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Data-analysis driven comparison of analytic and numerical coalescing binary waveforms: Nonspinning case

Yi Pan1, Alessandra Buonanno1, John G. Baker2, Joan Centrella2, Bernard J. Kelly2, Sean T. McWilliams1, Frans Pretorius3, and James R. van Meter2,4

  • 1Department of Physics, University of Maryland, College Park, Maryland 20742, USA
  • 2Gravitational Astrophysics Laboratory, NASA Goddard Space Flight Center, 8800 Greenbelt Rd., Greenbelt, Maryland 20771, USA
  • 3Department of Physics, Princeton University, Princeton, New Jersey 08544, USA
  • 4Center for Space Science & Technology, University of Maryland Baltimore County, Physics Department, 1000 Hilltop Circle, Baltimore, Maryland 21250, USA

Phys. Rev. D 77, 024014 – Published 10 January, 2008

DOI: https://doi.org/10.1103/PhysRevD.77.024014

Abstract

We compare waveforms obtained by numerically evolving nonspinning binary black holes to post-Newtonian (PN) template families currently used in the search for gravitational waves by ground-based detectors. We find that the time-domain 3.5PN template family, which includes the inspiral phase, has fitting factors (FFs) 0.96 for binary systems with total mass M=1020M. The time-domain 3.5PN effective-one-body template family, which includes the inspiral, merger, and ring-down phases, gives satisfactory signal-matching performance with FFs 0.96 for binary systems with total mass M=10120M. If we introduce a cutoff frequency properly adjusted to the final black-hole ring-down frequency, we find that the frequency-domain stationary-phase-approximated template family at 3.5PN order has FFs 0.96 for binary systems with total mass M=1020M. However, to obtain high matching performances for larger binary masses, we need to either extend this family to unphysical regions of the parameter space or introduce a 4PN order coefficient in the frequency-domain gravitational wave (GW) phase. Finally, we find that the phenomenological Buonanno-Chen-Vallisneri family has FFs 0.97 with total mass M=10120M. The main analyses use the noise-spectral density of LIGO, but several tests are extended to VIRGO and advanced LIGO noise-spectral densities.

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