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               <dc:title>Measurement of the B 0 → K ∗0 e + e - branching fraction at low dilepton mass</dc:title>
               <dc:creator>Abellan Beteta, Carlos</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>López Asamar, Elias</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>Vázquez Gómez, Ricard</dc:creator>
               <dc:creator>Calvo Gómez, Míriam</dc:creator>
               <dc:creator>Oyanguren Campos, Arantza de</dc:creator>
               <dc:creator>Pérez-Calero Yzquierdo, Antonio</dc:creator>
               <dc:creator>Ruiz Valls, Pablo</dc:creator>
               <dc:creator>Vilasis-Cardona, Xavier</dc:creator>
               <dc:creator>LHCb Collaboration</dc:creator>
               <dc:subject>Hadrons</dc:subject>
               <dc:subject>Cromodinàmica quàntica</dc:subject>
               <dc:subject>Gran Col·lisionador d'Hadrons</dc:subject>
               <dc:subject>Hadrons</dc:subject>
               <dc:subject>Quantum chromodynamics</dc:subject>
               <dc:subject>Large Hadron Collider (France and Switzerland)</dc:subject>
               <dc:description>The branching fraction of the rare decay B0→ K∗0 e +e− in the dilepton mass region from 30 to 1000 MeV/c2 has been measured by the LHCb experiment, using pp collision data, corresponding to an integrated luminosity of 1.0 fb−1, at a centre-of-mass energy of 7 TeV. The decay mode B0 → J/ψ(e+e−)K∗0 is utilized as a normalization&#xd;
channel. The branching fraction B(B0 → K∗0e+e−) is measured to beB(B&#xd;
0→ K∗0 e+e−)30−1000 MeV/c2= (3.1+0.9 +0.2−0.8 −0.3 ± 0.2) × 10−7&#xd;
, where the first error is statistical, the second is systematic, and the third comes from the uncertainties on the B0→ J/ψ K∗0 and J/ψ → e+e− branching fractions.</dc:description>
               <dc:date>2016-06-07T10:05:57Z</dc:date>
               <dc:date>2016-06-07T10:05:57Z</dc:date>
               <dc:date>2013-05-29</dc:date>
               <dc:date>2016-06-07T10:06:02Z</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: http://dx.doi.org/10.1007/JHEP05(2013)159</dc:relation>
               <dc:relation>Journal of High Energy Physics, 2013, vol. 159, num. 159</dc:relation>
               <dc:relation>http://dx.doi.org/10.1007/JHEP05(2013)159</dc:relation>
               <dc:rights>cc-by (c) LHCb Collaboration et al., 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>Springer Verlag</dc:publisher>
               <dc:source>Articles publicats en revistes (Física Quàntica i Astrofísica)</dc:source>
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