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dc.contributor.authorAbbott, Ren_US
dc.contributor.authorAbe, Hen_US
dc.contributor.authorAcernese, Fen_US
dc.contributor.authorAckley, Ken_US
dc.contributor.authorAdhikari, Nen_US
dc.contributor.authorAdhikari, RXen_US
dc.contributor.authorAdkins, VKen_US
dc.contributor.authorAdya, VBen_US
dc.contributor.authorAffeldt, Cen_US
dc.contributor.authorAgarwal, Den_US
dc.contributor.authorAgathos, Men_US
dc.contributor.authorAgatsuma, Ken_US
dc.contributor.authorAggarwal, Nen_US
dc.contributor.authorAguiar, ODen_US
dc.contributor.authorAiello, Len_US
dc.contributor.authorAin, Aen_US
dc.contributor.authorAjith, Pen_US
dc.contributor.authorAkutsu, Ten_US
dc.contributor.authorAlbanesi, Sen_US
dc.contributor.authorAlfaidi, RAen_US
dc.contributor.authorAllocca, Aen_US
dc.contributor.authorAltin, PAen_US
dc.contributor.authorAmato, Aen_US
dc.contributor.authorAnand, Cen_US
dc.contributor.authorAnand, Sen_US
dc.contributor.authorAnanyeva, Aen_US
dc.contributor.authorAnderson, SBen_US
dc.contributor.authorAnderson, WGen_US
dc.contributor.authorAndo, Men_US
dc.contributor.authorAndrade, Ten_US
dc.contributor.authorAndres, Nen_US
dc.contributor.authorAndres-Carcasona, Men_US
dc.contributor.authorAndric, Ten_US
dc.contributor.authorAngelova, SVen_US
dc.contributor.authorAnsoldi, Sen_US
dc.contributor.authorAntelis, JMen_US
dc.contributor.authorAntier, Sen_US
dc.contributor.authorApostolatos, Ten_US
dc.contributor.authorAppavuravther, EZen_US
dc.contributor.authorAppert, Sen_US
dc.contributor.authorApple, SKen_US
dc.contributor.authorArai, Ken_US
dc.contributor.authorAraya, Aen_US
dc.contributor.authorAraya, MCen_US
dc.contributor.authorAreeda, JSen_US
dc.contributor.authorArene, Men_US
dc.contributor.authorAritomi, Nen_US
dc.contributor.authorArnaud, Nen_US
dc.contributor.authorArogeti, Men_US
dc.contributor.authorAronson, SMen_US
dc.contributor.authorArun, KGen_US
dc.contributor.authorAsada, Hen_US
dc.contributor.authorAsali, Yen_US
dc.contributor.authorAshton, Gen_US
dc.contributor.authorAso, Yen_US
dc.contributor.authorAssiduo, Men_US
dc.contributor.authorDe Souza Melo, SAen_US
dc.contributor.authorAston, SMen_US
dc.contributor.authorAstone, Pen_US
dc.contributor.authorAubin, Fen_US
dc.contributor.authorAultONeal, Ken_US
dc.contributor.authorAustin, Cen_US
dc.contributor.authorBabak, Sen_US
dc.contributor.authorBadaracco, Fen_US
dc.contributor.authorBader, MKMen_US
dc.contributor.authorBadger, Cen_US
dc.contributor.authorBae, Sen_US
dc.contributor.authorBae, Yen_US
dc.contributor.authorBaer, AMen_US
dc.contributor.authorBagnasco, Sen_US
dc.contributor.authorBai, Yen_US
dc.contributor.authorBaird, Jen_US
dc.contributor.authorBajpai, Ren_US
dc.contributor.authorBaka, Ten_US
dc.contributor.authorBall, Men_US
dc.contributor.authorBallardin, Gen_US
dc.contributor.authorBallmer, SWen_US
dc.contributor.authorBalsamo, Aen_US
dc.contributor.authorBaltus, Gen_US
dc.contributor.authorBanagiri, Sen_US
dc.contributor.authorBanerjee, Ben_US
dc.contributor.authorBankar, Den_US
dc.contributor.authorBarayoga, JCen_US
dc.contributor.authorBarbieri, Cen_US
dc.contributor.authorBarbieri, Ren_US
dc.contributor.authorBarish, BCen_US
dc.contributor.authorBarker, Den_US
dc.contributor.authorBarneo, Pen_US
dc.contributor.authorBarone, Fen_US
dc.contributor.authorBarr, Ben_US
dc.contributor.authorBarsotti, Len_US
dc.contributor.authorBarsuglia, Men_US
dc.contributor.authorBarta, Den_US
dc.contributor.authorBartlett, Jen_US
dc.contributor.authorBarton, MAen_US
dc.contributor.authorBartos, Ien_US
dc.contributor.authorBasak, Sen_US
dc.contributor.authorBassiri, Ren_US
dc.contributor.authorBasti, Aen_US
dc.contributor.authorBawaj, Men_US
dc.date.accessioned2024-03-04T09:34:45Z
dc.date.issued2023-06-01en_US
dc.identifier.issn0004-637Xen_US
dc.identifier.urihttps://qmro.qmul.ac.uk/xmlui/handle/123456789/95048
dc.description.abstractWe use 47 gravitational wave sources from the Third LIGO-Virgo-Kamioka Gravitational Wave Detector Gravitational Wave Transient Catalog (GWTC-3) to estimate the Hubble parameter H(z), including its current value, the Hubble constant H0. Each gravitational wave (GW) signal provides the luminosity distance to the source, and we estimate the corresponding redshift using two methods: the redshifted masses and a galaxy catalog. Using the binary black hole (BBH) redshifted masses, we simultaneously infer the source mass distribution and H(z). The source mass distribution displays a peak around 34Me, followed by a drop-off. Assuming this mass scale does not evolve with the redshift results in a H(z) measurement, yielding H0 = 68+12-8 km s-1 Mpc-1 (68% credible interval) when combined with the H0 measurement from GW170817 and its electromagnetic counterpart. This represents an improvement of 17% with respect to the H0 estimate from GWTC-1. The second method associates each GW event with its probable host galaxy in the catalog GLADE+, statistically marginalizing over the redshifts of each event's potential hosts. Assuming a fixed BBH population, we estimate a value of H0 = 68+8-6 km s-1 Mpc-1 with the galaxy catalog method, an improvement of 42% with respect to our GWTC-1 result and 20% with respect to recent H0 studies using GWTC-2 events. However, we show that this result is strongly impacted by assumptions about the BBH source mass distribution; the only event which is not strongly impacted by such assumptions (and is thus informative about H0) is the well-localized event GW190814.en_US
dc.relation.ispartofAstrophysical Journalen_US
dc.rightsOriginal content from this work may be used under the terms of the Creative Commons Attribution 4.0 licence. Any further distribution of this work must maintain attribution to the author(s) and the title of the work, journal citation and DOI.
dc.titleConstraints on the Cosmic Expansion History from GWTC-3en_US
dc.typeArticle
dc.identifier.doi10.3847/1538-4357/ac74bben_US
pubs.issue2en_US
pubs.notesNot knownen_US
pubs.publication-statusPublisheden_US
pubs.volume949en_US
rioxxterms.funderDefault funderen_US
rioxxterms.identifier.projectDefault projecten_US


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