Search for production of four top quarks in final states with same-sign or multiple leptons in proton–proton collisions at √s=13TeV

dc.contributor.author Sirunyan, A. M.
dc.contributor.author Tumasyan, A.
dc.contributor.author Adam, W.
dc.contributor.author Ambrogi, F.
dc.contributor.author Bergauer, T.
dc.contributor.author Brandstetter, J.
dc.contributor.author Dragicevic, M.
dc.contributor.author Erö, J.
dc.contributor.author Del Valle, A. Escalante
dc.contributor.author Flechl, M.
dc.contributor.author Frühwirth, R.
dc.contributor.author Jeitler, M.
dc.contributor.author Krammer, N.
dc.contributor.author Krätschmer, I.
dc.contributor.author Liko, D.
dc.contributor.author Madlener, T.
dc.contributor.author Mikulec, I.
dc.contributor.author Rad, N.
dc.contributor.author Schieck, J.
dc.contributor.author Schöfbeck, R.
dc.contributor.author Spanring, M.
dc.contributor.author Spitzbart, D.
dc.contributor.author Waltenberger, W.
dc.contributor.author Wulz, C. E.
dc.contributor.author Zarucki, M.
dc.contributor.author Drugakov, V.
dc.contributor.author Mossolov, V.
dc.contributor.author Suarez Gonzalez, J.
dc.contributor.author Darwish, M. R.
dc.contributor.author De Wolf, E. A.
dc.contributor.author Di Croce, D.
dc.contributor.author Janssen, X.
dc.contributor.author Lelek, A.
dc.contributor.author Pieters, M.
dc.contributor.author Sfar, H. Rejeb
dc.contributor.author Van Haevermaet, H.
dc.contributor.author Van Mechelen, P.
dc.contributor.author Van Putte, S.
dc.contributor.author Van Remortel, N.
dc.contributor.author Blekman, F.
dc.contributor.author Bols, E. S.
dc.contributor.author Chhibra, S. S.
dc.contributor.author D’Hondt, J.
dc.contributor.author De Clercq, J.
dc.contributor.author Lontkovskyi, D.
dc.contributor.author Lowette, S.
dc.contributor.author Marchesini, I.
dc.contributor.author Moortgat, S.
dc.contributor.author Python, Q.
dc.contributor.author Skovpen, K.
dc.contributor.author Tavernier, S.
dc.contributor.author Van Doninck, W.
dc.contributor.author Van Mulders, P.
dc.contributor.author Beghin, D.
dc.contributor.author Bilin, B.
dc.contributor.author Brun, H.
dc.contributor.author Clerbaux, B.
dc.contributor.author De Lentdecker, G.
dc.contributor.author Delannoy, H.
dc.contributor.author Dorney, B.
dc.contributor.author Favart, L.
dc.contributor.author Grebenyuk, A.
dc.contributor.author Kalsi, A. K.
dc.contributor.author Popov, A.
dc.contributor.author Postiau, N.
dc.contributor.author Starling, E.
dc.contributor.author Thomas, L.
dc.contributor.author Velde, C. Vander
dc.contributor.author Vanlaer, P.
dc.contributor.author Vannerom, D.
dc.contributor.author Cornelis, T.
dc.contributor.author Dobur, D.
dc.contributor.author Khvastunov, I.
dc.contributor.author Niedziela, M.
dc.contributor.author Roskas, C.
dc.contributor.author Trocino, D.
dc.contributor.author Tytgat, M.
dc.contributor.author Verbeke, W.
dc.contributor.author Vermassen, B.
dc.contributor.author Vit, M.
dc.contributor.author Zaganidis, N.
dc.contributor.author Bondu, O.
dc.contributor.author Bruno, G.
dc.contributor.author Caputo, C.
dc.contributor.author David, P.
dc.contributor.author Delaere, C.
dc.contributor.author Delcourt, M.
dc.contributor.author Giammanco, A.
dc.contributor.author Lemaitre, V.
dc.contributor.author Magitteri, A.
dc.contributor.author Prisciandaro, J.
dc.contributor.author Saggio, A.
dc.contributor.author Marono, M. Vidal
dc.contributor.author Vischia, P.
dc.contributor.author Zobec, J.
dc.contributor.author Alves, F. L.
dc.contributor.author Alves, G. A.
dc.contributor.author Silva, G. Correia
dc.contributor.author Hensel, C.
dc.contributor.author Moraes, A.
dc.date.accessioned 2022-03-27T06:46:00Z
dc.date.available 2022-03-27T06:46:00Z
dc.date.issued 2020-02-01
dc.description.abstract The standard model (SM) production of four top quarks (t t ¯ t t ¯) in proton–proton collisions is studied by the CMS Collaboration. The data sample, collected during the 2016–2018 data taking of the LHC, corresponds to an integrated luminosity of 137fb-1 at a center-of-mass energy of 13TeV. The events are required to contain two same-sign charged leptons (electrons or muons) or at least three leptons, and jets. The observed and expected significances for the t t ¯ t t ¯ signal are respectively 2.6 and 2.7 standard deviations, and the t t ¯ t t ¯ cross section is measured to be 12.6-5.2+5.8fb. The results are used to constrain the Yukawa coupling of the top quark to the Higgs boson, yt, yielding a limit of |yt/ytSM| < 1.7 at 95 % confidence level, where ytSM is the SM value of yt. They are also used to constrain the oblique parameter of the Higgs boson in an effective field theory framework, H^ < 0.12. Limits are set on the production of a heavy scalar or pseudoscalar boson in Type-II two-Higgs-doublet and simplified dark matter models, with exclusion limits reaching 350–470GeV and 350–550GeV for scalar and pseudoscalar bosons, respectively. Upper bounds are also set on couplings of the top quark to new light particles.
dc.identifier.citation European Physical Journal C. v.80(2)
dc.identifier.issn 14346044
dc.identifier.uri 10.1140/epjc/s10052-019-7593-7
dc.identifier.uri http://link.springer.com/10.1140/epjc/s10052-019-7593-7
dc.identifier.uri https://dspace.uohyd.ac.in/handle/1/10111
dc.title Search for production of four top quarks in final states with same-sign or multiple leptons in proton–proton collisions at √s=13TeV
dc.type Journal. Article
dspace.entity.type
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