Search for heavy Majorana or Dirac neutrinos and right-handed W gauge bosons in final states with charged leptons and jets in pp collisions at s=13\\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$\\sqrt{s}=13$$\\end{document} TeV with the ATLAS detector

C Nellist,M Spousta,P Rivadeneira,J Fuster,M Xia,K E Varvell,J Mueller,S C Lee,D Emeliyanov,J Khubua,A Korn,D Robinson,M Shiyakova,R Kopeliansky,A Kahn,F Cirotto,E Gramstad,M Ince Lezki,J Schmeing,M Grandi,D J A Antrim,V Solovyev,G Crosetti,S M Wang,M Tost,S Tokár,J Zinsser,F Parodi,J P Gombas,C Wagner,K Cranmer,E S Haaland,E X L Ting,M Chatterjee,J P Mc Gowan,S Rajagopalan,Y Coadou,P Nilsson,N M Hartman,S Jiggins,P Federicova,B A Schumm,R J Hawkings,M Feickert,L Sawyer,M Barbero,D Schaile,P J Hsu,K Choi,D Akiyama,G Stoicea,K Nikolopoulos,R B Nickerson,O Kovanda,C Weiser,P Liu,A Cerri,L Ferencz,Z Zheng,P Sherwood,R Rosten,M Swiatlowski,M Naseri,J Tanaka,T Heim,M Xie,M Antonelli,J M Hays,J Hoya,M A Diaz,G Giugliarelli,M Rijssenbeek,B J Wilson,G Darbo,A Visibile,A Lebedev,S Goldfarb,T Moskalets,C Gonzalez Renteria,M Moreno Llácer,J W S Carter,D Mascione,N Krumnack,F Backman,A Gavrilyuk,Y Gao,S Yu Smirnov,O L Fedin,L Castillo Garcia,P J Bussey,L M Mir,F Schroeder,M Citterio,S Guindon,V 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Adiguzel,M Fujimoto,N Viaux Maira,M Morii,A M Sickles,Z Zhang,S Dahbi,P Staroba,S Roe,A De Salvo,G Otero Y Garzon,E Romano,M Perganti,H Zeng,R Hankache,H Li,E Antipov,L Shi,M Wu,E Mazzeo,V Sanchez Sebastian,D K Panchal,L Pascual Dominguez,L Massa,C A Gottardo,M Kagan,T Wamorkar,M Svatos,M J Kareem,K Tariq,H G Cooke,G Artoni,S Dungs,M Errenst,E Kajomovitz,M Cobal,J K K Liu,T Trefzger,B Moser,T Mkrtchyan,P Bartos,Y Tian,G Guerrieri,P Zhang,Z Jia,M N Agaras,K E Penski,T Wenaus,R Yuan,S M Farrington,C Li,B Rottler,S Sun,J -F Grivaz,N Govender,P G Scholer,P Gessinger-Befurt,R L Bates,G I Dyckes,R Shaheen,A E Dumitriu,Y Zhang,A Lanza,J K Anders,Y Yang,C Roda,N Bouchhar,C Helsens,R Teixeira De Lima,V Tsulaia,A Garcia Alonso,I Naryshkin,I N Aleksandrov,S Yan,S K Huiberts,A Klimentov,S P Amor Dos Santos,I Gnesi,E H Haines,J D Bossio Sola,J J Kempster,G Gagliardi,S Gurbuz,X Chu,J G Panduro Vazquez,J C Zeng,H Lacker,J M Iturbe Ponce,S Trincaz-Duvoid,T Yamazaki,F Monticelli,P Patel,M Cano Bret,T 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Wang,G F Tartarelli,A Rozanov,S Asai,E Sauvan,D Amidei,S W Alibocus,T C Gosart,C A Garner,W J Fawcett,S Krishnamurthy,O Burlayenko,N A Rusakovich,L Heinrich,T Li,G Mchedlidze,J Harrison,Y Hernández Jiménez,C Wang,B Batool,K Lantzsch,T Sano,C Issever,H Lyons,S Ye,S S Gurdasani,M Penzin,W D Heidorn,W A Leight,R Leitner,V S Bhopatkar,E Shabalina,P Reznicek,O K Baker,L Cerrito,S J Sekula,M Düren,S Pagan Griso,D M Gingrich,M G Barros Teixeira,C Santoni,M Vanadia,H A Weber,M Tsai,J D Shinner,J Roggel,N M Tamir,J A Mcfayden,M Lu,R D Schamberger,J A Zamora Saa,O Cakir,A Marantis,G S Virdee,A Leisos,M Lokajicek,G Palacino,M Wobisch,A Leopold,D Ta,K Uchida,P Calafiura,H Hanif,R Sobie,Z B Pollock,M E Vasile,M E Hesping,D R Tovey,S Hellesund,T Komarek,C Camincher,C P Hays,R Pedro,A C A Lee,M Robin,M Levchenko,J J Heinrich,M Mali,H Cui,M Vandenbroucke,D Fassouliotis,R C W Henderson,J Donini,O E Vickey Boeriu,P Francavilla,M Guth,H Zhao,D M Starko,S Koperny,W W Przygoda,B Konya,K Liu,H Stenzel,M M 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Mansoulie,S Williams,Y Huang,S Solomon,T Mitani,N F Castro,B Eckerova,S Nasri,M Fanti,B A Bullard,J Levêque,C Nass,M Benoit,L Iconomidou-Fayard,T Barillari,S Rosati,R De Asmundis,X Ju,R A Rojas,P Teixeira-Dias,K L Chu,T G Zorbas,J T Offermann,R Camacho Toro,J Kvita,M J R Olsson,S Lammers,D E Fellers,I Vukotic,P H Beauchemin,I Kalaitzidou,C Escobar,Y K Kim,E Kourlitis,E Arena,V O’Shea,J P Thomas,T T Rinn,J-F Arguin,S Veneziano,M Cristoforetti,B R Mellado Garcia,T Poulsen,X Lou,D Varouchas,M Mikuž,P F Harrison,A Sciandra,M Bomben,O Zenin,Z Farazpay,N Nishu,L J Levinson,A Sansoni,J Urban,L Xu,S Todt,C Dimitriadi,F Balli,M Ouchrif,J B Liu,C Valderanis,R Longo,D South,M M Czurylo,E E Khoda,V H Ruelas Rivera,J Wollrath,L Klein,H Maguire,Y Wu,V V Kostyukhin,A S Drobac,Z H Citron,P H Hansen,P Postolache,Z Zhao,E Lytken,A Behera,P Bauer,P Sinervo,H A Smith,J Dingfelder,E Gorini,A Verbytskyi,V Gratchev,N B Atlay,J S Tafoya Vargas,M Vreeswijk,E F Mcdonald,S Wozniewski,Z Xu,E J Gallas,J Metcalfe,O 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doi:10.1140/epjc/s10052-023-12021-9

Abstract

A search for heavy right-handed Majorana or Dirac neutrinos NR\\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$N_{\ extrm{R}}$$\\end{document} and heavy right-handed gauge bosons WR\\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$W_{\ extrm{R}}$$\\end{document} is performed in events with energetic electrons or muons, with the same or opposite electric charge, and energetic jets. The search is carried out separately for topologies of clearly separated final-state products (“resolved” channel) and topologies with boosted final states with hadronic and/or leptonic products partially overlapping and reconstructed as a large-radius jet (“boosted” channel). The events are selected from pp collision data at the LHC with an integrated luminosity of 139 fb-1\\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$^{-1}$$\\end{document} collected by the ATLAS detector at s=13\\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$\\sqrt{s} = 13$$\\end{document} TeV. No significant deviations from the Standard Model predictions are observed. The results are interpreted within the theoretical framework of a left-right symmetric model, and lower limits are set on masses in the heavy right-handed WR\\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$W_{\ extrm{R}}$$\\end{document} boson and NR\\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$N_{\ extrm{R}}$$\\end{document} plane. The excluded region extends to about m(WR)=6.4\\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$m(W_{\ extrm{R}}) = 6.4$$\\end{document} TeV for both Majorana and Dirac NR\\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$N_{\ extrm{R}}$$\\end{document} neutrinos at m(NR)<1\\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$m(N_{\ extrm{R}})<1$$\\end{document} TeV. NR\\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$N_{\ extrm{R}}$$\\end{document} with masses of less than 3.5 (3.6) TeV are excluded in the electron (muon) channel at m(WR)=4.8\\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$m(W_{\ extrm{R}})=4.8$$\\end{document} TeV for the Majorana neutrinos, and limits of m(NR)\\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$m(N_{\ extrm{R}})$$\\end{document} up to 3.6 TeV for m(WR)=5.2\\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$m(W_{\ extrm{R}}) = 5.2$$\\end{document} (5.0) TeV in the electron (muon) channel are set for the Dirac neutrinos. These constitute the most stringent exclusion limits to date for the model considered.

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