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Accurate and efficient waveforms for compact binaries on eccentric orbits

E. A. HuertaDepartment of Physics, West Virginia University, White Hall, Morgantown, West Virginia 26506, USAP. KumarCanadian Institute for Theoretical Astrophysics, University of Toronto, 60 St. George Street, Toronto, Ontario M5S 3H8, CanadaSean T. McWilliamsDepartment of Physics, West Virginia University, White Hall, Morgantown, West Virginia 26506, USAR. O’ShaughnessyCenter for Computational Relativity and Gravitation, School of Mathematical Sciences, and School of Physics and Astronomy, Rochester Institute of Technology, Rochester, New York 14623, USANicolás YunesDepartment of Physics, Montana State University, Bozeman, Montana 59717, USA
2014en
ABI

Аннотация

Compact binaries that emit gravitational waves in the sensitivity band of ground-based detectors can have non-negligible eccentricities just prior to merger, depending on the formation scenario. We develop a purely analytic, frequency-domain model for gravitational waves emitted by compact binaries on orbits with small eccentricity, which reduces to the quasicircular post-Newtonian approximant TaylorF2 at zero eccentricity and to the postcircular approximation of Yunes et al. [Phys. Rev. D 80, 084001 (2009)] at small eccentricity. Our model uses a spectral approximation to the (post-Newtonian) Kepler problem to model the orbital phase as a function of frequency, accounting for eccentricity effects up to $\mathcal{O}({e}^{8})$ at each post-Newtonian order. Our approach accurately reproduces an alternative time-domain eccentric waveform model for $e\ensuremath{\in}[0,0.4]$ and binaries with total mass $\ensuremath{\lesssim}12{M}_{\ensuremath{\bigodot}}$. As an application, we evaluate the signal amplitude that eccentric binaries produce in different networks of existing and forthcoming gravitational waves detectors. Assuming a population of eccentric systems containing black holes and neutron stars that is uniformly distributed in comoving volume, we estimate that second-generation detectors like Advanced LIGO could detect approximately 0.1--10 events per year out to redshift $z\ensuremath{\sim}0.2$, while an array of Einstein Telescope detectors could detect hundreds of events per year to redshift $z\ensuremath{\sim}2.3$.

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