4.7 Article

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

Journal

PHYSICAL REVIEW D
Volume 89, Issue 6, Pages -

Publisher

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevD.89.061502

Keywords

-

Funding

  1. NSF [PHY-0903631, PHY-1208881, PHY-1307489, PHY-0960291]
  2. NASA [NNX12AN10G]
  3. Maryland Center for Fundamental Physics
  4. NSERC of Canada
  5. Canada Chairs Program
  6. Canadian Institute for Advanced Research
  7. Sherman Fairchild Foundation
  8. NSF at Cornell [PHY-1306125, PHY-1005426]
  9. NSF at Caltech [PHY-106881, PHY-1005655, DMS-1065438]
  10. NSF XSEDE network [TG-PHY990007N]
  11. Cal State Fullerton
  12. GPC supercomputer at the SciNet HPC Consortium
  13. Canada Foundation for Innovation under Compute Canada
  14. Government of Ontario
  15. Ontario Research Fund-Research Excellence
  16. University of Toronto
  17. Direct For Mathematical & Physical Scien
  18. Division Of Physics [1306125, 1307489] Funding Source: National Science Foundation
  19. Direct For Mathematical & Physical Scien
  20. Division Of Physics [1068881, 1208881] Funding Source: National Science Foundation

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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(circle dot), 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 precessing effective-onebody (dominant mode) waveforms have overlap above 97% with two very long, strongly precessing numerical-relativity waveforms, when maximizing only on the initial phase and time.

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