{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.72792.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1424844"}},{"@id":"https://doi.org/10.1140/epjc/s10052-016-4095-8","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2016","description":"CERN-LHC.  A search for strongly produced supersymmetric particles is conducted using signatures involving multiple energetic jets and either two isolated leptons ($e$ or $\\mu$) with the same electric charge or at least three isolated leptons. The search also utilises $b$-tagged jets, missing transverse momentum and other observables to extend its sensitivity. The analysis uses a data sample of proton-proton collisions at $\\sqrt{s}=13$ TeV recorded with the ATLAS detector at the Large Hadron Collider in 2015 corresponding to a total integrated luminosity of 3.2 fb$^{-1}$. No significant excess over the Standard Model expectation is observed. The results are interpreted in several simplified supersymmetric models and extend the exclusion limits from previous searches. In the context of exclusive production and simplified decay modes, gluino masses are excluded at 95% confidence level up to 1.1-1.3 TeV for light neutralinos (depending on the decay channel), and bottom squark masses are also excluded up to 540 GeV. In the former scenarios, neutralino masses are also excluded up to 550-850 GeV for gluino masses around 1 TeV.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.72792.v1/t1","@type":"Dataset","description":"Missing transverse momentum distribution after SR0b3j selection, beside the $E_\\mathrm{T}^\\mathrm{miss}$ requirement. The results in the signal region correspond to the...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.72792.v1/t2","@type":"Dataset","description":"Missing transverse momentum distribution after SR0b5j selection, beside the $E_\\mathrm{T}^\\mathrm{miss}$ requirement. The results in the signal region correspond to the...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.72792.v1/t3","@type":"Dataset","description":"Missing transverse momentum distribution after SR1b selection, beside the $E_\\mathrm{T}^\\mathrm{miss}$ requirement. The results in the signal region correspond to the...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.72792.v1/t4","@type":"Dataset","description":"Missing transverse momentum distribution after SR3b selection, beside the $E_\\mathrm{T}^\\mathrm{miss}$ requirement. The results in the signal region correspond to the...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.72792.v1/t5","@type":"Dataset","description":"Observed exclusion limits on the $\\tilde g$ and $\\tilde\\chi_1^0$ masses in the context of SUSY scenarios with simplified mass spectra...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.72792.v1/t6","@type":"Dataset","description":"Expected exclusion limits on the $\\tilde g$ and $\\tilde\\chi_1^0$ masses in the context of SUSY scenarios with simplified mass spectra...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.72792.v1/t7","@type":"Dataset","description":"Upper limits on signal cross-sections as function of the $\\tilde g$ and $\\tilde\\chi_1^0$ masses in the context of SUSY scenarios...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.72792.v1/t8","@type":"Dataset","description":"Observed exclusion limits on the $\\tilde g$ and $\\tilde\\chi_1^0$ masses in the context of SUSY scenarios 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simplified mass spectra...","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.72792.v1/t13","@type":"Dataset","description":"Upper limits on signal cross-sections as function of the $\\tilde b_1$ and $\\tilde\\chi_1^0$ masses in the context of SUSY scenarios...","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.72792.v1/t14","@type":"Dataset","description":"Observed exclusion limits on the $\\tilde g$ and $\\tilde\\chi_1^0$ masses in the context of SUSY scenarios with simplified mass spectra...","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.72792.v1/t15","@type":"Dataset","description":"Expected exclusion limits on the $\\tilde g$ and $\\tilde\\chi_1^0$ masses in the context of SUSY scenarios with simplified mass spectra...","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.72792.v1/t16","@type":"Dataset","description":"Upper limits on signal cross-sections as function of the $\\tilde g$ and $\\tilde\\chi_1^0$ masses in the context of SUSY scenarios...","name":"Table 16"},{"@id":"https://doi.org/10.17182/hepdata.72792.v1/t17","@type":"Dataset","description":"SUSY scenario with $\\tilde g\\tilde g$ production and $\\tilde g\\to q\\bar q(\\tilde\\ell\\ell/\\tilde\\nu\\nu)$ decay: signal acceptance (in %) in the signal...","name":"Table 17"},{"@id":"https://doi.org/10.17182/hepdata.72792.v1/t18","@type":"Dataset","description":"SUSY scenario with $\\tilde g\\tilde g$ production and $\\tilde g\\to q\\bar q(\\tilde\\ell\\ell/\\tilde\\nu\\nu)$ decay: reconstruction efficiency (in %) in the signal...","name":"Table 18"},{"@id":"https://doi.org/10.17182/hepdata.72792.v1/t19","@type":"Dataset","description":"SUSY scenario with $\\tilde g\\tilde g$ production and $\\tilde g\\to q\\bar qWZ\\tilde\\chi_1^0$ decay: signal acceptance (in %) in the signal...","name":"Table 19"},{"@id":"https://doi.org/10.17182/hepdata.72792.v1/t20","@type":"Dataset","description":"SUSY scenario with $\\tilde g\\tilde g$ production and $\\tilde g\\to q\\bar qWZ\\tilde\\chi_1^0$ decay: reconstruction efficiency (in %) in the signal...","name":"Table 20"},{"@id":"https://doi.org/10.17182/hepdata.72792.v1/t21","@type":"Dataset","description":"SUSY scenario with $\\tilde b_1\\tilde b_1^*$ production and $\\tilde b_1\\to tW\\tilde\\chi_1^0$ decay: signal acceptance (in %) in the signal region...","name":"Table 21"},{"@id":"https://doi.org/10.17182/hepdata.72792.v1/t22","@type":"Dataset","description":"SUSY scenario with $\\tilde b_1\\tilde b_1^*$ production and $\\tilde b_1\\to tW\\tilde\\chi_1^0$ decay: reconstruction efficiency (in %) in the signal region...","name":"Table 22"},{"@id":"https://doi.org/10.17182/hepdata.72792.v1/t23","@type":"Dataset","description":"SUSY scenario with $\\tilde g\\tilde g$ production and $\\tilde g\\to t\\bar t\\tilde\\chi_1^0$ decay: signal acceptance (in %) in the signal...","name":"Table 23"},{"@id":"https://doi.org/10.17182/hepdata.72792.v1/t24","@type":"Dataset","description":"SUSY scenario with $\\tilde g\\tilde g$ production and $\\tilde g\\to t\\bar t\\tilde\\chi_1^0$ decay: reconstruction efficiency (in %) in the signal...","name":"Table 24"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1424844?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/72792"}],"inLanguage":"en","name":"Search for supersymmetry at $\\sqrt{s}=13$ TeV in final states with jets and two same-sign leptons or three leptons with the ATLAS detector","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1424844?version=1","version":1}