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               <dc:title>Observation of the Decay B+c→B0sπ+</dc:title>
               <dc:creator>Calvo Gómez, Míriam</dc:creator>
               <dc:creator>Camboni, Alessandro</dc:creator>
               <dc:creator>Comerma Montells, Albert</dc:creator>
               <dc:creator>Garrido Beltrán, Lluís</dc:creator>
               <dc:creator>Graciani Díaz, Ricardo</dc:creator>
               <dc:creator>Graugés Pous, Eugeni</dc:creator>
               <dc:creator>Oyanguren Campos, Arantza de</dc:creator>
               <dc:creator>Pérez-Calero Yzquierdo, Antonio</dc:creator>
               <dc:creator>Picatoste Olloqui, Eduardo</dc:creator>
               <dc:creator>Potterat, Cédric</dc:creator>
               <dc:creator>Rives Molina, Vicente José</dc:creator>
               <dc:creator>Ruiz, Hugo (Ruiz Pérez)</dc:creator>
               <dc:creator>Ruiz Valls, Pablo</dc:creator>
               <dc:creator>Vilasis-Cardona, Xavier</dc:creator>
               <dc:creator>LHCb Collaboration</dc:creator>
               <dc:subject>Física de partícules</dc:subject>
               <dc:subject>Experiments</dc:subject>
               <dc:subject>Particle physics</dc:subject>
               <dc:subject>Experiments</dc:subject>
               <dc:description>The result of a search for the decay B + c → B 0 s π + is presented, using the B 0 s → D − s π + and B 0 s → J / ψ ϕ channels. The analysis is based on a data sample of p p collisions collected with the LHCb detector, corresponding to an integrated luminosity of 1     fb − 1 taken at a center-of-mass energy of 7 TeV, and 2     fb − 1 taken at 8 TeV. The decay B + c → B 0 s π + is observed with significance in excess of 5 standard deviations independently in both decay channels. The measured product of the ratio of cross sections and branching fraction is [ σ ( B + c ) / σ ( B 0 s ) ] × B ( B + c → B 0 s π + ) = [ 2.37 ± 0.31   ( stat ) ± 0.11   ( syst ) + 0.17 − 0.13 ( τ B + c ) ] × 10 − 3 , in the pseudorapidity range 2 &lt; η ( B ) &lt; 5 , where the first uncertainty is statistical, the second is systematic, and the third is due to the uncertainty on the B + c lifetime. This is the first observation of a B meson decaying to another B meson via the weak interaction.</dc:description>
               <dc:date>2019-05-16T11:01:28Z</dc:date>
               <dc:date>2019-05-16T11:01:28Z</dc:date>
               <dc:date>2013-11-01</dc:date>
               <dc:date>2019-05-16T11:01:28Z</dc:date>
               <dc:type>info:eu-repo/semantics/article</dc:type>
               <dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
               <dc:relation>Reproducció del document publicat a: https://doi.org/10.1103/PhysRevLett.111.181801</dc:relation>
               <dc:relation>Physical Review Letters, 2013, vol. 111, num. 18, p. 181801</dc:relation>
               <dc:relation>https://doi.org/10.1103/PhysRevLett.111.181801</dc:relation>
               <dc:rights>cc by (c) CERN; LHCb Collaboration, 2013</dc:rights>
               <dc:rights>http://creativecommons.org/licenses/by/3.0/es/</dc:rights>
               <dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
               <dc:publisher>American Physical Society</dc:publisher>
               <dc:source>Articles publicats en revistes (Física Quàntica i Astrofísica)</dc:source>
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