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Tests of General Relativity with GW150914

B. P. AbbottLIGOR. AbbottLIGOT. D. AbbottLouisiana State UniversityM. R. AbernathyLIGOF. AcerneseComplesso Universitario di Monte Sant’AngeloK. AckleyUniversity of FloridaC. AdamsLIGO Livingston ObservatoryT. AdamsUniversité Savoie Mont BlancP. AddessoUniversità di SalernoR. X. AdhikariLIGOV. B. AdyaAlbert-Einstein-InstitutC. AffeldtAlbert-Einstein-InstitutM. AgathosNikhefK. AgatsumaNikhefN. AggarwalLIGOO. D. AguiarInstituto Nacional de Pesquisas EspaciaisL. AielloINFNA. AinInter-University Centre for Astronomy and AstrophysicsP. AjithInternational Centre for Theoretical SciencesB. AllenAlbert-Einstein-InstitutA. AlloccaINFNP. A. AltinAustralian National UniversityS. B. AndersonLIGOW. G. AndersonUniversity of Wisconsin–MilwaukeeK. AraiLIGOM. C. ArayaLIGOC. C. ArceneauxThe University of MississippiJ. S. AreedaCalifornia State University FullertonN. ArnaudUniversité Paris–SudK. G. ArunChennai Mathematical InstituteS. AscenziINFNG. AshtonUniversity of SouthamptonM. AstUniversität HamburgS. M. AstonLIGO Livingston ObservatoryP. AstoneINFNP. AufmuthAlbert-Einstein-InstitutC. AulbertAlbert-Einstein-InstitutS. BabakAlbert-Einstein-InstitutP. BaconUniversité Paris DiderotM. K. M. BaderNikhefP. T. BakerMontana State UniversityF. BaldacciniINFNG. BallardinEuropean Gravitational Observatory (EGO)S. W. BallmerSyracuse UniversityJ. C. BarayogaLIGOS. E. BarclayUniversity of GlasgowB. C. BarishLIGOD. BarkerF. BaroneComplesso Universitario di Monte Sant’AngeloB. BarrUniversity of GlasgowL. BarsottiLIGOM. BarsugliaUniversité Paris DiderotD. BartaWigner RCPJ. BartlettI. BartosColumbia UniversityR. BassiriStanford UniversityA. BastiINFNJ. C. BatchC. BauneAlbert-Einstein-InstitutV. BavigaddaEuropean Gravitational Observatory (EGO)M. BazzanINFNB. BehnkeAlbert-Einstein-InstitutM. BejgerA. S. BellUniversity of GlasgowC. BellUniversity of GlasgowB. K. BergerLIGOJ. BergmanG. BergmannAlbert-Einstein-InstitutC. P. L. BerryUniversity of BirminghamD. BersanettiINFNA. BertoliniNikhefJ. BetzwieserLIGO Livingston ObservatoryS. BhagwatSyracuse UniversityR. BhandareRRCATI. A. BilenkoLomonosov Moscow State UniversityG. BillingsleyLIGOJ. BirchLIGO Livingston ObservatoryR. BirneyUniversity of the West of ScotlandO. BirnholtzAlbert-Einstein-InstitutS. BiscansLIGOA. BishtAlbert-Einstein-InstitutM. BitossiEuropean Gravitational Observatory (EGO)C. BiwerSyracuse UniversityM. A. BizouardUniversité Paris–SudJ. K. BlackburnLIGOC. D. BlairUniversity of Western AustraliaD. G. BlairUniversity of Western AustraliaR. M. BlairS. BloemenRadboud University NijmegenO. BockAlbert-Einstein-InstitutT. P. BodiyaLIGOM. BoërUniversité Côte d’AzurG. BogaertUniversité Côte d’AzurC. BoganAlbert-Einstein-InstitutA. BohéAlbert-Einstein-InstitutP. BojtosMTA Eötvös UniversityC. BondUniversity of BirminghamF. BonduInstitut de Physique de RennesR. BonnandUniversité Savoie Mont BlancB. A. BoomNikhef
2016en
ABI

Annotatsiya

The LIGO detection of GW150914 provides an unprecedented opportunity to study the two-body motion of a compact-object binary in the large-velocity, highly nonlinear regime, and to witness the final merger of the binary and the excitation of uniquely relativistic modes of the gravitational field. We carry out several investigations to determine whether GW150914 is consistent with a binary black-hole merger in general relativity. We find that the final remnant's mass and spin, as determined from the low-frequency (inspiral) and high-frequency (postinspiral) phases of the signal, are mutually consistent with the binary black-hole solution in general relativity. Furthermore, the data following the peak of GW150914 are consistent with the least-damped quasinormal mode inferred from the mass and spin of the remnant black hole. By using waveform models that allow for parametrized general-relativity violations during the inspiral and merger phases, we perform quantitative tests on the gravitational-wave phase in the dynamical regime and we determine the first empirical bounds on several high-order post-Newtonian coefficients. We constrain the graviton Compton wavelength, assuming that gravitons are dispersed in vacuum in the same way as particles with mass, obtaining a 90%-confidence lower bound of 10^{13} km. In conclusion, within our statistical uncertainties, we find no evidence for violations of general relativity in the genuinely strong-field regime of gravity.

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