Abstract

We develop new strategies to build numerical relativity surrogate models for eccentric binary black hole systems, which are expected to play an increasingly important role in current and future gravitational-wave detectors. We introduce a new surrogate waveform model, \texttt{NRSur2dq1Ecc}, using 47 nonspinning, equal-mass waveforms with eccentricities up to $0.2$ when measured at a reference time of $5500M$ before merger. This is the first waveform model that is directly trained on eccentric numerical relativity simulations and does not require that the binary circularizes before merger. The model includes the $(2,2)$, $(3,2)$, and $(4,4)$ spin-weighted spherical harmonic modes. We also build a final black hole model, \texttt{NRSur2dq1EccRemnant}, which models the mass, and spin of the remnant black hole. We show that our waveform model can accurately predict numerical relativity waveforms with mismatches $\approx 10^{-3}$, while the remnant model can recover the final mass and dimensionless spin with absolute errors smaller than $\approx 5 \times 10^{-4}M$ and $\approx 2 \times10^{-3}$ respectively. We demonstrate that the waveform model can also recover subtle effects like mode-mixing in the ringdown signal without any special ad-hoc modeling steps. Finally, we show that despite being trained only on equal-mass binaries, \texttt{NRSur2dq1Ecc} can be reasonably extended up to mass ratio $q\approx3$ with mismatches $\simeq 10^{-2}$ for eccentricities smaller than $\sim 0.05$ as measured at a reference time of $2000M$ before merger. The methods developed here should prove useful in the building of future eccentric surrogate models over larger regions of the parameter space.

Highlights

  • Detection of gravitational waves (GWs) [1, 2] by the LIGO [3] and Virgo [4] detectors has opened a new window in astrophysics to probe binary compact objects – binary black holes (BBHs) being the most abundant source for these detectors

  • This is motivated by the expectation that even if a binary is formed with a nonzero eccentricity, it should circularize before reaching the frequency band of ground based detectors, as eccentricity gets radiated away via GWs during the long inspiral [23]

  • Where ∆AS22 ≈ ∆A22 and ∆φS22 ≈ ∆φ22 are the surrogate models for ∆A22 and ∆φ22 respectively while A022 and φ022 are the amplitude and phase of the quasicircular numerical relativity (NR) waveform used in the decompositions [cf

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Summary

Introduction

Detection of gravitational waves (GWs) [1, 2] by the LIGO [3] and Virgo [4] detectors has opened a new window in astrophysics to probe binary compact objects – binary black holes (BBHs) being the most abundant source for these detectors. Both detection and extraction of source properties from the GW signal relies on the availability of accurate inspiral-merger-ringdown (IMR) waveform models for BBHs. While numerical relativity (NR) provides the most accurate gravitational waveforms for BBHs, they are computationally expensive, taking weeks to months to generate a single waveform. Recent followup analysis of GW190521 [32] claim this event to be consistent with a BBH source with eccentricity ranging from ∼ 0.1 [33] up to ∼ 0.7 [34] (see [35, 36])

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