{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.172453.v2","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/3168562"}}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2026","description":"This paper presents a search for beyond the standard model physics using single-lepton events with a high multiplicity of jets, including those identified as bottom quark jets, without a requirement on missing transverse momentum. The analysis is based on proton-proton collision data collected with the CMS detector at the CERN LHC at a center-of-mass energy of 13 \\TeV, corresponding to an integrated luminosity of 138 fb${}^{-1}$. This search is sensitive to $R$-parity violating supersymmetry models, where supersymmetric particles can decay into standard-model particles through interactions that violate baryon number conservation. In particular, the signal model considered is gluino pair production, where each gluino decays into top, bottom, and strange quarks. The sum of large-radius jet masses is used to distinguish the signal from background, as it effectively captures the features of high jet multiplicity and high interaction energy. No significant excess of data over the background predictions is observed. Gluinos in this model have been excluded for masses below 1890 GeV at 95% confidence level.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.172453.v2/t1","@type":"Dataset","description":"Comparison of $M_{\\rm{J}}$ shapes between data and simulation in the control regions used to measure the $\\kappa$ factors for QCD...","name":"Figure 3a"},{"@id":"https://doi.org/10.17182/hepdata.172453.v2/t2","@type":"Dataset","description":"Comparison of $M_{\\rm{J}}$ shapes between data and simulation in the control regions used to measure the $\\kappa$ factors for W+jets.","name":"Figure 3b"},{"@id":"https://doi.org/10.17182/hepdata.172453.v2/t3","@type":"Dataset","description":"Comparison of $M_{\\rm{J}}$ shapes between data and simulation in the control regions used to measure the $\\kappa$ factors for ttbar.","name":"Figure 3c"},{"@id":"https://doi.org/10.17182/hepdata.172453.v2/t4","@type":"Dataset","description":"The $\\kappa$ factors measured in control regions for the QCD multijet, W+jets, and ttbar backgrounds.","name":"Figure 4"},{"@id":"https://doi.org/10.17182/hepdata.172453.v2/t5","@type":"Dataset","description":"Background-only post-fit $M_{\\rm{J}}$ distributions in the $N_{\\rm{lep}}=1$ region for all three data-taking years, with pre-fit signal overlaid.","name":"Figure 5"},{"@id":"https://doi.org/10.17182/hepdata.172453.v2/t6","@type":"Dataset","description":"Cross section upper limits at 95% CL compared to the predicted cross section of gluino pair production with decays to...","name":"Figure 6"},{"@id":"https://doi.org/10.17182/hepdata.172453.v2/t7","@type":"Dataset","description":"Signal yields and efficiencies at each selection step for the signal region, for gluino masses of 1200 and 1800 GeV,...","name":"Additional Table - Cutflows"},{"@id":"https://doi.org/10.17182/hepdata.172453.v2/t8","@type":"Dataset","description":"Signal efficiencies for all gluino mass points in each signal region, corresponding to the full Run 2. In addition to...","name":"Additional Table - Signal efficiency"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins3168562?version=2"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/172453"}],"inLanguage":"en","name":"Search for new physics using single-lepton events with high multiplicities of jets and b jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins3168562?version=2","version":2}