Directly comparing GW150914 with numerical solutions of Einstein's equations for binary black hole coalescence

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dc.identifier.uri Abbott, B.P. Allen, Bruce Aufmuth, Peter Bisht, A. Danzmann, Karsten Denker, T. Heurs, M. Kaufer, S. Krueger, C. Lough, J.D. Lück, Harald Sawadsky, A. Schütte, D. Steinmeyer, D. Vahlbruch, H. Willke, Benno Wimmer, M.H. Wittel, H. et al. LIGO Scientific Collaboration Virgo Collaboration 2017-10-26T07:04:20Z 2017-10-26T07:04:20Z 2016
dc.identifier.citation Abbott, B.P.; Abbott, R.; Abbott, T.D.; Abernathy, M.R.; Acernese, F. et al.: Directly comparing GW150914 with numerical solutions of Einstein's equations for binary black hole coalescence. In: Physical Review D 94 (2016), Nr. 6, No. 64035. DOI:
dc.description.abstract We compare GW150914 directly to simulations of coalescing binary black holes in full general relativity, including several performed specifically to reproduce this event. Our calculations go beyond existing semianalytic models, because for all simulations—including sources with two independent, precessing spins—we perform comparisons which account for all the spin-weighted quadrupolar modes, and separately which account for all the quadrupolar and octopolar modes. Consistent with the posterior distributions reported by Abbott et al. [Phys. Rev. Lett. 116, 241102 (2016)] (at the 90% credible level), we find the data are compatible with a wide range of nonprecessing and precessing simulations. Follow-up simulations performed using previously estimated binary parameters most resemble the data, even when all quadrupolar and octopolar modes are included. Comparisons including only the quadrupolar modes constrain the total redshifted mass Mz∈[64  M⊙−82  M⊙], mass ratio 1/q=m2/m1∈[0.6,1], and effective aligned spin χeff∈[−0.3,0.2], where χeff=(S1/m1+S2/m2)·L^/M. Including both quadrupolar and octopolar modes, we find the mass ratio is even more tightly constrained. Even accounting for precession, simulations with extreme mass ratios and effective spins are highly inconsistent with the data, at any mass. Several nonprecessing and precessing simulations with similar mass ratio and χeff are consistent with the data. Though correlated, the components’ spins (both in magnitude and directions) are not significantly constrained by the data: the data is consistent with simulations with component spin magnitudes a1,2 up to at least 0.8, with random orientations. Further detailed follow-up calculations are needed to determine if the data contain a weak imprint from transverse (precessing) spins. For nonprecessing binaries, interpolating between simulations, we reconstruct a posterior distribution consistent with previous results. The final black hole’s redshifted mass is consistent with Mf,z in the range 64.0  M⊙−73.5  M⊙ and the final black hole’s dimensionless spin parameter is consistent with af=0.62–0.73. As our approach invokes no intermediate approximations to general relativity and can strongly reject binaries whose radiation is inconsistent with the data, our analysis provides a valuable complement to Abbott et al. [Phys. Rev. Lett. 116, 241102 (2016)]. © 2016 The American Physical Society eng
dc.language.iso eng
dc.publisher College Park, MD : American Physical Society
dc.relation.ispartofseries Physical Review D 94 (2016), Nr. 6
dc.rights Es gilt deutsches Urheberrecht. Das Dokument darf zum eigenen Gebrauch kostenfrei genutzt, aber nicht im Internet bereitgestellt oder an Außenstehende weitergegeben werden.
dc.subject Gravitational waves eng
dc.subject Black Holes eng
dc.subject Gravitationswelle ger
dc.subject.ddc 530 | Physik ger
dc.title Directly comparing GW150914 with numerical solutions of Einstein's equations for binary black hole coalescence
dc.type article
dc.type Text
dc.relation.issn 2470-0010
dc.bibliographicCitation.issue 6
dc.bibliographicCitation.volume 94
dc.bibliographicCitation.firstPage 64035
dc.description.version publishedVersion
tib.accessRights frei zug�nglich

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