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 (¯b1 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 ¯b1 is the lightest squark and decays via ¯b1 → bχ¯01, where ¯χ01 is the lightest neutralino. The one-lepton final state targets models where bottom or top squarks are produced and can decay into multiple channels, ¯b1 → bχ¯01 and ¯b1 → tχ¯± 1, or t¯1 → tχ¯01 and t¯1 → bχ¯± 1, where ¯χ ± 1 is the lightest chargino and the mass difference m χ¯± 1 − mχ¯ 0 1 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.
Search for supersymmetry in events with b-tagged jets and missing transverse momentum in pp collisions at root s=13 TeV with the ATLAS detector
Bruscino NMembro del Collaboration Group
;Spanò FMembro del Collaboration Group
;
2017-01-01
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 (¯b1 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 ¯b1 is the lightest squark and decays via ¯b1 → bχ¯01, where ¯χ01 is the lightest neutralino. The one-lepton final state targets models where bottom or top squarks are produced and can decay into multiple channels, ¯b1 → bχ¯01 and ¯b1 → tχ¯± 1, or t¯1 → tχ¯01 and t¯1 → bχ¯± 1, where ¯χ ± 1 is the lightest chargino and the mass difference m χ¯± 1 − mχ¯ 0 1 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.| File | Dimensione | Formato | |
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JHEP11(2017)195.pdf
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