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dc.contributorUniversitat Ramon Llull. La Salle
dc.contributorCERN
dc.contributor.authorBadalov, Alexey
dc.contributor.authorCalvo Gómez, Míriam
dc.contributor.authorVilasís Cardona, Xavier
dc.contributor.authorLHCb Collaboration - CERN
dc.date.accessioned2020-11-19T12:18:34Z
dc.date.accessioned2023-10-02T06:27:58Z
dc.date.available2020-11-19T12:18:34Z
dc.date.available2023-10-02T06:27:58Z
dc.date.created2014
dc.date.issued2014-10-09
dc.identifier.urihttp://hdl.handle.net/20.500.14342/3193
dc.description.abstractFirst observations of the rare decays B + → K + π + π − μ + μ − and B +→ ϕK +μ+μ− are presented using data corresponding to an integrated luminosity of 3.0 fb−1, collected by the LHCb experiment at centre-of-mass energies of 7 and 8 TeV. The branching fractions of the decays are B(B+→K+π+π−μ+μ−)=(4.36−0.29−0.27(stat)±0.21 (syst)±0.18(norm))×10−7,B(B+→ϕK+μ+μ−)=(0.82−0.19−0.17(stat)−0.10−0.04(syst)±0.27(norm))×10−7, where the uncertainties are statistical, systematic, and due to the uncertainty on the branching fractions of the normalisation modes. A measurement of the differential branching fraction in bins of the invariant mass squared of the dimuon system is also presented for the decay B + → K + π + π − μ + μ −.eng
dc.format.extent18 p.ca
dc.language.isoengca
dc.publisherSpringerca
dc.relation.ispartofJournal of High Energy Physics, 2014, Vol. 2014, No.10 (Octubre)ca
dc.rightsAttribution 4.0 International
dc.rights© CERN
dc.rights.urihttp://creativecommons.org/licenses/by/4.0/
dc.sourceRECERCAT (Dipòsit de la Recerca de Catalunya)
dc.subject.otherGran col·lisionador d'hadrons (França i Suïssa)ca
dc.subject.otherPartícules (Física nuclear)ca
dc.titleFirst observations of the rare decays B + → K + π + π − μ + μ − and B +→ ϕK + μ + μ −ca
dc.typeinfo:eu-repo/semantics/articleca
dc.typeinfo:eu-repo/semantics/publishedVersionca
dc.rights.accessLevelinfo:eu-repo/semantics/openAccess
dc.embargo.termscapca
dc.subject.udc539
dc.identifier.doihttps://doi.org/10.1007/JHEP10(2014)064ca


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Attribution 4.0 International
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