{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.84426.v2","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1688943"}},{"@id":"https://doi.org/10.1103/PhysRevD.99.012009","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2018","description":"A search for supersymmetry in events with large missing transverse momentum, jets, and at least one hadronically decaying $\\tau$-lepton is presented. Two exclusive final states with either exactly one or at least two $\\tau$-leptons are considered. The analysis is based on proton-proton collisions at $\\sqrt{s}$ = 13 TeV corresponding to an integrated luminosity of 36.1 fb$^{-1}$ delivered by the Large Hadron Collider and recorded by the ATLAS detector in 2015 and 2016. No significant excess is observed over the Standard Model expectation. At 95% confidence level, model-independent upper limits on the cross section are set and exclusion limits are provided for two signal scenarios: a simplified model of gluino pair production with $\\tau$-rich cascade decays, and a model with gauge-mediated supersymmetry breaking (GMSB). In the simplified model, gluino masses up to 2000 GeV are excluded for low values of the mass of the lightest supersymmetric particle (LSP), while LSP masses up to 1000 GeV are excluded for gluino masses around 1400 GeV. In the GMSB model, values of the supersymmetry-breaking scale are excluded below 110 TeV for all values of $\\tan\\beta$ in the range $2 \\leq \\tan\\beta \\leq 60$, and below 120 TeV for $\\tan\\beta>30$.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.84426.v2/t1","@type":"Dataset","description":"1$\\tau$ Compressed SR eff.","name":"Efficiency 1"},{"@id":"https://doi.org/10.17182/hepdata.84426.v2/t2","@type":"Dataset","description":"1$\\tau$ MediumMass SR eff.","name":"Efficiency 2"},{"@id":"https://doi.org/10.17182/hepdata.84426.v2/t3","@type":"Dataset","description":"2$\\tau$ Compressed SR eff.","name":"Efficiency 3"},{"@id":"https://doi.org/10.17182/hepdata.84426.v2/t4","@type":"Dataset","description":"2$\\tau$ HighMass SR eff.","name":"Efficiency 4"},{"@id":"https://doi.org/10.17182/hepdata.84426.v2/t5","@type":"Dataset","description":"2$\\tau$ multibin SR eff.","name":"Efficiency 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acceptance.","name":"Acceptance 7"},{"@id":"https://doi.org/10.17182/hepdata.84426.v2/t20","@type":"Dataset","description":"1$\\tau$ MediumMass SR acceptance.","name":"Acceptance 8"},{"@id":"https://doi.org/10.17182/hepdata.84426.v2/t21","@type":"Dataset","description":"2$\\tau$ Compressed SR acceptance.","name":"Acceptance 9"},{"@id":"https://doi.org/10.17182/hepdata.84426.v2/t22","@type":"Dataset","description":"2$\\tau$ HighMass SR acceptance.","name":"Acceptance 10"},{"@id":"https://doi.org/10.17182/hepdata.84426.v2/t23","@type":"Dataset","description":"2$\\tau$ multibin SR acceptance.","name":"Acceptance 11"},{"@id":"https://doi.org/10.17182/hepdata.84426.v2/t24","@type":"Dataset","description":"2$\\tau$ GMSB SR acceptance.","name":"Acceptance 12"},{"@id":"https://doi.org/10.17182/hepdata.84426.v2/t25","@type":"Dataset","description":"Cutflow table of the $1\\tau$ compressed SR for the four signal benchmark scenarios of low, medium, and high mass-splitting in...","name":"Cutflow 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'S'...","name":"Best SR"},{"@id":"https://doi.org/10.17182/hepdata.84426.v2/t32","@type":"Dataset","description":"Observed exclusion contour at 95% CL as a function of tanBeta and the SUSY-breaking mass scale Lambda.","name":"Exclusion contour 2(obs.)"},{"@id":"https://doi.org/10.17182/hepdata.84426.v2/t33","@type":"Dataset","description":"Expected exclusion contour at 95% CL as a function of tanBeta and the SUSY-breaking mass scale Lambda.","name":"Exclusion contour 2(exp.)"},{"@id":"https://doi.org/10.17182/hepdata.84426.v2/t34","@type":"Dataset","description":"Observed exclusion contour at 95% CL as a function of the LSP mass and the gluino mass.","name":"Exclusion contour 1(obs.)"},{"@id":"https://doi.org/10.17182/hepdata.84426.v2/t35","@type":"Dataset","description":"Expected exclusion contour at 95% CL as a function of the LSP mass and the gluino mass.","name":"Exclusion contour 1(exp.)"},{"@id":"https://doi.org/10.17182/hepdata.84426.v2/t36","@type":"Dataset","description":"Observed upper limits on the production cross section at 95% CL in pb as a function of tanBeta and SUSY...","name":"X-section U.L. 2"},{"@id":"https://doi.org/10.17182/hepdata.84426.v2/t37","@type":"Dataset","description":"Observed upper limits on the production cross section at 95% CL in pb as a function of the LSP mass...","name":"X-section U.L. 1"},{"@id":"https://doi.org/10.17182/hepdata.84426.v2/t38","@type":"Dataset","description":"Yields of the expected background from the SM in the bins of the multibin SR of the $2\\tau$ channel with...","name":"Yieldtable 1"},{"@id":"https://doi.org/10.17182/hepdata.84426.v2/t39","@type":"Dataset","description":"$m_{\\mathrm{T}}^{\\tau}$ in the compressed $m_{\\mathrm{T}}^{\\tau}$ VR of the $1\\tau$ channel, illustrating the background modeling after the fit. 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