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A search for heavy neutral leptons (HNLs), the right-handed Dirac or Majorana neutrinos, is performed in final states with three charged leptons (electrons or muons) using proton-proton collision data collected by the CMS experiment at root s = 13 TeV at the CERN LHC. The data correspond to an integrated luminosity of 138 fb(-1). The HNLs could be produced through mixing with standard model neutrinos v. For small values of the HNL mass (<20 GeV) and the square of the HNL-v mixing parameter (10(-7)-10(-2)), the decay length of these particles can be large enough so that the secondary vertex of the HNL decay can be resolved with the CMS silicon tracker. The selected final state consists of one lepton emerging from the primary proton-proton collision vertex, and two leptons forming a displaced, secondary vertex. No significant deviations from the standard model expectations are observed, and constraints are obtained on the HNL mass and coupling strength parameters, excluding previously unexplored regions of parameter space in the mass range 1-20 GeV and squared mixing parameter values as low as 10(-7).
A. Tumasyan, W. Adam, J. W. Andrejkovic, T. Bergauer, S. Chatterjee, K. Damanakis, et al. (2022). Search for long-lived heavy neutral leptons with displaced vertices in proton-proton collisions at √s = 13 TeV. JOURNAL OF HIGH ENERGY PHYSICS, 2022(7), 1-55 [10.1007/jhep07(2022)081].
Search for long-lived heavy neutral leptons with displaced vertices in proton-proton collisions at √s = 13 TeV
A. Tumasyan;W. Adam;J. W. Andrejkovic;T. Bergauer;S. Chatterjee;K. Damanakis;M. Dragicevic;A. Escalante Del Valle;R. Fr??hwirth;M. Jeitler;N. Krammer;L. Lechner;D. Liko;I. Mikulec;P. Paulitsch;F. M. Pitters;J. Schieck;R. Sch??fbeck;D. Schwarz;S. Templ;W. Waltenberger;C. -E. Wulz;V. Chekhovsky;A. Litomin;V. Makarenko;M. R. Darwish;E. A. De Wolf;T. Janssen;T. Kello;A. Lelek;H. Rejeb Sfar;P. Van Mechelen;S. Van Putte;N. Van Remortel;F. Blekman;E. S. Bols;J. D???Hondt;M. Delcourt;H. El Faham;S. Lowette;S. Moortgat;A. Morton;D. M??ller;A. R. Sahasransu;S. Tavernier;W. Van Doninck;D. Beghin;B. Bilin;B. Clerbaux;G. De Lentdecker;L. Favart;A. Grebenyuk;A. K. Kalsi;K. Lee;M. Mahdavikhorrami;I. Makarenko;L. Moureaux;L. P??tr??;A. Popov;N. Postiau;E. Starling;L. Thomas;M. Vanden Bemden;C. Vander Velde;P. Vanlaer;T. Cornelis;D. Dobur;J. Knolle;L. Lambrecht;G. Mestdach;M. Niedziela;C. Roskas;A. Samalan;K. Skovpen;M. Tytgat;B. Vermassen;M. Vit;L. Wezenbeek;A. Benecke;A. Bethani;G. Bruno;F. Bury;C. 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Rathjens;A. Safonov;N. Akchurin;J. Damgov;V. Hegde;S. Kunori;K. Lamichhane;S. W. Lee;T. Mengke;S. Muthumuni;T. Peltola;I. Volobouev;Z. Wang;A. Whitbeck;E. Appelt;S. Greene;A. Gurrola;W. Johns;A. Melo;H. Ni;K. Padeken;F. Romeo;P. Sheldon;S. Tuo;J. Velkovska;M. W. Arenton;B. Cox;G. Cummings;J. Hakala;R. Hirosky;M. Joyce;A. Ledovskoy;A. Li;C. Neu;C. E. Perez Lara;B. Tannenwald;S. White;E. Wolfe;N. Poudyal;K. Black;T. Bose;C. Caillol;S. Dasu;I. De Bruyn;P. Everaerts;F. Fienga;C. Galloni;H. He;M. Herndon;A. Herv??;U. Hussain;A. Lanaro;A. Loeliger;R. Loveless;J. Madhusudanan Sreekala;A. Mallampalli;A. Mohammadi;D. Pinna;A. Savin;V. Shang;V. Sharma;W. H. Smith;D. Teague;S. Trembath-Reichert;W. Vetens
2022
Abstract
A search for heavy neutral leptons (HNLs), the right-handed Dirac or Majorana neutrinos, is performed in final states with three charged leptons (electrons or muons) using proton-proton collision data collected by the CMS experiment at root s = 13 TeV at the CERN LHC. The data correspond to an integrated luminosity of 138 fb(-1). The HNLs could be produced through mixing with standard model neutrinos v. For small values of the HNL mass (<20 GeV) and the square of the HNL-v mixing parameter (10(-7)-10(-2)), the decay length of these particles can be large enough so that the secondary vertex of the HNL decay can be resolved with the CMS silicon tracker. The selected final state consists of one lepton emerging from the primary proton-proton collision vertex, and two leptons forming a displaced, secondary vertex. No significant deviations from the standard model expectations are observed, and constraints are obtained on the HNL mass and coupling strength parameters, excluding previously unexplored regions of parameter space in the mass range 1-20 GeV and squared mixing parameter values as low as 10(-7).
A. Tumasyan, W. Adam, J. W. Andrejkovic, T. Bergauer, S. Chatterjee, K. Damanakis, et al. (2022). Search for long-lived heavy neutral leptons with displaced vertices in proton-proton collisions at √s = 13 TeV. JOURNAL OF HIGH ENERGY PHYSICS, 2022(7), 1-55 [10.1007/jhep07(2022)081].
A. Tumasyan; W. Adam; J. W. Andrejkovic; T. Bergauer; S. Chatterjee; K. Damanakis; M. Dragicevic; A. Escalante Del Valle; R. Fr??hwirth; M. Jeitler; N...espandi
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/11585/903665
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simulazione ASN
Il report seguente simula gli indicatori relativi alla propria produzione scientifica in relazione alle soglie ASN 2023-2025 del proprio SC/SSD. Si ricorda che il superamento dei valori soglia (almeno 2 su 3) è requisito necessario ma non sufficiente al conseguimento dell'abilitazione. La simulazione si basa sui dati IRIS e sugli indicatori bibliometrici alla data indicata e non tiene conto di eventuali periodi di congedo obbligatorio, che in sede di domanda ASN danno diritto a incrementi percentuali dei valori. La simulazione può differire dall'esito di un’eventuale domanda ASN sia per errori di catalogazione e/o dati mancanti in IRIS, sia per la variabilità dei dati bibliometrici nel tempo. Si consideri che Anvur calcola i valori degli indicatori all'ultima data utile per la presentazione delle domande.
La presente simulazione è stata realizzata sulla base delle specifiche raccolte sul tavolo ER del Focus Group IRIS coordinato dall’Università di Modena e Reggio Emilia e delle regole riportate nel DM 589/2018 e allegata Tabella A. Cineca, l’Università di Modena e Reggio Emilia e il Focus Group IRIS non si assumono alcuna responsabilità in merito all’uso che il diretto interessato o terzi faranno della simulazione. Si specifica inoltre che la simulazione contiene calcoli effettuati con dati e algoritmi di pubblico dominio e deve quindi essere considerata come un mero ausilio al calcolo svolgibile manualmente o con strumenti equivalenti.