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                  <mods:namePart>Badalov, Alexey</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>Camboni, Alessandro</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>Picatoste Olloqui, Eduardo</mods:namePart>
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               <mods:name>
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                  <mods:namePart>Rives Molina, Vicente José</mods:namePart>
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               <mods:name>
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                     <mods:roleTerm type="text">author</mods:roleTerm>
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                  <mods:namePart>Ruiz, Hugo (Ruiz Pérez)</mods:namePart>
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               <mods:name>
                  <mods:role>
                     <mods:roleTerm type="text">author</mods:roleTerm>
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                  <mods:namePart>Vilasis-Cardona, Xavier</mods:namePart>
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               <mods:name>
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                     <mods:roleTerm type="text">author</mods:roleTerm>
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                  <mods:namePart>LHCb Collaboration</mods:namePart>
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                  <mods:dateIssued encoding="iso8601">2019-04-02T11:31:29Z2019-04-02T11:31:29Z2014-07-092019-04-02T11:31:29Z</mods:dateIssued>
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               <mods:abstract>The resonant structure of the reaction ¯ B 0 → J / ψ π + π − is studied using data from 3     fb − 1 of integrated luminosity collected by the LHCb experiment, one third at 7 TeV center-of-mass energy and the remainder at 8 TeV. The invariant mass of the π + π − pair and three decay angular distributions are used to determine the fractions of the resonant and nonresonant components. Six interfering π + π − states, ρ ( 770 ) , f 0 ( 500 ) , f 2 ( 1270 ) , ρ ( 1450 ) , ω ( 782 ) and ρ ( 1700 ) , are required to give a good description of invariant mass spectra and decay angular distributions. The positive and negative charge parity fractions of each of the resonant final states are determined. The f 0 ( 980 ) meson is not seen and the upper limit on its presence, compared with the observed f 0 ( 500 ) rate, is inconsistent with a model where these scalar mesons are formed from two quarks and two antiquarks (tetraquarks) at the eight standard deviation level. In the q ¯ q model, the absolute value of the mixing angle between the f 0 ( 980 ) and the f 0 ( 500 ) scalar mesons is limited to be less than 17° at 90% confidence level.</mods:abstract>
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               <mods:accessCondition type="useAndReproduction">cc by (c) CERN; LHCb Collaboration, 2014 http://creativecommons.org/licenses/by/3.0/es/ info:eu-repo/semantics/openAccess</mods:accessCondition>
               <mods:subject>
                  <mods:topic>Física de partícules</mods:topic>
               </mods:subject>
               <mods:subject>
                  <mods:topic>Gran Col·lisionador d'Hadrons</mods:topic>
               </mods:subject>
               <mods:subject>
                  <mods:topic>Ressonància</mods:topic>
               </mods:subject>
               <mods:subject>
                  <mods:topic>Experiments</mods:topic>
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               <mods:subject>
                  <mods:topic>Particle physics</mods:topic>
               </mods:subject>
               <mods:subject>
                  <mods:topic>Large Hadron Collider (France and Switzerland)</mods:topic>
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               <mods:subject>
                  <mods:topic>Resonance</mods:topic>
               </mods:subject>
               <mods:subject>
                  <mods:topic>Experiments</mods:topic>
               </mods:subject>
               <mods:titleInfo>
                  <mods:title>Measurement of the resonant and CP components in ¯¯B0 → J/ψπ+π− decays</mods:title>
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