Results are presented from a search for the pair-production of heavy quarks, Q (A) over bar, that decay exclusively into a top quark and a W or Z boson. The search is performed using a sample of proton-proton collisions at root s = 7TeV corresponding to an integrated luminosity of 5.0 fb(-1), collected by the Compact Muon Solenoid experiment. The signal region is defined using a sample of events containing one electron or muon, missing transverse momentum, and at least four jets with large transverse momenta, where one jet is likely to originate from the decay of a bottom quark. No significant excess of events is observed with respect to the standard model expectations. Assuming a strong pair-production mechanism, quark masses below 675 (625) GeV decaying into tW (tZ) are excluded at the 95% confidence level.
Search for heavy quarks decaying into a top quark and a W or Z boson using lepton plus jets events in pp collisions at root s=7 TeV / Chatrchyan, S; Khachatryan, V; Sirunyan, Am; Tumasyan, A; Adam, W; Aguilo, E; Bergauer, T; Dragicevic, M; Ero, J; Fabjan, C; Friedl, M; Fruhwirth, R; Ghete, Vm; Hammer, J; Hormann, N; Hrubec, J; Jeitler, M; Kiesenhofer, W; Knunz, V; Krammer, M; Kratschmer, I; Liko, D; Mikulec, I; Pernicka, M; Rahbaran, B; Rohringer, C; Rohringer, H; Schofbeck, R; Strauss, J; Taurok, A; Waltenberger, W; Walzel, G; Widl, E; Wulz, Ce; Mossolov, V; Shumeiko, N; Gonzalez, Js; Bansal, M; Bansal, S; Cornelis, T; De Wolf, Ea; Janssen, X; Luyckx, S; Mucibello, L; Ochesanu, S; Roland, B; Rougny, R; Selvaggi, M; Staykova, Z; Van Haevermaet, H; Van Mechelen, P; Van Remortel, N; Van Spilbeeck, A; Blekman, F; Blyweert, S; D'Hondt, J; Suarez, Rg; Kalogeropoulos, A; Maes, M; Olbrechts, A; Van Doninck, W; Van Mulders, P; Van Onsem, Gp; Villella, I; Clerbaux, B; De Lentdecker, G; Dero, V; 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[10.1007/JHEP01(2013)154]
Search for heavy quarks decaying into a top quark and a W or Z boson using lepton plus jets events in pp collisions at root s=7 TeV
Chatrchyan S; Khachatryan V; Sirunyan AM; Tumasyan A; Adam W; Aguilo E; Bergauer T; Dragicevic M; Ero J; Fabjan C; Friedl M; Fruhwirth R; Ghete VM; Hammer J; Hormann N; Hrubec J; Jeitler M; Kiesenhofer W; Knunz V; Krammer M; Kratschmer I; Liko D; Mikulec I; Pernicka M; Rahbaran B; Rohringer C; Rohringer H; Schofbeck R; Strauss J; Taurok A; Waltenberger W; Walzel G; Widl E; Wulz CE; Mossolov V; Shumeiko N; Gonzalez JS; Bansal M; Bansal S; Cornelis T; De Wolf EA; Janssen X; Luyckx S; Mucibello L; Ochesanu S; Roland B; Rougny R; Selvaggi M; Staykova Z; Van Haevermaet H; Van Mechelen P; Van Remortel N; Van Spilbeeck A; Blekman F; Blyweert S; D'Hondt J; Suarez RG; Kalogeropoulos A; Maes M; Olbrechts A; Van Doninck W; Van Mulders P; Van Onsem GP; Villella I; Clerbaux B; De Lentdecker G; Dero V; Gay APR; Hreus T; Leonard A; Marage PE; Mohammadi A; Reis T; Thomas L; Vander Marcken G; Vander Velde C; Vanlaer P; Wang J; Adler V; Beernaert K; Cimmino A; Costantini S; Garcia G; Grunewald M; Klein B; Lellouch J; Marinov A; Mccartin J; Rios AAO; Ryckbosch D; Strobbe N; Thyssen F; Tytgat M; Verwilligen P; Walsh S; Yazgan E; Zaganidis N; Basegmez S; Bruno G; Castello R; Ceard L; Delaere C; du Pree T; Favart D; Forthomme L; Giammanco A; Hollar J; Lemaitre V; Liao J; Militaru O; Nuttens C; Pagano D; Pin A; Piotrzkowski K; Schul N; Garcia JMV; Beliy N; Caebergs T; Daubie E; Hammad GH; Alves GA; Martins MC; Martins T; Pol ME; Souza MHG; Alda WL; Carvalho W; Custodio A; Da Costa EM; Damiao DD; Martins CD; De Souza SF; Figueiredo DM; Mundim L; Nogima H; Oguri V; Da Silva WLP; Santoro A; Jorge LS; Sznajder A; Anjos TS; Bernardes CA; Dias FA; Tomei TRFP; Gregores EM; Lagana C; Marinho F; Mercadante PC; Novaes SF; Padula SS; Genchev V; Iaydjiev P; Piperov S; Rodozov M; Stoykova S; Sultanov G; Tcholakov V; Trayanov R; Vutova M; Dimitrov A; Hadjiiska R; Kozhuharov V; Litov L; Pavlov B; Petkov P; Bian JG; Chen GM; Chen HS; Jiang CH; Liang D; Liang S; Meng X; Tao J; Wang J; Wang X; Wang Z; Xiao H; Xu M; Zang J; Zhang Z; Asawatangtrakuldee C; Ban Y; Guo Y; Li W; Liu S; Mao Y; Qian SJ; Teng H; Wang D; Zhang L; Zou W; Avila C; Gomez JP; Moreno BG; Oliveros AFO; Sanabria JC; Godinovic N; Lelas D; Plestina R; Polic D; Puljak I; Antunovic Z; Kovac M; Brigljevic V; Duric S; Kadija K; Luetic J; Morovic S; Attikis A; Galanti M; Mavromanolakis G; Mousa J; Nicolaou C; Ptochos F; Razis PA; Finger M; Finger M; Assran Y; Elgamma S; Kamel AE; Mahmoud MA; Radi A; Kadastik M; Muntel M; Raidal M; Rebane L; Tiko A; Eerola P; Fedi G; Voutilainen M; Harkonen J; Heikkinen A; Karimaki V; Kinnunen R; Kortelainen MJ; Lampen T; Lassila Perini K; Lehti S; Linden T; Luukka P; Maenpaa T; Peltola T; Tuominen E; Tuominiemi J; Tuovinen E; Ungaro D; Wendland L; Banzuzi K; Karjalainen A; Korpela A; Tuuva T; Besancon M; Choudhury S; Dejardin M; Denegri D; Fabbro B; Faure JL; Ferri F; Ganjour S; Givernaud A; Gras P; de Monchenault GH; Jarry P; Locci E; Malcles J; Millischer L; Nayak A; Rander J; Rosowsky A; Shreyber I; 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Klabbers P; Klukas J; Lanaro A; Lazaridis C; Leonard J; Loveless R; Mohapatra A; Ojalvo I; Palmonari F; Pierro GA; Ross I; Savin A; Smith WH; Swanson J.
2013-01-01
Abstract
Results are presented from a search for the pair-production of heavy quarks, Q (A) over bar, that decay exclusively into a top quark and a W or Z boson. The search is performed using a sample of proton-proton collisions at root s = 7TeV corresponding to an integrated luminosity of 5.0 fb(-1), collected by the Compact Muon Solenoid experiment. The signal region is defined using a sample of events containing one electron or muon, missing transverse momentum, and at least four jets with large transverse momenta, where one jet is likely to originate from the decay of a bottom quark. No significant excess of events is observed with respect to the standard model expectations. Assuming a strong pair-production mechanism, quark masses below 675 (625) GeV decaying into tW (tZ) are excluded at the 95% confidence level.
Citazione
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[10.1007/JHEP01(2013)154]
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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.
