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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>Picatoste Olloqui, Eduardo</mods:namePart>
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                  <mods:namePart>Potterat, Cédric</mods:namePart>
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                  <mods:namePart>Ruiz, Hugo (Ruiz Pérez)</mods:namePart>
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                  <mods:namePart>Abellan Beteta, Carlos</mods:namePart>
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                  <mods:namePart>Calvo Gómez, Míriam</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>Vilasis-Cardona, Xavier</mods:namePart>
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               <mods:name>
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                  <mods:namePart>Domingo Bonal, Francesc</mods:namePart>
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                  <mods:dateIssued encoding="iso8601">2019-04-08T13:45:05Z2019-04-08T13:45:05Z2013-05-012019-04-08T13:45:05Z</mods:dateIssued>
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               <mods:abstract>Using proton-proton collision data collected by the LHCb experiment at √ s = 7     TeV , corresponding to an integrated luminosity of 1.0     fb − 1 , the ratio of branching fractions of the B 0 → D * − π + π − π + decay relative to the B 0 → D * − π + decay is measured to be B ( B 0 → D * − π + π − π + ) B ( B 0 → D * − π + ) = 2.64 ± 0.04 ( stat ) ± 0.13 ( syst ) . The Cabibbo-suppressed decay B 0 → D * − K + π − π + is observed for the first time, and the measured ratio of branching fractions is B ( B 0 → D * − K + π − π + ) B ( B 0 → D * − π + π − π + ) = ( 6.47 ± 0.37 ( stat ) ± 0.35 ( syst ) ) × 10 − 2 . A search for orbital excitations of charm mesons contributing to the B 0 → D * − π + π − π + final state is also performed, and the first observation of the B 0 → ¯¯¯ D 1 ( 2420 ) 0 π + π − decay is reported with the ratio of branching fractions B ( B 0 → ( ¯¯¯ D 1 ( 2420 ) 0 → D * − π + ) π − π + ) B ( B 0 → D * − π + π − π + ) = ( 2.04 ± 0.42 ( stat ) ± 0.22 ( syst ) ) × 10 − 2 , where the numerator represents a product of the branching fractions B ( B 0 → ¯¯¯ D 1 ( 2420 ) 0 π − π + ) and B ( ¯¯¯ D 1 ( 2420 ) 0 → D * − π + ) .</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:topic>Experiments</mods:topic>
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               <mods:subject>
                  <mods:topic>Particle physics</mods:topic>
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               <mods:subject>
                  <mods:topic>Experiments</mods:topic>
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                  <mods:title>Study of B0→D*-π+π-π+ and B0→D*-K+π-π+ decays</mods:title>
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