Search for supersymmetry in events with b-tagged jets and missing transverse momentum in pp collisions at √s=13 TeV with the ATLAS detector M. Aaboud, G. Aad, B. Abbott [et al.]
Material type: ArticleSubject(s): ATLAS, детектор | Большой адронный коллайдер | протон-протонные столкновения | суперсимметрияGenre/Form: статьи в журналах Online resources: Click here to access online In: Journal of high energy physics № 11. P. 195 (1-49)Abstract: 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→bχ¯01 , where χ¯01 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→bχ¯01 and b¯1→tχ¯±1 , or t¯1→tχ¯01 and t¯1→bχ¯±1 , where χ¯±1 is the lightest chargino and the mass difference mχ¯±1−mχ¯01 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.Библиогр.: 88 назв.
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→bχ¯01 , where χ¯01 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→bχ¯01 and b¯1→tχ¯±1 , or t¯1→tχ¯01 and t¯1→bχ¯±1 , where χ¯±1 is the lightest chargino and the mass difference mχ¯±1−mχ¯01 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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