Please use this identifier to cite or link to this item: http://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/6090
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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.accessioned2021-07-23T11:33:15Z
dc.date.available2021-07-23T11:33:15Z
dc.date.issued2021-07en_US
dc.identifier.citationAstrophysical Journal Letters, 915(1), L5.en_US
dc.identifier.issn2348-1269en_US
dc.identifier.issn2349-5138en_US
dc.identifier.urihttp://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/6090
dc.identifier.urihttps://doi.org/10.3847/2041-8213/ac082een_US
dc.description.abstractWe report the observation of gravitational waves from two compact binary coalescences in LIGO's and Virgo's third observing run with properties consistent with neutron star–black hole (NSBH) binaries. The two events are named GW200105_162426 and GW200115_042309, abbreviated as GW200105 and GW200115; the first was observed by LIGO Livingston and Virgo and the second by all three LIGO–Virgo detectors. The source of GW200105 has component masses $8.{9}_{-1.5}^{+1.2}$ and $1.{9}_{-0.2}^{+0.3}\,{M}_{\odot }$, whereas the source of GW200115 has component masses $5.{7}_{-2.1}^{+1.8}$ and $1.{5}_{-0.3}^{+0.7}\,{M}_{\odot }$ (all measurements quoted at the 90% credible level). The probability that the secondary's mass is below the maximal mass of a neutron star is 89%–96% and 87%–98%, respectively, for GW200105 and GW200115, with the ranges arising from different astrophysical assumptions. The source luminosity distances are ${280}_{-110}^{+110}$ and ${300}_{-100}^{+150}\,\mathrm{Mpc}$, respectively. The magnitude of the primary spin of GW200105 is less than 0.23 at the 90% credible level, and its orientation is unconstrained. For GW200115, the primary spin has a negative spin projection onto the orbital angular momentum at 88% probability. We are unable to constrain the spin or tidal deformation of the secondary component for either event. We infer an NSBH merger rate density of ${45}_{-33}^{+75}\,{\mathrm{Gpc}}^{-3}\,{\mathrm{yr}}^{-1}$ when assuming that GW200105 and GW200115 are representative of the NSBH population or ${130}_{-69}^{+112}\,{\mathrm{Gpc}}^{-3}\,{\mathrm{yr}}^{-1}$ under the assumption of a broader distribution of component masses.en_US
dc.language.isoenen_US
dc.publisherIOP Publishingen_US
dc.subjectPhysicsen_US
dc.subject2021-JUL-WEEK2en_US
dc.subjectTOC-JUL-2021en_US
dc.subject2021en_US
dc.titleObservation of Gravitational Waves from Two Neutron Star–Black Hole Coalescencesen_US
dc.typeArticleen_US
dc.contributor.departmentDept. of Physicsen_US
dc.identifier.sourcetitleAstrophysical Journal Lettersen_US
dc.publication.originofpublisherForeignen_US
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