2013
DOI: 10.1103/physrevlett.111.241104
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Catalog of 174 Binary Black Hole Simulations for Gravitational Wave Astronomy

Abstract: This paper presents a publicly available catalog of 174 numerical binary black-hole simulations following up to 35 orbits. The catalog includes 91 precessing binaries, mass ratios up to 8:1, orbital eccentricities from a few percent to 10 −5 , black-hole spins up to 98% of the theoretical maximum, and radiated energies up to 11.1% of the initial mass. We establish remarkably good agreement with post-Newtonian precession of orbital and spin directions for two new precessing simulations, and we discuss other app… Show more

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Cited by 375 publications
(330 citation statements)
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“…We provide a detailed evaluation of the source properties and inferred parameters of GW150914, GW151226, and LVT151012. We use models of the waveform covering the inspiral, merger, and ringdown phases based on combining post-Newtonian (PN) theory [19][20][21][22][23][24], the effective-onebody (EOB) formalism [25][26][27][28][29], and numerical relativity simulations [30][31][32][33][34][35][36]. One model is restricted to spins aligned with the orbital angular momentum [8,9], while the other allows for nonaligned orientation of the spins, which can lead to precession of the orbital plane [37,38].…”
Section: Introductionmentioning
confidence: 99%
“…We provide a detailed evaluation of the source properties and inferred parameters of GW150914, GW151226, and LVT151012. We use models of the waveform covering the inspiral, merger, and ringdown phases based on combining post-Newtonian (PN) theory [19][20][21][22][23][24], the effective-onebody (EOB) formalism [25][26][27][28][29], and numerical relativity simulations [30][31][32][33][34][35][36]. One model is restricted to spins aligned with the orbital angular momentum [8,9], while the other allows for nonaligned orientation of the spins, which can lead to precession of the orbital plane [37,38].…”
Section: Introductionmentioning
confidence: 99%
“…These PN approximants can differ from each other during the last hundreds of cycles before merger.] Yet NR simulations have been able to cover only tens of orbits [27][28][29] until now. This gap has emerged as one of the most important sources of uncertainty in present IMR waveform models.…”
mentioning
confidence: 99%
“…Halving the symmetric mass ratio ν (e.g., from m 1 =m 2 ¼ 2 to m 1 =m 2 ¼ 7) doubles T. Increasing the simulation length T is difficult: it becomes harder to preserve phase coherency, the outer boundary of a simulation is in causal contact for a larger fraction of the simulation, and existing codes would require many months or even years of wall-clock time. Therefore, progress toward longer simulations has been sluggish, with T increasing by only about a factor of 2 to 3 during the last five years [28,29,[31][32][33]. The duration T needed to close the gap depends on the binary parameters and the detector bandwidth.…”
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confidence: 99%
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“…Second row shows gravitationalwave strain projected onto each detector in the 35-to 350-Hz band. Solid lines show a numerical relativity waveform (waveform shown is SXS:BBH:0305 available for download at www.black-holes.org/ waveforms) for a system with parameters consistent with those recovered from GW150914 (38,39) confirmed to 99.9% by an independent calculation based on ref. 40.…”
Section: Initial Ligo-the Era Of Upper Limitsmentioning
confidence: 87%