{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.89408.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1748602"}},{"@id":"https://doi.org/10.1007/JHEP12(2019)060","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2019","description":"The result of a search for the pair production of the lightest supersymmetric partner of the bottom quark ($\\tilde{b}_{1}$) using 139 fb$^{-1}$ of proton-proton data collected at $\\sqrt{s} = 13$ TeV by the ATLAS detector is reported. In the supersymmetric scenarios considered both of the bottom-squarks decay into a $b$-quark and the second-lightest neutralino, $\\tilde{b}_{1} \\rightarrow b + \\tilde{\\chi}^{0}_{2}$. Each $\\tilde{\\chi}^{0}_{2}$ is assumed to subsequently decay with 100% branching ratio into a Higgs boson ($h$) like the one in the Standard Model and the lightest neutralino: $\\tilde{\\chi}^{0}_{2} \\rightarrow h + \\tilde{\\chi}^{0}_{1}$. The $\\tilde{\\chi}^{0}_{1}$ is assumed to be the lightest supersymmetric particle (LSP) and is stable. Two signal mass configurations are targeted: the first has a constant LSP mass of 60 GeV; and the second has a constant mass difference between the $\\tilde{\\chi}^{0}_{2}$ and $\\tilde{\\chi}^{0}_{1}$ of 130 GeV. The final states considered contain no charged leptons, three or more $b$-jets, and large missing transverse momentum. No significant excess of events over the Standard Model background expectation is observed in any of the signal regions considered. Limits at the 95% confidence level are placed in the supersymmetric models considered, and bottom-squarks with mass up to 1.5 TeV are excluded.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.89408.v1/t1","@type":"Dataset","description":"Distributions of ${E}_{\\mathrm{T}}^{\\mathrm{miss}}$ after the background-only fit. The backgrounds which contribute only a small amount (diboson, W+jets and ttbar+W/Z/h) are...","name":"Missing Transverse Energy"},{"@id":"https://doi.org/10.17182/hepdata.89408.v1/t2","@type":"Dataset","description":"Distributions of $m_{\\mathrm{eff}}$ after the background-only fit. The backgrounds which contribute only a small amount (diboson, W+jets and ttbar+W/Z/h) are...","name":"Effective Mass"},{"@id":"https://doi.org/10.17182/hepdata.89408.v1/t3","@type":"Dataset","description":"Distributions of Object-based $E_{\\mathrm{T}}^{\\mathrm{miss}} {Sig.}$ after the background-only fit. 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