{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.82585.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1667045"}},{"@id":"https://doi.org/10.1103/PhysRevD.98.032009","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2018","description":"Results from a search for supersymmetry in events with four or more charged leptons (electrons, muons and taus) are presented. The analysis uses a data sample corresponding to $36.1$ fb$^{-1}$ of proton--proton collisions delivered by the Large Hadron Collider at $\\sqrt{s}=13$ TeV and recorded by the ATLAS detector. Four-lepton signal regions with up to two hadronically decaying taus are designed to target a range of supersymmetric scenarios that can be either enriched in or depleted of events involving the production and decay of a $Z$ boson. Data yields are consistent with Standard Model expectations and results are used to set upper limits on the event yields from processes beyond the Standard Model. Exclusion limits are set at the 95% confidence level in simplified models of General Gauge Mediated supersymmetry, where higgsino masses are excluded up to $295$ GeV. In $R$-parity-violating simplified models with decays of the lightest supersymmetric particle to charged leptons, lower limits of $1.46$ TeV, $1.06$ TeV, and $2.25$ TeV are placed on wino, slepton and gluino masses, respectively.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t1","@type":"Dataset","description":"The $m_{\\mathrm{eff}}$ distribution for events passing the signal region requirements except the $m_{\\mathrm{eff}}$ requirement in SR0A and SR0B. Distributions for...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t2","@type":"Dataset","description":"The $E_{\\mathrm{T}}^{\\mathrm{miss}}$ distribution for events passing the signal region requirements except the $E_{\\mathrm{T}}^{\\mathrm{miss}}$ requirement in SR0C and SR0D. Distributions for...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t3","@type":"Dataset","description":"The $m_{\\mathrm{eff}}$ distribution for events passing the signal region requirements except the $m_{\\mathrm{eff}}$ requirement in SR1. Distributions for data, the...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t4","@type":"Dataset","description":"The $m_{\\mathrm{eff}}$ distribution for events passing the signal region requirements except the $m_{\\mathrm{eff}}$ requirement in SR2. Distributions for data, the...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t5","@type":"Dataset","description":"Expected 95% CL exclusion limits on wino $W/Z$ NLSP pair production with RPV $\\tilde{\\chi}_1^0$ decays via $\\lambda_{12k} \\neq 0$ where...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t6","@type":"Dataset","description":"Observed 95% CL exclusion limits on wino $W/Z$ NLSP pair production with RPV $\\tilde{\\chi}_1^0$ decays via $\\lambda_{12k} \\neq 0$ where...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t7","@type":"Dataset","description":"Expected 95% CL exclusion limits on wino $W/Z$ NLSP pair production with RPV $\\tilde{\\chi}_1^0$ decays via $\\lambda_{i33} \\neq 0$ where...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t8","@type":"Dataset","description":"Observed 95% CL exclusion limits on wino $W/Z$ NLSP pair production with RPV $\\tilde{\\chi}_1^0$ decays via $\\lambda_{i33} \\neq 0$ where...","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t9","@type":"Dataset","description":"Expected 95% CL exclusion limits on wino $W/h$ NLSP pair production with RPV $\\tilde{\\chi}_1^0$ decays via $\\lambda_{12k} \\neq 0$ where...","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t10","@type":"Dataset","description":"Observed 95% CL exclusion limits on wino $W/h$ NLSP pair production with RPV $\\tilde{\\chi}_1^0$ decays via $\\lambda_{12k} \\neq 0$ where...","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t11","@type":"Dataset","description":"Expected 95% CL exclusion limits on wino $W/h$ NLSP pair production with RPV $\\tilde{\\chi}_1^0$ decays via $\\lambda_{i33} \\neq 0$ where...","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t12","@type":"Dataset","description":"Observed 95% CL exclusion limits on wino $W/h$ NLSP pair production with RPV $\\tilde{\\chi}_1^0$ decays via $\\lambda_{i33} \\neq 0$ where...","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t13","@type":"Dataset","description":"Expected 95% CL exclusion limits on $\\tilde{\\ell}/\\tilde{\\nu}$ NLSP pair production with RPV $\\tilde{\\chi}_1^0$ decays via $\\lambda_{12k} \\neq 0$ where $i,k...","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t14","@type":"Dataset","description":"Observed 95% CL exclusion limits on $\\tilde{\\ell}/\\tilde{\\nu}$ NLSP pair production with RPV $\\tilde{\\chi}_1^0$ decays via $\\lambda_{12k} \\neq 0$ where $i,k...","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t15","@type":"Dataset","description":"Expected 95% CL exclusion limits on $\\tilde{\\ell}/\\tilde{\\nu}$ NLSP pair production with RPV $\\tilde{\\chi}_1^0$ decays via $\\lambda_{i33} \\neq 0$ where $i,k...","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t16","@type":"Dataset","description":"Observed 95% CL exclusion limits on $\\tilde{\\ell}/\\tilde{\\nu}$ NLSP pair production with RPV $\\tilde{\\chi}_1^0$ decays via $\\lambda_{i33} \\neq 0$ where $i,k...","name":"Table 16"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t17","@type":"Dataset","description":"Expected 95% CL exclusion limits on gluino NSLP pair production with RPV $\\tilde{\\chi}_1^0$ decays via $\\lambda_{12k} \\neq 0$ where $i,k...","name":"Table 17"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t18","@type":"Dataset","description":"Observed 95% CL exclusion limits on gluino NSLP pair production with RPV $\\tilde{\\chi}_1^0$ decays via $\\lambda_{12k} \\neq 0$ where $i,k...","name":"Table 18"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t19","@type":"Dataset","description":"Expected 95% CL exclusion limits on gluino NSLP pair production with RPV $\\tilde{\\chi}_1^0$ decays via $\\lambda_{i33} \\neq 0$ where $i,k...","name":"Table 19"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t20","@type":"Dataset","description":"Observed 95% CL exclusion limits on gluino NSLP pair production with RPV $\\tilde{\\chi}_1^0$ decays via $\\lambda_{i33} \\neq 0$ where $i,k...","name":"Table 20"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t21","@type":"Dataset","description":"Expected 95% CL exclusion limits on the higgsino GGM models. The limits are set using the statistical combination of disjoint...","name":"Table 21"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t22","@type":"Dataset","description":"Observed 95% CL exclusion limits on the higgsino GGM models. The limits are set using the statistical combination of disjoint...","name":"Table 22"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t23","@type":"Dataset","description":"Observed exclusion limits on the $\\tilde{\\chi}_1^{\\pm}/\\tilde{\\chi}_2^0$ masses in the context of the wino $W/Z$ RPV scenario with $\\lambda_{12k} \\neq 0$...","name":"Table 23"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t24","@type":"Dataset","description":"Observed exclusion limits on the $\\tilde{\\chi}_1^{\\pm}/\\tilde{\\chi}_2^0$ masses in the context of the wino $W/Z$ RPV scenario with $\\lambda_{i33} \\neq 0$...","name":"Table 24"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t25","@type":"Dataset","description":"Observed exclusion limits on the $\\tilde{\\chi}_1^{\\pm}/\\tilde{\\chi}_2^0$ masses in the context of the wino $W/Z$ RPV scenario with $\\lambda_{12k} \\neq 0$...","name":"Table 25"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t26","@type":"Dataset","description":"Observed exclusion limits on the $\\tilde{\\chi}_1^{\\pm}/\\tilde{\\chi}_2^0$ masses in the context of the wino $W/Z$ RPV scenario with $\\lambda_{i33} \\neq 0$...","name":"Table 26"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t27","@type":"Dataset","description":"Observed exclusion limits on the $\\tilde{\\chi}_1^{\\pm}/\\tilde{\\chi}_2^0$ masses in the context of the wino $W/h$ RPV scenario with $\\lambda_{12k} \\neq 0$...","name":"Table 27"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t28","@type":"Dataset","description":"Observed exclusion limits on the $\\tilde{\\chi}_1^{\\pm}/\\tilde{\\chi}_2^0$ masses in the context of the wino $W/h$ RPV scenario with $\\lambda_{i33} \\neq 0$...","name":"Table 28"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t29","@type":"Dataset","description":"Observed exclusion limits on the $\\tilde{\\chi}_1^{\\pm}/\\tilde{\\chi}_2^0$ masses in the context of the wino $W/h$ RPV scenario with $\\lambda_{12k} \\neq 0$...","name":"Table 29"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t30","@type":"Dataset","description":"Observed exclusion limits on the $\\tilde{\\chi}_1^{\\pm}/\\tilde{\\chi}_2^0$ masses in the context of the wino $W/h$ RPV scenario with $\\lambda_{i33} \\neq 0$...","name":"Table 30"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t31","@type":"Dataset","description":"Observed exclusion limits on the slepton/sneutrino masses in the context of the slepton/sneutrino RPV scenario with $\\lambda_{12k} \\neq 0$ couplings....","name":"Table 31"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t32","@type":"Dataset","description":"Observed exclusion limits on the slepton/sneutrino masses in the context of the slepton/sneutrino RPV scenario with $\\lambda_{i33} \\neq 0$ couplings....","name":"Table 32"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t33","@type":"Dataset","description":"Observed exclusion limits on the slepton/sneutrino masses in the context of the slepton/sneutrino RPV scenario with $\\lambda_{12k} \\neq 0$ couplings....","name":"Table 33"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t34","@type":"Dataset","description":"Observed exclusion limits on the slepton/sneutrino masses in the context of the slepton/sneutrino RPV scenario with $\\lambda_{i33} \\neq 0$ couplings....","name":"Table 34"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t35","@type":"Dataset","description":"Observed exclusion limits on the gluino masses in the context of the gluino RPV scenario with $\\lambda_{12k} \\neq 0$ couplings....","name":"Table 35"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t36","@type":"Dataset","description":"Observed exclusion limits on the gluino masses in the context of the gluino RPV scenario with $\\lambda_{i33} \\neq 0$ couplings....","name":"Table 36"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t37","@type":"Dataset","description":"Observed exclusion limits on the gluino masses in the context of the gluino RPV scenario with $\\lambda_{12k} \\neq 0$ couplings....","name":"Table 37"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t38","@type":"Dataset","description":"Observed exclusion limits on the gluino masses in the context of the gluino RPV scenario with $\\lambda_{i33} \\neq 0$ couplings....","name":"Table 38"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t39","@type":"Dataset","description":"Observed exclusion limits on the $\\tilde{\\chi}_1^{\\pm}\\tilde{\\chi}_2^{0}\\tilde{\\chi}_1^{0}$ masses in the context of the higgsino GGM scenario in SR0C. All limits are...","name":"Table 39"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t40","@type":"Dataset","description":"Observed exclusion limits on the $\\tilde{\\chi}_1^{\\pm}\\tilde{\\chi}_2^{0}\\tilde{\\chi}_1^{0}$ masses in the context of the higgsino GGM scenario in SR0D. All limits are...","name":"Table 40"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t41","@type":"Dataset","description":"The best expected exclusion power between signal regions at each signal point as is adopted in the limit calculation of...","name":"Table 41"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t42","@type":"Dataset","description":"The best expected exclusion power between signal regions at each signal point as is adopted in the limit calculation of...","name":"Table 42"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t43","@type":"Dataset","description":"The best expected exclusion power between signal regions at each signal point as is adopted in the limit calculation of...","name":"Table 43"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t44","@type":"Dataset","description":"The best expected exclusion power between signal regions at each signal point as is adopted in the limit calculation of...","name":"Table 44"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t45","@type":"Dataset","description":"The best expected exclusion power between signal regions at each signal point as is adopted in the limit calculation of...","name":"Table 45"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t46","@type":"Dataset","description":"The best expected exclusion power between signal regions at each signal point as is adopted in the limit calculation of...","name":"Table 46"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t47","@type":"Dataset","description":"The best expected exclusion power between signal regions at each signal point as is adopted in the limit calculation of...","name":"Table 47"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t48","@type":"Dataset","description":"The best expected exclusion power between signal regions at each signal point as is adopted in the limit calculation of...","name":"Table 48"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t49","@type":"Dataset","description":"The best expected exclusion power between the overlapping SR0C and SR0D at each signal point as is adopted in the...","name":"Table 49"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t50","@type":"Dataset","description":"Acceptance ($A$) at particle level and selection efficiency ($\\epsilon$) at reconstruction level for the Wino $\\tilde{\\chi}_1^{+}\\tilde{\\chi}_1^{-}$ $\\lambda_{12k} \\neq 0$ model...","name":"Table 50"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t51","@type":"Dataset","description":"Acceptance ($A$) at particle level and selection efficiency ($\\epsilon$) at reconstruction level for the Wino $\\tilde{\\chi}_1^{\\pm}\\tilde{\\chi}_2^{0}$ $W/Z$ $\\lambda_{12k} \\neq 0$...","name":"Table 51"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t52","@type":"Dataset","description":"Acceptance ($A$) at particle level and selection efficiency ($\\epsilon$) at reconstruction level for the Wino $\\tilde{\\chi}_1^{\\pm}\\tilde{\\chi}_2^{0}$ $W/h$ $\\lambda_{12k} \\neq 0$...","name":"Table 52"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t53","@type":"Dataset","description":"Acceptance ($A$) at particle level and selection efficiency ($\\epsilon$) at reconstruction level for the slepton/sneutrino $\\lambda_{12k} \\neq 0$ model fulfilling...","name":"Table 53"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t54","@type":"Dataset","description":"Acceptance ($A$) at particle level and selection efficiency ($\\epsilon$) at reconstruction level for the gluino $\\lambda_{12k} \\neq 0$ model fulfilling...","name":"Table 54"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t55","@type":"Dataset","description":"Acceptance ($A$) at particle level and selection efficiency ($\\epsilon$) at reconstruction level for the Wino $\\tilde{\\chi}_1^{+}\\tilde{\\chi}_1^{-}$ $\\lambda_{12k} \\neq 0$ model...","name":"Table 55"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t56","@type":"Dataset","description":"Acceptance ($A$) at particle level and selection efficiency ($\\epsilon$) at reconstruction level for the Wino $\\tilde{\\chi}_1^{\\pm}\\tilde{\\chi}_2^{0}$ $W/Z$ $\\lambda_{12k} \\neq 0$...","name":"Table 56"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t57","@type":"Dataset","description":"Acceptance ($A$) at particle level and selection efficiency ($\\epsilon$) at reconstruction level for the Wino $\\tilde{\\chi}_1^{\\pm}\\tilde{\\chi}_2^{0}$ $W/h$ $\\lambda_{12k} \\neq 0$...","name":"Table 57"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t58","@type":"Dataset","description":"Acceptance ($A$) at particle level and selection efficiency ($\\epsilon$) at reconstruction level for the slepton/sneutrino $\\lambda_{12k} \\neq 0$ model fulfilling...","name":"Table 58"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t59","@type":"Dataset","description":"Acceptance ($A$) at particle level and selection efficiency ($\\epsilon$) at reconstruction level for the gluino $\\lambda_{12k} \\neq 0$ model fulfilling...","name":"Table 59"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t60","@type":"Dataset","description":"Acceptance ($A$) at particle level and selection efficiency ($\\epsilon$) at reconstruction level for the GGM Higgsino models with BR($\\tilde{\\chi}_1^0 \\rightarrow...","name":"Table 60"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t61","@type":"Dataset","description":"Acceptance ($A$) at particle level and selection efficiency ($\\epsilon$) at reconstruction level for the GGM Higgsino models with BR($\\tilde{\\chi}_1^0 \\rightarrow...","name":"Table 61"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t62","@type":"Dataset","description":"Acceptance ($A$) at particle level and selection efficiency ($\\epsilon$) at reconstruction level for the Wino $\\tilde{\\chi}_1^{+}\\tilde{\\chi}_1^{-}$ $\\lambda_{i33} \\neq 0$ model...","name":"Table 62"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t63","@type":"Dataset","description":"Acceptance ($A$) at particle level and selection efficiency ($\\epsilon$) at reconstruction level for the Wino $\\tilde{\\chi}_1^{\\pm}\\tilde{\\chi}_2^{0}$ $W/Z$ $\\lambda_{i33} \\neq 0$...","name":"Table 63"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t64","@type":"Dataset","description":"Acceptance ($A$) at particle level and selection efficiency ($\\epsilon$) at reconstruction level for the Wino $\\tilde{\\chi}_1^{\\pm}\\tilde{\\chi}_2^{0}$ $W/h$ $\\lambda_{i33} \\neq 0$...","name":"Table 64"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t65","@type":"Dataset","description":"Acceptance ($A$) at particle level and selection efficiency ($\\epsilon$) at reconstruction level for the slepton/sneutrino $\\lambda_{i33} \\neq 0$ model fulfilling...","name":"Table 65"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t66","@type":"Dataset","description":"Acceptance ($A$) at particle level and selection efficiency ($\\epsilon$) at reconstruction level for the gluino $\\lambda_{i33} \\neq 0$ model fulfilling...","name":"Table 66"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t67","@type":"Dataset","description":"Acceptance ($A$) at particle level and selection efficiency ($\\epsilon$) at reconstruction level for the Wino $\\tilde{\\chi}_1^{+}\\tilde{\\chi}_1^{-}$ $\\lambda_{i33} \\neq 0$ model...","name":"Table 67"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t68","@type":"Dataset","description":"Acceptance ($A$) at particle level and selection efficiency ($\\epsilon$) at reconstruction level for the Wino $\\tilde{\\chi}_1^{\\pm}\\tilde{\\chi}_2^{0}$ $W/Z$ $\\lambda_{i33} \\neq 0$...","name":"Table 68"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t69","@type":"Dataset","description":"Acceptance ($A$) at particle level and selection efficiency ($\\epsilon$) at reconstruction level for the Wino $\\tilde{\\chi}_1^{\\pm}\\tilde{\\chi}_2^{0}$ $W/h$ $\\lambda_{i33} \\neq 0$...","name":"Table 69"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t70","@type":"Dataset","description":"Acceptance ($A$) at particle level and selection efficiency ($\\epsilon$) at reconstruction level for the slepton/sneutrino $\\lambda_{i33} \\neq 0$ model fulfilling...","name":"Table 70"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t71","@type":"Dataset","description":"Acceptance ($A$) at particle level and selection efficiency ($\\epsilon$) at reconstruction level for the gluino $\\lambda_{i33} \\neq 0$ model fulfilling...","name":"Table 71"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t72","@type":"Dataset","description":"Cutflow event yields in regions SR0A and SR0B for RPV models with the $\\lambda_{12k} \\neq 0$ coupling. All yields correspond...","name":"Table 72"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t73","@type":"Dataset","description":"Cutflow event yields in regions SR0C and SR0D for GGM Higgsino models with BR($\\tilde{\\chi}_1^0 \\rightarrow Z \\tilde{G}$)=100% or BR($\\tilde{\\chi}_1^0 \\rightarrow...","name":"Table 73"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t74","@type":"Dataset","description":"Cutflow event yields in region SR1 for RPV models with the $\\lambda_{i33} \\neq 0$ coupling. All yields correspond to weighted...","name":"Table 74"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t75","@type":"Dataset","description":"Cutflow event yields in region SR2 for RPV models with the $\\lambda_{i33} \\neq 0$ coupling. All yields correspond to weighted...","name":"Table 75"},{"@id":"https://doi.org/10.17182/hepdata.82585.v1/t76","@type":"Dataset","description":"Cross sections for the slepton/snuetrino model for different NLSP masses.","name":"Table 76"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1667045?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/82585"}],"inLanguage":"en","name":"Search for supersymmetry in events with four or more leptons in $\\sqrt{s}=13$ TeV $pp$ collisions with ATLAS","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1667045?version=1","version":1}