Please use this identifier to cite or link to this item: https://hdl.handle.net/2445/221840
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dc.contributor.authorCalefice, Lukas-
dc.contributor.authorComerma Montells, Albert-
dc.contributor.authorGarcia Moreno, Paula-
dc.contributor.authorGarrido Beltrán, Lluís-
dc.contributor.authorGioventù, Alessandra-
dc.contributor.authorGironella Gironell, Pere-
dc.contributor.authorGomez Fernandez, Sergio-
dc.contributor.authorGraugés Pous, Eugeni-
dc.contributor.authorLaguarta Gonzalez, P.-
dc.contributor.authorLobo Salvia, Aniol-
dc.contributor.authorLópez Huertas, Albert-
dc.contributor.authorManera Escalero, Rafel-
dc.contributor.authorMarin Benito, Carla-
dc.contributor.authorMauricio Ferre, Joan-
dc.contributor.authorVazquez Gomez, Ricardo-
dc.contributor.authorVidrier Villalba, Pol-
dc.contributor.authorBrossa Gonzalo, Arnau-
dc.contributor.authorLHCb Collaboration-
dc.date.accessioned2025-06-27T13:12:05Z-
dc.date.available2025-06-27T13:12:05Z-
dc.date.issued2024-
dc.identifier.issn1126-6708-
dc.identifier.urihttps://hdl.handle.net/2445/221840-
dc.description.abstractUsing pp collision data at √ s = 13 TeV, recorded by the LHCb experiment between 2016 and 2018 and corresponding to an integrated luminosity of 5.4 fb−1 , the forwardbackward asymmetry in the pp → Z/γ∗ → µ +µ − process is measured. The measurement is carried out in ten intervals of the diference between the muon pseudorapidities, within a fducial region covering dimuon masses between 66 and 116 GeV, muon pseudorapidities between 2.0 and 4.5 and muon transverse momenta above 20 GeV. These forward-backward asymmetries are compared with predictions, at next-to-leading order in the strong and electroweak couplings. The measured efective leptonic weak mixing angle is sin2 θ ℓ ef = 0.23147 ± 0.00044 ± 0.00005 ± 0.00023, where the frst uncertainty is statistical, the second arises from systematic uncertainties associated with the asymmetry measurement, and the third arises from uncertainties in the ft model used to extract sin2 θ ℓ ef from the asymmetry measurement. This result is based on an arithmetic average of results using the CT18, MSHT20, and NNPDF31 parameterisations of the proton internal structure, and is consistent with previous measurements and with predictions from the global electroweak ft.-
dc.format.extent28 p.-
dc.format.mimetypeapplication/pdf-
dc.language.isoeng-
dc.publisherSpringer Verlag-
dc.relation.isformatofReproducció del document publicat a: https://doi.org/10.1007/JHEP12(2024)026-
dc.relation.ispartofJournal of High Energy Physics, 2024, vol. 2024, num.26-
dc.relation.urihttps://doi.org/10.1007/JHEP12(2024)026-
dc.rightscc-by (c) Aaij, R. et al., 2024-
dc.rights.urihttp://creativecommons.org/licenses/by/4.0/-
dc.sourceArticles publicats en revistes (Física Quàntica i Astrofísica)-
dc.subject.classificationHadrons-
dc.subject.classificationFísica de partícules-
dc.subject.classificationModel estàndard (Física nuclear)-
dc.subject.otherHadrons-
dc.subject.otherParticle physics-
dc.subject.otherStandard model (Nuclear physics)-
dc.titleMeasurement of the efective leptonic weak mixing angle -
dc.typeinfo:eu-repo/semantics/article-
dc.typeinfo:eu-repo/semantics/publishedVersion-
dc.identifier.idgrec756460-
dc.date.updated2025-06-27T13:12:05Z-
dc.rights.accessRightsinfo:eu-repo/semantics/openAccess-
Appears in Collections:Articles publicats en revistes (Física Quàntica i Astrofísica)

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