{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.79414.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1599402"}},{"@id":"https://doi.org/10.1103/PhysRevLett.119.151802","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2018","description":"CERN-LHC. CMS. Results are reported from a search for supersymmetric particles in proton-proton collisions in the final state with a single lepton; multiple jets, including at least one b-tagged jet; and large missing transverse momentum. The search uses a sample of proton-proton collision data at sqrt{s}= 13 TeV recorded by the CMS experiment at the LHC, corresponding to an integrated luminosity of 35.9 fb\u22121. The observed event yields in the signal regions are consistent with those expected from standard model backgrounds. The results are interpreted in the context of simplified models of supersymmetry involving gluino pair production, with gluino decay into either on- or off-mass-shell top squarks. Assuming that the top squarks decay into a top quark plus a stable, weakly interacting neutralino, scenarios with gluino masses up to about 1.9 TeV are excluded at 95% confidence level for neutralino masses up to about 1 TeV.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.79414.v1/t1","@type":"Dataset","description":"Figure 2. Cross section upper limit (95% CL) on T1tttt cross section","name":"Figure 2 Upper limit (95% CL) on T1tttt cross section"},{"@id":"https://doi.org/10.17182/hepdata.79414.v1/t2","@type":"Dataset","description":"Figure 2. Excluded gluino and neutralino masses at 95% CL for the T1tttt.","name":"Figure 2 T1tttt Observed limit"},{"@id":"https://doi.org/10.17182/hepdata.79414.v1/t3","@type":"Dataset","description":"Figure 2. +1 sigma excluded gluino and neutralino masses at 95% CL for the T1tttt.","name":"Figure 2 T1tttt Observed limit (+1sigma)"},{"@id":"https://doi.org/10.17182/hepdata.79414.v1/t4","@type":"Dataset","description":"Figure 2. -1 sigma excluded gluino and neutralino masses at 95% CL for the T1tttt.","name":"Figure 2 T1tttt Observed limit (-1sigma)"},{"@id":"https://doi.org/10.17182/hepdata.79414.v1/t5","@type":"Dataset","description":"Figure 2. Expected exclusion for the T1tttt model.","name":"Figure 2 T1tttt expected limit"},{"@id":"https://doi.org/10.17182/hepdata.79414.v1/t6","@type":"Dataset","description":"Figure 2. +1 sigma expected exclusion for the T1tttt model.","name":"Figure 2 T1tttt expected limit (+1sigma)"},{"@id":"https://doi.org/10.17182/hepdata.79414.v1/t7","@type":"Dataset","description":"Figure 2. -1 sigma expected exclusion for the T1tttt model.","name":"Figure 2 T1tttt expected limit (-1sigma)"},{"@id":"https://doi.org/10.17182/hepdata.79414.v1/t8","@type":"Dataset","description":"Figure 2. Excluded gluino and neutralino masses at 95% CL for the T5tttt.","name":"Figure 2 T5tttt observed limit"},{"@id":"https://doi.org/10.17182/hepdata.79414.v1/t9","@type":"Dataset","description":"Figure 2. Expected exclusion for the T5tttt model.","name":"Figure 2 T5tttt expected limit"},{"@id":"https://doi.org/10.17182/hepdata.79414.v1/t10","@type":"Dataset","description":"Table 1. Observed event yields and mean background yields from the predictive fit in the 18 bins of the signal...","name":"Table 1 Yields in the 18 bins of the signal region R4."},{"@id":"https://doi.org/10.17182/hepdata.79414.v1/t11","@type":"Dataset","description":"Table 2. Observed event yields and mean background yields from the predictive fit in four aggregate search bins.","name":"Table 2 Yields in aggregate search bins."}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1599402?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/79414"}],"inLanguage":"en","name":"Search for Supersymmetry in $pp$ Collisions at $\\sqrt{s}=13\\text{ }\\text{ }\\mathrm{TeV}$ in the Single-Lepton Final State Using the Sum of Masses of Large-Radius Jets","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1599402?version=1","version":1}