{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.65323.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1304457"}},{"@id":"https://doi.org/10.1007/JHEP10(2014)024","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2014","description":"CERN-LHC.  This paper reports the results of a search for strong production of supersymmetric particles in 20.1 fb-1 of proton-proton collisions at a centre-of-mass energy of 8 TeV using the ATLAS detector at the LHC. The search is performed separately in events with either zero or at least one high-pT lepton (electron or muon), large missing transverse momentum, high jet multiplicity and at least three jets identified as originated from the fragmentation of a b-quark. No excess is observed with respect to the Standard Model predictions. The results are interpreted in the context of several supersymmetric models involving gluinos and scalar top and bottom quarks, as well as a mSUGRA/CMSSM model. Gluino masses up to 1340 GeV are excluded, depending on the model, significantly extending the previous ATLAS limits.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.65323.v1/t1","@type":"Dataset","description":".","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.65323.v1/t2","@type":"Dataset","description":".","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.65323.v1/t3","@type":"Dataset","description":".","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.65323.v1/t4","@type":"Dataset","description":".","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.65323.v1/t5","@type":"Dataset","description":".","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.65323.v1/t6","@type":"Dataset","description":".","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.65323.v1/t7","@type":"Dataset","description":".","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.65323.v1/t8","@type":"Dataset","description":".","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.65323.v1/t9","@type":"Dataset","description":".","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.65323.v1/t10","@type":"Dataset","description":"Observed 95% CL exclusion contour.","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.65323.v1/t11","@type":"Dataset","description":"Expected 95% CL exclusion contour.","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.65323.v1/t12","@type":"Dataset","description":"Observed 95% CL exclusion contour.","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.65323.v1/t13","@type":"Dataset","description":"Expected 95% CL exclusion contour.","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.65323.v1/t14","@type":"Dataset","description":"Observed 95% CL exclusion contour.","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.65323.v1/t15","@type":"Dataset","description":"Expected 95% CL exclusion contour.","name":"Table 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events.","name":"Table 29"},{"@id":"https://doi.org/10.17182/hepdata.65323.v1/t30","@type":"Dataset","description":"Acceptance [%].","name":"Table 30"},{"@id":"https://doi.org/10.17182/hepdata.65323.v1/t31","@type":"Dataset","description":"Efficiency [%].","name":"Table 31"},{"@id":"https://doi.org/10.17182/hepdata.65323.v1/t32","@type":"Dataset","description":"Experimental uncertainty.","name":"Table 32"},{"@id":"https://doi.org/10.17182/hepdata.65323.v1/t33","@type":"Dataset","description":"Expected CLs.","name":"Table 33"},{"@id":"https://doi.org/10.17182/hepdata.65323.v1/t34","@type":"Dataset","description":"Observed CLs.","name":"Table 34"},{"@id":"https://doi.org/10.17182/hepdata.65323.v1/t35","@type":"Dataset","description":"Best signal region.","name":"Table 35"},{"@id":"https://doi.org/10.17182/hepdata.65323.v1/t36","@type":"Dataset","description":"Observed 95% CL exclusion contour.","name":"Table 36"},{"@id":"https://doi.org/10.17182/hepdata.65323.v1/t37","@type":"Dataset","description":"Expected 95% CL exclusion contour.","name":"Table 37"},{"@id":"https://doi.org/10.17182/hepdata.65323.v1/t38","@type":"Dataset","description":"95% CL upper limits on the cross section [fb].","name":"Table 38"},{"@id":"https://doi.org/10.17182/hepdata.65323.v1/t39","@type":"Dataset","description":"Observed 95% CL exclusion contour.","name":"Table 39"},{"@id":"https://doi.org/10.17182/hepdata.65323.v1/t40","@type":"Dataset","description":"Expected 95% CL exclusion contour.","name":"Table 40"},{"@id":"https://doi.org/10.17182/hepdata.65323.v1/t41","@type":"Dataset","description":"95% CL upper limits on the cross section [fb].","name":"Table 41"},{"@id":"https://doi.org/10.17182/hepdata.65323.v1/t42","@type":"Dataset","description":"Number of signal events.","name":"Table 42"},{"@id":"https://doi.org/10.17182/hepdata.65323.v1/t43","@type":"Dataset","description":"Acceptance [%].","name":"Table 43"},{"@id":"https://doi.org/10.17182/hepdata.65323.v1/t44","@type":"Dataset","description":"Efficiency [%].","name":"Table 44"},{"@id":"https://doi.org/10.17182/hepdata.65323.v1/t45","@type":"Dataset","description":"Uncertainty [%].","name":"Table 45"},{"@id":"https://doi.org/10.17182/hepdata.65323.v1/t46","@type":"Dataset","description":"Expected CLs.","name":"Table 46"},{"@id":"https://doi.org/10.17182/hepdata.65323.v1/t47","@type":"Dataset","description":"Observed CLs.","name":"Table 47"},{"@id":"https://doi.org/10.17182/hepdata.65323.v1/t48","@type":"Dataset","description":"Best signal region.","name":"Table 48"},{"@id":"https://doi.org/10.17182/hepdata.65323.v1/t49","@type":"Dataset","description":"Best signal region.","name":"Table 49"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1304457?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/65323"}],"inLanguage":"en","name":"Search for strong production of supersymmetric particles in final states with missing transverse momentum and at least three $b$-jets at $\\sqrt{s}$= 8 TeV proton-proton collisions with the ATLAS detector","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1304457?version=1","version":1}