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dc.contributor.author천병구-
dc.date.accessioned2016-09-02T02:12:52Z-
dc.date.available2016-09-02T02:12:52Z-
dc.date.issued2015-03-
dc.identifier.citationPHYSICAL REVIEW D, v. 91, NO 5, Page. 51101-51101en_US
dc.identifier.issn1550-7998-
dc.identifier.issn1550-2368-
dc.identifier.urihttp://journals.aps.org/prd/abstract/10.1103/PhysRevD.91.051101-
dc.identifier.urihttp://hdl.handle.net/20.500.11754/22969-
dc.description.abstractWe report the first observation of B-0 -˃ X(3872)(K+pi(-)) and evidence for B+ -˃ X(3872)(K-0 pi(+)). We measure the product of branching fractions for the former to be B(B-0 -˃ X(3872)(K+pi(-)) x B(X(3872) -˃ J/psi pi(+)pi(-)) = (7.9 +/- 1.3(stat) +/- 0.4(syst) x 10(-6) and find that B-0 -˃ X(3872)K*(892)(0) does not dominate the B-0 -˃ X(3872)K+pi(-) decay mode. We also measure B(B+ -˃ X(3872)(K-0 pi(+))) x B(X(3872) -˃ J/psi pi(+)pi(-)) = (10.6 +/- 3.0(stat) +/- 0.9(syst) x 10(-6). This study is based on the full data sample of 711 fb(-1) (772 x 10(6)B (B) over bar pairs) collected at the Upsilon(4S) resonance with the Belle detector at the KEKB collider.en_US
dc.language.isoenen_US
dc.publisherAMER PHYSICAL SOCen_US
dc.subjectPHOTOS MONTE-CARLOen_US
dc.titleObservation of X(3872) in B -˃ X(3872)K pi decaysen_US
dc.typeArticleen_US
dc.relation.no5-
dc.relation.volume91-
dc.identifier.doi10.1103/PhysRevD.91.051101-
dc.relation.page51101-51101-
dc.relation.journalPHYSICAL REVIEW D-
dc.contributor.googleauthorBala, A.-
dc.contributor.googleauthorBhardwaj, V.-
dc.contributor.googleauthorTrabelsi, K.-
dc.contributor.googleauthorSingh, J. B-
dc.contributor.googleauthorAbdesselam, A.-
dc.contributor.googleauthorAdachi, I.-
dc.contributor.googleauthorAihara, H.-
dc.contributor.googleauthorArinstein, K.-
dc.contributor.googleauthorAsner, D. M.-
dc.contributor.googleauthorCheon, B. G.-
dc.relation.code2015002842-
dc.sector.campusS-
dc.sector.daehakCOLLEGE OF NATURAL SCIENCES[S]-
dc.sector.departmentDEPARTMENT OF PHYSICS-
dc.identifier.pidbgcheon-


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