{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.135454.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2182749"}},{"@id":"https://doi.org/10.1007/JHEP09(2023)149","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2023","description":"A search for supersymmetry is presented in events with a single charged lepton, electron or muon, and multiple hadronic jets. The data correspond to an integrated luminosity of 138 $\\textrm{fb}^{-1}$ of proton-proton collisions at a center-of-mass energy of 13 $\\textrm{TeV}$, recorded by the CMS experiment at the CERN LHC. The search targets gluino pair production, where the gluinos decay into final states with the lightest supersymmetric particle (LSP) and either a top quark-antiquark ($\\textrm{t}\\bar{\\textrm{t}}$) pair, or a light-flavor quark-antiquark ($\\textrm{q}\\bar{\\textrm{q}}$) pair and a virtual or on-shell $\\textrm{W}$ boson. The main backgrounds, $\\textrm{t}\\bar{\\textrm{t}}$ pair and $\\textrm{W}$+jets production, are suppressed by requirements on the azimuthal angle between the momenta of the lepton and of its reconstructed parent $\\textrm{W}$ boson candidate, and by top quark and $\\textrm{W}$ boson identification based on a machine-learning technique. The number of observed events is consistent with the expectations from standard model processes. Limits are evaluated on supersymmetric particle masses in the context of two simplified models of gluino pair production. Exclusions for gluino masses reach up to 2120 (2050) $\\textrm{GeV}$ at 95% confidence level for a model with gluino decay to a $\\textrm{t}\\bar{\\textrm{t}}$ pair (a $\\textrm{q}\\bar{\\textrm{q}}$ pair and a $\\textrm{W}$ boson) and the LSP. For the same models, limits on the mass of the LSP reach up to 1250 (1070) $\\textrm{GeV}$.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.135454.v1/t1","@type":"Dataset","description":"Signal and background distributions of the $\\Delta \\phi$ variable, as predicted by simulation, for the multi-b analysis, requiring $n_{\\textrm{jet}}\\geq6$, $L_T>250~\\mathrm{GeV}$,...","name":"Figure 2a"},{"@id":"https://doi.org/10.17182/hepdata.135454.v1/t2","@type":"Dataset","description":"Signal and background distributions of the $\\Delta \\phi$ variable, as predicted by simulation, for the zero-b analysis, requiring $n_{\\textrm{jet}}\\geq6$, $L_T>350~\\mathrm{GeV}$,...","name":"Figure 2b"},{"@id":"https://doi.org/10.17182/hepdata.135454.v1/t3","@type":"Dataset","description":"Distributions of $\\Delta\\phi$ as obtained from simulation, requiring various $\\textrm{t}$ tag multiplicities for the total background.","name":"Figure 3a"},{"@id":"https://doi.org/10.17182/hepdata.135454.v1/t4","@type":"Dataset","description":"Distributions of $\\Delta\\phi$ as obtained from simulation, requiring various $\\textrm{t}$ tag multiplicities for the signal in two representative combinations of...","name":"Figure 3b"},{"@id":"https://doi.org/10.17182/hepdata.135454.v1/t5","@type":"Dataset","description":"Results of fits to the $n_{\\textrm{b}}$ multiplicity for control regions for the muon channel and with the requirements $3\\leq n_{\\textrm{jet}}\\leq4$,...","name":"Figure 6a"},{"@id":"https://doi.org/10.17182/hepdata.135454.v1/t6","@type":"Dataset","description":"Results of fits to the $n_{\\textrm{b}}$ multiplicity for control regions for the muon channel and with the requirements $3\\leq n_{\\textrm{jet}}\\leq4$,...","name":"Figure 6b"},{"@id":"https://doi.org/10.17182/hepdata.135454.v1/t7","@type":"Dataset","description":"Jet multiplicity distribution after the single-lepton baseline selection excluding the SRs for the multi-b analysis. The simulation is normalized to...","name":"Figure 7a"},{"@id":"https://doi.org/10.17182/hepdata.135454.v1/t8","@type":"Dataset","description":"Jet multiplicity distribution after the single-lepton baseline selection excluding the SRs for the the zero-b analysis (right). The simulation is...","name":"Figure 7b"},{"@id":"https://doi.org/10.17182/hepdata.135454.v1/t9","@type":"Dataset","description":"Jet multiplicity distribution in the dilepton CRs for the multi-b analysis. The simulation is normalized to data with the SF...","name":"Figure 7c"},{"@id":"https://doi.org/10.17182/hepdata.135454.v1/t10","@type":"Dataset","description":"Jet multiplicity distribution in the dilepton CRs for the zero-b analysis. The simulation is normalized to data with the SF...","name":"Figure 7d"},{"@id":"https://doi.org/10.17182/hepdata.135454.v1/t11","@type":"Dataset","description":"The double ratio of the single-lepton and dilepton ratio between data and simulation together with fit results and their uncertainties...","name":"Figure 7e"},{"@id":"https://doi.org/10.17182/hepdata.135454.v1/t12","@type":"Dataset","description":"The double ratio of the single-lepton and dilepton ratio between data and simulation together with fit results and their uncertainties...","name":"Figure 7f"},{"@id":"https://doi.org/10.17182/hepdata.135454.v1/t13","@type":"Dataset","description":"The prefit $L_{\\mathrm{P}}$ distribution for selected electron candidates in the baseline QCD selection, with modified requirements of $n_{\\text{jet}}\\in[3,4]$ and $n_{\\mathrm{b}}=0$.","name":"Figure 8a"},{"@id":"https://doi.org/10.17182/hepdata.135454.v1/t14","@type":"Dataset","description":"The prefit $L_{\\mathrm{P}}$ distribution for anti-selected electron candidates in the baseline QCD selection, with modified requirements of $n_{\\text{jet}}\\in[3,4]$ and $n_{\\mathrm{b}}=0$.","name":"Figure 8b"},{"@id":"https://doi.org/10.17182/hepdata.135454.v1/t15","@type":"Dataset","description":"Observed event yields in the MB SRs of the multi-b analysis compared to signal and background predictions. The relative fraction...","name":"Figure 9"},{"@id":"https://doi.org/10.17182/hepdata.135454.v1/t16","@type":"Dataset","description":"Observed event yields in the MB SRs of the zero-b analysis compared to signal and background predictions. 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