{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.69241.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1383884"}},{"@id":"https://doi.org/10.1007/JHEP10(2015)054","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2015","description":"CERN-LHC.  A summary is presented of ATLAS searches for gluinos and first- and second-generation squarks in final states containing jets and missing transverse momentum, with or without leptons or b-jets, in the $\\sqrt{s}$ = 8 TeV data set collected at the Large Hadron Collider in 2012. This paper reports the results of new interpretations and statistical combinations of previously published analyses, as well as a new analysis. Since no significant excess of events over the Standard Model expectation is observed, the data are used to set limits in a variety of models. In all the considered simplified models that assume R-parity conservation, the limit on the gluino mass exceeds 1150 GeV at 95% confidence level, for an LSP mass smaller than 100 GeV. Furthermore, exclusion limits are set for left-handed squarks in a phenomenological MSSM model, a minimal Supergravity/Constrained MSSM model, R-parity-violation scenarios, a minimal gauge-mediated supersymmetry breaking model, a natural gauge mediation model, a non-universal Higgs mass model with gaugino mediation and a minimal model of universal extra dimensions.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.69241.v1/t1","@type":"Dataset","description":"Acceptance for the loose channel of the Razor analysis for the direct squark-squark model.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.69241.v1/t2","@type":"Dataset","description":"Acceptance times efficiency for the loose channel of the Razor analysis for the direct squark-squark model.","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.69241.v1/t3","@type":"Dataset","description":"Acceptance for the tight channel of the Razor analysis for the direct squark-squark model.","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.69241.v1/t4","@type":"Dataset","description":"Acceptance times efficiency for the tight channel of the Razor analysis for the direct squark-squark model.","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.69241.v1/t5","@type":"Dataset","description":"Acceptance for the 1tau channel of the Taus+jets+MET analysis for the gluino simplified model.","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.69241.v1/t6","@type":"Dataset","description":"Efficiency for the 1tau channel of the Taus+jets+MET analysis for the gluino simplified model.","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.69241.v1/t7","@type":"Dataset","description":"Acceptance for the 2tau channel of the Taus+jets+MET analysis for the gluino simplified model.","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.69241.v1/t8","@type":"Dataset","description":"Efficiency for the 2tau channel of the Taus+jets+MET analysis for the gluino simplified model.","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.69241.v1/t9","@type":"Dataset","description":"Acceptance for the 1tau channel of the Taus+jets+MET analysis for the squark simplified model.","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.69241.v1/t10","@type":"Dataset","description":"Efficiency for the 1tau channel of the Taus+jets+MET analysis for the squark simplified model.","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.69241.v1/t11","@type":"Dataset","description":"Acceptance for the 2tau channel of the Taus+jets+MET analysis for the squark simplified model.","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.69241.v1/t12","@type":"Dataset","description":"Efficiency for the 2tau channel of the Taus+jets+MET analysis for the squark simplified model.","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.69241.v1/t13","@type":"Dataset","description":"Observed limit on the cross-section times branching ratio in fb at 95% CL for the direct squark-squark model.","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.69241.v1/t14","@type":"Dataset","description":"Observed limit on the cross-section times branching ratio in fb at 95% CL for the gluino simplified model, obtained by...","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.69241.v1/t15","@type":"Dataset","description":"Observed limit on the cross-section times branching ratio in fb at 95% CL for the squark simplified model, obtained by...","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.69241.v1/t16","@type":"Dataset","description":"Observed 95% CL cross section times branching ratio upper limit on pMSSM qLqL production with M1=60 GeV and $m_{\\tilde g}=$1.6...","name":"Table 16"},{"@id":"https://doi.org/10.17182/hepdata.69241.v1/t17","@type":"Dataset","description":"Observed 95% CL cross section times branching ratio upper limit on pMSSM qLqL production with M2=(M1+mqL)/2 and $m_{\\tilde g}=$1.6 TeV...","name":"Table 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The point used...","name":"Table 23"},{"@id":"https://doi.org/10.17182/hepdata.69241.v1/t24","@type":"Dataset","description":"Cut flow for the 1L(H)_7-jet SR (electron channel) for the main background from the $t\\bar{t}$ production. The events are normalized...","name":"Table 24"},{"@id":"https://doi.org/10.17182/hepdata.69241.v1/t25","@type":"Dataset","description":"Cut flow for the 1L(H)_7-jet SR (muon channel) for the main background from the $t\\bar{t}$ production. The events are normalized...","name":"Table 25"},{"@id":"https://doi.org/10.17182/hepdata.69241.v1/t26","@type":"Dataset","description":"Cut flow for 1L(H)_7-jet SR (electron channel). The signal point is taken from the gluino simplified model with 1-step decay...","name":"Table 26"},{"@id":"https://doi.org/10.17182/hepdata.69241.v1/t27","@type":"Dataset","description":"Cut flow for 1L(H)_7-jet SR (muon channel). The signal point is taken from the gluino simplified model with 1-step decay...","name":"Table 27"},{"@id":"https://doi.org/10.17182/hepdata.69241.v1/t28","@type":"Dataset","description":"Cut flow for 1L(H)_7-jet SR (electron channel). The signal point is taken from the gluino simplified model with 1-step decay...","name":"Table 28"},{"@id":"https://doi.org/10.17182/hepdata.69241.v1/t29","@type":"Dataset","description":"Cut flow for 1L(H)_7-jet SR (muon channel). The signal point is taken from the gluino simplified model with 1-step decay...","name":"Table 29"},{"@id":"https://doi.org/10.17182/hepdata.69241.v1/t30","@type":"Dataset","description":"Cut flow for 0LRaz_SR$_{\\rm loose}$ and 0LRaz_SR$_{\\rm tight}$ signal regions of baseline signal point ($m(\\tilde{q}, \\tilde{\\chi}_1^0)=(850, 100)$ GeV) normalized to...","name":"Table 30"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1383884?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/69241"}],"inLanguage":"en","name":"Summary of the searches for squarks and gluinos using $\\sqrt{s}$ = 8 TeV pp collisions with the ATLAS experiment at the LHC","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1383884?version=1","version":1}