{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.66986.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1339376"}},{"@id":"https://doi.org/10.1007/JHEP04(2015)116","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2015","description":"CERN-LHC. The results of a search for supersymmetry in final states containing at least one isolated lepton (electron or muon), jets and large missing transverse momentum with the ATLAS detector at the Large Hadron Collider (LHC) are reported. The search is based on proton-proton collision data at a centre-of-mass energy $\\sqrt{s}=8$ TeV collected in 2012, corresponding to an integrated luminosity of 20 fb$^{-1}$. No significant excess above the Standard Model expectation is observed. Limits are set on the parameters of a minimal universal extra dimensions model, excluding a compactification radius of $1/R_{c}=950$ GeV for a cut-off scale times radius ($\\Lambda R_{c}$) of approximately 30, as well as on sparticle masses for various supersymmetric models. Depending on the model, the search excludes gluino masses up to 1.32 TeV and squark masses up to 840 GeV.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t1","@type":"Dataset","description":"Observed and expected $E_T^{miss}/m_{eff}$ distribution in soft single-lepton 3-jet signal region. The last bin includes the overflow.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t2","@type":"Dataset","description":"Observed and expected $E_T^{miss}/m_{eff}$ distribution in soft single-lepton 5-jet signal region. The last bin includes the overflow.","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t3","@type":"Dataset","description":"Observed and expected $E_T^{miss}/m_{eff}$ distribution in soft single-lepton 3-jet inclusive signal region. The last bin includes the overflow.","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t4","@type":"Dataset","description":"Observed and expected $E_T^{miss}$ distribution in soft dimuon signal region. The last bin includes the overflow.","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t5","@type":"Dataset","description":"Observed and expected $m_{eff}^{incl}$ distribution in hard single-lepton 3-jet signal region. The last bin includes the overflow.","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t6","@type":"Dataset","description":"Observed and expected $m_{eff}^{incl}$ distribution for hard single-lepton 5-jet signal region. The last bin includes the overflow.","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t7","@type":"Dataset","description":"Observed and expected $E_{T}^{miss}$ distribution for hard single-lepton 6-jet signal region. The last bin includes the overflow.","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t8","@type":"Dataset","description":"Observed and expected $M_{R}'$ distribution for hard same-flavour dilepton low-multiplicity signal region. The last bin includes the overflow.","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t9","@type":"Dataset","description":"Observed and expected $M_{R}'$ distribution for hard same-flavour dilepton 3-jet signal region. The last bin includes the overflow.","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t10","@type":"Dataset","description":"Observed and expected $M_{R}'$ distribution for hard opposite-flavour dilepton low-multiplicity signal region. The last bin includes the overflow.","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t11","@type":"Dataset","description":"Observed and expected $M_{R}'$ distribution for hard opposite-flavour dilepton 3-jet opposite-flavour signal region. The last bin includes the overflow.","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t12","@type":"Dataset","description":"Observed 95% exclusion contour for the mSUGRA/CMSSM model with $\\tan\\beta=30$, $A_{0}=-2m_{0}$ and $\\mu > 0$.","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t13","@type":"Dataset","description":"Expected 95% exclusion contour for the mSUGRA/CMSSM model with $\\tan\\beta=30$, $A_{0}=-2m_{0}$ and $\\mu > 0$.","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t14","@type":"Dataset","description":"Observed 95% exclusion contour for the bRPV MSUGRA/CMSSM model.","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t15","@type":"Dataset","description":"Expected 95% exclusion contour for the bRPV MSUGRA/CMSSM model.","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t16","@type":"Dataset","description":"Observed 95% exclusion contour for the natural gauge mediation with a stau NLSP model (nGM).","name":"Table 16"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t17","@type":"Dataset","description":"Expected 95% exclusion contour for the natural gauge mediation with a stau NLSP model (nGM).","name":"Table 17"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t18","@type":"Dataset","description":"Observed 95% exclusion contour for the non-universal higgs masses with gaugino mediation model (NUHMG).","name":"Table 18"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t19","@type":"Dataset","description":"Expected 95% exclusion contour for the non-universal higgs masses with gaugino mediation model (NUHMG).","name":"Table 19"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t20","@type":"Dataset","description":"Observed 95% exclusion contour for the minimal UED model from the combination of the hard dilepton and soft dilepton analyses.","name":"Table 20"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t21","@type":"Dataset","description":"Expected 95% exclusion contour for the minimal UED model from the combination of the hard dilepton and soft dilepton analyses.","name":"Table 21"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t22","@type":"Dataset","description":"Observed 95% exclusion contour for the minimal UED model from the hard dilepton analysis.","name":"Table 22"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t23","@type":"Dataset","description":"Expected 95% exclusion contour for the minimal UED model from the hard dilepton analysis.","name":"Table 23"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t24","@type":"Dataset","description":"Observed 95% exclusion contour for the minimal UED model from the soft dilepton analysis.","name":"Table 24"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t25","@type":"Dataset","description":"Expected 95% exclusion contour for the minimal UED model from the soft dilepton analysis.","name":"Table 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the...","name":"Table 41"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t42","@type":"Dataset","description":"Observed 95% exclusion contour for the gluino simplified model from the combination of the soft single-lepton and hard single-lepton analyses...","name":"Table 42"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t43","@type":"Dataset","description":"Expected 95% exclusion contour for the gluino simplified model from the combination of the soft single-lepton and hard single-lepton analyses...","name":"Table 43"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t44","@type":"Dataset","description":"Observed 95% exclusion contour for the gluino simplified model from the hard single-lepton analysis for the case in which x...","name":"Table 44"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t45","@type":"Dataset","description":"Expected 95% exclusion contour for the gluino simplified model from the hard single-lepton analysis for the case in which x...","name":"Table 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49"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t50","@type":"Dataset","description":"Observed 95% exclusion contour for the first- and second-generation squark simplified model from the hard single-lepton analyses for the case...","name":"Table 50"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t51","@type":"Dataset","description":"Expected 95% exclusion contour for the first- and second-generation squark simplified model from the hard single-lepton analyses for the case...","name":"Table 51"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t52","@type":"Dataset","description":"Observed 95% exclusion contour for the first- and second-generation squark simplified model from the soft single-lepton analyses for the case...","name":"Table 52"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t53","@type":"Dataset","description":"Expected 95% exclusion contour for the first- and second-generation squark simplified model from the soft single-lepton analyses for the case...","name":"Table 53"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t54","@type":"Dataset","description":"Observed 95% exclusion contour for the two-step gluino simplified model with sleptons from the combination of the hard dilepton and...","name":"Table 54"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t55","@type":"Dataset","description":"Expected 95% exclusion contour for the two-step gluino simplified model with sleptons from the combination of the hard dilepton and...","name":"Table 55"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t56","@type":"Dataset","description":"Observed 95% exclusion contour for the two-step gluino simplified model with sleptons from the hard single-lepton analysis.","name":"Table 56"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t57","@type":"Dataset","description":"Expected 95% exclusion contour for the two-step gluino simplified model with sleptons from the hard single-lepton analysis.","name":"Table 57"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t58","@type":"Dataset","description":"Observed 95% exclusion contour for the two-step gluino simplified model with sleptons from the hard dilepton analysis.","name":"Table 58"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t59","@type":"Dataset","description":"Expected 95% exclusion contour for the two-step gluino simplified model with sleptons from the hard dilepton analysis.","name":"Table 59"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t60","@type":"Dataset","description":"Observed 95% exclusion contour for the two-step first- and second-generation squark simplified model with sleptons from the hard dilepton analysis.","name":"Table 60"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t61","@type":"Dataset","description":"Expected 95% exclusion contour for the two-step first- and second-generation squark simplified model with sleptons from the hard dilepton analysis.","name":"Table 61"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t62","@type":"Dataset","description":"Observed 95% exclusion contour for the two-step gluino simplified model without sleptons from the hard single-lepton analysis.","name":"Table 62"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t63","@type":"Dataset","description":"Expected 95% exclusion contour for the two-step gluino simplified model without sleptons from the hard single-lepton analysis.","name":"Table 63"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t64","@type":"Dataset","description":"Number of generated events in the gluino simplified model for the case in which the chargino mass is fixed at...","name":"Table 64"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t65","@type":"Dataset","description":"Production cross-section in the gluino simplified model for the case in which the chargino mass is fixed at x =...","name":"Table 65"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t66","@type":"Dataset","description":"Number of generated events in the the first- and second-generation squark simplified model for the case in which x =...","name":"Table 66"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t67","@type":"Dataset","description":"Production cross-section in the the first- and second-generation squark simplified model for the case in which x = (m(squark)-m(chargino))/(m(squark)-m(LSP)) is...","name":"Table 67"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t68","@type":"Dataset","description":"Number of generated evens in the minimal UED model.","name":"Table 68"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t69","@type":"Dataset","description":"Production cross-section in the minimal UED model in pb.","name":"Table 69"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t70","@type":"Dataset","description":"Number of generated events in the two-step first- and second-generation squark simplified model with sleptons.","name":"Table 70"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t71","@type":"Dataset","description":"Production cross-section in the two-step first- and second-generation squark simplified model with sleptons.","name":"Table 71"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t72","@type":"Dataset","description":"Acceptance for soft single-lepton 3-jet signal region in the gluino simplified model for the case in which the chargino mass...","name":"Table 72"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t73","@type":"Dataset","description":"Efficiency for soft single-lepton 3-jet signal region in the gluino simplified model for the case in which the chargino mass...","name":"Table 73"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t74","@type":"Dataset","description":"Acceptance for soft single-lepton 5-jet signal region in the gluino simplified model for the case in which the chargino mass...","name":"Table 74"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t75","@type":"Dataset","description":"Efficiency for soft single-lepton 5-jet signal region in the gluino simplified model for the case in which the chargino mass...","name":"Table 75"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t76","@type":"Dataset","description":"Acceptance for soft single-lepton 3-jet inclusive signal region in the gluino simplified model for the case in which x =...","name":"Table 76"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t77","@type":"Dataset","description":"Efficiency for the soft single-lepton 3-jet inclusive signal region in the gluino simplified model for the case in x =...","name":"Table 77"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t78","@type":"Dataset","description":"Expected CLs from the combination of the soft single-lepton and hard single-lepton analyses in the gluino simplified model for the...","name":"Table 78"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t79","@type":"Dataset","description":"Expected CLs from the combination of the soft single-lepton and hard single-lepton analyses in the gluino simplified model for the...","name":"Table 79"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t80","@type":"Dataset","description":"Observed CLs from the combination of the soft single-lepton and hard single-lepton analyses in the gluino simplified model for the...","name":"Table 80"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t81","@type":"Dataset","description":"Observed CLs from the combination of the soft single-lepton and hard single-lepton analyses in the gluino simplified model for the...","name":"Table 81"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t82","@type":"Dataset","description":"Acceptance for soft dimuon signal region in the minimal UED model (mUED).","name":"Table 82"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t83","@type":"Dataset","description":"Efficiency for soft dimuon signal region in minimal UED model (mUED).","name":"Table 83"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t84","@type":"Dataset","description":"Acceptance for hard dilepton 3-jet opposite-flavour signal region in the two-step first- and second-generation squark simplified model with sleptons.","name":"Table 84"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t85","@type":"Dataset","description":"Efficiency for hard dilepton 3jet opposite-flavour signal region in the two-step first- and second-generation squark simplified model with sleptons.","name":"Table 85"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t86","@type":"Dataset","description":"Acceptance for hard dilepton 3-jet same-flavour signal region in the two-step first- and second-generation squark simplified model with sleptons.","name":"Table 86"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t87","@type":"Dataset","description":"Efficiency for hard dilepton 3-jet same-flavour signal region in the two-step first- and second-generation squark simplified model with sleptons.","name":"Table 87"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t88","@type":"Dataset","description":"Acceptance for hard dilepton low-multiplicity opposite-flavour signal region in the two-step first- and second-generation squark simplified model with sleptons.","name":"Table 88"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t89","@type":"Dataset","description":"Efficiency for hard dilepton low-multiplicity opposite-flavour signal region in the two-step first- and second-generation squark simplified model with sleptons.","name":"Table 89"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t90","@type":"Dataset","description":"Acceptance for hard dilepton low-multiplicity same-flavour signal region in the two-step first- and second-generation squark simplified model with sleptons.","name":"Table 90"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t91","@type":"Dataset","description":"Efficiency for hard dilepton low-multiplicity same-flavour signal region in the two-step first- and second-generation squark simplified model with sleptons.","name":"Table 91"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t92","@type":"Dataset","description":"Best expected signal region in the minimal UED model (mUED).","name":"Table 92"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t93","@type":"Dataset","description":"Expected CLs from hard dilepton analysis in the two-step first- and second-generation squark simplified model with sleptons.","name":"Table 93"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t94","@type":"Dataset","description":"Observed CLs from the hard dilepton analysis in the two-step first- and second-generation squark simplified model with sleptons.","name":"Table 94"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t95","@type":"Dataset","description":"Expected CLs from the combination of the soft dimuon and hard dilepton analyses in the minimal UED model (mUED).","name":"Table 95"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t96","@type":"Dataset","description":"Observed CLs from the combination of the soft dimuon and hard dilepton analyses in the minimal UED model (mUED).","name":"Table 96"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t97","@type":"Dataset","description":"Acceptance for hard single-lepton 3-jet signal region in the gluino simplified model for the case in which the chargino mass...","name":"Table 97"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t98","@type":"Dataset","description":"Efficiency for hard single-lepton 3-jet signal region in the gluino simplified model for the case in which the chargino mass...","name":"Table 98"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t99","@type":"Dataset","description":"Acceptance for hard single-lepton 5-jet signal region in the gluino simplified model for the case in which the chargino mass...","name":"Table 99"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t100","@type":"Dataset","description":"Efficiency for hard single-lepton 5-jet signal region in the gluino simplified model for the case in which the chargino mass...","name":"Table 100"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t101","@type":"Dataset","description":"Acceptance for hard single-lepton 6-jet signal region in the gluino simplified model for the case in which the chargino mass...","name":"Table 101"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t102","@type":"Dataset","description":"Efficiency for hard single-lepton 6-jet signal region in the gluino simplified model for the case in which the chargino mass...","name":"Table 102"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t103","@type":"Dataset","description":"Acceptance for hard single-lepton 3-jet signal region in the first- and second-generation squark simplified model for the case in which...","name":"Table 103"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t104","@type":"Dataset","description":"Efficiency for hard single-lepton 3-jet signal region in the first- and second-generation squark simplified model for the case in which...","name":"Table 104"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t105","@type":"Dataset","description":"Acceptance for hard single-lepton 5-jet signal region in the first- and second-generation squark simplified model for the case in which...","name":"Table 105"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t106","@type":"Dataset","description":"Efficiency for hard single-lepton 5-jet signal region in the first- and second-generation squark simplified model for the case in which...","name":"Table 106"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t107","@type":"Dataset","description":"Acceptance for hard single-lepton 6-jet signal region in the first- and second-generation squark simplified model for the case in which...","name":"Table 107"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t108","@type":"Dataset","description":"Efficiency for hard single-lepton 6-jet signal region in the first- and second-generation squark simplified model for the case in which...","name":"Table 108"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t109","@type":"Dataset","description":"Observed 95% upper limit on the visible cross-section in the gluino simplified model from the combination of the soft single-lepton...","name":"Table 109"},{"@id":"https://doi.org/10.17182/hepdata.66986.v1/t110","@type":"Dataset","description":"Observed 95% upper limit on the visible cross-section in the first- and second-generation squark simplified model from the combination of...","name":"Table 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