{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.61814.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1466302"}},{"@id":"https://doi.org/10.1103/PhysRevD.94.032003","@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 involving the pair production of gluinos decaying via third-generation squarks to the lightest neutralino is reported. It uses an LHC proton--proton dataset at a center-of-mass energy $\\sqrt{s} = 13$ TeV with an integrated luminosity of 3.2 fb$^{-1}$ collected with the ATLAS detector in 2015. The signal is searched for in events containing several energetic jets, of which at least three must be identified as $b$-jets, large missing transverse momentum and, potentially, isolated electrons or muons. Large-radius jets with a high mass are also used to identify highly boosted top quarks. No excess is found above the predicted background. For neutralino masses below approximately 700 GeV, gluino masses of less than 1.78 TeV and 1.76 TeV are excluded at the 95% CL in simplified models of the pair production of gluinos decaying via sbottom and stop, respectively. These results significantly extend the exclusion limits obtained with the $\\sqrt{s} = 8$ TeV dataset.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.61814.v1/t1","@type":"Dataset","description":"Distribution of missing transverse energy for SR-Gbb-B.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.61814.v1/t2","@type":"Dataset","description":"Distribution of missing transverse energy for SR-Gtt-0L-C.","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.61814.v1/t3","@type":"Dataset","description":"Distribution of missing transverse energy for SR-Gtt-1L-A.","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.61814.v1/t4","@type":"Dataset","description":"Expected 95% CL exclusion contour for the Gbb signal.","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.61814.v1/t5","@type":"Dataset","description":"Observed 95% CL exclusion contour for the Gbb signal.","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.61814.v1/t6","@type":"Dataset","description":"Expected 95% CL exclusion contour for the Gtt combination.","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.61814.v1/t7","@type":"Dataset","description":"Observed 95% CL exclusion contour for the Gtt combination.","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.61814.v1/t8","@type":"Dataset","description":"Acceptances for the Gbb model in SR-Gbb-A. Acceptance is evaluated at truth level, with only leptons from heavy bosons and...","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.61814.v1/t9","@type":"Dataset","description":"Acceptances for the Gbb model in SR-Gbb-B. Acceptance is evaluated at truth level, with only leptons from heavy bosons and...","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.61814.v1/t10","@type":"Dataset","description":"Acceptances for the Gbb model in SR-Gbb-C. Acceptance is evaluated at truth level, with only leptons from heavy bosons and...","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.61814.v1/t11","@type":"Dataset","description":"Acceptances for the Gtt model in SR-Gtt-0L-A. Acceptance is evaluated at truth level, with only leptons from heavy bosons and...","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.61814.v1/t12","@type":"Dataset","description":"Acceptances for the Gtt model in SR-Gtt-0L-B. Acceptance is evaluated at truth level, with only leptons from heavy bosons and...","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.61814.v1/t13","@type":"Dataset","description":"Acceptances for the Gtt model in SR-Gtt-0L-C. Acceptance is evaluated at truth level, with only leptons from heavy bosons and...","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.61814.v1/t14","@type":"Dataset","description":"Acceptances for the Gtt model in SR-Gtt-1L-A. Acceptance is evaluated at truth level, with only leptons from heavy bosons and...","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.61814.v1/t15","@type":"Dataset","description":"Acceptances for the Gtt model in SR-Gtt-1L-B. Acceptance is evaluated at truth level, with only leptons from heavy bosons and...","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.61814.v1/t16","@type":"Dataset","description":"Acceptance times efficiency for the Gbb model in SR-Gbb-A.","name":"Table 16"},{"@id":"https://doi.org/10.17182/hepdata.61814.v1/t17","@type":"Dataset","description":"Acceptance times efficiency for the Gbb model in SR-Gbb-B.","name":"Table 17"},{"@id":"https://doi.org/10.17182/hepdata.61814.v1/t18","@type":"Dataset","description":"Acceptance times efficiency for the Gbb model in SR-Gbb-C.","name":"Table 18"},{"@id":"https://doi.org/10.17182/hepdata.61814.v1/t19","@type":"Dataset","description":"Acceptance times efficiency for the Gtt model in SR-Gtt-0L-A.","name":"Table 19"},{"@id":"https://doi.org/10.17182/hepdata.61814.v1/t20","@type":"Dataset","description":"Acceptance times efficiency for the Gtt model in SR-Gtt-0L-B.","name":"Table 20"},{"@id":"https://doi.org/10.17182/hepdata.61814.v1/t21","@type":"Dataset","description":"Acceptance times efficiency for the Gtt model in SR-Gtt-0L-C.","name":"Table 21"},{"@id":"https://doi.org/10.17182/hepdata.61814.v1/t22","@type":"Dataset","description":"Acceptance times efficiency for the Gtt model in SR-Gtt-1L-A.","name":"Table 22"},{"@id":"https://doi.org/10.17182/hepdata.61814.v1/t23","@type":"Dataset","description":"Acceptance times efficiency for the Gtt model in SR-Gtt-1L-B.","name":"Table 23"},{"@id":"https://doi.org/10.17182/hepdata.61814.v1/t24","@type":"Dataset","description":"95% CL upper limit on the cross-section times branching ratio (in fb) for the Gbb model in SR-Gbb-A.","name":"Table 24"},{"@id":"https://doi.org/10.17182/hepdata.61814.v1/t25","@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 25"},{"@id":"https://doi.org/10.17182/hepdata.61814.v1/t26","@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 26"},{"@id":"https://doi.org/10.17182/hepdata.61814.v1/t27","@type":"Dataset","description":"95% CL upper limit on the cross-section times branching ratio (in fb) for the Gtt model in SR-Gtt-0L-A.","name":"Table 27"},{"@id":"https://doi.org/10.17182/hepdata.61814.v1/t28","@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 28"},{"@id":"https://doi.org/10.17182/hepdata.61814.v1/t29","@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 29"},{"@id":"https://doi.org/10.17182/hepdata.61814.v1/t30","@type":"Dataset","description":"95% CL upper limit on the cross-section times branching ratio (in fb) for the Gtt model in SR-Gtt-1L-A.","name":"Table 30"},{"@id":"https://doi.org/10.17182/hepdata.61814.v1/t31","@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 31"},{"@id":"https://doi.org/10.17182/hepdata.61814.v1/t32","@type":"Dataset","description":"Signal region yielding the best expected sensitivity for each point of the parameter space in the Gbb model.","name":"Table 32"},{"@id":"https://doi.org/10.17182/hepdata.61814.v1/t33","@type":"Dataset","description":"Signal region yielding the best expected sensitivity for each point of the parameter space in the Gtt model for the...","name":"Table 33"},{"@id":"https://doi.org/10.17182/hepdata.61814.v1/t34","@type":"Dataset","description":"Signal region yielding the best expected sensitivity for each point of the parameter space in the Gtt model for the...","name":"Table 34"},{"@id":"https://doi.org/10.17182/hepdata.61814.v1/t35","@type":"Dataset","description":"Combination of two 0-lepton and 1-lepton signal regions yielding the best expected sensitivity for each point of the parameter space...","name":"Table 35"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1466302?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/61814"}],"inLanguage":"en","name":"Search for pair production of gluinos decaying via stop and sbottom in events with $b$-jets and large missing transverse momentum in $pp$ 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/ins1466302?version=1","version":1}