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dc.contributorUniversitat Ramon Llull. La Salle
dc.contributorCERN
dc.contributor.authorBadalov, Alexey
dc.contributor.authorCalvo Gómez, Míriam
dc.contributor.authorCamboni, Alessandro
dc.contributor.authorVilasís Cardona, Xavier
dc.contributor.authorLHCb Collaboration - CERN
dc.date.accessioned2021-05-07T06:52:38Z
dc.date.accessioned2023-10-02T06:46:44Z
dc.date.available2021-05-07T06:52:38Z
dc.date.available2023-10-02T06:46:44Z
dc.date.created2014-04
dc.date.issued2014-09
dc.identifier.urihttp://hdl.handle.net/20.500.14342/3468
dc.description.abstractEvidence for the decay mode X(3872) →ψ(2S)γ in B+→X(3872)K+decays is found with a sig-nificance of 4.4 standard deviations. The analysis is based on a data sample of proton–proton collisions, corresponding to an integrated luminosity of 3 fb−1, collected with the LHCb detector, at centre-of-mass energies of 7and 8 TeV. The ratio of the branching fraction of the X(3872) →ψ(2S)γ decay to that of the X(3872) →J/ψγdecay is measured to be B(X(3872)→ψ(2S)γ)B(X(3872)→J/ψγ)=2.46±0.64±0.29, where the first uncertainty is statistical and the second is systematic. The measured value does not support a pure D ̄D∗molecular interpretation of the X(3872) state.eng
dc.format.extent16 p.cat
dc.language.isoengcat
dc.publisherElseviercat
dc.relation.ispartofNuclear Physics B, 2014, Vol. 886cat
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)cat
dc.subject.otherInteraccions d'hadronscat
dc.subject.otherCol·lisions (Física nuclear)cat
dc.subject.otherPartícules (Física nuclear)cat
dc.subject.otherProtonscat
dc.titleEvidence for the decay X(3872) →ψ(2S)γcat
dc.typeinfo:eu-repo/semantics/articlecat
dc.typeinfo:eu-repo/semantics/publishedVersioncat
dc.rights.accessLevelinfo:eu-repo/semantics/openAccess
dc.embargo.termscapcat
dc.subject.udc539
dc.identifier.doihttps://doi.org/10.1016/j.nuclphysb.2014.06.011cat


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