Searches for pair production of third-generation squarks in [Formula: see text][Formula: see text] pp collisions.
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Akchurin, C Cowden, J Damgov, F De Guio, C Dragoiu, P R Dudero, J Faulkner, E Gurpinar, S Kunori, K Lamichhane, S W Lee, T Libeiro, T Peltola, S Undleeb, I Volobouev, Z Wang, S Greene, A Gurrola, R Janjam, W Johns, C Maguire, A Melo, H Ni, P Sheldon, S Tuo, J Velkovska, Q Xu, M W Arenton, P Barria, B Cox, J Goodell, R Hirosky, A Ledovskoy, H Li, C Neu, T Sinthuprasith, X Sun, Y Wang, E Wolfe, F Xia, C Clarke, R Harr, P E Karchin, J Sturdy, D A Belknap, J Buchanan, C Caillol, S Dasu, L Dodd, S Duric, B Gomber, M Grothe, M Herndon, A Hervé, P Klabbers, A Lanaro, A Levine, K Long, R Loveless, I Ojalvo, T Perry, G A Pierro, G Polese, T Ruggles, A Savin, N Smith, W H Smith, D Taylor, N Woods, CMS Collaboration
The European physical journal. C, Particles and fields（2017）
引用 34|浏览167
摘要
Searches are presented for direct production of top or bottom squark pairs in proton-proton collisions at the CERN LHC. Two searches, based on complementary techniques, are performed in all-jet final states that are characterized by a significant imbalance in transverse momentum. An additional search requires the presence of a charged lepton isolated from other activity in the event. The data were collected in 2015 at a centre-of-mass energy of 13[Formula: see text] with the CMS detector and correspond to an integrated luminosity of 2.3[Formula: see text]. No statistically significant excess of events is found beyond the expected contribution from standard model processes. Exclusion limits are set in the context of simplified models of top or bottom squark pair production. Models with top and bottom squark masses up to 830 and 890[Formula: see text], respectively, are probed for light neutralinos. For models with top squark masses of 675[Formula: see text], neutralino masses up to 260[Formula: see text] are excluded at 95% confidence level.
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