Please use this identifier to cite or link to this item: http://hdl.handle.net/2445/185379
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dc.contributor.authorAlfonso Albero, Alejandro-
dc.contributor.authorCalvo Gomez, M.-
dc.contributor.authorCamboni, Alessandro-
dc.contributor.authorCoquereau, Samuel-
dc.contributor.authorGarrido Beltrán, Lluís-
dc.contributor.authorGascón Fora, David-
dc.contributor.authorGraciani Díaz, Ricardo-
dc.contributor.authorGraugés Pous, Eugeni-
dc.contributor.authorMarin Benito, Carla-
dc.contributor.authorLHCb Collaboration-
dc.date.accessioned2022-05-04T16:30:57Z-
dc.date.available2022-05-04T16:30:57Z-
dc.date.issued2018-
dc.identifier.issn1126-6708-
dc.identifier.urihttp://hdl.handle.net/2445/185379-
dc.description.abstractAbstract: A binned Dalitz plot analysis of B± → DK± decays, with D → K0 S π +π − and D → K0 SK+K−, is used to perform a measurement of the CP-violating observables x± and y±, which are sensitive to the Cabibbo-Kobayashi-Maskawa angle γ. The analysis is performed without assuming any D decay model, through the use of information on the strong-phase variation over the Dalitz plot from the CLEO collaboration. Using a sample of proton-proton collision data collected with the LHCb experiment in 2015 and 2016, and corresponding to an integrated luminosity of 2.0 fb−1 , the values of the CP violation parameters are found to be x− = (9.0±1.7±0.7±0.4)×10−2 , y− = (2.1±2.2±0.5±1.1)× 10−2 , x+ = (−7.7±1.9±0.7±0.4)×10−2 , and y+ = (−1.0±1.9±0.4±0.9)×10−2 . The first uncertainty is statistical, the second is systematic, and the third is due to the uncertainty on the strong-phase measurements. These values are used to obtain γ = 87 +11 −12 ◦ , rB = 0.086+0.013 −0.014, and δB = (101±11)◦ , where rB is the ratio between the suppressed and favoured B-decay amplitudes and δB is the corresponding strong-interaction phase difference. This measurement is combined with the result obtained using 2011 and 2012 data collected with the LHCb experiment, to give γ = 80 +10 −9 ◦ , rB = 0.080 ± 0.011, and δB = (110 ± 10)◦-
dc.format.extent36 p.-
dc.format.mimetypeapplication/pdf-
dc.language.isoeng-
dc.publisherSpringer Verlag-
dc.relation.isformatofReproducció del document publicat a: https://doi.org/10.1007/JHEP08(2018)176-
dc.relation.ispartofJournal of High Energy Physics, 2018, vol. 2018, num. 8, p. 1-36-
dc.relation.urihttps://doi.org/10.1007/JHEP08(2018)176-
dc.rightscc-by (c) LHCb Collaboration (UB: Alfonso Albero, A. et al., 2018-
dc.rights.urihttps://creativecommons.org/licenses/by/4.0/-
dc.sourceArticles publicats en revistes (Física Quàntica i Astrofísica)-
dc.subject.classificationHadrons-
dc.subject.classificationGran Col·lisionador d'Hadrons-
dc.subject.classificationFísica de partícules-
dc.subject.classificationExperiments-
dc.subject.otherHadrons-
dc.subject.otherLarge Hadron Collider (France and Switzerland)-
dc.subject.otherParticle physics-
dc.subject.otherExperiments-
dc.titleMeasurement of the CKM angle γ using B ± → DK ± with D → K S 0 π + π −, K S 0 K + K − decays-
dc.typeinfo:eu-repo/semantics/article-
dc.typeinfo:eu-repo/semantics/publishedVersion-
dc.identifier.idgrec684616-
dc.date.updated2022-05-04T16:30:57Z-
dc.rights.accessRightsinfo:eu-repo/semantics/openAccess-
Appears in Collections:Articles publicats en revistes (Física Quàntica i Astrofísica)

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