{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.74253.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1458270"}},{"@id":"https://doi.org/10.1140/epjc/s10052-016-4184-8","@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 squarks and gluinos in final states containing hadronic jets, missing transverse momentum but no electrons or muons is presented. The data were recorded in 2015 by the ATLAS experiment in $\\sqrt{s}=$ 13 TeV proton--proton collisions at the Large Hadron Collider. No excess above the Standard Model background expectation was observed in 3.2 fb$^{-1}$ of analyzed data. Results are interpreted within simplified models that assume R-parity is conserved and the neutralino is the lightest supersymmetric particle. An exclusion limit at the 95% confidence level on the mass of the gluino is set at 1.51 TeV for a simplified model incorporating only a gluino octet and the lightest neutralino, assuming the lightest neutralino is massless. For a simplified model involving the strong production of mass-degenerate first- and second-generation squarks, squark masses below 1.03 TeV are excluded for a massless lightest neutralino. These limits substantially extend the region of supersymmetric parameter space excluded by previous measurements with the ATLAS detector.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t1","@type":"Dataset","description":"Observed and expected background effective mass distributions in control region CRgamma for SR4jt.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t2","@type":"Dataset","description":"Observed and expected background effective mass distributions in control region CRW for SR4jt.","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t3","@type":"Dataset","description":"Observed and expected background effective mass distributions in control region CRT for SR4jt.","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t4","@type":"Dataset","description":"Observed and expected background and signal effective mass distributions for SR2jl. For signal, a squark direct decay model with $m(\\tilde...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t5","@type":"Dataset","description":"Observed and expected background and signal effective mass distributions for SR2jm. For signal, a gluino direct decay model with $m(\\tilde...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t6","@type":"Dataset","description":"Observed and expected background and signal effective mass distributions for SR2jt. For signal, a squark direct decay model with $m(\\tilde...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t7","@type":"Dataset","description":"Observed and expected background and signal effective mass distributions for SR4jt. For signal, a gluino direct decay model with $m(\\tilde...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t8","@type":"Dataset","description":"Observed and expected background and signal effective mass distributions for SR5j. For signal, a gluino one-step decay model with $m(\\tilde...","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t9","@type":"Dataset","description":"Observed and expected background and signal effective mass distributions for SR6jm. For signal, a gluino one-step decay model with $m(\\tilde...","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t10","@type":"Dataset","description":"Observed and expected background and signal effective mass distributions for SR6jt. For signal, a gluino one-step decay model with $m(\\tilde...","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t11","@type":"Dataset","description":"Expected limit at 95% CL for squark direct decay model grid.","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t12","@type":"Dataset","description":"Expected limits at 95% CL +1 sigma excursion due to experimental and background-only theoretical uncertainties for squark direct decay model...","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t13","@type":"Dataset","description":"Expected limits at 95% CL -1 sigma excursion due to experimental and background-only theoretical uncertainties for squark direct decay model...","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t14","@type":"Dataset","description":"Observed limits at 95% CL for squark direct decay model grid.","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t15","@type":"Dataset","description":"Observed limits at 95% CL +1 sigma excursion due to the signal cross-section uncertainty for squark direct decay model grid.","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t16","@type":"Dataset","description":"Observed limits at 95% CL -1 sigma excursion due to the signal cross-section uncertainty for squark direct decay model grid.","name":"Table 16"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t17","@type":"Dataset","description":"Expected limit at 95% CL for gluino direct decay model grid.","name":"Table 17"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t18","@type":"Dataset","description":"Expected limits at 95% CL +1 sigma excursion due to experimental and background-only theoretical uncertainties for gluino direct decay model...","name":"Table 18"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t19","@type":"Dataset","description":"Expected limits at 95% CL -1 sigma excursion due to experimental and background-only theoretical uncertainties for gluino direct decay model...","name":"Table 19"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t20","@type":"Dataset","description":"Observed limits at 95% CL for gluino direct decay model grid.","name":"Table 20"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t21","@type":"Dataset","description":"Observed limits at 95% CL +1 sigma excursion due to the signal cross-section uncertainty for gluino direct decay model grid.","name":"Table 21"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t22","@type":"Dataset","description":"Observed limits at 95% CL -1 sigma excursion due to the signal cross-section uncertainty for gluino direct decay model grid.","name":"Table 22"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t23","@type":"Dataset","description":"Expected limit at 95% CL for gluino one-step decay model grid.","name":"Table 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27"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t28","@type":"Dataset","description":"Observed limits at 95% CL -1 sigma excursion due to the signal cross-section uncertainty for gluino one-step decay model grid.","name":"Table 28"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t29","@type":"Dataset","description":"Observed and expected background effective mass distributions in control region CRgamma for SR2jl.","name":"Table 29"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t30","@type":"Dataset","description":"Observed and expected background effective mass distributions in validation region VRZ for SR2jl.","name":"Table 30"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t31","@type":"Dataset","description":"Observed and expected background effective mass distributions in control region CRW for SR2jl.","name":"Table 31"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t32","@type":"Dataset","description":"Observed and expected background effective mass distributions in control region CRT for SR2jl.","name":"Table 32"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t33","@type":"Dataset","description":"Observed and expected background effective mass distributions in control region CRgamma for SR2jm.","name":"Table 33"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t34","@type":"Dataset","description":"Observed and expected background effective mass distributions in validation region VRZ for SR2jm.","name":"Table 34"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t35","@type":"Dataset","description":"Observed and expected background effective mass distributions in control region CRW for SR2jm.","name":"Table 35"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t36","@type":"Dataset","description":"Observed and expected background effective mass distributions in control region CRT for SR2jm.","name":"Table 36"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t37","@type":"Dataset","description":"Observed and expected background effective mass distributions in control region CRgamma for SR2jt.","name":"Table 37"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t38","@type":"Dataset","description":"Observed and expected background effective mass distributions in validation region VRZ for SR2jt.","name":"Table 38"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t39","@type":"Dataset","description":"Observed and expected background effective mass distributions in control region CRW for SR2jt.","name":"Table 39"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t40","@type":"Dataset","description":"Observed and expected background effective mass distributions in control region CRT for SR2jt.","name":"Table 40"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t41","@type":"Dataset","description":"Observed and expected background effective mass distributions in control region CRgamma for SR4jt.","name":"Table 41"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t42","@type":"Dataset","description":"Observed and expected background effective mass distributions in validation region VRZ for SR4jt.","name":"Table 42"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t43","@type":"Dataset","description":"Observed and expected background effective mass distributions in control region CRW for SR4jt.","name":"Table 43"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t44","@type":"Dataset","description":"Observed and expected background effective mass distributions in control region CRT for SR4jt.","name":"Table 44"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t45","@type":"Dataset","description":"Observed and expected background effective mass distributions in control region CRgamma for SR5j.","name":"Table 45"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t46","@type":"Dataset","description":"Observed and expected background effective mass distributions in validation region VRZ for SR5j.","name":"Table 46"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t47","@type":"Dataset","description":"Observed and expected background effective mass distributions in control region CRW for SR5j.","name":"Table 47"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t48","@type":"Dataset","description":"Observed and expected background effective mass distributions in control region CRT for SR5j.","name":"Table 48"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t49","@type":"Dataset","description":"Observed and expected background effective mass distributions in control region CRgamma for SR6jm.","name":"Table 49"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t50","@type":"Dataset","description":"Observed and expected background effective mass distributions in validation region VRZ for SR6jm.","name":"Table 50"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t51","@type":"Dataset","description":"Observed and expected background effective mass distributions in control region CRW for SR6jm.","name":"Table 51"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t52","@type":"Dataset","description":"Observed and expected background effective mass distributions in control region CRT for SR6jm.","name":"Table 52"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t53","@type":"Dataset","description":"Observed and expected background effective mass distributions in control region CRgamma for SR6jt.","name":"Table 53"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t54","@type":"Dataset","description":"Observed and expected background effective mass distributions in validation region VRZ for SR6jt.","name":"Table 54"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t55","@type":"Dataset","description":"Observed and expected background effective mass distributions in control region CRW for SR6jt.","name":"Table 55"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t56","@type":"Dataset","description":"Observed and expected background effective mass distributions in control region CRT for SR6jt.","name":"Table 56"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t57","@type":"Dataset","description":"Observed and expected event yields in VRZ as a function of signal region.","name":"Table 57"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t58","@type":"Dataset","description":"Observed and expected event yields in VRW as a function of signal region.","name":"Table 58"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t59","@type":"Dataset","description":"Observed and expected event yields in VRWv as a function of signal region.","name":"Table 59"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t60","@type":"Dataset","description":"Observed and expected event yields in VRT as a function of signal region.","name":"Table 60"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t61","@type":"Dataset","description":"Observed and expected event yields in VRTv as a function of signal region.","name":"Table 61"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t62","@type":"Dataset","description":"Observed and expected event yields in VRQa as a function of signal region.","name":"Table 62"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t63","@type":"Dataset","description":"Observed and expected event yields in VRQb as a function of signal region.","name":"Table 63"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t64","@type":"Dataset","description":"Signal acceptance for SR2jl in squark direct decay model grid.","name":"Table 64"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t65","@type":"Dataset","description":"Signal acceptance times efficiency for SR2jl in squark direct decay model grid.","name":"Table 65"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t66","@type":"Dataset","description":"Signal acceptance for SR2jm in squark direct decay model grid.","name":"Table 66"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t67","@type":"Dataset","description":"Signal acceptance times efficiency for SR2jm in squark direct decay model grid.","name":"Table 67"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t68","@type":"Dataset","description":"Signal acceptance for SR2jt in squark direct decay model grid.","name":"Table 68"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t69","@type":"Dataset","description":"Signal acceptance times efficiency for SR2jt in squark direct decay model grid.","name":"Table 69"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t70","@type":"Dataset","description":"Signal acceptance for SR4jt in squark direct decay model grid.","name":"Table 70"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t71","@type":"Dataset","description":"Signal acceptance times efficiency for SR4jt in squark direct decay model grid.","name":"Table 71"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t72","@type":"Dataset","description":"Signal acceptance for SR5j in squark direct decay model grid.","name":"Table 72"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t73","@type":"Dataset","description":"Signal acceptance times efficiency for SR5j in squark direct decay model grid.","name":"Table 73"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t74","@type":"Dataset","description":"Signal acceptance for SR6jm in squark direct decay model grid.","name":"Table 74"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t75","@type":"Dataset","description":"Signal acceptance times efficiency for SR6jm in squark direct decay model grid.","name":"Table 75"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t76","@type":"Dataset","description":"Signal acceptance for SR6jt in squark direct decay model grid.","name":"Table 76"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t77","@type":"Dataset","description":"Signal acceptance times efficiency for SR6jt in squark direct decay model grid.","name":"Table 77"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t78","@type":"Dataset","description":"Signal acceptance for SR2jl in gluino direct decay model grid.","name":"Table 78"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t79","@type":"Dataset","description":"Signal acceptance times efficiency for SR2jl in gluino direct decay model grid.","name":"Table 79"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t80","@type":"Dataset","description":"Signal acceptance for SR2jm in gluino direct decay model grid.","name":"Table 80"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t81","@type":"Dataset","description":"Signal acceptance times efficiency for SR2jm in gluino direct decay model grid.","name":"Table 81"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t82","@type":"Dataset","description":"Signal acceptance for SR2jt in gluino direct decay model grid.","name":"Table 82"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t83","@type":"Dataset","description":"Signal acceptance times efficiency for SR2jt in gluino direct decay model grid.","name":"Table 83"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t84","@type":"Dataset","description":"Signal acceptance for SR4jt in gluino direct decay model grid.","name":"Table 84"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t85","@type":"Dataset","description":"Signal acceptance times efficiency for SR4jt in gluino direct decay model grid.","name":"Table 85"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t86","@type":"Dataset","description":"Signal acceptance for SR5j in gluino direct decay model grid.","name":"Table 86"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t87","@type":"Dataset","description":"Signal acceptance times efficiency for SR5j in gluino direct decay model grid.","name":"Table 87"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t88","@type":"Dataset","description":"Signal acceptance for SR6jm in gluino direct decay model grid.","name":"Table 88"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t89","@type":"Dataset","description":"Signal acceptance times efficiency for SR6jm in gluino direct decay model grid.","name":"Table 89"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t90","@type":"Dataset","description":"Signal acceptance for SR6jt in gluino direct decay model grid.","name":"Table 90"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t91","@type":"Dataset","description":"Signal acceptance times efficiency for SR6jt in gluino direct decay model grid.","name":"Table 91"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t92","@type":"Dataset","description":"Signal acceptance for SR2jl in gluino one-step decay model grid.","name":"Table 92"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t93","@type":"Dataset","description":"Signal acceptance times efficiency for SR2jl in gluino one-step decay model grid.","name":"Table 93"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t94","@type":"Dataset","description":"Signal acceptance for SR2jm in gluino one-step decay model grid.","name":"Table 94"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t95","@type":"Dataset","description":"Signal acceptance times efficiency for SR2jm in gluino one-step decay model grid.","name":"Table 95"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t96","@type":"Dataset","description":"Signal acceptance for SR2j5 in gluino one-step decay model grid.","name":"Table 96"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t97","@type":"Dataset","description":"Signal acceptance times efficiency for SR2jt in gluino one-step decay model grid.","name":"Table 97"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t98","@type":"Dataset","description":"Signal acceptance for SR4jt in gluino one-step decay model grid.","name":"Table 98"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t99","@type":"Dataset","description":"Signal acceptance times efficiency for SR4jt in gluino one-step decay model grid.","name":"Table 99"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t100","@type":"Dataset","description":"Signal acceptance for SR5j in gluino one-step decay model grid.","name":"Table 100"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t101","@type":"Dataset","description":"Signal acceptance times efficiency for SR5j in gluino one-step decay model grid.","name":"Table 101"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t102","@type":"Dataset","description":"Signal acceptance for SR6jm in gluino one-step decay model grid.","name":"Table 102"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t103","@type":"Dataset","description":"Signal acceptance times efficiency for SR6jm in gluino one-step decay model grid.","name":"Table 103"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t104","@type":"Dataset","description":"Signal acceptance for SR6jt in gluino one-step decay model grid.","name":"Table 104"},{"@id":"https://doi.org/10.17182/hepdata.74253.v1/t105","@type":"Dataset","description":"Signal acceptance times efficiency for SR6jt in gluino one-step decay model grid.","name":"Table 105"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1458270?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/74253"}],"inLanguage":"en","name":"Search for squarks and gluinos in final states with jets and missing transverse momentum at $\\sqrt{s}=$ 13 TeV with the ATLAS detector","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1458270?version=1","version":1}