Please use this identifier to cite or link to this item: http://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/6709
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dc.contributor.authorLIGO Scientific Collaborationen_US
dc.contributor.authorVirgo Collaborationen_US
dc.contributor.authorKAGRA Collaborationen_US
dc.contributor.authorAbbott, R.en_US
dc.contributor.authorRAPOL, UMAKANT D.en_US
dc.contributor.authorSOURADEEP, TARUN et al.en_US
dc.date.accessioned2022-04-04T08:56:30Z-
dc.date.available2022-04-04T08:56:30Z-
dc.date.issued2021-05en_US
dc.identifier.citationAstrophysical Journal Letters, 913(1).en_US
dc.identifier.issn2041-8213en_US
dc.identifier.urihttps://doi.org/10.3847/2041-8213/abe949en_US
dc.identifier.urihttp://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/6709-
dc.description.abstractWe report on the population of 47 compact binary mergers detected with a false-alarm rate of <$1\,{\mathrm{yr}}^{-1}$ in the second LIGO–Virgo Gravitational-Wave Transient Catalog. We observe several characteristics of the merging binary black hole (BBH) population not discernible until now. First, the primary mass spectrum contains structure beyond a power law with a sharp high-mass cutoff; it is more consistent with a broken power law with a break at ${39.7}_{-9.1}^{+20.3}\,\,{M}_{\odot }$ or a power law with a Gaussian feature peaking at ${33.1}_{-5.6}^{+4.0}\,\,{M}_{\odot }$ (90% credible interval). While the primary mass distribution must extend to $\sim 65\,{M}_{\odot }$ or beyond, only ${2.9}_{-1.7}^{+3.5} \% $ of systems have primary masses greater than $45\,{M}_{\odot }$. Second, we find that a fraction of BBH systems have component spins misaligned with the orbital angular momentum, giving rise to precession of the orbital plane. Moreover, $12$%–$44$% of BBH systems have spins tilted by more than 90°, giving rise to a negative effective inspiral spin parameter, ${\chi }_{\mathrm{eff}}$. Under the assumption that such systems can only be formed by dynamical interactions, we infer that between 25% and 93% of BBHs with nonvanishing $| {\chi }_{\mathrm{eff}}| \gt 0.01$ are dynamically assembled. Third, we estimate merger rates, finding ${{ \mathcal R }}_{\mathrm{BBH}}={23.9}_{-8.6}^{+14.3}\,\,{\mathrm{Gpc}}^{-3}\,{\mathrm{yr}}^{-1}$ for BBHs and ${{ \mathcal R }}_{\mathrm{BNS}}={320}_{-240}^{+490}\,\,{\mathrm{Gpc}}^{-3}\,{\mathrm{yr}}^{-1}$ for binary neutron stars. We find that the BBH rate likely increases with redshift ($85 \% $ credibility) but not faster than the star formation rate ($86 \% $ credibility). Additionally, we examine recent exceptional events in the context of our population models, finding that the asymmetric masses of GW190412 and the high component masses of GW190521 are consistent with our models, but the low secondary mass of GW190814 makes it an outlier.en_US
dc.language.isoenen_US
dc.publisherIOP Publishingen_US
dc.subjectGravitational wavesen_US
dc.subjectAstrophysical black holesen_US
dc.subjectStellar mass black holesen_US
dc.subjectMassive starsen_US
dc.subjectCompact objectsen_US
dc.subjectBayesian statisticsen_US
dc.subject2021en_US
dc.titlePopulation Properties of Compact Objects from the Second LIGO–Virgo Gravitational-Wave Transient Catalogen_US
dc.typeArticleen_US
dc.contributor.departmentDept. of Physicsen_US
dc.identifier.sourcetitleAstrophysical Journal Lettersen_US
dc.publication.originofpublisherForeignen_US
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