{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.79165.v2","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1620694"}},{"@id":"https://doi.org/10.1007/JHEP11(2017)195","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2018","description":"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 $\\sqrt{s}=13$ TeV collected by the ATLAS experiment at the Large Hadron Collider. Direct production of pairs of bottom and top squarks ($\\tilde{b}_{1}$ and $\\tilde{t}_{1}$) 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 $\\tilde{b}_{1}$ is the lightest squark and decays via $\\tilde{b}_{1} \\rightarrow b \\tilde{\\chi}^{0}_{1}$, where $\\tilde{\\chi}^{0}_{1}$ is the lightest neutralino. The one-lepton final state targets models where bottom or top squarks are produced and can decay into multiple channels, $\\tilde{b}_{1} \\rightarrow b \\tilde{\\chi}^{0}_{1}$ and $\\tilde{b}_{1} \\rightarrow t \\tilde{\\chi}^{\\pm}_{1}$, or $\\tilde{t}_{1} \\rightarrow t \\tilde{\\chi}^{0}_{1}$ and $\\tilde{t}_{1} \\rightarrow b \\tilde{\\chi}^{\\pm}_{1}$, where $\\tilde{\\chi}^{\\pm}_{1}$ is the lightest chargino and the mass difference $m_{\\tilde{\\chi}^{\\pm}_{1}}- m_{\\tilde{\\chi}^{0}_{1}}$ 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.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.79165.v2/t1","@type":"Dataset","description":"- - - - - - - - - - - - - - - - - - - -...","name":"Overview"},{"@id":"https://doi.org/10.17182/hepdata.79165.v2/t2","@type":"Dataset","description":"Signal acceptance (in %) in the ( M(SBOTTOM), M(NEUTRALINO) ) mass plane for the symmetric decay of the sbottom into...","name":"Acceptance 1"},{"@id":"https://doi.org/10.17182/hepdata.79165.v2/t3","@type":"Dataset","description":"Signal acceptance (in %) in the ( M(SBOTTOM), M(NEUTRALINO) ) mass plane for the symmetric decay of the sbottom into...","name":"Acceptance 2"},{"@id":"https://doi.org/10.17182/hepdata.79165.v2/t4","@type":"Dataset","description":"Signal acceptance (in %) in the ( M(SBOTTOM), M(NEUTRALINO) ) mass plane for the symmetric decay of the sbottom into...","name":"Acceptance 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