Measurement of Z → τ + τ − production in proton-proton collisions at √s=8 TeV

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.authorGironella Gironell, Pere
dc.contributor.authorGraciani Díaz, Ricardo
dc.contributor.authorGraugés Pous, Eugeni
dc.contributor.authorVazquez Gomez, R.
dc.contributor.authorMarin Benito, Carla
dc.contributor.authorLHCb Collaboration
dc.date.accessioned2022-05-10T15:49:39Z
dc.date.available2022-05-10T15:49:39Z
dc.date.issued2018
dc.date.updated2022-05-10T15:49:40Z
dc.description.abstractA measurement of Z → τ +τ − production cross-section is presented using data, corresponding to an integrated luminosity of 2 fb−1 , from pp collisions at √ s = 8 TeV collected by the LHCb experiment. The τ +τ − candidates are reconstructed in final states with the first tau lepton decaying leptonically, and the second decaying either leptonically or to one or three charged hadrons. The production cross-section is measured for Z bosons with invariant mass between 60 and 120 GeV/c2 , which decay to tau leptons with transverse momenta greater than 20 GeV/c and pseudorapidities between 2.0 and 4.5. The crosssection is determined to be σpp→Z→τ+τ− = 95.8 ± 2.1 ± 4.6 ± 0.2 ± 1.1 pb, where the first uncertainty is statistical, the second is systematic, the third is due to the LHC beam energy uncertainty, and the fourth to the integrated luminosity uncertainty. This result is compatible with NNLO Standard model predictions. The ratio of the cross-sections for Z → τ +τ − to Z → µ +µ − (Z → e +e −), determined to be 1.01 ± 0.05 (1.02 ± 0.06), is consistent with the lepton-universality hypothesis in Z decays.
dc.format.extent19 p.
dc.format.mimetypeapplication/pdf
dc.identifier.idgrec684530
dc.identifier.issn1126-6708
dc.identifier.urihttps://hdl.handle.net/2445/185500
dc.language.isoeng
dc.publisherSpringer Verlag
dc.relation.isformatofReproducció del document publicat a: https://doi.org/10.1007/JHEP09(2018)159
dc.relation.ispartofJournal of High Energy Physics, 2018, vol. 2018, num. 9, p. 1-19
dc.relation.urihttps://doi.org/10.1007/JHEP09(2018)159
dc.rightscc-by (c) Alfonso Albero, Alejandro et al., 2018
dc.rights.accessRightsinfo:eu-repo/semantics/openAccess
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 Z → τ + τ − production in proton-proton collisions at √s=8 TeV
dc.typeinfo:eu-repo/semantics/article
dc.typeinfo:eu-repo/semantics/publishedVersion

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