{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.78219.v1/t40","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1615470"}},{"@id":"https://doi.org/10.1140/epjc/s10052-017-5445-x","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Dataset","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2017","description":"Observed exclusion contour as a function of $m_{\\tilde{t}_1}$ and $m_{\\tilde{\\chi}^0_1}$ in the pMSSM model described in the text. Pair production...","distribution":[{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/128764/root","description":"ROOT file","encodingFormat":"https://root.cern"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/128764/yaml","description":"YAML file","encodingFormat":"https://yaml.org"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/128764/csv","description":"CSV file","encodingFormat":"text/csv"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/128764/yoda","description":"YODA file","encodingFormat":"https://yoda.hepforge.org"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/128764/yoda.h5","description":"YODA.H5 file","encodingFormat":"https://yoda.hepforge.org"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1615470?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/78219"}],"inLanguage":"en","includedInDataCatalog":{"@id":"https://doi.org/10.17182/hepdata.78219.v1","@type":"DataCatalog","url":"https://www.hepdata.net/record/ins1615470?version=1"},"isPartOf":{"@id":"https://doi.org/10.17182/hepdata.78219.v1","@type":"Dataset","description":"The results of a search for direct pair production of top squarks in events with two leptons (electrons or muons) are reported, using 36.1 fb$^{-1}$ of integrated luminosity from proton--proton collisions at $\\sqrt{s}=13$ TeV collected by the ATLAS detector at the Large Hadron Collider. To cover a range of mass differences between the top squark $\\tilde{t}$ and lighter supersymmetric particles, four possible decay modes of the top squark are targeted with dedicated selections: the decay $\\tilde{t} \\rightarrow b \\tilde{\\chi}_{1}^{\\pm}$ into a $b$-quark and the lightest chargino, the decay $\\tilde{t} \\rightarrow t \\tilde{\\chi}_{1}^{0}$ into an on-shell top quark and the lightest neutralino, the three-body decay $\\tilde{t} \\rightarrow b W \\tilde{\\chi}_{1}^{0}$ and the four-body decay $\\tilde{t} \\rightarrow b \\ell \\nu \\tilde{\\chi}_{1}^{0}$. No significant excess of events is observed above the Standard Model background for any selection, and limits on top squarks are set as a function of the $\\tilde{t}$ and $\\tilde{\\chi}_{1}^{0}$  masses. The results exclude at 95% confidence level $\\tilde{\\chi}_{1}^{0}$ masses up to about 720 GeV, extending the exclusion region of supersymmetric parameter space covered by previous searches.","name":"Search for direct top squark pair production in final states with two leptons in $\\sqrt{s} = 13$ TeV $pp$ collisions with the ATLAS detector","url":"https://www.hepdata.net/record/ins1615470?version=1"},"keywords":"pp --> STOP1 STOP1, pp --> SBOTTOM1 SBOTTOM1, STOP1 --> TOP NEUTRALINO1, STOP1 --> TOP NEUTRALINO2, SBOTTOM1 --> BOTTOM NEUTRALINO1, SBOTTOM1 --> BOTTOM NEUTRALINO2, STOP1 --> BOTTOM CHARGINO1, SBOTTOM1 --> TOP CHARGINO1, SUSY, Third Generation, squark, stop, 13000.0","name":"Exclusion contour (obs) 4","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/78779","version":1}