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   <dc:title>Observation of the Λb0→χc1 (3872) pK− decay</dc:title>
   <dc:creator>LHCb Collaboration</dc:creator>
   <dc:creator>Alfonso Albero, Alejandro</dc:creator>
   <dc:creator>Calvo Gómez, Míriam</dc:creator>
   <dc:creator>Camboni, Alessandro</dc:creator>
   <dc:creator>Coquereau, Samuel</dc:creator>
   <dc:creator>Garrido Beltrán, Lluís</dc:creator>
   <dc:creator>Gascón Fora, David</dc:creator>
   <dc:creator>Gironella Gironell, Pere</dc:creator>
   <dc:creator>Graciani Díaz, Ricardo</dc:creator>
   <dc:creator>Graugés Pous, Eugeni</dc:creator>
   <dc:creator>Vilasis-Cardona, Xavier</dc:creator>
   <dc:subject>Hadrons</dc:subject>
   <dc:subject>Col·lisions (Física)</dc:subject>
   <dc:subject>Experiments</dc:subject>
   <dc:subject>Hadrons</dc:subject>
   <dc:subject>Collisions (Physics)</dc:subject>
   <dc:subject>Experiments</dc:subject>
   <dc:description>Using proton-proton collision data, collected with the LHCb detector and corresponding to 1.0, 2.0 and 1.9 fb−1 of integrated luminosity at the centre-of-mass energies of 7, 8, and 13 TeV, respectively, the decay Λ0 b → χc1(3872)pK− with χc1(3872) → J/ψ π+π − is observed for the first time. The significance of the observed signal is in excess of seven standard deviations. It is found that (58 ± 15)% of the decays proceed via the two-body intermediate state χc1(3872)Λ(1520). The branching fraction with respect to that of the Λ0 b → ψ(2S)pK− decay mode, where the ψ(2S) meson is reconstructed in the J/ψ π+π − final state, is measured to be: B(Λ0b → χc1(3872)pK−)B(Λ0b → ψ(2S)pK−)×B(χc1(3872) → J/ψ π+π−)B(ψ(2S) → J/ψ π+π−)= (5.4 ± 1.1 ± 0.2) × 10−2, where the first uncertainty is statistical and the second is systematic</dc:description>
   <dc:date>2020-05-24T16:20:01Z</dc:date>
   <dc:date>2020-05-24T16:20:01Z</dc:date>
   <dc:date>2019-09-03</dc:date>
   <dc:date>2020-05-24T16:20:02Z</dc:date>
   <dc:type>info:eu-repo/semantics/article</dc:type>
   <dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
   <dc:identifier>1126-6708</dc:identifier>
   <dc:identifier>https://hdl.handle.net/2445/162157</dc:identifier>
   <dc:identifier>696336</dc:identifier>
   <dc:language>eng</dc:language>
   <dc:relation>Reproducció del document publicat a: https://doi.org/10.1007/JHEP09(2019)028</dc:relation>
   <dc:relation>Journal of High Energy Physics, 2019, p. 28</dc:relation>
   <dc:relation>https://doi.org/10.1007/JHEP09(2019)028</dc:relation>
   <dc:rights>cc-by (c) LHCb Collaboration et al., 2019</dc:rights>
   <dc:rights>http://creativecommons.org/licenses/by/3.0/es</dc:rights>
   <dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
   <dc:format>19 p.</dc:format>
   <dc:format>application/pdf</dc:format>
   <dc:publisher>Springer Verlag</dc:publisher>
   <dc:source>Articles publicats en revistes (Física Quàntica i Astrofísica)</dc:source>
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