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dc.contributor.authorOsland, Per
dc.contributor.authorPankov, A.A.
dc.contributor.authorSerenkova, I.A.
dc.date.accessioned2022-05-03T08:22:00Z
dc.date.available2022-05-03T08:22:00Z
dc.date.created2021-08-26T15:36:22Z
dc.date.issued2021
dc.identifier.issn2470-0010
dc.identifier.urihttps://hdl.handle.net/11250/2993778
dc.description.abstractThe full ATLAS run 2 dataset with a time-integrated luminosity of 139  fb−1 in the diboson and dilepton channels is used to probe benchmark models with extended gauge sectors: the E6-motivated grand unification models, the left-right symmetric model, and the sequential standard model [extended gauge model (EGM)]. These all predict neutral Z′ vector bosons, decaying into lepton pairs ℓℓ or into electroweak gauge boson pairs WW, where one W in turn decays semileptonically. The 95% C.L. exclusion limits on the Z′ resonance production cross section times the branching ratio to electroweak gauge boson pairs and to lepton pairs in the mass range of ∼1 to 6 TeV are converted to constraints on the Z−Z′ mixing parameter and the heavy resonance mass. We present exclusion regions on the parameter space of the Z′ which are significantly extended compared to those obtained from the previous analyses performed with LHC data collected at 7 and 8 TeV in run 1 as well as at 13 TeV in run 2 at a time-integrated luminosity of 36.1  fb−1 and are the most stringent bounds to date. Also presented, from a similar analysis of electrically charged W′ bosons arising in the EGM, which can decay through W′→WZ and W′→ℓν, are limits on the W−W′ mixing parameter and the charged W′ vector boson mass.en_US
dc.language.isoengen_US
dc.publisherAmerican Physical Societyen_US
dc.rightsNavngivelse 4.0 Internasjonal*
dc.rights.urihttp://creativecommons.org/licenses/by/4.0/deed.no*
dc.titleUpdated constraints on Z′ and W′ bosons decaying into bosonic and leptonic final states using the run 2 ATLAS dataen_US
dc.typeJournal articleen_US
dc.typePeer revieweden_US
dc.description.versionpublishedVersionen_US
dc.source.articlenumber053009en_US
cristin.ispublishedtrue
cristin.fulltextoriginal
cristin.qualitycode1
dc.identifier.doi10.1103/PhysRevD.103.053009
dc.identifier.cristin1929048
dc.source.journalPhysical Review Den_US
dc.identifier.citationPhysical Review D. 2021, 103 (5), 053009.en_US
dc.source.volume103en_US
dc.source.issue5en_US


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