Probing modified gravity theories and cosmology using gravitational-waves and associated electromagnetic counterparts

The direct detection of gravitational waves by the LIGO/Virgo Collaboration has opened a new window with which to measure cosmological parameters such as the Hubble constant H0, and also probe general relativity on large scales. In this paper we present a new phenomenological approach, together with...

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Veröffentlicht in:Physical review. D 2020-08, Vol.102 (4), p.1, Article 044009
Hauptverfasser: Mastrogiovanni, S., Steer, D. A., Barsuglia, M.
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Sprache:eng
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Zusammenfassung:The direct detection of gravitational waves by the LIGO/Virgo Collaboration has opened a new window with which to measure cosmological parameters such as the Hubble constant H0, and also probe general relativity on large scales. In this paper we present a new phenomenological approach, together with its inferential implementation, for measuring deviations from general relativity (GR) on cosmological scales concurrently with a determination of H0. We consider gravitational waves (GWs) propagating in an expanding homogeneous and isotropic background, but with a modified friction term and dispersion relation relative to that of GR. We find that a single binary neutron star GW detection will poorly constrain the GW friction term. However, a joint analysis including the GW phase and GW-GRB detection delay could improve constraints on some GW dispersion relations provided the delay is measured with millisecond precision. We also show that, for massive gravity, by combining 100 binary neutron stars detections with observed electromagnetic counterparts and host galaxy identification, we will be able to constrain the Hubble constant, the GW damping term and the GW dispersion relation with 2%, 15% and 2% accuracy, respectively. We emphasize that these three parameters should be measured together in order to avoid biases. Finally we apply the method to GW170817, and demonstrate that for all of the GW dispersions relations we consider, including massive gravity, the GW must be emitted ∼ 1.74 s before the gamma-ray burst. Furthermore, at the GW merger peak frequency, we show that the fractional difference between the GW group velocity and c is ≲ 10−17.
ISSN:2470-0010
2470-0029
DOI:10.1103/PhysRevD.102.044009