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Search for electroweak production of charginos and neutralinos at √s=13 Tev in final states containing hadronic decays of WW, WZ, or WH and missing transverse momentum

dc.contributor.authorTumasyan, A.
dc.contributor.authorAdam, W.
dc.contributor.authorAndrejkovic, J. W.
dc.contributor.authorBergauer, T.
dc.contributor.authorChatterjee, S.
dc.contributor.authorDamanakis, K.
dc.contributor.authorDragicevic, M.
dc.contributor.authorDel Valle, A. Escalante
dc.contributor.authorFruehwirth, R.
dc.contributor.authorJeitler, M.
dc.contributor.authorFinger, Michael
dc.contributor.authorFinger, Miroslav
dc.contributor.authorKvětoň, Antonín
dc.date.accessioned2024-03-04T09:11:01Z
dc.date.available2024-03-04T09:11:01Z
dc.date.issued2023
dc.identifier.urihttps://hdl.handle.net/20.500.14178/2308
dc.description.abstractThis Letter presents a search for direct production of charginos and neutralinos via electroweak interactions. The results are based on data from proton-proton collisions at a center-of-mass energy of 13 TeV collected with the CMS detector at the LHC, corresponding to an integrated luminosity of 137 fb-1. The search considers final states with large missing transverse momentum and pairs of hadronically decaying bosons WW, WZ, and WH, where H is the Higgs boson. These bosons are identified using novel algorithms. No significant excess of events is observed relative to the expectations from the standard model. Limits at the 95% confidence level are placed on the cross section for production of mass-degenerate wino-like supersymmetric particles & chi;⠂& PLUSMN; 1 and & chi;⠂02, and mass-degenerate higgsino-like supersymmetric particles & chi;⠂& PLUSMN;1,& chi;⠂02, and & chi;⠂03. In the limit of a nearly-massless lightest supersymmetric particle & chi;⠂01, wino-like particles with masses up to 870 and 960 GeV are excluded in the cases of & chi;⠂02 & RARR; Z & chi;⠂01 and & chi;⠂02 & RARR; H & chi;⠂01, respectively, and higgsino-like particles are excluded between 300 and 650 GeV. & COPY; 2022 The Author(s). Published by Elsevier B.V. This is an open access article under the CC BY license (http://creativecommons .org /licenses /by /4 .0/). Funded by SCOAP3.en
dc.language.isoen
dc.relation.urlhttps://doi.org/10.1016/j.physletb.2022.137460
dc.rightsCreative Commons Uveďte původ 4.0 Internationalcs
dc.rightsCreative Commons Attribution 4.0 Internationalen
dc.titleSearch for electroweak production of charginos and neutralinos at SQUARE ROOTs=13 Tev in final states containing hadronic decays of WW, WZ, or WH and missing transverse momentumen
dcterms.accessRightsopenAccess
dcterms.licensehttps://creativecommons.org/licenses/by/4.0/legalcode
dc.date.updated2024-03-04T09:11:01Z
dc.subject.keywordCMSen
dc.subject.keywordGauginoen
dc.subject.keywordElectroweakinoen
dc.subject.keywordSupersymmetryen
dc.subject.keyworden
dc.relation.fundingReferenceinfo:eu-repo/grantAgreement/MSM/LG/LG14004
dc.date.embargoStartDate2024-03-04
dc.type.obd73
dc.type.versioninfo:eu-repo/semantics/publishedVersion
dc.identifier.doi10.1016/j.physletb.2022.137460
dc.identifier.utWos001025977500001
dc.identifier.eidScopus2-s2.0-85162748879
dc.identifier.obd638584
dc.subject.rivPrimary10000::10300
dcterms.isPartOf.namePhysics Letters, Section B: Nuclear, Elementary Particle and High-Energy Physics
dcterms.isPartOf.issn0370-2693
dcterms.isPartOf.journalYear2023
dcterms.isPartOf.journalVolume842
dcterms.isPartOf.journalIssue2023
uk.faculty.primaryId116
uk.faculty.primaryNameMatematicko-fyzikální fakultacs
uk.faculty.primaryNameFaculty of Mathematics and Physicsen
uk.department.primaryId1251
uk.department.primaryNameKatedra fyziky nízkých teplotcs
uk.department.primaryNameDepartment of Low Temperature Physicsen
dc.type.obdHierarchyCsČLÁNEK V ČASOPISU::článek v časopisu::původní článekcs
dc.type.obdHierarchyEnJOURNAL ARTICLE::journal article::original articleen
dc.type.obdHierarchyCode73::152::206en
uk.displayTitleSearch for electroweak production of charginos and neutralinos at &radic;<em>s</em>=13 Tev in final states containing hadronic decays of WW, WZ, or WH and missing transverse momentumen


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