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Properties of the Binary Black Hole Merger GW150914

B. P. AbbottCalifornia Institute of TechnologyR. AbbottCalifornia Institute of TechnologyT. D. AbbottLouisiana State UniversityM. R. AbernathyCalifornia Institute of TechnologyF. AcerneseComplesso Universitario di Monte S.AngeloK. AckleyUniversity of FloridaC. AdamsLIGO Livingston ObservatoryT. AdamsUniversité Savoie Mont BlancP. AddessoUniversità di SalernoR. X. AdhikariCalifornia Institute of TechnologyV. B. AdyaAlbert-Einstein-InstitutC. AffeldtAlbert-Einstein-InstitutM. AgathosNikhef, Science ParkK. AgatsumaNikhef, Science ParkN. AggarwalMassachusetts Institute of TechnologyO. D. AguiarInstituto Nacional de Pesquisas EspaciaisL. AielloGran Sasso Science InstituteA. AinInter-University Centre for Astronomy and AstrophysicsP. AjithTata Institute of Fundamental ResearchB. AllenAlbert-Einstein-InstitutA. AlloccaSezione di PisaP. A. AltinAustralian National UniversityS. B. AndersonCalifornia Institute of TechnologyW. G. AndersonUniversity of Wisconsin-MilwaukeeK. AraiCalifornia Institute of TechnologyM. C. ArayaCalifornia Institute of TechnologyC. C. ArceneauxThe University of MississippiJ. S. AreedaCalifornia State University FullertonN. ArnaudUniversité Paris-SudK. G. ArunChennai Mathematical InstituteS. AscenziUniversità di Roma Tor VergataG. AshtonUniversity of SouthamptonM. AstUniversität HamburgS. M. AstonLIGO Livingston ObservatoryP. AstoneSezione di RomaP. AufmuthAlbert-Einstein-InstitutC. AulbertAlbert-Einstein-InstitutS. BabakAlbert-Einstein-InstitutP. BaconAstroParticule et CosmologieM. K. M. BaderNikhef, Science ParkP. T. BakerMontana State UniversityF. BaldacciniSezione di PerugiaG. BallardinEuropean Gravitational Observatory (EGO)S. W. BallmerSyracuse UniversityJ. C. BarayogaCalifornia Institute of TechnologyS. E. BarclayUniversity of GlasgowB. C. BarishCalifornia Institute of TechnologyD. BarkerF. BaroneComplesso Universitario di Monte S.AngeloB. BarrUniversity of GlasgowL. BarsottiMassachusetts Institute of TechnologyM. BarsugliaAstroParticule et CosmologieD. BartaWigner RCPJ. BartlettI. BartosColumbia UniversityR. BassiriStanford UniversityA. BastiSezione di PisaJ. C. BatchC. BauneAlbert-Einstein-InstitutV. BavigaddaEuropean Gravitational Observatory (EGO)M. BazzanSezione di PadovaB. BehnkeAlbert-Einstein-InstitutM. BejgerA. S. BellUniversity of GlasgowC. BellUniversity of GlasgowB. K. BergerCalifornia Institute of TechnologyJ. BergmanG. BergmannAlbert-Einstein-InstitutC. P. L. BerryUniversity of BirminghamD. BersanettiSezione di GenovaA. BertoliniNikhef, Science ParkJ. BetzwieserLIGO Livingston ObservatoryS. BhagwatSyracuse UniversityR. BhandareRRCATI. A. BilenkoLomonosov Moscow State UniversityG. BillingsleyCalifornia Institute of TechnologyJ. BirchLIGO Livingston ObservatoryR. BirneyUniversity of the West of ScotlandO. BirnholtzAlbert-Einstein-InstitutS. BiscansMassachusetts Institute of TechnologyA. BishtAlbert-Einstein-InstitutM. BitossiEuropean Gravitational Observatory (EGO)C. BiwerSyracuse UniversityM. A. BizouardUniversité Paris-SudJ. K. BlackburnCalifornia Institute of TechnologyC. D. BlairUniversity of Western AustraliaD. G. BlairUniversity of Western AustraliaR. M. BlairS. BloemenRadboud University NijmegenO. BockAlbert-Einstein-InstitutT. P. BodiyaMassachusetts Institute of TechnologyM. 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, Science Park
2016en
ABI

Аннотация

On September 14, 2015, the Laser Interferometer Gravitational-Wave Observatory (LIGO) detected a gravitational-wave transient (GW150914); we characterize the properties of the source and its parameters. The data around the time of the event were analyzed coherently across the LIGO network using a suite of accurate waveform models that describe gravitational waves from a compact binary system in general relativity. GW150914 was produced by a nearly equal mass binary black hole of masses 36_{-4}^{+5}M_{⊙} and 29_{-4}^{+4}M_{⊙}; for each parameter we report the median value and the range of the 90% credible interval. The dimensionless spin magnitude of the more massive black hole is bound to be <0.7 (at 90% probability). The luminosity distance to the source is 410_{-180}^{+160} Mpc, corresponding to a redshift 0.09_{-0.04}^{+0.03} assuming standard cosmology. The source location is constrained to an annulus section of 610 deg^{2}, primarily in the southern hemisphere. The binary merges into a black hole of mass 62_{-4}^{+4}M_{⊙} and spin 0.67_{-0.07}^{+0.05}. This black hole is significantly more massive than any other inferred from electromagnetic observations in the stellar-mass regime.

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