Abstract

We investigate the ability of the Laser Interferometer Space Antenna (LISA) to measure the center of mass acceleration of stellar-origin black hole binaries emitting gravitational waves. Our analysis is based on the idea that the acceleration of the center of mass induces a time variation in the redshift of the gravitational wave, which in turn modifies its waveform. We confirm that while the cosmological acceleration is too small to leave a detectable imprint on the gravitational waveforms observable by LISA, larger peculiar accelerations may be measurable for sufficiently long lived sources. We focus on stellar mass black hole binaries, which will be detectable at low frequencies by LISA and near coalescence by ground based detectors. These sources may have large peculiar accelerations, for instance, if they form in nuclear star clusters or in AGN accretion disks. If that is the case, we find that in an astrophysical population calibrated to the LIGO-Virgo observed merger rate, LISA will be able to measure the peculiar acceleration of a small but significant fraction of the events if the mission lifetime is extended beyond the nominal duration of 4 years. In this scenario LISA will be able to assess whether black hole binaries form close to galactic centers, particularly in AGN disks, and will thus help discriminate between different formation mechanisms. Although for a nominal 4 years LISA mission the peculiar acceleration effect cannot be measured, a consistent fraction of events may be biased by strong peculiar accelerations which, if present, may imprint large systematic errors on some waveform parameters. In particular, estimates of the luminosity distance could be strongly biased and consequently induce large systematic errors on LISA measurements of the Hubble constant with stellar mass black hole binaries.

Highlights

  • The long awaited detection [1,2,3,4] of gravitational waves (GWs) by the LIGO interferometer, followed by Virgo [5,6], opened a new era in the history of astronomy

  • If that is the case, we find that in an astrophysical population calibrated to the LIGO-Virgo observed merger rate, Laser Interferometer Space Antenna (LISA) will be able to measure the peculiar acceleration of a small but significant fraction of the events if the mission lifetime is extended beyond the nominal duration of 4 years

  • By adopting the official LISA configuration of [22] and astrophysical binary BH populations calibrated to the LIGO/Virgo detection rate, we investigate via a Fisher matrix approach the precision with which the peculiar acceleration can be inferred from the data, improving on the estimates of [35,44]

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Summary

INTRODUCTION

The long awaited detection [1,2,3,4] of gravitational waves (GWs) by the LIGO interferometer, followed by Virgo [5,6], opened a new era in the history of astronomy. This will make these sources excellent probes of putative tiny deviations away from GR (orders of magnitude weaker than those detectable with ground interferometers) [32,33] or even environmental effects from the interaction of the binary with the surrounding matter [16,34] Among these environmental effects, an especially attractive one is provided by the peculiar acceleration of the binary’s center of mass (c.m.) with respect to the observer. The waveform parameter most strongly biased is the luminosity distance of the source This suggests that strong peculiar accelerations can induce a large systematic error on measurements of the Hubble constant with stellar-mass black hole binaries (BHBs) observed by LISA (see e.g., [31,52]).

THE EFFECT OF THE CENTER OF MASS ACCELERATION ON THE GRAVITATIONAL
Constant redshift
Time dependent redshift
Implementation of the peculiar acceleration effect
Astrophysical black hole binary populations
Waveform generation and parameter estimation
LISA mission simulations
RESULTS
Number of detections
Effect across the parameter space
Biases
Intermediate mass black holes
DISCUSSION AND CONCLUSION
Derivation of the redshift perturbation
Derivation of the perturbed phase
Derivation of the perturbed amplitude
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