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Search for heavy neutral leptons in final states with electrons, muons, and hadronically decaying tau leptons in proton-proton collisions at $$ \sqrt{s} $$ = 13 TeV

Arsen HayrapetyanYerevan Physics InstituteA. TumasyanUniversiteit Antwerpen, Antwerpen, BelgiumW. AdamYerevan Physics Institute, Yerevan, ArmeniaJanik Walter AndrejkovicInstitut für HochenergiephysikT. BergauerYerevan Physics Institute, Yerevan, ArmeniaS. ChatterjeeInstitut f ür Hochenergiephysik, Vienna, AustriaK. DamanakisYerevan Physics Institute, Yerevan, ArmeniaM. DragicevicInstitut f ür Hochenergiephysik, Vienna, AustriaPriya Sajid HussainInstitut für HochenergiephysikM. JeitlerTU WienNatascha KrammerInstitut für HochenergiephysikA. LiUniversity of California, Santa Barbara — Department of PhysicsD. LikoYerevan Physics Institute, Yerevan, ArmeniaI. MikulecInstitut für HochenergiephysikJ. SchieckUniversiteit Antwerpen, Antwerpen, BelgiumR. SchöfbeckInstitut für HochenergiephysikD. SchwarzYerevan Physics Institute, Yerevan, ArmeniaM. SonawaneInstitut für HochenergiephysikS. TemplInstitut für HochenergiephysikW. WaltenbergerInstitut für HochenergiephysikC.-E. WulzInstitut f ür Hochenergiephysik, Vienna, AustriaM. R. DarwishInstitut f ür Hochenergiephysik, Vienna, AustriaX. JanssenInstitut f ür Hochenergiephysik, Vienna, AustriaP. Van MechelenUniversiteit AntwerpenE. S. BolsYerevan Physics Institute, Yerevan, ArmeniaNordin BreugelmansUniversiteit Antwerpen, Antwerpen, BelgiumJ. D’HondtUniversiteit Antwerpen, Antwerpen, BelgiumSoumya DansanaUniversiteit Antwerpen, Antwerpen, BelgiumA. De MoorVrije Universiteit BrusselM. DelcourtInstitut f ür Hochenergiephysik, Vienna, AustriaFelix HeyenYerevan Physics Institute, Yerevan, ArmeniaS. LowetteVrije Universiteit BrusselI. MakarenkoYerevan Physics Institute, Yerevan, ArmeniaD. MüllerVrije Universiteit BrusselS. TavernierUniversiteit Antwerpen, Antwerpen, BelgiumM. TytgatYerevan Physics Institute, Yerevan, ArmeniaG. P. Van OnsemInstitut f ür Hochenergiephysik, Vienna, AustriaS. Van PutteVrije Universiteit BrusselD. VanneromUniversiteit Antwerpen, Antwerpen, BelgiumB. ClerbauxYerevan Physics Institute, Yerevan, ArmeniaA. K. DasInstitut f ür Hochenergiephysik, Vienna, AustriaG. De LentdeckerYerevan Physics Institute, Yerevan, ArmeniaHugues EvardYerevan Physics Institute, Yerevan, ArmeniaL. FavartUniversité Libre de BruxellesP. GianneiosYerevan Physics Institute, Yerevan, ArmeniaD. HohovInstitut f ür Hochenergiephysik, Vienna, AustriaJ. JaramilloYerevan Physics Institute, Yerevan, ArmeniaMohammad A. KhalilzadehYerevan Physics Institute, Yerevan, ArmeniaFakhri Alam KhanInstitut f ür Hochenergiephysik, Vienna, AustriaK. LeeKorea UniversityM. MahdavikhorramiInstitut f ür Hochenergiephysik, Vienna, AustriaA. MalaraInstitut f ür Hochenergiephysik, Vienna, AustriaS. ParedesYerevan Physics Institute, Yerevan, ArmeniaL. ThomasUniversiteit Antwerpen, Antwerpen, BelgiumM. Vanden BemdenUniversiteit Antwerpen, Antwerpen, BelgiumC. Vander VeldeYerevan Physics Institute, Yerevan, ArmeniaP. VanlaerInstitut f ür Hochenergiephysik, Vienna, AustriaM. De CoenUniversiteit Antwerpen, Antwerpen, BelgiumD. DoburInstitut f ür Hochenergiephysik, Vienna, AustriaYang HongYerevan Physics Institute, Yerevan, ArmeniaJ. KnolleInstitut f ür Hochenergiephysik, Vienna, AustriaLuka LambrechtUniversiteit Antwerpen, Antwerpen, BelgiumG. MestdachUniversiteit Antwerpen, Antwerpen, BelgiumK. Mota AmariloYerevan Physics Institute, Yerevan, ArmeniaCésar RendónInstitut f ür Hochenergiephysik, Vienna, AustriaAmrutha SamalanGhent UniversityK. SkovpenInstitut f ür Hochenergiephysik, Vienna, AustriaN. Van Den BosscheUniversiteit Antwerpen, Antwerpen, BelgiumJan van der LindenUniversiteit Antwerpen, Antwerpen, BelgiumLiam WezenbeekYerevan Physics Institute, Yerevan, ArmeniaA. BeneckeUniversiteit Antwerpen, Antwerpen, BelgiumA. BethaniUniversiteit Antwerpen, Antwerpen, BelgiumG. BrunoInstitut f ür Hochenergiephysik, Vienna, AustriaC. CaputoUniversiteit Antwerpen, Antwerpen, BelgiumC. DelaereInstitut f ür Hochenergiephysik, Vienna, AustriaI. S. DonertasUniversité Catholique de LouvainA. GiammancoYerevan Physics Institute, Yerevan, ArmeniaSa. JainInstitut f ür Hochenergiephysik, Vienna, AustriaV. LemaitreUniversité Catholique de LouvainPaola MastrapasquaUniversiteit Antwerpen, Antwerpen, BelgiumT. T. TranUniversiteit Antwerpen, Antwerpen, BelgiumS. WertzYerevan Physics Institute, Yerevan, ArmeniaG. A. AlvesCentro Brasileiro de Pesquisas FisicasE. CoelhoInstitut f ür Hochenergiephysik, Vienna, AustriaC. HenselInstitut f ür Hochenergiephysik, Vienna, AustriaT. Menezes De OliveiraCentro Brasileiro de Pesquisas FisicasA. MoraesCentro Brasileiro de Pesquisas FisicasP. Rebello TelesUniversiteit Antwerpen, Antwerpen, BelgiumM. SoeiroInstitut f ür Hochenergiephysik, Vienna, AustriaA. Vilela PereiraCentro Brasileiro de Pesquisas FisicasW. L. Aldá JúniorYerevan Physics Institute, Yerevan, ArmeniaM. Alves Gallo PereiraYerevan Physics Institute, Yerevan, ArmeniaM. Barroso Ferreira FilhoUniversidade do Estado do Rio de JaneiroH. Brandao MalbouissonInstitut f ür Hochenergiephysik, Vienna, AustriaW. CarvalhoUniversiteit Antwerpen, Antwerpen, BelgiumJ. ChinellatoUniversiteit Antwerpen, Antwerpen, BelgiumE. M. Da CostaUniversiteit Antwerpen, Antwerpen, BelgiumG. G. Da SilveiraYerevan Physics Institute, Yerevan, ArmeniaD. De Jesus DamiãoYerevan Physics Institute, Yerevan, Armenia
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A bstract A search for heavy neutral leptons (HNLs) of Majorana or Dirac type using proton-proton collision data at $$ \sqrt{s} $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msqrt> <mml:mi>s</mml:mi> </mml:msqrt> </mml:math> = 13 TeV is presented. The data were collected by the CMS experiment at the CERN LHC and correspond to an integrated luminosity of 138 fb − 1 . Events with three charged leptons (electrons, muons, and hadronically decaying tau leptons) are selected, corresponding to HNL production in association with a charged lepton and decay of the HNL to two charged leptons and a standard model (SM) neutrino. The search is performed for HNL masses between 10 GeV and 1.5 TeV. No evidence for an HNL signal is observed in data. Upper limits at 95% confidence level are found for the squared coupling strength of the HNL to SM neutrinos, considering exclusive coupling of the HNL to a single SM neutrino generation, for both Majorana and Dirac HNLs. The limits exceed previously achieved experimental constraints for a wide range of HNL masses, and the limits on tau neutrino coupling scenarios with HNL masses above the W boson mass are presented for the first time.

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