Please use this identifier to cite or link to this item: http://hdl.handle.net/2445/186430
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dc.contributor.authorGarrido Beltrán, Lluís-
dc.contributor.authorGascon, D.-
dc.contributor.authorGraciani Díaz, Ricardo-
dc.contributor.authorGraugés Pous, Eugeni-
dc.contributor.authorMarin Benito, Carla-
dc.contributor.authorPicatoste Olloqui, E.-
dc.contributor.authorRives Molina, V.-
dc.contributor.authorLHCb Collaboration-
dc.date.accessioned2022-06-07T17:56:30Z-
dc.date.available2022-06-07T17:56:30Z-
dc.date.issued2017-06-
dc.identifier.issn0370-2693-
dc.identifier.urihttp://hdl.handle.net/2445/186430-
dc.description.abstractThe first observation of the decay ηc (2 S) → p p bar is reported using proton-proton collision data corresponding to an integrated luminosity of 3.0 fb-1 recorded by the LHCb experiment at centre-of-mass energies of 7 and 8 TeV. The ηc (2 S) resonance is produced in the decay B+ → [ c c bar ]K+. The product of branching fractions normalised to that for the J / ψ intermediate state, R ηc (2 S), is measured to be R-eta c,(2s) equivalent to B(B+-> eta c (2S)K+) x B(eta c(2s)(2S) -> p<<(p)over bar> )/B(B+ -> J/psi k(+)) x B(J/psi -> p<<(p)over bar> ) = (1.58 +/- 0.33 +/- 0.09) x 10(-2), where the first uncertainty is statistical and the second systematic. No signals for the decays B+ -> X(3872)(-> p (p) over bar )K+ and B+ psi(3770)(-> p (p) over bar )K+ are seen, and the 95% confidence level upper limits on their relative branching ratios are found to be R-x(3872) < 0.25 x 10(-2) and R-psi(3770) < 0.10. In addition, the mass differences between the nc(1S) and the J/psi states, between the eta(c)(2S) and the eta(c)(2S) states, and the natural width of the psi(1S) are measured as M-J/psi - M-eta c(7s)= 110.2 +/- 0.5 +/- 0.9 MeV, M psi(2S) - M-eta c (2S) = 52.5 +/- 1.7 +/- 0.6 MeV, Gamma(eta c) (1s) = 34.0 +/- 1.9 +/- 1.3 MeV.-
dc.format.extent9 p.-
dc.format.mimetypeapplication/pdf-
dc.language.isoeng-
dc.publisherElsevier B.V.-
dc.relation.isformatofReproducció del document publicat a: https://doi.org/10.1016/j.physletb.2017.03.046-
dc.relation.ispartofPhysics Letters B, 2017, vol. 769, p. 305-313-
dc.relation.urihttps://doi.org/10.1016/j.physletb.2017.03.046-
dc.rightscc-by (c) Garrido Beltrán, Lluis et al., 2017-
dc.rights.urihttps://creativecommons.org/licenses/by/4.0/-
dc.sourceArticles publicats en revistes (Física Quàntica i Astrofísica)-
dc.subject.classificationHadrons-
dc.subject.classificationGran Col·lisionador d'Hadrons-
dc.subject.classificationFísica de partícules-
dc.subject.classificationExperiments-
dc.subject.otherHadrons-
dc.subject.otherLarge Hadron Collider (France and Switzerland)-
dc.subject.otherParticle physics-
dc.subject.otherExperiments-
dc.titleObservation of ηc (2 S) → p p bar and search for X (3872) → p p bar decays-
dc.typeinfo:eu-repo/semantics/article-
dc.typeinfo:eu-repo/semantics/publishedVersion-
dc.identifier.idgrec678002-
dc.date.updated2022-06-07T17:56:30Z-
dc.rights.accessRightsinfo:eu-repo/semantics/openAccess-
Appears in Collections:Articles publicats en revistes (Física Quàntica i Astrofísica)

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