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dc.contributor.authorAbedi, Jahed
dc.contributor.authorCapano, Collin D.
dc.contributor.authorKastha, Shilpa
dc.contributor.authorNitz, Alexander H.
dc.contributor.authorWang, Yi-Fan
dc.contributor.authorWesterweck, Julian
dc.contributor.authorNielsen, Alex Bentley
dc.contributor.authorKrishnan, Badri
dc.date.accessioned2024-03-14T09:46:24Z
dc.date.available2024-03-14T09:46:24Z
dc.date.created2023-12-01T14:05:24Z
dc.date.issued2023
dc.identifier.citationAbedi, J., Capano, C. D., Kastha, S., Nitz, A. H., Wang, Y. F., Westerweck, J., ... & Krishnan, B. (2023). Spectroscopy for asymmetric binary black hole mergers. Physical Review D, 108(10), 104009.en_US
dc.identifier.issn2470-0010
dc.identifier.urihttps://hdl.handle.net/11250/3122340
dc.description.abstractBlack hole spectroscopy is the proposal to observe multiple quasinormal modes in the ringdown of a binary black hole merger. In addition to the fundamental quadrupolar mode, overtones and higher harmonics may be present and detectable in the gravitational wave signal, allowing for tests of the no-hair theorem. We analyze in detail the strengths and weaknesses of the standard Rayleigh criterion supplied with a Fisher matrix error estimation, and we find that the criterion is useful, but too restrictive. Therefore, we motivate the use of a conservative high Bayes factor threshold to obtain the black hole spectroscopy horizons of current and future detectors; i.e., the distance (averaged in sky location and binary inclination) up to which one or more additional modes can be detected and confidently distinguished from each other. We set up all of our searches for additional modes starting at t = 10(M-1 + M-2) after the peak amplitude in simulated signals of circular nonspinning binaries. An agnostic multimode analysis allows us to rank the subdominant modes: for nearly equal mass binaries, we find (l, m, n) = (2, 2, 1) and (3,3,0) and, for very asymmetric binaries, (3,3,0) and (4,4,0), for the secondary and tertiary modes, respectively. At the current estimated rates for heavy stellar mass binary black hole mergers, with primary masses between 45 and 100 solar masses, we expect an event rate of mergers within our conservative estimate for the (2,2,1) spectroscopy horizon of 0.03-0.10 yr(-1) for LIGO at design sensitivity and (0.6 - 2.4) x 10(3 )yr(-1) for the future third generation ground-based detector Cosmic Explorer.en_US
dc.language.isoengen_US
dc.publisherAmerican Physical Societyen_US
dc.rightsNavngivelse 4.0 Internasjonal*
dc.rights.urihttp://creativecommons.org/licenses/by/4.0/deed.no*
dc.titleSpectroscopy for asymmetric binary black hole mergersen_US
dc.typePeer revieweden_US
dc.typeJournal articleen_US
dc.description.versionpublishedVersionen_US
dc.rights.holderThe authorsen_US
dc.subject.nsiVDP::Matematikk og Naturvitenskap: 400::Fysikk: 430::Astrofysikk, astronomi: 438en_US
dc.source.pagenumber12en_US
dc.source.volume108en_US
dc.source.journalPhysical Review Den_US
dc.source.issue10en_US
dc.identifier.doi10.1103/PhysRevD.108.104009
dc.identifier.cristin2207460
cristin.ispublishedtrue
cristin.fulltextoriginal
cristin.qualitycode1


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