Abstract

While most binary inspirals are expected to have circularized before they enter the LIGO/Virgo frequency band, a small fraction of those binaries could have non-negligible orbital eccentricity depending on their formation channel. Hence, it is important to accurately model eccentricity effects in waveform models used to detect those binaries, infer their properties, and shed light on their astrophysical environment. We develop a multipolar effective-one-body (EOB) eccentric waveform model for compact binaries whose components have spins aligned or antialigned with the orbital angular momentum. The waveform model contains eccentricity effects in the radiation-reaction force and gravitational modes through second post-Newtonian (PN) order, including tail effects, and spin-orbit and spin-spin couplings. We recast the PN-expanded, eccentric radiation-reaction force and modes in factorized form so that the newly derived terms can be directly included in the state-of-the-art, quasi-circular--orbit EOB model currently used in LIGO/Virgo analyses (i.e., the SEOBNRv4HM model).

Highlights

  • The observation of gravitational waves (GWs) by the LIGO-Virgo detectors [1,2] have corroborated the existence of binary black holes (BBHs) in our universe

  • Extending the waveform models used today in GW astronomy from quasicircular to eccentric orbits is important for future observations with LIGO, Virgo, and KAGRA detectors [21], and with new facilities on the ground (Cosmic Explorer and Einstein Telescope), and in space (LISA)

  • While this presents a challenge for waveform modeling and data analysis, it offers the unique opportunity to unveil the formation channels of compact binaries and probe their environment

Read more

Summary

INTRODUCTION

The observation of gravitational waves (GWs) by the LIGO-Virgo detectors [1,2] have corroborated the existence of binary black holes (BBHs) in our universe. Binaries are expected to circularize [9,10] as they approach merger due to the emission of gravitational radiation Depending on their astrophysical formation channel, a small fraction of binaries could have nonnegligible orbital eccentricity, as they enter the frequency bands of current detectors. [82] added eccentric corrections in the SEOBNRv4 [74,83] waveform model, notably in the (2,2),(2,1),(3,3),(4,4) modes through 2PN order, including spin-orbit (SO) and spin-spin (SS) couplings, but not tail effects. [84,85] incorporated noncircular effects in the TEOBResumS_SM [76,86] model at leading PN order in the azimuthal component of the RR force and used a quasicircular 2PN-expanded radial RR force without spin or tail effects They included eccentric corrections at leading PN order to all modes m ≠ 0 up to l 1⁄4 jmj 1⁄4 5. We provide our results for the RR force and waveform modes as Mathematica files in the Supplemental Material [88]

Notation
RADIATION REACTION FORCE
Summary of the approach used in this paper for the RR force
EOB Hamiltonian and angular momentum
H SEOOB pφ 2c3r3
Energy and angular momentum fluxes
Ansatz for the Schott terms
F Lr Opφ
Solving for the eccentric-orbits RR force
F F rpφ φpr
LO spin orbit
LO spin-spin ζ1
F SrS: ð55Þ
INITIAL CONDITIONS
Initial conditions for quasicircular orbits
Initial conditions for eccentric orbits
GRAVITATIONAL WAVEFORM MODES
Instantaneous nonspinning contributions
Hereditary contributions
Aligned-spin contributions
Factorized modes
CONCLUSIONS
ADM to EOB transformation
Harmonic to EOB transformation
Transformation for the SSC

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.