{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.156121.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2962374"}},{"@id":"https://doi.org/10.1103/b26z-zmpy","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2025","description":"A general search is presented for supersymmetric particles (sparticles) in scenarios featuring compressed mass spectra using proton-proton collisions at a center-of-mass energy of 13 TeV, recorded with the CMS detector at the LHC. The analyzed data sample corresponds to an integrated luminosity of 138 fb$^{-1}$ . A wide range of potential sparticle signatures are targeted, including pair production of electroweakinos, sleptons, and top squarks. The search focuses on events with a high transverse momentum system from initial-state-radiation jets recoiling against a potential sparticle system with significant missing transverse momentum. Events are categorized based on their lepton multiplicity, jet multiplicity, number of b-tagged jets, and kinematic variables sensitive to the sparticle masses and mass splittings. The sensitivity extends to higher parent sparticle masses than previously probed at the LHC for production of pairs of electroweakinos, sleptons, and top squarks with mass spectra featuring small mass splittings (compressed mass spectra). The observed results demonstrate agreement with the predictions of the background-only model. Lower mass limits are set at 95% confidence level on production of pairs of electroweakinos, sleptons, and top squarks that extend to 325, 275, and 780 GeV, respectively, for the most favorable compressed mass regime cases.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.156121.v1/t1","@type":"Dataset","description":"Event counts observed in data, $N_{\\rm{obs}}$, in each of the model-independent bins, compared with predictions from the control region fit,...","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.156121.v1/t2","@type":"Dataset","description":"Top squark pair production. Observed upper limits at 95% CL on the product of the cross section and relevant branching...","name":"Figure 24 T2tt"},{"@id":"https://doi.org/10.17182/hepdata.156121.v1/t3","@type":"Dataset","description":"Top squark pair production. Observed upper limits at 95% CL on the product of the cross section and relevant branching...","name":"Figure 24 T2bW"},{"@id":"https://doi.org/10.17182/hepdata.156121.v1/t4","@type":"Dataset","description":"Observed upper limits at 95% CL on the product of the cross section and branching fraction squared, $\\sigma (\\tilde{\\mathrm{t}} \\,...","name":"Figure 25 T2cc"},{"@id":"https://doi.org/10.17182/hepdata.156121.v1/t5","@type":"Dataset","description":"Chargino-neutralino production. Observed upper limits at 95% CL on the product of the cross section and the two branching fractions,...","name":"Figure 26 TChiWZ Wino"},{"@id":"https://doi.org/10.17182/hepdata.156121.v1/t6","@type":"Dataset","description":"Chargino-neutralino production. Observed upper limits at 95% CL on the product of the cross section and the two branching fractions,...","name":"Figure 26 TChiWZ Higgsino"},{"@id":"https://doi.org/10.17182/hepdata.156121.v1/t7","@type":"Dataset","description":"Chargino pair production. The left panel shows the observed upper limits at 95% CL on the product of the cross...","name":"Figure 27 TChipmWW Wino"},{"@id":"https://doi.org/10.17182/hepdata.156121.v1/t8","@type":"Dataset","description":"Chargino pair production. The left panel shows the observed upper limits at 95% CL on the product of the cross...","name":"Figure 27 TChiSlepSnu Wino"},{"@id":"https://doi.org/10.17182/hepdata.156121.v1/t9","@type":"Dataset","description":"Slepton pair production. Observed 95% CL upper limits on the product of the cross section and branching fraction squared for...","name":"Figure 29 TSlepSlep e mu LR"},{"@id":"https://doi.org/10.17182/hepdata.156121.v1/t10","@type":"Dataset","description":"Slepton pair production. Observed 95% CL upper limits on the product of the cross section and branching fraction squared for...","name":"Figure 29 TSlepSlep e mu L"},{"@id":"https://doi.org/10.17182/hepdata.156121.v1/t11","@type":"Dataset","description":"Slepton pair production. Observed 95% CL upper limits on the product of the cross section and branching fraction squared for...","name":"Figure 29 TSlepSlep e mu R"},{"@id":"https://doi.org/10.17182/hepdata.156121.v1/t12","@type":"Dataset","description":"Slepton pair production. Observed 95% CL upper limits on the cross section times branching fraction squared for direct selectron pair...","name":"Figure 30 TSlepSlep e LR"},{"@id":"https://doi.org/10.17182/hepdata.156121.v1/t13","@type":"Dataset","description":"Slepton pair production. Observed 95% CL upper limits on the cross section times branching fraction squared for direct selectron pair...","name":"Figure 30 TSlepSlep e L"},{"@id":"https://doi.org/10.17182/hepdata.156121.v1/t14","@type":"Dataset","description":"Slepton pair production. Observed 95% CL upper limits on the cross section times branching fraction squared for direct selectron pair...","name":"Figure 30 TSlepSlep e R"},{"@id":"https://doi.org/10.17182/hepdata.156121.v1/t15","@type":"Dataset","description":"Slepton pair production. Observed 95% CL upper limits on the cross section times branching fraction squared for direct selectron pair...","name":"Figure 30 TSlepSlep mu LR"},{"@id":"https://doi.org/10.17182/hepdata.156121.v1/t16","@type":"Dataset","description":"Slepton pair production. Observed 95% CL upper limits on the cross section times branching fraction squared for direct selectron pair...","name":"Figure 30 TSlepSlep mu L"},{"@id":"https://doi.org/10.17182/hepdata.156121.v1/t17","@type":"Dataset","description":"Slepton pair production. Observed 95% CL upper limits on the cross section times branching fraction squared for direct selectron pair...","name":"Figure 30 TSlepSlep mu R"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins2962374?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/156121"}],"inLanguage":"en","name":"General search for supersymmetric particles in scenarios with compressed mass spectra using proton-proton collisions at $\\sqrt{s}$ = 13 TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins2962374?version=1","version":1}
