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Binary Black Hole Mergers in the First Advanced LIGO Observing Run

B. P. AbbottCalifornia Institute of TechnologyR. AbbottCalifornia Institute of TechnologyT. D. AbbottLouisiana State UniversityM. R. AbernathyAmerican UniversityF. AcerneseComplesso Universitario di Monte S.AngeloK. AckleyUniversity of FloridaC. AdamsLIGO Livingston ObservatoryT. AdamsUniversité Savoie Mont BlancP. AddessoUniversity of Sannio at BeneventoR. X. AdhikariCalifornia Institute of TechnologyV. B. AdyaMax-Planck-Institut für GravitationsphysikC. AffeldtMax-Planck-Institut für GravitationsphysikM. AgathosScience ParkK. AgatsumaScience ParkN. AggarwalMassachusetts Institute of TechnologyO. D. AguiarInstituto Nacional de Pesquisas EspaciaisL. AielloA. AinInter-University Centre for Astronomy and AstrophysicsP. AjithTata Institute of Fundamental ResearchB. AllenLeibniz Universität HannoverA. AlloccaINFNP. 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. AscenziINFNG. AshtonUniversity of SouthamptonM. AstUniversität HamburgS. M. AstonLIGO Livingston ObservatoryP. AstoneP. AufmuthLeibniz Universität HannoverC. AulbertMax-Planck-Institut für GravitationsphysikS. BabakMax-Planck-Institut für Gravitations-physikP. BaconUniversité Paris DiderotM. K. M. BaderScience ParkP. T. BakerMontana State UniversityF. BaldacciniINFNG. 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. BarsugliaUniversité Paris DiderotD. BartaWigner RCPJ. BartlettI. BartosColumbia UniversityR. BassiriStanford UniversityA. BastiINFNJ. C. BatchC. BauneMax-Planck-Institut für GravitationsphysikV. BavigaddaEuropean Gravitational Observatory (EGO)M. BazzanINFNM. BejgerA. S. BellUniversity of GlasgowB. K. BergerCalifornia Institute of TechnologyG. BergmannMax-Planck-Institut für GravitationsphysikC. P. L. BerryUniversity of BirminghamD. BersanettiINFNA. BertoliniScience ParkJ. BetzwieserLIGO Livingston ObservatoryS. BhagwatSyracuse UniversityR. BhandareI. A. BilenkoLomonosov Moscow State UniversityG. BillingsleyCalifornia Institute of TechnologyJ. BirchLIGO Livingston ObservatoryI. A. BirneyUniversity of the West of ScotlandO. BirnholtzMax-Planck-Institut für GravitationsphysikS. BiscansMassachusetts Institute of TechnologyA. BishtLeibniz Universität HannoverM. 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. BockMax-Planck-Institut für GravitationsphysikM. BoerArtemis, Université Côte d’AzurG. BogaertArtemis, Université Côte d’AzurC. BoganMax-Planck-Institut für GravitationsphysikA. BoheMax-Planck-Institut für Gravitations-physikC. BondUniversity of BirminghamF. BonduUniversité de Rennes 1R. BonnandUniversité Savoie Mont BlancB. A. BoomScience ParkR. BorkCalifornia Institute of TechnologyV. BoschiINFNS. BoseInter-University Centre for Astronomy and AstrophysicsY. BouffanaisUniversité Paris DiderotA. BozziEuropean Gravitational Observatory (EGO)
2016en
ABI

Аннотация

The first observational run of the Advanced LIGO detectors, from September 12, 2015 to January 19, 2016, saw the first detections of gravitational waves from binary black hole mergers. In this paper, we present full results from a search for binary black hole merger signals with total masses up to <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"><a:mrow><a:mn>100</a:mn><a:msub><a:mrow><a:mi mathvariant="normal">M</a:mi></a:mrow><a:mrow><a:mo stretchy="false">⊙</a:mo></a:mrow></a:msub></a:mrow></a:math> and detailed implications from our observations of these systems. Our search, based on general-relativistic models of gravitational-wave signals from binary black hole systems, unambiguously identified two signals, GW150914 and GW151226, with a significance of greater than <e:math xmlns:e="http://www.w3.org/1998/Math/MathML" display="inline"><e:mn>5</e:mn><e:mi>σ</e:mi></e:math> over the observing period. It also identified a third possible signal, LVT151012, with substantially lower significance and with an 87% probability of being of astrophysical origin. We provide detailed estimates of the parameters of the observed systems. Both GW150914 and GW151226 provide an unprecedented opportunity to study the two-body motion of a compact-object binary in the large velocity, highly nonlinear regime. We do not observe any deviations from general relativity, and we place improved empirical bounds on several high-order post-Newtonian coefficients. From our observations, we infer stellar-mass binary black hole merger rates lying in the range <g:math xmlns:g="http://www.w3.org/1998/Math/MathML" display="inline"><g:mrow><g:mn>9</g:mn><g:mi>–</g:mi><g:mn>240</g:mn><g:mtext> </g:mtext><g:mtext> </g:mtext><g:msup><g:mrow><g:mi>Gpc</g:mi></g:mrow><g:mrow><g:mo>−</g:mo><g:mn>3</g:mn></g:mrow></g:msup><g:mtext> </g:mtext><g:msup><g:mrow><g:mi>yr</g:mi></g:mrow><g:mrow><g:mo>−</g:mo><g:mn>1</g:mn></g:mrow></g:msup></g:mrow></g:math>. These observations are beginning to inform astrophysical predictions of binary black hole formation rates and indicate that future observing runs of the Advanced detector network will yield many more gravitational-wave detections. Published by the American Physical Society 2016

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