{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.91374.v5","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1767649"}},{"@id":"https://doi.org/10.1103/PhysRevD.101.052005","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2022","description":"This paper presents results of searches for electroweak production of supersymmetric particles in models with compressed mass spectra.  The searches use 139/fb of sqrt(s) = 13 TeV proton-proton collision data collected by the ATLAS experiment at the Large Hadron Collider.  Events with missing transverse momentum and two same-flavor, oppositely charged, low transverse momentum leptons are selected, and are further categorized by the presence of hadronic activity from initial-state radiation or a topology compatible with vector-boson fusion processes.  The data are found to be consistent with predictions from the Standard Model.  The results are interpreted using simplified models of R-parity-conserving supersymmetry in which the lightest supersymmetric partner is a neutralino with a mass similar to the lightest chargino, the second-to-lightest neutralino or the slepton.  Lower limits on the masses of charginos in different simplified models range from 193 GeV to 240 GeV for moderate mass splittings, and extend down to mass splittings of 1.5 GeV to 2.4 GeV at the LEP chargino bounds (92.4 GeV). Similar lower limits on degenerate light-flavor sleptons extend up to masses of 251 GeV and down to mass splittings of 550 MeV. Constraints on vector-boson fusion production of electroweak SUSY states are also presented.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t1","@type":"Dataset","description":"Expected 95% CL exclusion sensitivity for simplified models of direct higgsino production.","name":"Figure 14a Expected"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t2","@type":"Dataset","description":"Observed 95% CL exclusion sensitivity for simplified models of direct higgsino production.","name":"Figure 14a Observed"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t3","@type":"Dataset","description":"Expected 95% CL exclusion sensitivity for simplified models of direct wino-bino production, assuming $m(\\tilde{\\chi}_{2}^{0}) \\times m(\\tilde{\\chi}_{1}^{0})<0$.","name":"Figure 14b Expected"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t4","@type":"Dataset","description":"Observed 95% CL exclusion sensitivity for simplified models of direct wino-bino production, assuming $m(\\tilde{\\chi}_{2}^{0}) \\times m(\\tilde{\\chi}_{1}^{0})<0$.","name":"Figure 14b Observed"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t5","@type":"Dataset","description":"Expected 95% CL exclusion sensitivity for simplified models of direct wino-bino production, assuming $m(\\tilde{\\chi}_{2}^{0}) \\times m(\\tilde{\\chi}_{1}^{0})>0$.","name":"Figure 14c Expected"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t6","@type":"Dataset","description":"Observed 95% CL exclusion sensitivity for simplified models of direct wino-bino production, assuming $m(\\tilde{\\chi}_{2}^{0}) \\times m(\\tilde{\\chi}_{1}^{0})>0$.","name":"Figure 14c Observed"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t7","@type":"Dataset","description":"Expected 95% CL exclusion sensitivity for simplified models of VBF wino-bino production.","name":"Figure 15b Expected"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t8","@type":"Dataset","description":"Observed 95% CL exclusion sensitivity for simplified models of direct wino-bino production.","name":"Figure 15b Observed"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t9","@type":"Dataset","description":"Expected 95% CL exclusion sensitivity for simplified models of direct slepton production.","name":"Figure 16a Expected"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t10","@type":"Dataset","description":"Observed 95% CL exclusion sensitivity for simplified models of direct slepton production.","name":"Figure 16a Observed"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t11","@type":"Dataset","description":"Expected 95% CL exclusion sensitivity for simplified models of direct smuon production.","name":"Figure 2b smuon Expected"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t12","@type":"Dataset","description":"Observed 95% CL exclusion sensitivity for simplified models of direct smuon production.","name":"Figure 2b smuon Observed"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t13","@type":"Dataset","description":"Expected 95% CL exclusion sensitivity for simplified models of direct selectron production.","name":"Figure 2b selectron Expected"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t14","@type":"Dataset","description":"Observed 95% CL exclusion sensitivity for simplified models of direct selectron production.","name":"Figure 2b selectron Observed"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t15","@type":"Dataset","description":"Expected 95% CL exclusion sensitivity for simplified models of direct LH slepton production.","name":"Figure 2a LH slepton Expected"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t16","@type":"Dataset","description":"Observed 95% CL exclusion sensitivity for simplified models of direct LH slepton production.","name":"Figure 2a LH slepton Observed"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t17","@type":"Dataset","description":"Expected 95% CL exclusion sensitivity for simplified models of direct RH slepton production.","name":"Figure 2a RH slepton Expected"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t18","@type":"Dataset","description":"Observed 95% CL exclusion sensitivity for simplified models of direct RH slepton production.","name":"Figure 2a RH slepton Observed"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t19","@type":"Dataset","description":"Expected 95% CL exclusion sensitivity for simplified models of direct LH smuon production.","name":"Figure 16b LH smuon Expected"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t20","@type":"Dataset","description":"Observed 95% CL exclusion sensitivity for simplified models of direct LH smuon production.","name":"Figure 16b LH smuon Observed"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t21","@type":"Dataset","description":"Expected 95% CL exclusion sensitivity for simplified models of direct RH smuon production.","name":"Figure 16b RH smuon Expected"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t22","@type":"Dataset","description":"Observed 95% CL exclusion sensitivity for simplified models of direct RH smuon production.","name":"Figure 16b RH smuon Observed"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t23","@type":"Dataset","description":"Expected 95% CL exclusion sensitivity for simplified models of direct LH selectron production.","name":"Figure 16b LH selectron Expected"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t24","@type":"Dataset","description":"Observed 95% CL exclusion sensitivity for simplified models of direct LH selectron production.","name":"Figure 16b LH selectron Observed"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t25","@type":"Dataset","description":"Expected 95% CL exclusion sensitivity for simplified models of direct RH selectron production.","name":"Figure 16b RH selectron Expected"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t26","@type":"Dataset","description":"Observed 95% CL exclusion sensitivity for simplified models of direct RH selectron production.","name":"Figure 16b RH selectron Observed"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t27","@type":"Dataset","description":"Acceptance (note the $z$-axis is in units of $10^{-4}$) for the C1C1 higgsino process in the SR-E-high region. Truth dilepton...","name":"Figure 28a"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t28","@type":"Dataset","description":"Efficiency for the C1C1 higgsino process in the SR-E-high region. Truth dilepton invariant mass is constrained to be within the...","name":"Figure 28b"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t29","@type":"Dataset","description":"Acceptance (note the $z$-axis is in units of $10^{-4}$) for the C1C1 higgsino process in the SR-E-low region. Truth dilepton...","name":"Figure 28c"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t30","@type":"Dataset","description":"Efficiency for the C1C1 higgsino process in the SR-E-low region. Truth dilepton invariant mass is constrained to be within the...","name":"Figure 28d"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t31","@type":"Dataset","description":"Acceptance (note the $z$-axis is in units of $10^{-4}$) for the C1C1 higgsino process in the SR-E-med region. Truth dilepton...","name":"Figure 28e"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t32","@type":"Dataset","description":"Efficiency for the C1C1 higgsino process in the SR-E-med region. Truth dilepton invariant mass is constrained to be within the...","name":"Figure 28f"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t33","@type":"Dataset","description":"Acceptance (note the $z$-axis is in units of $10^{-4}$) for the N2N1 higgsino process in the SR-E-high region. Truth dilepton...","name":"Figure 29a"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t34","@type":"Dataset","description":"Efficiency for the N2N1 higgsino process in the SR-E-high region. Truth dilepton invariant mass is constrained to be within the...","name":"Figure 29b"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t35","@type":"Dataset","description":"Acceptance (note the $z$-axis is in units of $10^{-4}$) for the N2N1 higgsino process in the SR-E-low region. Truth dilepton...","name":"Figure 29c"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t36","@type":"Dataset","description":"Efficiency for the N2N1 higgsino process in the SR-E-low region. Truth dilepton invariant mass is constrained to be within the...","name":"Figure 29d"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t37","@type":"Dataset","description":"Acceptance (note the $z$-axis is in units of $10^{-4}$) for the N2N1 higgsino process in the SR-E-med region. Truth dilepton...","name":"Figure 29e"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t38","@type":"Dataset","description":"Efficiency for the N2N1 higgsino process in the SR-E-med region. Truth dilepton invariant mass is constrained to be within the...","name":"Figure 29f"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t39","@type":"Dataset","description":"Acceptance (note the $z$-axis is in units of $10^{-4}$) for the N2N1 higgsino process in the SR-E-1l1T region. Truth dilepton...","name":"Figure 29g"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t40","@type":"Dataset","description":"Efficiency for the N2N1 higgsino process in the SR-E-1l1T region. Truth dilepton invariant mass is constrained to be within the...","name":"Figure 29h"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t41","@type":"Dataset","description":"Acceptance (note the $z$-axis is in units of $10^{-4}$) for the N2C1p higgsino process in the SR-E-high region. Truth dilepton...","name":"Figure 30a"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t42","@type":"Dataset","description":"Efficiency for the N2C1p higgsino process in the SR-E-high region. Truth dilepton invariant mass is constrained to be within the...","name":"Figure 30b"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t43","@type":"Dataset","description":"Acceptance (note the $z$-axis is in units of $10^{-4}$) for the N2C1p higgsino process in the SR-E-low region. Truth dilepton...","name":"Figure 30c"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t44","@type":"Dataset","description":"Efficiency for the N2C1p higgsino process in the SR-E-low region. Truth dilepton invariant mass is constrained to be within the...","name":"Figure 30d"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t45","@type":"Dataset","description":"Acceptance (note the $z$-axis is in units of $10^{-4}$) for the N2C1p higgsino process in the SR-E-med region. Truth dilepton...","name":"Figure 30e"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t46","@type":"Dataset","description":"Efficiency for the N2C1p higgsino process in the SR-E-med region. Truth dilepton invariant mass is constrained to be within the...","name":"Figure 30f"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t47","@type":"Dataset","description":"Acceptance (note the $z$-axis is in units of $10^{-4}$) for the N2C1p higgsino process in the SR-E-1l1T region. Truth dilepton...","name":"Figure 30g"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t48","@type":"Dataset","description":"Efficiency for the N2C1p higgsino process in the SR-E-1l1T region. Truth dilepton invariant mass is constrained to be within the...","name":"Figure 30h"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t49","@type":"Dataset","description":"Acceptance (note the $z$-axis is in units of $10^{-4}$) for the N2C1m higgsino process in the SR-E-high region. Truth dilepton...","name":"Figure 31a"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t50","@type":"Dataset","description":"Efficiency for the N2C1m higgsino process in the SR-E-high region. Truth dilepton invariant mass is constrained to be within the...","name":"Figure 31b"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t51","@type":"Dataset","description":"Acceptance (note the $z$-axis is in units of $10^{-4}$) for the N2C1m higgsino process in the SR-E-low region. Truth dilepton...","name":"Figure 31c"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t52","@type":"Dataset","description":"Efficiency for the N2C1m higgsino process in the SR-E-low region. Truth dilepton invariant mass is constrained to be within the...","name":"Figure 31d"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t53","@type":"Dataset","description":"Acceptance (note the $z$-axis is in units of $10^{-4}$) for the N2C1m higgsino process in the SR-E-med region. Truth dilepton...","name":"Figure 31e"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t54","@type":"Dataset","description":"Efficiency for the N2C1m higgsino process in the SR-E-med region. Truth dilepton invariant mass is constrained to be within the...","name":"Figure 31f"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t55","@type":"Dataset","description":"Acceptance (note the $z$-axis is in units of $10^{-4}$) for the N2C1m higgsino process in the SR-E-1l1T region. Truth dilepton...","name":"Figure 31g"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t56","@type":"Dataset","description":"Efficiency for the N2C1m higgsino process in the SR-E-1l1T region. Truth dilepton invariant mass is constrained to be within the...","name":"Figure 31h"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t57","@type":"Dataset","description":"Acceptance (note the $z$-axis is in units of $10^{-3}$) for the slepton process in the SR-S region. Truth stransverse mass...","name":"Figure 32a"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t58","@type":"Dataset","description":"Efficiency for the slepton process in the SR-S region. Truth stransverse mass is constrained to be within the range [100,140]...","name":"Figure 32b"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t59","@type":"Dataset","description":"Acceptance (note the $z$-axis is in units of $10^{-3}$) for the slepton process in the SR-S-high region. Truth stransverse mass...","name":"Figure 32c"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t60","@type":"Dataset","description":"Efficiency for the slepton process in the SR-S-high region. Truth stransverse mass is constrained to be within the range [100,140]...","name":"Figure 32d"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t61","@type":"Dataset","description":"Acceptance (note the $z$-axis is in units of $10^{-3}$) for the slepton process in the SR-S-low region. Truth stransverse mass...","name":"Figure 32e"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t62","@type":"Dataset","description":"Efficiency for the slepton process in the SR-S-low region. Truth stransverse mass is constrained to be within the range [100,140]...","name":"Figure 32f"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t63","@type":"Dataset","description":"Acceptance (note the $z$-axis is in units of $10^{-4}$) for the C1C1 VBF higgsino process in the SR-VBF-high region. Truth...","name":"Figure 33a"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t64","@type":"Dataset","description":"Efficiency for the C1C1 VBF higgsino process in the SR-VBF-high region. Truth dilepton invariant mass is constrained to be within...","name":"Figure 33b"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t65","@type":"Dataset","description":"Acceptance (note the $z$-axis is in units of $10^{-4}$) for the C1C1 VBF higgsino process in the SR-VBF-low region. Truth...","name":"Figure 33c"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t66","@type":"Dataset","description":"Efficiency for the C1C1 VBF higgsino process in the SR-VBF-low region. Truth dilepton invariant mass is constrained to be within...","name":"Figure 33d"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t67","@type":"Dataset","description":"Acceptance (note the $z$-axis is in units of $10^{-4}$) for the C1C1 VBF higgsino process in the SR-VBF region. Truth...","name":"Figure 33e"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t68","@type":"Dataset","description":"Efficiency for the C1C1 VBF higgsino process in the SR-VBF region. Truth dilepton invariant mass is constrained to be within...","name":"Figure 33f"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t69","@type":"Dataset","description":"Acceptance (note the $z$-axis is in units of $10^{-4}$) for the N2N1 VBF higgsino process in the SR-VBF-high region. Truth...","name":"Figure 34a"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t70","@type":"Dataset","description":"Efficiency for the N2N1 VBF higgsino process in the SR-VBF-high region. Truth dilepton invariant mass is constrained to be within...","name":"Figure 34b"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t71","@type":"Dataset","description":"Acceptance (note the $z$-axis is in units of $10^{-4}$) for the N2N1 VBF higgsino process in the SR-VBF-low region. Truth...","name":"Figure 34c"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t72","@type":"Dataset","description":"Efficiency for the N2N1 VBF higgsino process in the SR-VBF-low region. Truth dilepton invariant mass is constrained to be within...","name":"Figure 34d"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t73","@type":"Dataset","description":"Acceptance (note the $z$-axis is in units of $10^{-4}$) for the N2N1 VBF higgsino process in the SR-VBF region. Truth...","name":"Figure 34e"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t74","@type":"Dataset","description":"Efficiency for the N2N1 VBF higgsino process in the SR-VBF region. Truth dilepton invariant mass is constrained to be within...","name":"Figure 34f"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t75","@type":"Dataset","description":"Acceptance (note the $z$-axis is in units of $10^{-4}$) for the N2C1p VBF higgsino process in the SR-VBF-high region. Truth...","name":"Figure 35a"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t76","@type":"Dataset","description":"Efficiency for the N2C1p VBF higgsino process in the SR-VBF-high region. Truth dilepton invariant mass is constrained to be within...","name":"Figure 35b"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t77","@type":"Dataset","description":"Acceptance (note the $z$-axis is in units of $10^{-4}$) for the N2C1p VBF higgsino process in the SR-VBF-low region. Truth...","name":"Figure 35c"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t78","@type":"Dataset","description":"Efficiency for the N2C1p VBF higgsino process in the SR-VBF-low region. Truth dilepton invariant mass is constrained to be within...","name":"Figure 35d"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t79","@type":"Dataset","description":"Acceptance (note the $z$-axis is in units of $10^{-4}$) for the N2C1p VBF higgsino process in the SR-VBF region. Truth...","name":"Figure 35e"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t80","@type":"Dataset","description":"Efficiency for the N2C1p VBF higgsino process in the SR-VBF region. Truth dilepton invariant mass is constrained to be within...","name":"Figure 35f"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t81","@type":"Dataset","description":"Acceptance (note the $z$-axis is in units of $10^{-4}$) for the N2C1m VBF higgsino process in the SR-VBF-high region. Truth...","name":"Figure 36a"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t82","@type":"Dataset","description":"Efficiency for the N2C1m VBF higgsino process in the SR-VBF-high region. Truth dilepton invariant mass is constrained to be within...","name":"Figure 36b"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t83","@type":"Dataset","description":"Acceptance (note the $z$-axis is in units of $10^{-4}$) for the N2C1m VBF higgsino process in the SR-VBF-low region. Truth...","name":"Figure 36c"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t84","@type":"Dataset","description":"Efficiency for the N2C1m VBF higgsino process in the SR-VBF-low region. Truth dilepton invariant mass is constrained to be within...","name":"Figure 36d"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t85","@type":"Dataset","description":"Acceptance (note the $z$-axis is in units of $10^{-4}$) for the N2C1m VBF higgsino process in the SR-VBF region. Truth...","name":"Figure 36e"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t86","@type":"Dataset","description":"Efficiency for the N2C1m VBF higgsino process in the SR-VBF region. Truth dilepton invariant mass is constrained to be within...","name":"Figure 36f"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t87","@type":"Dataset","description":"Observed and Expected upper cross-section limits for wino-bino scenarios, assuming $m(\\tilde{\\chi}_{2}^{0}) \\times m(\\tilde{\\chi}_{1}^{0})>0$.","name":"Figure 41ab"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t88","@type":"Dataset","description":"Observed and Expected upper cross-section limits for wino-bino scenarios, assuming $m(\\tilde{\\chi}_{2}^{0}) \\times m(\\tilde{\\chi}_{1}^{0})<0$.","name":"Figure 41cd"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t89","@type":"Dataset","description":"Observed and Expected upper cross-section limits for higgsino scenarios.","name":"Figure 42ab"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t90","@type":"Dataset","description":"Observed and Expected upper cross-section limits for higgsino scenarios, assuming VBF production..","name":"Figure 43ab"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t91","@type":"Dataset","description":"Observed and Expected upper cross-section limits for direct slepton scenarios.","name":"Figure 44ab"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t92","@type":"Dataset","description":"Observed and Expected upper cross-section limits for direct LH slepton scenarios.","name":"Figure 44cd"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t93","@type":"Dataset","description":"Observed and Expected upper cross-section limits for direct RH slepton scenarios.","name":"Figure 44ef"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t94","@type":"Dataset","description":"Observed and Expected upper cross-section limits for direct smuon scenarios.","name":"Figure 45ab"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t95","@type":"Dataset","description":"Observed and Expected upper cross-section limits for direct LH smuon scenarios.","name":"Figure 45cd"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t96","@type":"Dataset","description":"Observed and Expected upper cross-section limits for direct RH smuon scenarios.","name":"Figure 45ef"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t97","@type":"Dataset","description":"Observed and Expected upper cross-section limits for direct selectron scenarios.","name":"Figure 46ab"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t98","@type":"Dataset","description":"Observed and Expected upper cross-section limits for direct LH selectron scenarios.","name":"Figure 46cd"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t99","@type":"Dataset","description":"Observed and Expected upper cross-section limits for direct RH selectron scenarios.","name":"Figure 46ef"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t100","@type":"Dataset","description":"Number of signal events in SR-E-1L1T for the (m($\\tilde{\\chi}_{2}^{0}$),m($\\tilde{\\chi}_{1}^{0}$)) = (155 GeV, 150 GeV) Higgsino signal model at different stages...","name":"Table 18"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t101","@type":"Dataset","description":"Number of signal events in SR-E-high for the (m($\\tilde{\\chi}_{2}^{0}$),m($\\tilde{\\chi}_{1}^{0}$)) = (155 GeV, 150 GeV) Higgsino signal model at different stages...","name":"Table 19"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t102","@type":"Dataset","description":"Number of signal events in SR-E-low for the (m($\\tilde{\\chi}_{2}^{0}$),m($\\tilde{\\chi}_{1}^{0}$)) = (155 GeV, 150 GeV) Higgsino signal model at different stages...","name":"Table 20"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t103","@type":"Dataset","description":"Number of signal events in SR-E-med for the (m($\\tilde{\\chi}_{2}^{0}$),m($\\tilde{\\chi}_{1}^{0}$)) = (155 GeV, 150 GeV) Higgsino signal model at different stages...","name":"Table 21"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t104","@type":"Dataset","description":"Number of signal events in SR-S-high for the (m($\\tilde{\\ell}$),m($\\tilde{\\chi}_{1}^{0}$)) = (150 GeV, 140 GeV) Slepton signal model at different stages...","name":"Table 22"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t105","@type":"Dataset","description":"Number of signal events in SR-S-low for the (m($\\tilde{\\ell}$),m($\\tilde{\\chi}_{1}^{0}$)) = (150 GeV, 140 GeV) Slepton signal model at different stages...","name":"Table 23"},{"@id":"https://doi.org/10.17182/hepdata.91374.v5/t106","@type":"Dataset","description":"Number of signal events in SR-VBF for the (m($\\tilde{\\chi}_{2}^{0}$),m($\\tilde{\\chi}_{1}^{0}$)) = (100 GeV, 95 GeV) Higgsino signal model at different stages...","name":"Table 24"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1767649?version=5"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/91374"}],"inLanguage":"en","name":"Searches for electroweak production of supersymmetric particles with compressed mass spectra in $\\sqrt{s}=13$ TeV $pp$ collisions with the ATLAS detector","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1767649?version=5","version":5}