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Properties of the Binary Neutron Star Merger GW170817

B. P. AbbottCalifornia Institute of TechnologyR. AbbottCalifornia Institute of TechnologyT. D. AbbottLouisiana State UniversityF. AcerneseComplesso Universitario di Monte S. AngeloK. AckleyMonash UniversityC. AdamsLIGO Livingston ObservatoryT. AdamsUniv. Grenoble AlpesP. AddessoUniversity of Sannio at BeneventoR. X. AdhikariCalifornia Institute of TechnologyV. B. AdyaLeibniz Universität HannoverC. AffeldtLeibniz Universität HannoverB. AgarwalUniversity of Illinois at Urbana-ChampaignM. AgathosUniversity of CambridgeK. AgatsumaNikhefN. AggarwalMassachusetts Institute of TechnologyO. D. AguiarInstituto Nacional de Pesquisas EspaciaisL. AielloGran Sasso Science Institute (GSSI)A. AinInter-University Centre for Astronomy and AstrophysicsP. AjithTata Institute of Fundamental ResearchB. AllenLeibniz Universität HannoverA. 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. AntierUniversité Paris-SaclayS. AppertCalifornia Institute of TechnologyK. AraiCalifornia Institute of TechnologyM. C. ArayaCalifornia Institute of TechnologyJ. S. AreedaCalifornia State University FullertonM. ArèneUniversité Paris DiderotN. ArnaudEuropean Gravitational Observatory (EGO)K. G. ArunChennai Mathematical InstituteS. AscenziINFNG. AshtonMonash UniversityM. AstUniversität HamburgS. M. AstonLIGO Livingston ObservatoryP. AstoneINFND. V. AtallahCardiff UniversityF. AubinUniv. Grenoble AlpesP. AufmuthLeibniz Universität HannoverC. AulbertMax Planck Institute for Gravitational Physics (Albert Einstein Institute)K. AultONealEmbry-Riddle Aeronautical UniversityC. AustinLouisiana State UniversityA. Avila-AlvarezCalifornia State University FullertonS. BabakMax Planck Institute for Gravitational Physics (Albert Einstein Institute)P. BaconUniversité Paris DiderotF. BadaraccoGran Sasso Science Institute (GSSI)M. K. M. BaderNikhefS. BaeKorea Institute of Science and Technology InformationP. T. BakerWest Virginia UniversityF. BaldacciniINFNG. BallardinEuropean Gravitational Observatory (EGO)S. BallmerSyracuse UniversityS. BanagiriUniversity of MinnesotaJ. C. BarayogaCalifornia Institute of TechnologyS. E. BarclayUniversity of GlasgowB. C. BarishCalifornia Institute of TechnologyD. BarkerK. BarkettCaltech CaRTS. 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. BastiINFNJ. C. BatchM. BawajINFNJ. C. BayleyUniversity of GlasgowM. BazzanINFNB. BécsyEötvös UniversityC. BeerMax Planck Institute for Gravitational Physics (Albert Einstein Institute)M. BejgerPolish Academy of SciencesI. BelahceneUniversité Paris-SaclayA. S. BellUniversity of GlasgowD. BeniwalUniversity of AdelaideM. BenschLeibniz Universität HannoverB. K. BergerCalifornia Institute of TechnologyG. BergmannLeibniz Universität HannoverSebastiano BernuzziINFNJ. J. BeroRochester Institute of TechnologyC. P. L. BerryUniversity of BirminghamD. BersanettiINFNA. BertoliniNikhefJ. BetzwieserLIGO Livingston ObservatoryR. BhandareRRCATI. A. BilenkoLomonosov Moscow State UniversityS. A. BilgiliWest Virginia UniversityG. BillingsleyCalifornia Institute of TechnologyC. R. BillmanUniversity of FloridaJ. BirchLIGO Livingston ObservatoryR. BirneyUniversity of Strathclyde
2019en
ABI

Аннотация

On August 17, 2017, the Advanced LIGO and Advanced Virgo gravitational-wave detectors observed a low-mass compact binary inspiral. The initial sky localization of the source of the gravitational-wave signal, GW170817, allowed electromagnetic observatories to identify NGC 4993 as the host galaxy. In this work, we improve initial estimates of the binary’s properties, including component masses, spins, and tidal parameters, using the known source location, improved modeling, and recalibrated Virgo data. We extend the range of gravitational-wave frequencies considered down to 23 Hz, compared to 30 Hz in the initial analysis. We also compare results inferred using several signal models, which are more accurate and incorporate additional physical effects as compared to the initial analysis. We improve the localization of the gravitational-wave source to a 90% credible region of <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"><a:mrow><a:mn>16</a:mn><a:mtext> </a:mtext><a:mtext> </a:mtext><a:msup><a:mrow><a:mi>deg</a:mi></a:mrow><a:mrow><a:mn>2</a:mn></a:mrow></a:msup></a:mrow></a:math>. We find tighter constraints on the masses, spins, and tidal parameters, and continue to find no evidence for nonzero component spins. The component masses are inferred to lie between 1.00 and <c:math xmlns:c="http://www.w3.org/1998/Math/MathML" display="inline"><c:mrow><c:mn>1.89</c:mn><c:mtext> </c:mtext><c:mtext> </c:mtext><c:msub><c:mrow><c:mi mathvariant="normal">M</c:mi></c:mrow><c:mrow><c:mo stretchy="false">⊙</c:mo></c:mrow></c:msub></c:mrow></c:math> when allowing for large component spins, and to lie between 1.16 and <g:math xmlns:g="http://www.w3.org/1998/Math/MathML" display="inline"><g:mrow><g:mn>1.60</g:mn><g:mtext> </g:mtext><g:mtext> </g:mtext><g:msub><g:mrow><g:mi mathvariant="normal">M</g:mi></g:mrow><g:mrow><g:mo stretchy="false">⊙</g:mo></g:mrow></g:msub></g:mrow></g:math> (with a total mass <k:math xmlns:k="http://www.w3.org/1998/Math/MathML" display="inline"><k:mrow><k:msubsup><k:mrow><k:mn>2.73</k:mn></k:mrow><k:mrow><k:mo>−</k:mo><k:mn>0.01</k:mn></k:mrow><k:mrow><k:mo>+</k:mo><k:mn>0.04</k:mn></k:mrow></k:msubsup><k:mtext> </k:mtext><k:mtext> </k:mtext><k:msub><k:mrow><k:mi mathvariant="normal">M</k:mi></k:mrow><k:mrow><k:mo stretchy="false">⊙</k:mo></k:mrow></k:msub></k:mrow></k:math>) when the spins are restricted to be within the range observed in Galactic binary neutron stars. Using a precessing model and allowing for large component spins, we constrain the dimensionless spins of the components to be less than 0.50 for the primary and 0.61 for the secondary. Under minimal assumptions about the nature of the compact objects, our constraints for the tidal deformability parameter <o:math xmlns:o="http://www.w3.org/1998/Math/MathML" display="inline"><o:mover accent="true"><o:mi mathvariant="normal">Λ</o:mi><o:mo accent="true" stretchy="false">˜</o:mo></o:mover></o:math> are (0,630) when we allow for large component spins, and <u:math xmlns:u="http://www.w3.org/1998/Math/MathML" display="inline"><u:mrow><u:msubsup><u:mrow><u:mn>300</u:mn></u:mrow><u:mrow><u:mo>−</u:mo><u:mn>230</u:mn></u:mrow><u:mrow><u:mo>+</u:mo><u:mn>420</u:mn></u:mrow></u:msubsup></u:mrow></u:math> (using a 90% highest posterior density interval) when restricting the magnitude of the component spins, ruling out several equation-of-state models at the 90% credible level. Finally, with LIGO and GEO600 data, we use a Bayesian analysis to place upper limits on the amplitude and spectral energy density of a possible postmerger signal. Published by the American Physical Society 2019

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