{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.57742.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/893493"}},{"@id":"https://doi.org/10.1016/j.physletb.2011.06.015","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2011","description":"CERN-LHC. A search for SUSY particles in 7 TeV proton-proton collisions in events with large  missing transverse momentum and at least one heavy flavour jet.  The data, with a total integrated luminosity of 35 pb-1, are analysed in the zero-lepton plus 3 jets and one-lepton plus 2 jet  channels with at least one of the jets being a heavy flavour candidate.  Jets are defined with the anti-Kt algorithm with R=0.4. In the zero-lepton data the effective mass (M(C=EFFECTIVE)) is defined as the scalar sum of the missing transverse energy and  the transverse momenta of the highest PT jets.  In the one-lepton data the transverse mas (MT) is  constructed from the highest PT lepton and the missing ET.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.57742.v1/t1","@type":"Dataset","description":"Distribution of the effective mass for data and the SM expectation in the zero-lepton plus 3 jet channel.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.57742.v1/t2","@type":"Dataset","description":"Distribution of the missing ET for data and the SM expectation in the zero-lepton plus 3 jet channel.","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.57742.v1/t3","@type":"Dataset","description":"Distribution of the effective mass for data and the SM expectation in the one-lepton plus 2 jet channel.","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.57742.v1/t4","@type":"Dataset","description":"Distribution of the missing ET for data and the SM expectation in the one-lepton plus 2 jet channel.","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.57742.v1/t5","@type":"Dataset","description":"Observed 95 PCT exclusion limit in the M(gluino), M(sbottom) plane obtained with the zero-lepton channel data.","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.57742.v1/t6","@type":"Dataset","description":"Expected 95 PCT exclusion limit in the M(gluino), M(sbottom) plane obtained with the zero-lepton channel data.","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.57742.v1/t7","@type":"Dataset","description":"Observed and expected 95 PCT CL upper limits on the gluino-mediated and stop pair production cross section as a function...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.57742.v1/t8","@type":"Dataset","description":"Observed and expected 95 PCT CL upper limits on the gluino-mediated and stop pair production cross section as a function...","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.57742.v1/t9","@type":"Dataset","description":"Observed 95 PCT CL exclusion limits from the zero-lepton analysis on the MSUGRA/CMSSM scenario with tan(beta) = 40, A0 =...","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.57742.v1/t10","@type":"Dataset","description":"Expected 95 PCT CL exclusion limits from the zero-lepton analysis on the MSUGRA/CMSSM scenario with tan(beta) = 40, A0 =...","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.57742.v1/t11","@type":"Dataset","description":"Observed 95 PCT CL exclusion limits from the one-lepton analysis on the MSUGRA/CMSSM scenario with tan(beta) = 40, A0 =...","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.57742.v1/t12","@type":"Dataset","description":"Expected 95 PCT CL exclusion limits from the one-lepton analysis on the MSUGRA/CMSSM scenario with tan(beta) = 40, A0 =...","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.57742.v1/t13","@type":"Dataset","description":"Observed 95 PCT CL exclusion limits from the combined zero and one-lepton analyses on the MSUGRA/CMSSM scenario with tan(beta) =...","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.57742.v1/t14","@type":"Dataset","description":"Expected 95 PCT CL exclusion limits from the combined zero and one-lepton analyses on the MSUGRA/CMSSM scenario with tan(beta) =...","name":"Table 14"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins893493?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/57742"}],"inLanguage":"en","name":"Search for supersymmetry in pp collisions at sqrt{s} = 7TeV in final states with missing transverse momentum and b-jets","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins893493?version=1","version":1}