{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.75330.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1477209"}},{"@id":"https://doi.org/10.1140/epjc/s10052-016-4481-2","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2016","description":"CERN-LHC.  A search for supersymmetry in events with large missing transverse momentum, jets, and at least one hadronically decaying tau lepton has been performed using 3.2 fb$^{-1}$ of proton-proton collision data at $\\sqrt{s}=13$ TeV recorded by the ATLAS detector at the Large Hadron Collider in 2015. Two exclusive final states are considered, with either exactly one or at least two tau leptons. No excess over the Standard Model prediction is observed in the data. Results are interpreted in the context of gauge-mediated supersymmetry breaking and a simplified model of gluino pair production with tau-rich cascade decays, substantially improving on previous limits. In the GMSB model considered, supersymmetry-breaking scale ($\\Lambda$) values below 92 TeV are excluded at the 95% confidence level, corresponding to gluino masses below 2000 GeV. For large values of $\\tan\\beta$, values of $\\Lambda$ up to 107 TeV and gluino masses up to 2300 GeV are excluded. In the simplified model, gluino masses are excluded up to 1570 GeV for neutralino masses around 100 GeV. Neutralino masses up to 700 GeV are excluded for all gluino masses between 800 GeV and 1500 GeV, while the strongest exclusion of 750 GeV is achieved for gluino masses around 1400 GeV.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.75330.v1/t1","@type":"Dataset","description":"mTtau distributions for \"extended SR selections\" of the 1 tau channel, for the Compressed SR selection without the mTtau >...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.75330.v1/t2","@type":"Dataset","description":"mTtau distributions for \"extended SR selections\" of the 1 tau channel, for the Medium Mass SR selection without the mTtau...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.75330.v1/t3","@type":"Dataset","description":"mTtau distributions for \"extended SR selections\" of the 1 tau channel, for the High Mass SR selection without the mTtau...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.75330.v1/t4","@type":"Dataset","description":"Kinematic distributions for \"extended SR selections\" of the 2-tau channel, for mTsum in the Compressed SR selection without the mTsum>1400...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.75330.v1/t5","@type":"Dataset","description":"Kinematic distributions for \"extended SR selections\" of the 2-tau channel, for mTtau1+mTtau2 in the High-Mass SR selection without the mTtau1+mTtau2>350GeV...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.75330.v1/t6","@type":"Dataset","description":"Kinematic distributions for \"extended SR selections\" of the 2-tau channel, for HT in the GMSB SR selection without the HT...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.75330.v1/t7","@type":"Dataset","description":"Expected exclusion contour at the 95% confidence level for the simplified model of gluino pair production, based on the combined...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.75330.v1/t8","@type":"Dataset","description":"Observed exclusion contour at the 95% confidence level for the simplified model of gluino pair production, based on the combined...","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.75330.v1/t9","@type":"Dataset","description":"Expected exclusion contour at the 95% confidence level for the simplified model of gluino pair production, based on results from...","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.75330.v1/t10","@type":"Dataset","description":"Expected exclusion contour at the 95% confidence level for the simplified model of gluino pair production, based on results from...","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.75330.v1/t11","@type":"Dataset","description":"Observed exclusion contours at the 95% confidence level for the gauge-mediated supersymmetry-breaking model, based on results from the 2 tau...","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.75330.v1/t12","@type":"Dataset","description":"Expected exclusion contours at the 95% confidence level for the gauge-mediated supersymmetry-breaking model, based on results from the 2 tau...","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.75330.v1/t13","@type":"Dataset","description":"Observed upper cross section limits in pb for the simplified model of gluino pair production for the combination of all...","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.75330.v1/t14","@type":"Dataset","description":"Best expected signal region for the simplified model of gluino pair production. The respective SR has been used in the...","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.75330.v1/t15","@type":"Dataset","description":"Acceptance for the gluino production simplified model grid in the Compressed 1tau signal region.","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.75330.v1/t16","@type":"Dataset","description":"Efficiency for the gluino production simplified model grid in the Compressed 1tau signal region.","name":"Table 16"},{"@id":"https://doi.org/10.17182/hepdata.75330.v1/t17","@type":"Dataset","description":"Acceptance times Efficiency for the gluino production simplified model grid in the Compressed 1tau signal region.","name":"Table 17"},{"@id":"https://doi.org/10.17182/hepdata.75330.v1/t18","@type":"Dataset","description":"Acceptance for the gluino production simplified model grid in the medium mass 1tau signal region.","name":"Table 18"},{"@id":"https://doi.org/10.17182/hepdata.75330.v1/t19","@type":"Dataset","description":"Efficiency for the gluino production simplified model grid in the medium mass 1tau signal region.","name":"Table 19"},{"@id":"https://doi.org/10.17182/hepdata.75330.v1/t20","@type":"Dataset","description":"Acceptance times Efficiency for the gluino production simplified model grid in the medium mass 1tau signal region.","name":"Table 20"},{"@id":"https://doi.org/10.17182/hepdata.75330.v1/t21","@type":"Dataset","description":"Acceptance for the gluino production simplified model grid in the high mass 1tau signal region.","name":"Table 21"},{"@id":"https://doi.org/10.17182/hepdata.75330.v1/t22","@type":"Dataset","description":"Efficiency for the gluino production simplified model grid in the high mass 1tau signal region.","name":"Table 22"},{"@id":"https://doi.org/10.17182/hepdata.75330.v1/t23","@type":"Dataset","description":"Acceptance times Efficiency for the gluino production simplified model grid in the high mass 1tau signal region.","name":"Table 23"},{"@id":"https://doi.org/10.17182/hepdata.75330.v1/t24","@type":"Dataset","description":"Acceptance for the gluino production simplified model grid in the compressed 2tau signal region.","name":"Table 24"},{"@id":"https://doi.org/10.17182/hepdata.75330.v1/t25","@type":"Dataset","description":"Efficiency for the gluino production simplified model grid in the compressed 2tau signal region.","name":"Table 25"},{"@id":"https://doi.org/10.17182/hepdata.75330.v1/t26","@type":"Dataset","description":"Acceptance times Efficiency for the gluino production simplified model grid in the compressed 2tau signal region.","name":"Table 26"},{"@id":"https://doi.org/10.17182/hepdata.75330.v1/t27","@type":"Dataset","description":"Acceptance for the gluino production simplified model grid in the high mass 2tau signal region.","name":"Table 27"},{"@id":"https://doi.org/10.17182/hepdata.75330.v1/t28","@type":"Dataset","description":"Efficiency for the gluino production simplified model grid in the high mass 2tau signal region.","name":"Table 28"},{"@id":"https://doi.org/10.17182/hepdata.75330.v1/t29","@type":"Dataset","description":"Acceptance times Efficiency for the gluino production simplified model grid in the high mass 2tau signal region.","name":"Table 29"},{"@id":"https://doi.org/10.17182/hepdata.75330.v1/t30","@type":"Dataset","description":"Acceptance for the GMSB model grid in the 2tau signal region.","name":"Table 30"},{"@id":"https://doi.org/10.17182/hepdata.75330.v1/t31","@type":"Dataset","description":"Efficiency for the GMSB model grid in the 2tau signal region.","name":"Table 31"},{"@id":"https://doi.org/10.17182/hepdata.75330.v1/t32","@type":"Dataset","description":"Acceptance times Efficiency for the GMSB model grid in the 2tau signal region.","name":"Table 32"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1477209?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/75330"}],"inLanguage":"en","name":"Search for squarks and gluinos in events with hadronically decaying tau leptons, jets and missing transverse momentum in proton-proton collisions at $\\sqrt{s}=13$ TeV recorded with the ATLAS detector","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1477209?version=1","version":1}