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Tests of general relativity with the binary black hole signals from the LIGO-Virgo catalog GWTC-1

B. P. AbbottCalifornia Institute of TechnologyR. AbbottCalifornia Institute of TechnologyT. D. AbbottLouisiana State UniversityS. AbrahamInter-University Centre for Astronomy and AstrophysicsF. AcerneseComplesso Universitario di Monte S.AngeloK. AckleyMonash UniversityC. AdamsLIGO Livingston ObservatoryR. X. AdhikariCalifornia Institute of TechnologyV. B. AdyaLeibniz Universität HannoverC. AffeldtLeibniz Universität HannoverM. AgathosUniversity of CambridgeK. AgatsumaUniversity of BirminghamN. AggarwalMassachusetts Institute of TechnologyO. D. AguiarInstituto Nacional de Pesquisas EspaciaisL. AielloLaboratori Nazionali del Gran SassoA. AinInter-University Centre for Astronomy and AstrophysicsP. AjithTata Institute of Fundamental ResearchB. AllenUniversity of Illinois at Urbana-ChampaignA. AlloccaINFNM. Á. AloyUniversitat de ValènciaP. A. AltinAustralian National UniversityA. AmatoLaboratoire des Matériaux Avancés (LMA)A. AnanyevaCalifornia Institute of TechnologyS. B. AndersonCalifornia Institute of TechnologyW. G. AndersonUniversity of Wisconsin-MilwaukeeS. V. AngelovaUniversity of StrathclydeS. AntierLAL - Laboratoire de l'Accélérateur Linéaire (Centre Scientifique d'Orsay B.P. 34 91898 ORSAY Cedex - France)S. AppertCalifornia Institute of TechnologyK. AraiCalifornia Institute of TechnologyM. C. ArayaCalifornia Institute of TechnologyJ. S. AreedaCalifornia State University FullertonM. ArèneUniversité Paris DiderotN. ArnaudUniversité Paris-SaclayK. G. ArunChennai Mathematical InstituteS. AscenziINFNG. AshtonMonash UniversityS. M. AstonLIGO Livingston ObservatoryP. AstoneF. AubinUniversité Savoie Mont BlancP. AufmuthLeibniz Universität HannoverK. AultONealC. AustinLouisiana State UniversityV. AvendanoMontclair State UniversityA. Avila-AlvarezCalifornia State University FullertonS. BabakUniversité Paris DiderotP. BaconUniversité Paris DiderotF. BadaraccoLaboratori Nazionali del Gran SassoM. K. M. BaderNikhefS. BaeKorea Institute of Science and Technology InformationP. T. BakerWest Virginia UniversityF. BaldacciniINFNG. BallardinEuropean Gravitational Observatory (EGO)S. W. BallmerSyracuse UniversityS. BanagiriUniversity of MinnesotaJ. C. BarayogaCalifornia Institute of TechnologyS. E. BarclayUniversity of GlasgowB. C. BarishCalifornia Institute of TechnologyD. BarkerK. BarkettS. BarnumMassachusetts Institute of TechnologyF. BaroneComplesso Universitario di Monte S.AngeloB. BarrUniversity of GlasgowL. BarsottiMassachusetts Institute of TechnologyM. BarsugliaUniversité Paris DiderotD. BartaWigner RCPJ. BartlettI. BartosUniversity of FloridaR. BassiriStanford UniversityA. BastiINFNM. BawajINFNJ. C. BayleyUniversity of GlasgowM. BazzanINFNB. BécsyMontana State UniversityM. BejgerPolish Academy of SciencesI. BelahceneLAL - Laboratoire de l'Accélérateur Linéaire (Centre Scientifique d'Orsay B.P. 34 91898 ORSAY Cedex - France)A. S. BellUniversity of GlasgowD. BeniwalUniversity of AdelaideB. K. BergerStanford UniversityG. BergmannLeibniz Universität HannoverSebastiano BernuzziFriedrich-Schiller-Universität JenaJ. J. BeroRochester Institute of TechnologyC. P. L. BerryD. BersanettiA. BertoliniNikhefJ. BetzwieserLIGO Livingston ObservatoryR. BhandareJ. BidlerCalifornia State University FullertonI. A. BilenkoLomonosov Moscow State UniversityS. A. BilgiliWest Virginia UniversityG. BillingsleyCalifornia Institute of TechnologyJ. BirchLIGO Livingston ObservatoryR. BirneyUniversity of StrathclydeO. BirnholtzRochester Institute of TechnologyS. BiscansMassachusetts Institute of TechnologyS. BiscoveanuMonash UniversityA. BishtLeibniz Universität HannoverM. BitossiEuropean Gravitational Observatory (EGO)M. A. BizouardLAL - Laboratoire de l'Accélérateur Linéaire (Centre Scientifique d'Orsay B.P. 34 91898 ORSAY Cedex - France)J. K. BlackburnCalifornia Institute of TechnologyC. D. BlairLIGO Livingston Observatory
2019en
ABI

Annotatsiya

The detection of gravitational waves by Advanced LIGO and Advanced Virgo provides an opportunity to test general relativity in a regime that is inaccessible to traditional astronomical observations and laboratory tests. We present four tests of the consistency of the data with binary black hole gravitational waveforms predicted by general relativity. One test subtracts the best-fit waveform from the data and checks the consistency of the residual with detector noise. The second test checks the consistency of the low- and high-frequency parts of the observed signals. The third test checks that phenomenological deviations introduced in the waveform model (including in the post-Newtonian coefficients) are consistent with 0. The fourth test constrains modifications to the propagation of gravitational waves due to a modified dispersion relation, including that from a massive graviton. We present results both for individual events and also results obtained by combining together particularly strong events from the first and second observing runs of Advanced LIGO and Advanced Virgo, as collected in the catalog GWTC-1. We do not find any inconsistency of the data with the predictions of general relativity and improve our previously presented combined constraints by factors of 1.1 to 2.5. In particular, we bound the mass of the graviton to be ${m}_{g}\ensuremath{\le}4.7\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}23}\text{ }\text{ }\mathrm{eV}/{c}^{2}$ (90% credible level), an improvement of a factor of 1.6 over our previously presented results. Additionally, we check that the four gravitational-wave events published for the first time in GWTC-1 do not lead to stronger constraints on alternative polarizations than those published previously.

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