Abstract

As gravitational-wave detectors become more sensitive, we will access a greater variety of signals emitted by compact binary systems, shedding light on their astrophysical origin and environment. A key physical effect that can distinguish among formation scenarios is the misalignment of the spins with the orbital angular momentum, causing the spins and the binary's orbital plane to precess. To accurately model such systems, it is crucial to include multipoles beyond the dominant quadrupole. Here, we develop the first multipolar precessing waveform model in the effective-one-body (EOB) formalism for the inspiral, merger and ringdown (IMR) of binary black holes: SEOBNRv4PHM. In the nonprecessing limit, the model reduces to SEOBNRv4HM, which was calibrated to numerical-relativity (NR) simulations, and waveforms from perturbation theory. We validate SEOBNRv4PHM by comparing it to the public catalog of 1405 precessing NR waveforms of the Simulating eXtreme Spacetimes (SXS) collaboration, and also to new 118 precessing NR waveforms, which span mass ratios 1-4 and spins up to 0.9. We stress that SEOBNRv4PHM is not calibrated to NR simulations in the precessing sector. We compute the unfaithfulness against the 1523 SXS precessing NR waveforms, and find that, for $94\%$ ($57\%$) of the cases, the maximum value, in the total mass range $20-200 M_\odot$, is below $3\%$ ($1\%$). Those numbers become $83\%$ ($20\%$) when using the IMR, multipolar, precessing phenomenological model IMRPhenomPv3HM. We investigate the impact of such unfaithfulness values with two parameter-estimation studies on synthetic signals. We also compute the unfaithfulness between those waveform models and identify in which part of the parameter space they differ the most. We validate them also against the multipolar, precessing NR surrogate model NRSur7dq4, and find that the SEOBNRv4PHM model outperforms IMRPhenomPv3HM.

Highlights

  • Since the Laser Interferometer Gravitational wave Observatory (LIGO) detected a gravitational wave (GWs) from a binary–black-hole (BBH) in 2015 [1], multiple observations of GWs from BBHs have been made with2470-0010=2020=102(4)=044055(24)Published by the American Physical SocietyPHYS

  • Following previous precessing SEOBNR models [26,33,86], we have built such a model twisting up the aligned-spin waveforms of SEOBNRv4HM [45,46] from the coprecessing [21,23,42,43,44] to the inertial frame, through the EOB equations of motion for the spins and orbital angular momentum

  • With respect to the previous precessing SEOBNR model, SEOBNRv3P [33], which has been used in LIGO/Virgo data analysis [5,59,60], the new model (i) employs a more accurate aligned-spin two-body dynamics, since, in the nonprecessing limit, it reduces to SEOBNRv4HM, which was calibrated to 157 Simulating eXtreme Spacetimes (SXS) NR simulations [47,48], and 13 waveforms [49] from BH perturbation theory, (ii) includes in the coprecessing frame the modes ð2; Æ2Þ; ð2; Æ1Þ; ð3; Æ3Þ; ð4; Æ4Þ and ð5; Æ5Þ, instead of only ð2; Æ2Þ; ð2; Æ1Þ, (iii) incorporates the merger-ringdown signal in the coprecessing frame instead of the inertial frame, (iv) describes the merger-ringdown stage through a phenomenological fit to NR waveforms

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Summary

INTRODUCTION

Since the Laser Interferometer Gravitational wave Observatory (LIGO) detected a gravitational wave (GWs) from a binary–black-hole (BBH) in 2015 [1], multiple observations of GWs from BBHs have been made with. We consider the state-ofthe-art surrogate waveform model with full spin precession and higher modes [52] (NRSur7dq4), developed for binaries with mass ratios 1–4, (dimensionless) BH’s spins up to 0.8 and binary’s total masses larger than ∼60 M⊙. It includes in the coprecessing frame all modes up to l 1⁄4 4.

New 118 precessing numerical-relativity waveforms
Accuracy of new numerical-relativity waveforms
Inspiral-plunge waveforms
Merger-ringdown waveforms
On the fits of calibration parameters in presence of precession
BAYESIAN ANALYSIS WITH MULTIPOLAR PRECESSING WAVEFORM MODELS
Findings
CONCLUSIONS
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