2017
DOI: 10.1016/j.physletb.2017.04.033
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Test of the Weak Equivalence Principle using LIGO observations of GW150914 and Fermi observations of GBM transient 150914

Abstract: About 0.4 s after the Laser Interferometer Gravitational-Wave Observatory (LIGO) detected a transient gravitational-wave (GW) signal GW150914, the Fermi Gamma-ray Burst Monitor (GBM) also found a weak electromagnetic transient (GBM transient 150914). Time and location coincidences favor a possible association between GW150904 and GBM transient 150914. Under this possible association, we adopt Fermi's electromagnetic (EM) localization and derive constraints on possible violations of the Weak Equivalence Princip… Show more

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Cited by 18 publications
(14 citation statements)
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“…We first use a toy model in order to show arithmetically the appearance of a divergence in the metric perturbation used to compute the Shapiro delay when one is using the set of gauge restrictions [Eqs. (16)(17)] that is commonly implicitly used in the literature. We show that the divergence appears because of an unsuitable choice of coordinate time in order to describe the metric, and is therefore simply cured by using an appropriate (nonambiguous) coordinate time -for instance, a coordinate time that corresponds to the proper time of any given observer.…”
Section: Discussionmentioning
confidence: 99%
“…We first use a toy model in order to show arithmetically the appearance of a divergence in the metric perturbation used to compute the Shapiro delay when one is using the set of gauge restrictions [Eqs. (16)(17)] that is commonly implicitly used in the literature. We show that the divergence appears because of an unsuitable choice of coordinate time in order to describe the metric, and is therefore simply cured by using an appropriate (nonambiguous) coordinate time -for instance, a coordinate time that corresponds to the proper time of any given observer.…”
Section: Discussionmentioning
confidence: 99%
“…Based on the associations between five TeV neutrinos and gamma-ray photons from gamma-ray bursts (GRBs), Wei et al (2016a) tightened the constraint on the deviation from WEP to an accuracy of ∼ 10 −11 − 10 −13 when adopting the gravitational potential of the Laniakea supercluster of galaxies. Besides the neutrino-photon delays, such a test has been also applied to the delays of photons with different energies (e.g., GRBs Sang, Lin, & Chang, 2016;Yu, Xi, & Wang, 2018), fast radio bursts (Wei et al, 2015;Tingay & Kaplan, 2016), TeV blazars (Wei et al, 2016b), and the Crab pulsar (Yang & Zhang, 2016;Zhang & Gong, 2017;Leung et al, 2018)), and the delays between photons and gravitational waves (Kahya & Desai, 2016;Li et al, 2016;Wu et al, 2016;Abbott et al, 2017;Liu et al, 2017;Wang et al, 2017;Wei et al, 2017;Shoemaker & Murase, 2018).…”
Section: Introductionmentioning
confidence: 99%
“…The majority of previous attempts to constrain violations of the WEP via ∆γ ij with GRBs [18,[51][52][53][54], FRBs [6,[55][56][57][58], Supernovae [59,60], Gravitational Waves [61][62][63][64][65][66][67][68][69], Blazar Flares [70][71][72][73][74] or Pulsars [75][76][77][78] have assumed that the gravitational potential is dominated by the contribution from the Milky Way and/or other massive objects such as the Laniakea supercluster. This has two major shortcomings for distant sources: firstly the gravitational potential in Equation 2 should be a fluctuation about the cosmological mean (and thus can take either sign, unlike in the multiple-source approximation where it is strictly additive), and secondly the long range behaviour of the gravitational potential means that we cannot neglect the large-scale distribution of mass [8,9].…”
Section: B Comparison With the Literaturementioning
confidence: 99%