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Tests of general relativity with GWTC-3

R. AbbottCalifornia Institute of TechnologyH. AbeTokyo Institute of TechnologyF. AcerneseINFNK. AckleyMonash UniversityN. AdhikariUniversity of Wisconsin-MilwaukeeR. X. AdhikariCalifornia Institute of TechnologyV.K AdkinsLouisiana State UniversityV. B. AdyaAustralian National UniversityC. AffeldtLeibniz Universität HannoverD. AgarwalInter-University Centre for Astronomy and AstrophysicsM. AgathosFriedrich-Schiller-Universität JenaK. AgatsumaUniversity of BirminghamN. AggarwalNorthwestern UniversityOdylio D. AguiarInstituto Nacional de Pesquisas EspaciaisL. AielloCardiff UniversityA. AinINFNP. AjithTata Institute of Fundamental ResearchT. AkutsuNational Astronomical Observatory of Japan (NAOJ)P. F. de AlarcónUniversitat de les Illes BalearsS. AlbanesiINFN Sezione di TorinoR. A. AlfaidiUniversity of GlasgowA. AlloccaINFNP. A. AltinAustralian National UniversityA. AmatoUniversité de LyonChristopher Kumar AnandMonash UniversityShreya AnandCalifornia Institute of TechnologyA. AnanyevaCalifornia Institute of TechnologyS. B. AndersonCalifornia Institute of TechnologyW. G. AndersonUniversity of Wisconsin-MilwaukeeMakoto AndoThe University of TokyoT. AndradeUniversitat de BarcelonaN. AndresLaboratoire d’Annecy de Physique des Particules - IN2P3M. Andrés‐CarcasonaBarcelona Institute of Science and TechnologyT. AndrićGran Sasso Science Institute (GSSI)S. V. AngelovaUniversity of StrathclydeStefano AnsoldiINFNJavier M. AntelisEmbry-Riddle Aeronautical UniversityS. AntierUniversity of AmsterdamTheocharis A. ApostolatosNational and Kapodistrian University of AthensE. Z. AppavuravtherINFNS. AppertCalifornia Institute of TechnologyS. K. AppleAmerican UniversityK. AraiCalifornia Institute of TechnologyA. ArayaThe University of TokyoM. C. ArayaCalifornia Institute of TechnologyJ. S. AreedaCalifornia State University FullertonM. ArèneUniversité de ParisN. AritomiNational Astronomical Observatory of Japan (NAOJ)N. ArnaudEuropean Gravitational Observatory (EGO)M. ArogetiGeorgia Institute of TechnologyS. M. AronsonLouisiana State UniversityK. G. ArunChennai Mathematical InstituteHideki AsadaHirosaki UniversityY. AsaliColumbia UniversityG. AshtonUniversity of PortsmouthY. AsoNational Astronomical Observatory of Japan (NAOJ)M. AssiduoINFNS. Assis de Souza MeloEuropean Gravitational Observatory (EGO)S. M. AstonLIGO Livingston ObservatoryP. AstoneINFNF. AubinINFNK. AultONealEmbry-Riddle Aeronautical UniversityC. AustinLouisiana State UniversityS. BabakUniversité de ParisF. BadaraccoUniversité catholique de LouvainM. K. M. BaderNikhefC. BadgerUniversity of LondonS. BaeKorea Institute of Science and Technology InformationY. BaeNational Institute for Mathematical SciencesA. M. BaerChristopher Newport UniversityS. BagnascoINFN Sezione di TorinoY. BaiCalifornia Institute of TechnologyJ. BairdUniversité de ParisR. BajpaiThe Graduate University for Advanced Studies (SOKENDAI)T. BakaUtrecht UniversityM. BallUniversity of OregonG. BallardinEuropean Gravitational Observatory (EGO)S. BallmerSyracuse UniversityA. BalsamoChristopher Newport UniversityG. BaltusUniversité de LiègeS. BanagiriNorthwestern UniversityB. BanerjeeGran Sasso Science Institute (GSSI)D. BankarInter-University Centre for Astronomy and AstrophysicsJ. C. BarayogaCalifornia Institute of TechnologyC. BarbieriINAFB. C. BarishCalifornia Institute of TechnologyD. BarkerP. BarneoUniversitat de BarcelonaF. BaroneINFNB. BarrUniversity of GlasgowL. BarsottiMassachusetts Institute of TechnologyM. BarsugliaUniversité de ParisD. BartaRMKIJ. BartlettM. A. BartonUniversity of GlasgowI. BartosUniversity of FloridaS. BasakTata Institute of Fundamental ResearchR. BassiriStanford UniversityA. BastiINFNM. BawajINFN
2025en
ABI

Abstract

The ever-increasing number of detections of gravitational waves from compact binaries by the Advanced LIGO and Advanced Virgo detectors allows us to perform ever-more sensitive tests of general relativity (GR) in the dynamical and strong-field regime of gravity. We perform a suite of tests of GR using the compact binary signals observed during the second half of the third observing run of those detectors. We restrict our analysis to the 15 confident signals that have false alarm rates ≤10<sup>−3</sup> yr<sup>−1</sup>. In addition to signals consistent with binary black hole mergers, the new events include GW200115_042309, a signal consistent with a neutron star–black hole merger. We find the residual power, after subtracting the best fit waveform from the data for each event, to be consistent with the detector noise. Additionally, we find all the post-Newtonian deformation coefficients to be consistent with the predictions from GR, with an improvement by a factor of ∼2 in the −1⁢PN parameter. We also find that the spin-induced quadrupole moments of the binary black hole constituents are consistent with those of Kerr black holes in GR. We find no evidence for dispersion of gravitational waves, non-GR modes of polarization, or post-merger echoes in the events that were analyzed. We update the bound on the mass of the graviton, at 90% credibility, to ≤2.42×10<sup>−23</sup> ⁢eV/<sup>2</sup>. The final mass and final spin as inferred from the premerger and postmerger parts of the waveform are consistent with each other. The studies of the properties of the remnant black holes, including deviations of the quasinormal mode frequencies and damping times, show consistency with the predictions of GR. In addition to considering signals individually, we also combine results from the catalog of gravitational waves signals to calculate more precise population constraints. We find no evidence in support of physics beyond general relativity.

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Cited by 10 references