Search for direct production of electroweakinos in final states with one lepton, jets and missing transverse momentum in pp collisions at s\\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$ \\sqrt{s} $$\\end{document} = 13 TeV with the ATLAS detector

M F Daneri,C Wang,M Weirich,S Ketabchi Haghighat,T Djobava,E Yu Soldatov,T Yamazaki,V Kartvelishvili,M Flores,M Wu,L Heinrich,M Dubovsky,L A O Laatu,C Klein,R B Garg,D Zhong,C Sbarra,N Korotkova,N Govender,W Vandelli,F Safai Tehrani,D Biswas,A Leisos,M K Kingston,Y F Han,H Ye,A S Kozhin,Z Wu,O Thielmann,K Becker,E M Riefel,X Ye,S Li,L L Ma,B Rottler,C Seitz,T Kuhl,W-M Yao,Y C Yap,O E Vickey Boeriu,L Cadamuro,A Klimentov,S Hirose,A Straessner,J P Thomas,S C Lee,A Ventura,X Ju,L Roos,E J Marshall,C David,R Coelho Lopes De Sa,I Brock,Y Abulaiti,G L Alberghi,D Whiteson,H-C Schultz-Coulon,V Franco Lima,M Citterio,N Krumnack,T Klioutchnikova,V S Bobrovnikov,S J Dittmeier,S M Shaw,J A M Guhit,I Turk Cakir,D Zerwas,A J Barr,S Bhatta,R Teixeira De Lima,M H Klein,L F Ehrke,C Marcon,Q Hu,F Meloni,O Toldaiev,L Franco,G Cesarini,L Zhang,K Ma,G Iakovidis,G Redlinger,M Mikestikova,T Wenaus,D R Van Arneman,I Fleck,K Hara,S Mehlhase,S El Farkh,Y Chou,E N Umaka,J Jejelava,J Blumenthal,A Ruggiero,Ph Schwemling,B Stugu,M Owen,S Shirabe,D Babal,J Harrison,P Skubic,J P Biswal,E Gramstad,L Xu,M Xie,M Dyndal,A M Cooper-Sarkar,J Stupak,S Gurbuz,B Gokturk,A N Tuna,B S Acharya,L Mao,P Steinberg,H Zhou,N Nishu,P Moskvitina,E Ramakoti,P Iengo,M A Postill,H Sandaker,S Rave,T Giani,P Strizenec,S V Peleganchuk,D M Starko,X Yang,M Furukawa,U Parzefall,S Tokár,A L Maslennikov,J E García Navarro,P A Erland,E Karentzos,W Dabrowski,K Zheng,R Ferrari,E L Woodward,S Atashi,C Meyer,F Winklmeier,A M Mendes Jacques Da Costa,F Pastore,T Herrmann,S Chekanov,F L Lucio Alves,M Gutsche,M Feng,L Varriale,A A Snesarev,L Wickremasinghe,W Y Song,Y Yu,A Sidoti,M M Schefer,M Romano,S Timoshenko,C Doglioni,M Khandoga,D Salvatore,F Bartels,S Ali,N D Simpson,S Rettie,E Bakos,D V Dedovich,R Iguchi,P Gadow,A Skaf,C Lacasta,J C Burzynski,S A Gotz,K Abeling,S Falciano,A Di Luca,G Alimonti,J Moss,D Calvet,R A Khan,S G Grewe,A Kamenshchikov,P J Falke,A Filipčič,M Calvetti,A Nayaz,V Gautam,D F Rassloff,F Parodi,S Yan,D Schaile,A E Barton,S Zambito,H Chen,E Lipeles,P Staroba,A Ezhilov,M Verissimo De Araujo,A J Bailey,K Hamano,E L Barberio,B Chen,G Panizzo,E Richter-Was,Z Wolffs,T M Pham,A Berthold,A De Salvo,A M Deiana,H Mildner,L Morvaj,J F Laporte,V Petousis,D Sperlich,J I Carlotto,S Tsuno,S Fuenzalida Garrido,M Hamer,W Wiedenmann,M Glisic,C Grefe,J Urban,M Pedersen,J M Silva,H Maguire,D Salamani,H Otono,A I Hagan,G Otero Y Garzon,V Croft,N Kakati,M Iodice,G Mokgatitswane,E Meoni,T Junkermann,R C W Henderson,T J Khoo,R M Bianchi,L Merola,P Jackson,R Tanaka,R P Mcgovern,Y Enari,J Huth,X Mapekula,J A Raine,D S Bhattacharya,D Tsybychev,K W Janas,A Zoccoli,F Anulli,J Lieber Marin,J Poveda,M Murin,T Geralis,S Sindhu,S Malyukov,A M Henriques Correia,P Seema,R Y González Andana,R Poettgen,S I Fernandez Luengo,A Badea,S Schramm,Y T Harris,B Eckerova,A B Lux,B H Hooberman,T H Park,C A Allendes Flores,S Burdin,H J Lubatti,T Maeno,M Sykora,T Saito,D Kobylianskii,A J Gomez Delegido,K Solovieva,H A Smith,L Pontecorvo,D Dal Santo,Y A Kurochkin,J Zinsser,O Kurdysh,D Duda,I Dawson,M Ait Tamlihat,D Varouchas,R Vari,T G Zorbas,R Ströhmer,M Capua,E Egidio Purcino De Souza,K Lohwasser,Ö O Öncel,M Hrabovsky,G Gustavino,D Rafanoharana,J Erdmann,M Lu,H A Pacey,E A Starchenko,P Sharma,G Introzzi,C S Jagfeld,S Stonjek,G A Bird,B Stelzer,M Martinez,R E Lindley,T Zhao,I Bloch,F Derue,G J Bobbink,R Müller,S M Wang,R Hertenberger,D Zanzi,D D Hofer,S Lu,L Feligioni,A Chen,M D’Onofrio,C G Zhu,D Paredes Hernandez,O Majersky,B A Roberts,E Celebi,M Villa,O Jinnouchi,M Robles Manzano,D L Noel,P Fleischmann,S W Alibocus,I R Boyko,E Antipov,J Von Ahnen,S Wozniewski,D Munoz Perez,J C Zeng,V Fadeyev,K Reeves,Y Ma,E Skorda,B C Pinheiro Pereira,G D Hallewell,D Giugni,J L Oliver,L B A H Hommels,I M Maniatis,M A Aparo,M W Krasny,M Noury,O Røhne,B J Gallop,A Rodriguez Rodriguez,S Passaggio,D Cameron,C G Lester,F Scuri,M Unal,S Hellman,J Niermann,A Onofre,J G R Guerrero Rojas,G H Eberwein,A Polini,L Fountas,C Santoni,R Gonçalo,A Di Domenico,M Vandenbroucke,A X Y Kong,K Kreul,L Adamczyk,D J Lewis,H Zhao,R W Gardner,C Da Via,C Tosciri,E M Lobodzinska,M Faucci Giannelli,A R Weidberg,L Rinaldi,L Iconomidou-Fayard,M Birman,N Kumari,O Stelzer-Chilton,I Mandić,M S Neubauer,M Verducci,J Manjarres Ramos,Y Hayashi,Y Zhao,M Morii,S Tapia Araya,A Ferrari,Y Rodriguez Garcia,K Krizka,E J Staats,A M Nairz,G Manco,J Heilman,A A Affolder,G A Mullier,N Ribaric,R J Langenberg,M Biglietti,V P Maleev,A Marantis,P Bagnaia,P Savard,S Pagan Griso,K Petukhova,C Varni,A Tsiamis,X Zheng,B P Kerridge,E Jones,C Alexa,B Kortman,K E Schleicher,S Aktas,C Merlassino,R A M Ferguson,A V Anisenkov,G E Orellana,C M Robles Gajardo,E Nurse,F Sopkova,N Bouchhar,Y Tu,S Lee,R Gonzalez Lopez,B Aitbenchikh,J F Allen,A Robson,P Kluit,C Weber,B Wendland,N Calace,O Karkout,A Negri,F I Winkel,M M Czurylo,A Andreazza,E R Vandewall,I Van Vulpen,H Atmani,F Costanza,N D Hehir,I Sykora,M Stolarski,S Cheong,V Latonova,P Dougan,F Schenck,T Heim,S Grancagnolo,S Harkusha,K Liu,E Banas,J A Frost,M Wakida,E Sauvan,J D Shinner,L Zwalinski,G Khoriauli,S Ezzarqtouni,K Peters,I Yeletskikh,S Francescato,H F-W Sadrozinski,R Brenner,P Ferrari,R A Rojas,M I Gostkin,H D N Nguyen,C Luci,T Flick,F Sili,P Tzanis,A Hoecker,A Laurier,F Hinterkeuser,L Pintucci,W D Heidorn,C W Ng,E Duchovni,J M Hays,A Ciocio,M Alhroob,V Senthilkumar,S Calvet,A Pacheco Pages,T M Hong,Y Fang,A Pirttikoski,M Hance,A Vgenopoulos,E Pianori,M Fanti,P Sinervo,L S Evans,C D Booth,R Astalos,M Naseri,R M Fakhrutdinov,S Tsigaridas,I Luise,J M Sonneveld,H P Beck,E Torrence,T Mkrtchyan,T Madula,S Y Andrean,M Ouchrif,S Alderweireldt,M Vanadia,H Simpson,T Mlinarevic,N P Rapheeha,A Canesse,M Cristinziani,A S Tee,A Lounis,F G Gravili,A C A Lee,G Glemža,J Pearkes,C J Wells,J M Wagner,D Godin,M Marinescu,A C Martyniuk,D J Sheppard,D Pyatiizbyantseva,J R Batley,J Haley,I Sayago Galvan,L Dell’Asta,M P Lewicki,T Poulsen,M R Sutton,D Ponomarenko,S Kersten,D Pietreanu,G L Albouy,H Pernegger,T Ekelof,O Perrin,A T Doyle,M Toscani,G F Tartarelli,G Azuelos,Y Benhammou,Y Takubo,A E Mcdougall,Y Ke,B M M Allbrooke,M Bhamjee,G Mchedlidze,A Mastroberardino,R Kopeliansky,P Urrejola,G Brooijmans,M T Dova,D Britzger,A Laudrain,I Lopez Paz,M O Evans,J Chudoba,Y Amaral Coutinho,J Montejo Berlingen,E Shabalina,K Li,F Malek,S H Abidi,J-E Nitschke,A Oh,A Lipniacka,J H Lindon,S Ahuja,K M Dona,A Baroncelli,S Mobius,K Karava,C Moreno Martinez,O Vujinovic,P Mastrandrea,A Bachiu,O Biebel,F Bernon,J S Keller,M Bindi,G Proto,M Penzin,T Ženiš,G A Vasquez,T Kawamoto,A M Wharton,F Z Lahbabi,J Nielsen,M A L Leite,R Staszewski,V Maksimovic,M Hirose,J Y Beaucamp,C Gutschow,M P Connell,A W Fortman,R Walker,K Assamagan,D Golubkov,K Beloborodov,J Zang,F Luehring,G Gomes Da Silva,N Brahimi,P D Thompson,M Trzebinski,Z Jia,G Merz,G Stoicea,A Lebedev,V S Lang,R Richter,P Sherwood,C Chauhan,A V Akimov,F Corriveau,J Zhu,K Kordas,R J Ward,V Cavaliere,Q Buat,K Terashi,T G Hitchings,Y Hasegawa,P Fiedler,B A Schumm,G Kramberger,M Vranjes Milosavljevic,A S Sharma,S Grinstein,S H Robertson,K Tsuri,E F Mcdonald,P Bechtle,O Kepka,G H A Viehhauser,A De Santo,F Fiedler,M Drnevich,D Cieri,G Löschcke Centeno,H Lien,B Ali,X Ai,D Timoshyn,J Hofer,A Sbrizzi,M Kumar,S Sharma,I Kalaitzidou,X Shi,H Lyons,S Keshri,K Nagano,M B Rendel,M Begel,M Y Liu,Y Nakahama,M Garcia-Sciveres,B Gocke,A Sopczak,R Hyneman,V Smakhtin,C J Potter,R Hankache,P A Love,Z Hubacek,M L Ojeda,M J V Fernoux,E Rossi,J Steentoft,M A Draguet,P Berta,C Wu,H Wang,B Stapf,G Aad,A Sfyrla,M Aly,D Benchekroun,J Weingarten,A Strubig,B Liberti,V Ellajosyula,H Bachacou,E Valdes Santurio,I A Ramirez-Berend,M Wittgen,P Jones,M E Hesping,M Rotaru,C A Hugli,A Juste Rozas,M Perganti,R Leitner,M Leblanc,C A Gottardo,J Tojo,S Caron,E X L Ting,L Martinelli,M Gouighri,M Donadelli,Y Hernández Jiménez,Q Liu,M Elsing,M Huebner,W Wagner,M S Weber,A G Goussiou,S A Cetin,M Drozdova,P H Hansen,V D’Amico,M J Shroff,Y Qin,D Ta,T Ingebretsen Carlson,Dj Sijacki,W J Murray,A Coccaro,J G Saraiva,M G Vincter,P Kramer,S Maltezos,C Bernius,G L Gardner,M Mineev,S M Gibson,A D Auriol,H A Day-Hall,R W L Jones,J O Rieger,A Stabile,A D Pilkington,S V Addepalli,T Strebler,M Fujimoto,F Lasagni Manghi,R Schwienhorst,S Yu Smirnov,J Dopke,P M Gravila,S Kuleshov,O Sasaki,S Nasri,T Masubuchi,J M Keaveney,V Tsulaia,B Vormwald,D P Mungo,C D Burton,M P Kawale,B P Jaeger,J Dingfelder,J Mueller,L Ferencz,A Cervelli,K Smolek,S Auricchio,L N Smirnova,C Gay,A G Myagkov,S Giagu,V Polychronakos,A E Pinto Pinoargote,S L Lloyd,J Wollrath,M V Silva Oliveira,V F Kazanin,U Schäfer,J M Gargan,S Darmora,M Antonelli,Y Mitsumori,A Palazzo,P Y Nechaeva,J R Dandoy,E Dreyer,T Barklow,L F Gutierrez Zagazeta,B K Wosiek,T Andeen,A Tanaka,P Van Gemmeren,P Federic,J A Sandesara,A Mitra,G Unal,B K Yeo,D Sampsonidou,X Xie,M Schumacher,F Renner,T Min,N E K Gillwald,Y Smirnov,D Bakshi Gupta,A K Morley,O A Ducu,A F Wongel,T Lenz,J-P Meyer,A M Sickles,A Leopold,M Smizanska,D Kar,B Ngair,N F Castro,P Johansson,M Sahinsoy,D M Mac Donell,H Ma,S A Olivares Pino,T F Lee,N Proklova,N S Wenke,M Mali,D Derendarz,V Nikolaenko,E Petit,N Ilic,J D Hansen,G Chiarelli,D Liu,C A Garner,L Novotny,S Cabrera Urbán,S Jézéquel,R Nisius,B M Wynne,A J Lankford,S J Hillier,F Crescioli,L F Oleiro Seabra,B R Mellado Garcia,A Cerri,D G Charlton,S Nemecek,H J Stelzer,A Giannini,R Mazini,C Heidegger,M Belfkir,E M Carlson,E M Shrif,S Batlamous,M Muškinja,M-S Barisits,F Lanni,Y Tian,R J Atkin,W Walkowiak,H Asada,N Soybelman,L Helary,C Grieco,J Pan,X Jia,J E Brau,T M Baer,J Wuerzinger,X Wu,G R Gledhill,C Arcangeletti,E Mazzeo,F Braren,E I Conroy,J G Reyes Rivera,R K Irwin,M Standke,R Camacho Toro,V Kukhtin,D M Gingrich,T Wengler,V H Ruelas Rivera,P C Machado De Abreu Farias,R Lysak,S Hou,K Prokofiev,N M Tamir,R F Coelho Barrue,E Zaid,B S Dziedzic,P Tas,H M Borecka-Bielska,E Fortin,E Cheremushkina,P Czodrowski,M Lokajicek,S Kortner,H El Jarrari,Z M A Rozario,F Giuli,S Ozturk,F Celli,A C Forti,D Cremonini,X Su,A Dudarev,P Calfayan,V Castillo Gimenez,J A Valls Ferrer,F Schroeder,Z Zheng,Z Rurikova,A J Schuy,T Vickey,A Bruni,H Lacker,H Zeng,P Giannetti,J B Hansen,K Bouaouda,O Kuchinskaia,N A Asbah,D Scheirich,K Ntekas,L E Bruce,A Blue,W A Leight,D T Zenger,T Komarek,J S Tafoya Vargas,D Lynn,M Mosidze,L Manhaes De Andrade Filho,S Tarem,G Frattari,R Novotny,Y Cai,G Myers,K A Saoucha,F Gonnella,H Santos,S Stärz,B H Hodkinson,B Zhou,C Clement,V Vorobel,M J Kareem,W H Kostecka,A Kotsokechagia,D M Rebuzzi,X Ruan,A Kilgallon,L Xia,H T Yang,D Bortoletto,M Dunford,D Du,K Lie,M Klein,S Ventura Gonzalez,F Piazza,M Danninger,P Bauer,B Le,T Harenberg,K Cheung,T Barillari,J R Pater,K E Penski,D Robinson,T Li,V A Bednyakov,L M Mir,Y Zhang,J C Voigt,A Vishwakarma,C M Garvey,A Visibile,M F Watson,L J Levinson,U Klein,W Ma,D Gillberg,M Wielers,R Bouquet,R Tafirout,J Elmsheuser,M Feickert,D T Gil,T Kharlamova,M Lefebvre,S Tapprogge,S Yu Sivoklokov,D W Kim,N Schmitt,C Agheorghiesei,A A Grillo,A S White,D Hayden,S Singh,H Hibi,S Williams,L Vannoli,H D Pandya,A Gorišek,S Kaur,K Tackmann,B M Waugh,W Alkakhi,C Diaconu,J B Beacham,H H Williams,J Terron,A D Gentry,J Hobbs,M Ziolkowski,E J W Moyse,K Lantzsch,O Meshkov,J Albert,W Buttinger,J Assahsah,V Raskina,R De Asmundis,D Buchin,I A Minashvili,D A Baron Moreno,H Herde,K Köneke,M Z Barel,R Narayan,P Federicova,H L Joos,J Guo,V Sanchez Sebastian,M Testa,J L Gonski,T Koffas,J Mamuzic,M Marjanovic,C Gubbels,S Koperny,B J Wilson,J M Izen,J Schmeing,T B Huffman,M Lassnig,B Vachon,J Carmignani,A Aikot,E A Pender,S Schlenker,V Canale,P U E Onyisi,B R Roberts,P Baron,A Alvarez Fernandez,G Borissov,M Holzbock,D F Zhang,V Lyubushkin,G Chiodini,A Gomes,P S Miyagawa,S Angelidakis,G Ninio,M Gignac,D A Hangal,C Clarry,F Siegert,M Bauce,G Brandt,O Cakir,B Schlag,L Beresford,N Chiedde,K W Woźniak,G R Gonzalvo Rodriguez,M Escalier,M Amerl,Z Zhang,P Kontaxakis,O Lukianchuk,V Büscher,L Guan,M Dam,N Berger,B Mondal,N Konstantinidis,N M Harrison,D A Ciubotaru,N A Rusakovich,B Pascual Dias,D Sengupta,I M Gregor,W K Brooks,F Ould-Saada,P Schacht,P Postolache,M Bosman,A Angerami,M Guth,B M Cote,M Van Rijnbach,S Barsov,J Roloff,R Pedro,M E Geyik,J K Behr,R F Y Peters,V Boisvert,S Asai,L Guo,T Beau,K S Krowpman,M Saimpert,C Sandoval,Y Fu,B P Nachman,G Mikenberg,S M Mazza,T Fitschen,T Iizawa,A Farbin,F Guo,J J Chwastowski,E A Thompson,F L Castillo,I Drivas-Koulouris,W Y Chan,V M M Cairo,A Kirchhoff,J Schovancova,J Kretzschmar,E Yamashita,P Camarri,S Van Stroud,I Siral,A J Beddall,A Tsirigotis,F Beisiegel,G Jain,F Conventi,J Neundorf,A Chitan,E Kajomovitz,K A Johns,M Marcisovsky,L Cerrito,T Aoki,M Ghani,W Kozanecki,J Novak,A A Talyshev,G Duckeck,A Bassalat,M A Schmidt,A Jinaru,J A Zamora Saa,P Riedler,Y C Cekmecelioglu,S Majewski,F Guescini,C A Solans Sanchez,M Sessa,H Y Meng,L Tompkins,J-F Arguin,L Serkin,C Escobar,E Pasqualucci,E Bergeaas Kuutmann,W Zou,Y Coadou,L Živković,A J Mullin,M Franchini,S Jin,J 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doi:10.1007/jhep12(2023)167

Abstract

Searches for electroweak production of wino-like chargino pairs, χ~1+χ~1−\\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$ {\\overset{\\sim }{\\chi}}_1^{+}{\\overset{\\sim }{\\chi}}_1^{-} $$\\end{document}, and of wino-like chargino and next-to-lightest neutralino, χ~1±χ~20\\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$ {\\overset{\\sim }{\\chi}}_1^{\\pm }{\\overset{\\sim }{\\chi}}_2^0 $$\\end{document}, are presented. The models explored assume that the charginos decay into a W boson and the lightest neutralino, χ~1±→W±χ~10\\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$ {\\overset{\\sim }{\\chi}}_1^{\\pm}\ o {W}^{\\pm }{\\overset{\\sim }{\\chi}}_1^0 $$\\end{document}. The next-to-lightest neutralinos are degenerate in mass with the chargino and decay to χ~10\\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$ {\\overset{\\sim }{\\chi}}_1^0 $$\\end{document} and either a Z or a Higgs boson, χ~20→Zχ~10\\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$ {\\overset{\\sim }{\\chi}}_2^0\ o Z{\\overset{\\sim }{\\chi}}_1^0 $$\\end{document} or hχ~10\\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$ h{\\overset{\\sim }{\\chi}}_1^0 $$\\end{document}. The searches exploit the presence of a single isolated lepton and missing transverse momentum from the W boson decay products and the lightest neutralinos, and the presence of jets from hadronically decaying Z or W bosons or from the Higgs boson decaying into a pair of b-quarks. The searches use 139 fb−1 of s\\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$ \\sqrt{s} $$\\end{document} = 13 TeV proton-proton collisions data collected by the ATLAS detector at the Large Hadron Collider between 2015 and 2018. No deviations from the Standard Model expectations are found, and 95% confidence level exclusion limits are set. Chargino masses ranging from 260 to 520 GeV are excluded for a massless χ~10\\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$ {\\overset{\\sim }{\\chi}}_1^0 $$\\end{document} in chargino pair production models. Degenerate chargino and next-to-lightest neutralino masses ranging from 260 to 420 GeV are excluded for a massless χ~10\\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$ {\\overset{\\sim }{\\chi}}_1^0 $$\\end{document} for χ~20→Zχ~10\\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$ {\\overset{\\sim }{\\chi}}_2^0\ o Z{\\overset{\\sim }{\\chi}}_1^0 $$\\end{document}. For decays through an on-shell Higgs boson and for mass-splitting between χ~1±/χ~20\\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$ {\\overset{\\sim }{\\chi}}_1^{\\pm }/{\\overset{\\sim }{\\chi}}_2^0 $$\\end{document} and χ~10\\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$ {\\overset{\\sim }{\\chi}}_1^0 $$\\end{document} as small as the Higgs boson mass, mass limits are improved by up to 40 GeV in the range of 200–260 GeV and 280–470 GeV compared to previous ATLAS constraints.

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