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dc.contributor.authorNecefoğlu, Hacali
dc.contributor.authorMaracı, Ali
dc.contributor.authorAktaş, Vedat
dc.contributor.authorTercan, Barış
dc.contributor.authorHökelek, Tuncer
dc.date.accessioned2019-12-13T06:31:37Z
dc.date.available2019-12-13T06:31:37Z
dc.date.issued2016
dc.identifier.issn0370-2693
dc.identifier.urihttps://doi.org/10.1016/j.physletb.2016.10.054
dc.identifier.urihttp://hdl.handle.net/11655/18412
dc.description.abstractFour-lepton production in proton-proton collisions, pp -> (Z/gamma*)(Z/gamma*)-> l(+)l(-)l '(+)l '(-), where l,l '(-) = e or mu, is studied at a center-of-mass energy of 13 TeV with the CMS detector at the LHC. The data sample corresponds to an integrated luminosity of 2.6fb(-1). The ZZ production cross section, sigma(pp -> ZZ) = 14.6(-1.8)(+1.9)(stat)(-0.3)(+0.5) (syst) +/-0.2 (theo) +/-0.4 (lumi) pb, is measured for events with two opposite-sign, sameflavor lepton pairs produced in the mass region 60 < m(l+l-) m (l'+l'-) < 120GeV. The Z boson branching fraction to four leptons is measured to be B(Z -> l(+)l(-)l '(+)l '(-)) = 4.9(-0.7)(+0.8)(stat)(-0.2)(+0.3)(syst)(-0.1)(+0.2)(theo) +/- 0.1 (lumi) x10(-6) for the four-lepton invariant mass in the range 80 < m(l+)l-l'+l' < 100GeVand dilepton mass m(l+l-) > 4GeVfor all opposite-sign, same-flavor lepton pairs. The results are in agreement with standard model predictions. (C) 2016 The Author. Published by Elsevier B. V. This is an open access article under the CC BY license
dc.language.isoen
dc.publisherElsevier
dc.relation.isversionof10.1016/j.physletb.2016.10.054
dc.rightsinfo:eu-repo/semantics/openAccess
dc.subjectAstronomy & Astrophysics
dc.subjectPhysics
dc.titleMeasurement Of The Zz Production Cross Section And Z -> L(+)L(-)L '(+)L '(-) Branching Fraction In Pp Collisions At Root S=13Tev
dc.typeinfo:eu-repo/semantics/article
dc.relation.journalPhysics Letters B
dc.contributor.departmentFizik Mühendisliği
dc.identifier.volume763
dc.identifier.startpage280
dc.identifier.endpage303
dc.description.indexWoS
dc.description.indexScopus


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