Inspiral-merger-ringdown waveforms of spinning, precessing black-hole binaries in the effective-one-body formalism
Abstract
We describe a general procedure to generate spinning, precessing waveforms that include inspiral, merger, and ringdown stages in the effective-one-body (EOB) approach. The procedure uses a precessing frame in which precession-induced amplitude and phase modulations are minimized, and an inertial frame, aligned with the spin of the final black hole, in which we carry out the matching of the inspiral-plunge to merger-ringdown waveforms. As a first application, we build spinning, precessing EOB waveforms for the gravitational modes ℓ=2 such that in the nonprecessing limit those waveforms agree with the EOB waveforms recently calibrated to numerical-relativity waveforms. Without recalibrating the EOB model, we then compare EOB and post-Newtonian precessing waveforms to two numerical-relativity waveforms produced by the Caltech-Cornell-CITA collaboration. The numerical waveforms are strongly precessing and have 35 and 65 gravitational-wave cycles. We find a remarkable agreement between EOB and numerical-relativity precessing waveforms and spins' evolutions. The phase difference is ∼0.2 rad rad at merger, while the mismatches, computed using the advanced-LIGO noise spectral density, are below 2% when maximizing only on the time and phase at coalescence and on the polarization angle.
Additional Information
© 2014 American Physical Society. Received 1 August 2013; published 2 April 2014. We thank Anıl Zenginoğlu, Geoffrey Lovelace, and Mike Boyle for their contributions to the productions of the NR waveforms used in this paper. A. B., Y. P., and A. T. acknowledge partial support from NSF Grants No. PHY-0903631 and No. PHY-1208881. A. B. also acknowledges partial support from the NASA Grant No. NNX12AN10 G. A. M. and H. P. gratefully acknowledge support from NSERC of Canada, the Canada Chairs Program, and the Canadian Institute for Advanced Research. L. K. gratefully acknowledges support from the Sherman Fairchild Foundation and from NSF Grants No. PHY-0969111 and No. PHY-1005426. Simulations used in this work were computed with the SpEC code [75]. Computations were performed on the Zwicky cluster at Caltech, which is supported by the Sherman Fairchild Foundation and by NSF Award No. PHY-0960291, on the NSF XSEDE network under Grant No. TG-PHY990007N, and on the GPC supercomputer at the SciNet HPC Consortium [76]. SciNet is funded by the Canada Foundation for Innovation under the auspices of Compute Canada, the Government of Ontario, Ontario Research Fund–Research Excellence, and the University of Toronto.Attached Files
Published - PhysRevD.89.084006.pdf
Submitted - 1307.6232v1.pdf
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Additional details
- Eprint ID
- 46214
- Resolver ID
- CaltechAUTHORS:20140611-135106521
- NSF
- PHY-0903631
- NSF
- PHY-1208881
- NASA
- NNX12AN10G
- NSERC (Canada)
- Canada Chairs Program
- Canadian Institute for Advanced Research
- Sherman Fairchild Foundation
- NSF
- PHY-0969111
- NSF
- PHY-1005426
- NSF
- PHY-0960291
- NSF XSEDE network
- TG-PHY990007N
- Canada Foundation for Innovation under the auspices of Compute Canada
- Government of Ontario
- Ontario Research Fund–Research Excellence
- University of Toronto
- Created
-
2014-06-11Created from EPrint's datestamp field
- Updated
-
2021-11-10Created from EPrint's last_modified field
- Caltech groups
- TAPIR