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Search for long-lived heavy neutrinos in the decays of B mesons produced in proton-proton collisions at $$ \sqrt{s} $$ = 13 TeV

A. HayrapetyanYerevan Physics InstituteA. TumasyanYerevan Physics InstituteW. AdamInstitut f ür Hochenergiephysik, Vienna, AustriaJanik Walter AndrejkovicInstitut f ür Hochenergiephysik, Vienna, AustriaT. BergauerInstitut für HochenergiephysikS. ChatterjeeYerevan Physics Institute, Yerevan, ArmeniaK. DamanakisUniversiteit Antwerpen, Antwerpen, BelgiumM. DragicevicInstitut f ür Hochenergiephysik, Vienna, AustriaPriya Sajid HussainYerevan Physics Institute, Yerevan, ArmeniaM. JeitlerInstitut f ür Hochenergiephysik, Vienna, AustriaNatascha KrammerYerevan Physics Institute, Yerevan, ArmeniaA. LiUniversity of California, Santa Barbara — Department of PhysicsD. LikoInstitut f ür Hochenergiephysik, Vienna, AustriaI. MikulecYerevan Physics Institute, Yerevan, ArmeniaJ. SchieckUniversiteit Antwerpen, Antwerpen, BelgiumR. SchöfbeckYerevan Physics Institute, Yerevan, ArmeniaD. SchwarzInstitut f ür Hochenergiephysik, Vienna, AustriaM. SonawaneYerevan Physics Institute, Yerevan, ArmeniaS. TemplInstitut f ür Hochenergiephysik, Vienna, AustriaW. WaltenbergerYerevan Physics Institute, Yerevan, ArmeniaC.-E. WulzInstitut für HochenergiephysikM. R. DarwishInstitut f ür Hochenergiephysik, Vienna, AustriaX. JanssenYerevan Physics Institute, Yerevan, ArmeniaP. Van MechelenYerevan Physics Institute, Yerevan, ArmeniaNordin BreugelmansYerevan Physics Institute, Yerevan, ArmeniaJ. D’HondtUniversiteit Antwerpen, Antwerpen, BelgiumSoumya DansanaInstitut f ür Hochenergiephysik, Vienna, AustriaA. De MoorVrije Universiteit BrusselM. DelcourtInstitut f ür Hochenergiephysik, Vienna, AustriaFelix HeyenInstitut f ür Hochenergiephysik, Vienna, AustriaS. LowetteUniversiteit Antwerpen, Antwerpen, BelgiumI. MakarenkoUniversiteit Antwerpen, Antwerpen, BelgiumD. MüllerYerevan Physics Institute, Yerevan, ArmeniaS. TavernierYerevan Physics Institute, Yerevan, ArmeniaM. TytgatYerevan Physics Institute, Yerevan, ArmeniaG. P. Van OnsemUniversiteit Antwerpen, Antwerpen, BelgiumS. Van PutteYerevan Physics Institute, Yerevan, ArmeniaD. VanneromVrije Universiteit BrusselB. ClerbauxInstitut f ür Hochenergiephysik, Vienna, AustriaAloke Kumar DasUniversité Libre de BruxellesG. De LentdeckerUniversiteit Antwerpen, Antwerpen, BelgiumHugues EvardUniversité Libre de BruxellesL. FavartInstitut f ür Hochenergiephysik, Vienna, AustriaP. GianneiosYerevan Physics Institute, Yerevan, ArmeniaD. HohovYerevan Physics Institute, Yerevan, ArmeniaJ. JaramilloUniversité Libre de BruxellesMohammad A. KhalilzadehYerevan Physics Institute, Yerevan, ArmeniaFakhri Alam KhanUniversité Libre de BruxellesK. LeeInstitut f ür Hochenergiephysik, Vienna, AustriaM. MahdavikhorramiUniversiteit Antwerpen, Antwerpen, BelgiumA. MalaraInstitut f ür Hochenergiephysik, Vienna, AustriaS. ParedesUniversiteit Antwerpen, Antwerpen, BelgiumL. ThomasYerevan Physics Institute, Yerevan, ArmeniaM. Vanden BemdenUniversité Libre de BruxellesC. Vander VeldeUniversité Libre de BruxellesP. VanlaerInstitut f ür Hochenergiephysik, Vienna, AustriaM. De CoenYerevan Physics Institute, Yerevan, ArmeniaD. DoburYerevan Physics Institute, Yerevan, ArmeniaG. GökbulutYerevan Physics Institute, Yerevan, ArmeniaYang HongInstitut f ür Hochenergiephysik, Vienna, AustriaJ. KnolleInstitut f ür Hochenergiephysik, Vienna, AustriaLuka LambrechtYerevan Physics Institute, Yerevan, ArmeniaDavid MarckxYerevan Physics Institute, Yerevan, ArmeniaG. MestdachUniversiteit Antwerpen, Antwerpen, BelgiumK. Mota AmariloUniversiteit Antwerpen, Antwerpen, BelgiumCésar RendónGhent UniversityAmrutha SamalanYerevan Physics Institute, Yerevan, ArmeniaK. SkovpenYerevan Physics Institute, Yerevan, ArmeniaN. Van Den BosscheYerevan Physics Institute, Yerevan, ArmeniaJan van der LindenUniversiteit Antwerpen, Antwerpen, BelgiumLiam WezenbeekGhent UniversityA. BeneckeInstitut f ür Hochenergiephysik, Vienna, AustriaA. BethaniInstitut f ür Hochenergiephysik, Vienna, AustriaG. BrunoInstitut f ür Hochenergiephysik, Vienna, AustriaC. CaputoUniversiteit Antwerpen, Antwerpen, BelgiumJ. De Favereau De JeneretUniversité Catholique de LouvainC. DelaereUniversiteit Antwerpen, Antwerpen, BelgiumI. S. DonertasUniversiteit Antwerpen, Antwerpen, BelgiumA. GiammancoInstitut f ür Hochenergiephysik, Vienna, AustriaAhmet Oguz GuzelYerevan Physics Institute, Yerevan, ArmeniaSa. JainUniversité Catholique de LouvainV. LemaitreUniversiteit Antwerpen, Antwerpen, BelgiumPaola MastrapasquaUniversité Catholique de LouvainT. T. TranUniversiteit Antwerpen, Antwerpen, BelgiumS. WertzUniversité Catholique de LouvainG. A. AlvesYerevan Physics Institute, Yerevan, ArmeniaE. CoelhoCentro Brasileiro de Pesquisas FisicasC. HenselYerevan Physics Institute, Yerevan, ArmeniaT. Menezes De OliveiraInstitut f ür Hochenergiephysik, Vienna, AustriaA. MoraesUniversiteit Antwerpen, Antwerpen, BelgiumP. Rebello TelesUniversiteit Antwerpen, Antwerpen, BelgiumM. SoeiroYerevan Physics Institute, Yerevan, ArmeniaA. Vilela PereiraCentro Brasileiro de Pesquisas FisicasW. L. Aldá JúniorYerevan Physics Institute, Yerevan, ArmeniaM. Alves Gallo PereiraUniversidade do Estado do Rio de JaneiroM. Barroso Ferreira FilhoYerevan Physics Institute, Yerevan, ArmeniaH. Brandao MalbouissonInstitut f ür Hochenergiephysik, Vienna, AustriaW. CarvalhoUniversidade do Estado do Rio de JaneiroJ. ChinellatoInstitut f ür Hochenergiephysik, Vienna, Austria
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A bstract A search for long-lived heavy neutrinos (N) in the decays of B mesons produced in proton-proton collisions 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 sample corresponds to an integrated luminosity of 41.6 fb − 1 collected in 2018 by the CMS experiment at the CERN LHC, using a dedicated data stream that enhances the number of recorded events containing B mesons. The search probes heavy neutrinos with masses in the range 1 &lt; m N &lt; 3 GeV and decay lengths in the range 10 − 2 &lt; c τ N &lt; 10 4 mm, where τ N is the N proper mean lifetime. Signal events are defined by the signature B → ℓ B NX; N → ℓ ± π ∓ , where the leptons ℓ B and ℓ can be either a muon or an electron, provided that at least one of them is a muon. The hadronic recoil system, X, is treated inclusively and is not reconstructed. No significant excess of events over the standard model background is observed in any of the ℓ ± π ∓ invariant mass distributions. Limits at 95% confidence level on the sum of the squares of the mixing amplitudes between heavy and light neutrinos, | V N | 2 , and on c τ N are obtained in different mixing scenarios for both Majorana and Dirac-like N particles. The most stringent upper limit |V N | 2 &lt; 2.0 × 10 − 5 is obtained at m N = 1.95 GeV for the Majorana case where N mixes exclusively with muon neutrinos. The limits on |V N | 2 for masses 1 &lt; m N &lt; 1.7 GeV are the most stringent from a collider experiment to date.

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