Effective-one-body model for black-hole binaries with generic mass ratios and spins

Gravitational waves emitted by black-hole binary systems have the highest signal-to-noise ratio in LIGO and Virgo detectors when black-hole spins are aligned with the orbital angular momentum and extremal. For such systems, we extend the effective-one-body inspiral-merger-ringdown waveforms to gener...

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Veröffentlicht in:Physical review. D, Particles, fields, gravitation, and cosmology Particles, fields, gravitation, and cosmology, 2014-03, Vol.89 (6), Article 061502
Hauptverfasser: Taracchini, Andrea, Buonanno, Alessandra, Pan, Yi, Hinderer, Tanja, Boyle, Michael, Hemberger, Daniel A., Kidder, Lawrence E., Lovelace, Geoffrey, Mroué, Abdul H., Pfeiffer, Harald P., Scheel, Mark A., Szilágyi, Béla, Taylor, Nicholas W., Zenginoglu, Anil
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Sprache:eng
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Zusammenfassung:Gravitational waves emitted by black-hole binary systems have the highest signal-to-noise ratio in LIGO and Virgo detectors when black-hole spins are aligned with the orbital angular momentum and extremal. For such systems, we extend the effective-one-body inspiral-merger-ringdown waveforms to generic mass ratios and spins calibrating them to 38 numerical-relativity nonprecessing waveforms produced by the SXS Collaboration. The numerical-relativity simulations span mass ratios from 1 to 8, spin magnitudes up to 98% of extremality, and last for 40 to 60 gravitational-wave cycles. When the total mass of the binary is between 20 and 200M sub([middot in circle]), the effective-one-body nonprecessing (dominant mode) waveforms have overlap above 99% (using the advanced-LIGO design noise spectral density) with all of the 38 nonprecessing numerical waveforms, when maximizing only on initial phase and time. This implies a negligible loss in event rate due to modeling. We also show that-without further calibration-the processing effective-one-body (dominant mode) waveforms have overlap above 97% with two very long, strongly processing numerical-relativity waveforms, when maximizing only on the initial phase and time.
ISSN:1550-7998
1550-2368
DOI:10.1103/PhysRevD.89.061502