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Alison, J; Amor Dos Santos, S P; Amoroso, S; Arabidze, G; Artz, S; Augsten, K; Balli, F; Beermann, T A; Bell, A S; Boerner, D; Calvet, T P; Capeans Garrido, M D M; Caron, S; Chelstowska, M A; Chen, H; Cheng, H C; Chiarella, V; Chizhov, M V; Ciftci, A K; Clark, B L; Dano Hoffmann, M; De Vivie De Regie, J B; Dell'Acqua, A; Derendarz, D; Deterre, C; Edson, W; Edwards, N C; El Kacimi, M; Fassnacht, P; Feng, C; Fiolhais, M C N; Flick, T; Garelli, N; Gatti, C; Geisler, M P; Giraud, P F; Giuliani, C; Giulini, M; Gorini, E; Goshaw, A T; Gratchev, V; Gross, E; Hamilton, A; Hartjes, F; Heim, S; Henriques Correia, A M; Johns, K A; Kanzaki, J; Kass, R D; Khubua, J; Kono, T; Krumnack, N; Kruse, M C; Kuechler, J T; Law, A T; Lazovich, T; Limosani, A; Lopez Mateos, D; Lorenzo Martinez, N; Lou, X; Lu, H; Lucotte, A; Lynn, D; Lytken, E; Lyubushkin, V; Makida, Y; Mallik, U; Malyukov, S; Manjarres Ramos, J; Marshall, Z; Martin Dit Latour, B; Massa, I; Mazza, S M; Mehta, A; Myska, M; Nikolic-Audit, I; Onyisi, P U E; Ouraou, A; Paredes Hernandez, D; Perini, L; Pilcher, J E; Poppleton, A; Quayle, W B; Rizvi, E; Schulz, H; Serin, L; Soffer, A; Soldevila, U; Soloshenko, A; Son, H; Styles, N A; Taiblum, N; Takeda, H; Tipton, P; Ughetto, M; Urrejola, P; Whalen, K; Wozniak, K W; Yang, H; Yuen, S P Y
The European physical journal. C, Particles and fields, 2016, Letnik: 76, Številka: 5Journal Article
A search for strongly produced supersymmetric particles is conducted using signatures involving multiple energetic jets and either two isolated leptons ( or Formula: see text) with the same electric charge or at least three isolated leptons. The search also utilises -tagged jets, missing transverse momentum and other observables to extend its sensitivity. The analysis uses a data sample of proton-proton collisions at Formula: see text TeV recorded with the ATLAS detector at the Large Hadron Collider in 2015 corresponding to a total integrated luminosity of 3.2 fbFormula: see text. No significant excess over the Standard Model expectation is observed. The results are interpreted in several simplified supersymmetric models and extend the exclusion limits from previous searches. In the context of exclusive production and simplified decay modes, gluino masses are excluded at Formula: see text confidence level up to 1.1-1.3 TeV for light neutralinos (depending on the decay channel), and bottom squark masses are also excluded up to 540 GeV. In the former scenarios, neutralino masses are also excluded up to 550-850 GeV for gluino masses around 1 TeV.
