall parameter correlation is reduced in full signal.

Additional Information

© 2021 American Physical Society. (Received 10 July 2021; accepted 9 August 2021; published 1 October 2021) We want to thank Serguei Ossokine, Alvin Chua, Gregorio Carullo, and Sean McWilliams for useful discussions. S. M. and Y. C. are supported by the Simons Foundation (Grant No. 568762), the Brinson Foundation, and the National Science Foundation (Grants No. PHY–2011968, No. PHY–2011961, and No. PHY–1836809). V. V. is generously supported by a Klarman Fellowship at Cornell, the Sherman Fairchild Foundation, and NSF Grants No. PHY–170212 and No. PHY–1708213 at Caltech. The computations presented here were conducted on the Caltech High Performance Cluster, partially supported by a grant from the Gordon and Betty Moore Foundation.

Attached Files

Published - PhysRevD.104.084003.pdf

Submitted - 2107.04890.pdf

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Additional details

Identifiers

Eprint ID
111455
Resolver ID
CaltechAUTHORS:20211014-212144527

Related works

Funding

Simons Foundation
568762
Brinson Foundation
NSF
PHY-2011968
NSF
PHY-2011961
NSF
PHY-1836809
Cornell University
Sherman Fairchild Foundation
NSF
PHY-170212
NSF
PHY-1708213
Gordon and Betty Moore Foundation

Dates

Created
2021-10-18
Created from EPrint's datestamp field
Updated
2023-04-28
Created from EPrint's last_modified field

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