Measurement of the efective leptonic weak mixing angle 

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.date.updated2025-06-27T13:12:05Z
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.identifier.idgrec756460
dc.identifier.issn1126-6708
dc.identifier.urihttps://hdl.handle.net/2445/221840
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.accessRightsinfo:eu-repo/semantics/openAccess
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

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