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Afik, Y.; Amoroso, S.; Armitage, L. J.; Backes, M.; Barnes, S. L.; Batista, S. J.; Benekos, N.; Berger, N.; Bisanz, T.; Boumediene, D.; Brost, E.; Cakir, O.; Cameron, D.; Cervelli, A.; Chen, Y.; Chow, Y. S.; Coadou, Y.; Cochran, J.; Conti, G.; David, C.; Deliot, F.; Dobre, M.; Doria, A.; Duarte-Campderros, J.; Dudarev, A.; Dumancic, M.; Galhardo, B.; Gallas, E. J.; Gallus, P.; Gaudio, G.; Gjelsten, B. K.; González de la Hoz, S.; Gutierrez, P.; Hauswald, L.; Havener, L. B.; Heim, T.; Hesketh, G. G.; Higón-Rodriguez, E.; Hostachy, J-Y.; Hristova, I.; Hu, S.; Istin, S.; Kahn, S. J.; Kajomovitz, E.; Kasahara, K.; Keyes, R. A.; Khramov, E.; Khubua, J.; Kitali, V.; Korcyl, K.; Kreutzfeldt, K.; Kroseberg, J.; Lapertosa, A.; Leite, M. A. L.; Lellouch, D.; Lerner, G.; Li, S.; Liu, H.; Loesle, A.; Love, J.; Lutz, M. S.; Madsen, A.; Maeda, J.; Maier, A. A.; Massa, L.; Maximov, D. A.; Merritt, F. S.; Nisati, A.; Pachal, K.; Palestini, S.; Panduro Vazquez, J. G.; Papadopoulou, Th. D.; Pater, J. R.; Petersen, B. A.; Picazio, A.; Polifka, R.; Prokoshin, F.; Quilty, D.; Reichert, J.; Robichaud-Veronneau, A.; Sacerdoti, S.; Saimpert, M.; Sampsonidou, D.; Sauvan, E.; Saxon, J.; Sekhon, K.; Shaikh, N. W.; Sherwood, P.; Silva, J.; Sulin, V. V.; Taylor, G. N.; Tsuno, S.; Unal, G.; Wang, C.; Wanotayaroj, C.; Wozniak, K. W.; Xu, D.; Yu, J.; Zacharis, G.; Zhang, L.
The journal of high energy physics, 11/2017, Volume: 2017, Issue: 11Journal Article
A bstract A search for the supersymmetric partners of the Standard Model bottom and top quarks is presented. The search uses 36.1 fb −1 of pp collision data at s = 13 TeV collected by the ATLAS experiment at the Large Hadron Collider. Direct production of pairs of bottom and top squarks ( b ¯ 1 and t ¯ 1 ) is searched for in final states with b -tagged jets and missing transverse momentum. Distinctive selections are defined with either no charged leptons (electrons or muons) in the final state, or one charged lepton. The zero-lepton selection targets models in which the b ¯ 1 is the lightest squark and decays via b ¯ 1 → b χ ¯ 1 0 , where χ ¯ 1 0 is the lightest neutralino. The one-lepton final state targets models where bottom or top squarks are produced and can decay into multiple channels, b ¯ 1 → b χ ¯ 1 0 and b ¯ 1 → t χ ¯ 1 ± , or t ¯ 1 → t χ ¯ 1 0 and t ¯ 1 → b χ ¯ 1 ± , where χ ¯ 1 ± is the lightest chargino and the mass difference m χ ¯ 1 ± − m χ ¯ 1 0 is set to 1 GeV. No excess above the expected Standard Model background is observed. Exclusion limits at 95% confidence level on the mass of third-generation squarks are derived in various supersymmetry-inspired simplified models.
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