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                  <mods:namePart>Camboni, Alessandro</mods:namePart>
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                  <mods:namePart>Comerma Montells, Albert</mods:namePart>
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                  <mods:namePart>Garrido Beltrán, Lluís</mods:namePart>
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                  <mods:namePart>Graciani Díaz, Ricardo</mods:namePart>
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                  <mods:namePart>Graugés Pous, Eugeni</mods:namePart>
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                  <mods:namePart>López Asamar, Elias</mods:namePart>
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                  <mods:namePart>Pérez-Calero Yzquierdo, Antonio</mods:namePart>
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                  <mods:namePart>Picatoste Olloqui, Eduardo</mods:namePart>
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                  <mods:namePart>Potterat, Cédric</mods:namePart>
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                  <mods:namePart>Rives Molina, Vicente José</mods:namePart>
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                  <mods:namePart>Ruiz, Hugo (Ruiz Pérez)</mods:namePart>
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                  <mods:namePart>Vázquez Gómez, Ricard</mods:namePart>
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                  <mods:namePart>Abellan Beteta, Carlos</mods:namePart>
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               <mods:name>
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                  <mods:namePart>Calvo Gómez, Míriam</mods:namePart>
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                  <mods:namePart>Vilasis-Cardona, Xavier</mods:namePart>
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                  <mods:namePart>Domingo Bonal, Francesc</mods:namePart>
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               <mods:name>
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                  <mods:namePart>LHCb Collaboration</mods:namePart>
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               <mods:originInfo>
                  <mods:dateIssued encoding="iso8601">2019-04-08T13:40:17Z2019-04-08T13:40:17Z2013-04-012019-04-08T13:40:17Z</mods:dateIssued>
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               <mods:abstract>An amplitude analysis of the final state structure in the ¯¯¯ B 0 s → J / ψ K + K − decay mode is performed using 1.0     fb − 1 of data collected by the LHCb experiment in 7 TeV center-of-mass energy p p collisions produced by the LHC. A modified Dalitz plot analysis of the final state is performed using both the invariant mass spectra and the decay angular distributions. Resonant structures are observed in the K + K − mass spectrum as well as a significant nonresonant S -wave contribution over the entire K + K − mass range. The largest resonant component is the ϕ ( 1020 ) , accompanied by f 0 ( 980 ) , f ′ 2 ( 1525 ) , and four additional resonances. The overall branching fraction is measured to be B ( ¯¯¯ B 0 s → J / ψ K + K − ) = ( 7.70 ± 0.08 ± 0.39 ± 0.60 ) × 10 − 4 , where the first uncertainty is statistical, the second systematic, and the third due to the ratio of the number of ¯¯¯ B 0 s to B − mesons produced. The mass and width of the f ′ 2 ( 1525 ) are measured to be 1522.2 ± 2.8 + 5.3 − 2.0     MeV and 84 ± 6 + 10 − 5     MeV , respectively. The final state fractions of the other resonant states are also reported.</mods:abstract>
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               <mods:accessCondition type="useAndReproduction">cc by (c) CERN; LHCb Collaboration, 2013 http://creativecommons.org/licenses/by/3.0/es/ info:eu-repo/semantics/openAccess</mods:accessCondition>
               <mods:subject>
                  <mods:topic>Física de partícules</mods:topic>
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               <mods:subject>
                  <mods:topic>Experiments</mods:topic>
               </mods:subject>
               <mods:subject>
                  <mods:topic>Particle physics</mods:topic>
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               <mods:subject>
                  <mods:topic>Experiments</mods:topic>
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               <mods:titleInfo>
                  <mods:title>Amplitude analysis and branching fraction measurement of B¯s0→J/ψK+K-</mods:title>
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