{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.79538.v7","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1623207"}},{"@id":"https://doi.org/10.1007/JHEP12(2017)085","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2018","description":"A search for pair production of a scalar partner of the top quark in events with four or more jets plus missing transverse momentum is presented. An analysis of 36.1 fb$^{-1}$ of $\\sqrt{s}$=13 TeV proton--proton collisions collected using the ATLAS detector at the LHC yields no significant excess over the expected Standard Model background. To interpret the results a simplified supersymmetric model is used where the top squark is assumed to decay via $\\tilde{t}_1 \\rightarrow t^{(*)} \\tilde\\chi^0_1$ and $\\tilde{t}_1\\rightarrow b\\tilde\\chi^\\pm_1 \\rightarrow b  W^{(*)} \\tilde\\chi^0_1$, where $\\tilde\\chi^0_1$ ($\\chi^\\pm_1$) denotes the lightest neutralino (chargino). Exclusion limits are placed in terms of the top-squark and neutralino masses. Assuming a branching ratio of 100% to $t \\tilde\\chi^0_1$, top-squark masses in the range 450--950 GeV are excluded for $\\tilde\\chi^0_1$ masses below 160 GeV. In the case where $m_{\\tilde{t}_1}\\sim m_t+m_{\\tilde\\chi^0_1}$, top-squark masses in the range 235--590 GeV are excluded.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.79538.v7/t1","@type":"Dataset","description":"Distribution of $E_\\text{T}^\\text{miss}$ for SRA-TT after the likelihood fit. 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