{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.79060.v4","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1634607"}},{"@id":"https://doi.org/10.1007/JHEP06(2018)107","@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 involving the pair production of gluinos decaying via third-generation squarks into the lightest neutralino ($\\displaystyle\\tilde\\chi^0_1$) is reported. It uses LHC proton--proton collision data at a centre-of-mass energy $\\sqrt{s} = 13$ TeV with an integrated luminosity of 36.1 fb$^{-1}$ collected with the ATLAS detector in 2015 and 2016. The search is performed in events containing large missing transverse momentum and several energetic jets, at least three of which must be identified as originating from $b$-quarks. To increase the sensitivity, the sample is divided into subsamples based on the presence or absence of electrons or muons. No excess is found above the predicted background. For $\\displaystyle\\tilde\\chi^0_1$ masses below approximately 300 GeV, gluino masses of less than 1.97 (1.92) TeV are excluded at 95% confidence level in simplified models involving the pair production of gluinos that decay via top (bottom) squarks. An interpretation of the limits in terms of the branching ratios of the gluinos into third-generation squarks is also provided. These results improve upon the exclusion limits obtained with the 3.2 fb$^{-1}$ of data collected in 2015.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t1","@type":"Dataset","description":"Observed 95% CL exclusion contour for Gtt model.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t2","@type":"Dataset","description":"Expected 95% CL exclusion contour for Gtt model.","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t3","@type":"Dataset","description":"Observed 95% CL exclusion contour for Gbb model.","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t4","@type":"Dataset","description":"Expected 95% CL exclusion contour for Gbb model.","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t5","@type":"Dataset","description":"Expected 95% CL exclusion contour for Gluino mass = 1.8 TeV, Neutralino mass = 1 GeV.","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t6","@type":"Dataset","description":"Observed 95% CL exclusion contour for Gluino mass = 1.8 TeV, Neutralino mass = 1 GeV.","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t7","@type":"Dataset","description":"Expected 95% CL exclusion contour for Gluino mass = 1.9 TeV, Neutralino mass = 1 GeV.","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t8","@type":"Dataset","description":"Observed 95% CL exclusion contour for Gluino mass = 1.9 TeV, Neutralino mass = 1 GeV.","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t9","@type":"Dataset","description":"Expected 95% CL exclusion contour for Gluino mass = 2.0 TeV, Neutralino mass = 1 GeV.","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t10","@type":"Dataset","description":"Observed 95% CL exclusion contour for Gluino mass = 2.0 TeV, Neutralino mass = 1 GeV.","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t11","@type":"Dataset","description":"Expected 95% CL exclusion contour for Gluino mass = 1.9 TeV, Neutralino mass = 1 GeV.","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t12","@type":"Dataset","description":"Observed 95% CL exclusion contour for Gluino mass = 1.9 TeV, Neutralino mass = 1 GeV.","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t13","@type":"Dataset","description":"Expected 95% CL exclusion contour for Gluino mass = 1.9 TeV, Neutralino mass = 600 GeV.","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t14","@type":"Dataset","description":"Observed 95% CL exclusion contour for Gluino mass = 1.9 TeV, Neutralino mass = 600 GeV.","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t15","@type":"Dataset","description":"Expected 95% CL exclusion contour for Gluino mass = 1.9 TeV, Neutralino mass = 1 TeV.","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t16","@type":"Dataset","description":"Observed 95% CL exclusion contour for Gluino mass = 1.9 TeV, Neutralino mass = 1 TeV.","name":"Table 16"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t17","@type":"Dataset","description":"Distribution of ETMISS for SR-Gbb-VC.","name":"Table 17"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t18","@type":"Dataset","description":"Distribution of ETMISS for SR-Gtt-1l-B.","name":"Table 18"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t19","@type":"Dataset","description":"Distribution of ETMISS for SR-1L-II.","name":"Table 19"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t20","@type":"Dataset","description":"Distribution of ETMISS for SR-0L-HI.","name":"Table 20"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t21","@type":"Dataset","description":"Distribution of ETMISS for SR-0L-HH.","name":"Table 21"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t22","@type":"Dataset","description":"Acceptances for Gbb model in SR-Gbb-B.","name":"Table 22"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t23","@type":"Dataset","description":"Acceptances for Gbb model in SR-Gbb-M.","name":"Table 23"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t24","@type":"Dataset","description":"Acceptances for Gbb model in SR-Gbb-C.","name":"Table 24"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t25","@type":"Dataset","description":"Acceptances for Gbb model in SR-Gbb-VC.","name":"Table 25"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t26","@type":"Dataset","description":"Acceptances for Gtt model in SR-Gtt-0l-B.","name":"Table 26"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t27","@type":"Dataset","description":"Acceptances for Gtt model in SR-Gtt-0l-M.","name":"Table 27"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t28","@type":"Dataset","description":"Acceptances for Gtt model in SR-Gtt-0l-C.","name":"Table 28"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t29","@type":"Dataset","description":"Acceptances for Gtt model in SR-Gtt-1l-B.","name":"Table 29"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t30","@type":"Dataset","description":"Acceptances for Gtt model in SR-Gtt-1l-M.","name":"Table 30"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t31","@type":"Dataset","description":"Acceptances for Gtt model in SR-Gtt-1l-C.","name":"Table 31"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t32","@type":"Dataset","description":"Experimental efficiencies for Gbb model in SR-Gbb-B.","name":"Table 32"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t33","@type":"Dataset","description":"Experimental efficiencies for Gbb model in SR-Gbb-M.","name":"Table 33"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t34","@type":"Dataset","description":"Experimental efficiencies for Gbb model in SR-Gbb-C.","name":"Table 34"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t35","@type":"Dataset","description":"Experimental efficiencies for Gbb model in SR-Gbb-VC.","name":"Table 35"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t36","@type":"Dataset","description":"Experimental efficiencies for Gtt model in SR-Gtt-0l-B.","name":"Table 36"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t37","@type":"Dataset","description":"Experimental efficiencies for Gtt model in SR-Gtt-0l-M.","name":"Table 37"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t38","@type":"Dataset","description":"Experimental efficiencies for Gtt model in SR-Gtt-0l-C.","name":"Table 38"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t39","@type":"Dataset","description":"Experimental efficiencies for Gtt model in SR-Gtt-1l-B.","name":"Table 39"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t40","@type":"Dataset","description":"Experimental efficiencies for Gtt model in SR-Gtt-1l-M.","name":"Table 40"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t41","@type":"Dataset","description":"Experimental efficiencies for Gtt model in SR-Gtt-0l-C.","name":"Table 41"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t42","@type":"Dataset","description":"95% CL upper limit on the cross-section times branching ratio (in fb) for the Gbb model.","name":"Table 42"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t43","@type":"Dataset","description":"95% CL upper limit on the cross-section times branching ratio (in fb) for the Gtt model.","name":"Table 43"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t44","@type":"Dataset","description":"95% CL upper limit on the cross-section times branching ratio (in fb) for the Gbb model in SR-Gbb-B.","name":"Table 44"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t45","@type":"Dataset","description":"95% CL upper limit on the cross-section times branching ratio (in fb) for the Gbb model in SR-Gbb-M.","name":"Table 45"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t46","@type":"Dataset","description":"95% CL upper limit on the cross-section times branching ratio (in fb) for the Gbb model in SR-Gbb-C.","name":"Table 46"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t47","@type":"Dataset","description":"95% CL upper limit on the cross-section times branching ratio (in fb) for the Gbb model in SR-Gbb-VC.","name":"Table 47"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t48","@type":"Dataset","description":"95% CL upper limit on the cross-section times branching ratio (in fb) for the Gtt model in SR-Gtt-0l-B.","name":"Table 48"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t49","@type":"Dataset","description":"95% CL upper limit on the cross-section times branching ratio (in fb) for the Gtt model in SR-Gtt-0l-M.","name":"Table 49"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t50","@type":"Dataset","description":"95% CL upper limit on the cross-section times branching ratio (in fb) for the Gtt model in SR-Gtt-0l-C.","name":"Table 50"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t51","@type":"Dataset","description":"95% CL upper limit on the cross-section times branching ratio (in fb) for the Gtt model in SR-Gtt-1l-B.","name":"Table 51"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t52","@type":"Dataset","description":"95% CL upper limit on the cross-section times branching ratio (in fb) for the Gtt model in SR-Gtt-1l-M.","name":"Table 52"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t53","@type":"Dataset","description":"95% CL upper limit on the cross-section times branching ratio (in fb) for the Gtt model in SR-Gtt-1l-C.","name":"Table 53"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t54","@type":"Dataset","description":"Observed 95% CL exclusion contour for Gbb model in SR-Gbb-B.","name":"Table 54"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t55","@type":"Dataset","description":"Expected 95% CL exclusion contour for Gbb model in SR-Gbb-B.","name":"Table 55"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t56","@type":"Dataset","description":"Observed 95% CL exclusion contour for Gbb model in SR-Gbb-M.","name":"Table 56"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t57","@type":"Dataset","description":"Expected 95% CL exclusion contour for Gbb model in SR-Gbb-M.","name":"Table 57"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t58","@type":"Dataset","description":"Observed 95% CL exclusion contour for Gbb model in SR-Gbb-C.","name":"Table 58"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t59","@type":"Dataset","description":"Expected 95% CL exclusion contour for Gbb model in SR-Gbb-C.","name":"Table 59"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t60","@type":"Dataset","description":"Observed 95% CL exclusion contour for Gbb model in SR-Gbb-VC.","name":"Table 60"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t61","@type":"Dataset","description":"Expected 95% CL exclusion contour for Gbb model in SR-Gbb-VC.","name":"Table 61"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t62","@type":"Dataset","description":"Observed 95% CL exclusion contour for Gtt model in SR-Gtt-0l-B.","name":"Table 62"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t63","@type":"Dataset","description":"Expected 95% CL exclusion contour for Gtt model in SR-Gtt-0l-B.","name":"Table 63"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t64","@type":"Dataset","description":"Observed 95% CL exclusion contour for Gtt model in SR-Gtt-0l-M.","name":"Table 64"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t65","@type":"Dataset","description":"Expected 95% CL exclusion contour for Gtt model in SR-Gtt-0l-M.","name":"Table 65"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t66","@type":"Dataset","description":"Observed 95% CL exclusion contour for Gtt model in SR-Gtt-0l-C.","name":"Table 66"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t67","@type":"Dataset","description":"Expected 95% CL exclusion contour for Gtt model in SR-Gtt-0l-C.","name":"Table 67"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t68","@type":"Dataset","description":"Observed 95% CL exclusion contour for Gtt model in SR-Gtt-1l-B.","name":"Table 68"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t69","@type":"Dataset","description":"Expected 95% CL exclusion contour for Gtt model in SR-Gtt-1l-B.","name":"Table 69"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t70","@type":"Dataset","description":"Observed 95% CL exclusion contour for Gtt model in SR-Gtt-1l-M.","name":"Table 70"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t71","@type":"Dataset","description":"Expected 95% CL exclusion contour for Gtt model in SR-Gtt-1l-M.","name":"Table 71"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t72","@type":"Dataset","description":"Observed 95% CL exclusion contour for Gtt model in SR-Gtt-1l-C.","name":"Table 72"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t73","@type":"Dataset","description":"Expected 95% CL exclusion contour for Gtt model in SR-Gtt-1l-C.","name":"Table 73"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t74","@type":"Dataset","description":"Expected number of signal events after each step of the Gbb-0L-B selection for a Gbb signal point (MGLUON,MNEUTRALINO) = (1900,1400)...","name":"Table 74"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t75","@type":"Dataset","description":"Expected number of signal events after each step of the Gbb-0L-M selection for a Gbb signal point (MGLUON,MNEUTRALINO) = (1900,1400)...","name":"Table 75"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t76","@type":"Dataset","description":"Expected number of signal events after each step of the Gbb-0L-C selection for a Gbb signal point (MGLUON,MNEUTRALINO) = (1900,1400)...","name":"Table 76"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t77","@type":"Dataset","description":"Expected number of signal events after each step of the Gbb-0L-VC selection for a Gbb signal point (MGLUON,MNEUTRALINO) = (1900,1400)...","name":"Table 77"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t78","@type":"Dataset","description":"Expected number of signal events after each step of the Gtt-1L-B selection for a Gtt signal point (MGLUON,MNEUTRALINO) = (1900,1)...","name":"Table 78"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t79","@type":"Dataset","description":"Expected number of signal events after each step of the Gtt-1L-M selection for a Gtt signal point (MGLUON,MNEUTRALINO) = (1900,1)...","name":"Table 79"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t80","@type":"Dataset","description":"Expected number of signal events after each step of the Gtt-1L-C selection for a Gtt signal point (MGLUON,MNEUTRALINO) = (1900,1)...","name":"Table 80"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t81","@type":"Dataset","description":"Expected number of signal events after each step of the Gtt-0L-B selection for a Gtt signal point (MGLUON,MNEUTRALINO) = (1900,1)...","name":"Table 81"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t82","@type":"Dataset","description":"Expected number of signal events after each step of the Gtt-0L-M selection for a Gtt signal point (MGLUON,MNEUTRALINO) = (1900,1)...","name":"Table 82"},{"@id":"https://doi.org/10.17182/hepdata.79060.v4/t83","@type":"Dataset","description":"Expected number of signal events after each step of the Gtt-0L-C selection for a Gtt signal point (MGLUON,MNEUTRALINO) = (1900,1)...","name":"Table 83"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1634607?version=4"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/79060"}],"inLanguage":"en","name":"Search for Supersymmetry in final states with missing transverse momentum and multiple $b$-jets in proton--proton collisions 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/ins1634607?version=4","version":4}