{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.74005.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1472822"}},{"@id":"https://doi.org/10.1140/epjc/s10052-016-4382-4","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2016","description":"CERN-LHC.  The result of a search for pair production of the supersymmetric partner of the Standard Model bottom quark ($\\tilde{b}_1$) is reported. The search uses 3.2 fb$^{-1}$ of $pp$ collisions at $\\sqrt{s}=$13 TeV collected by the ATLAS experiment at the Large Hadron Collider in 2015. Bottom squarks are searched for in events containing large missing transverse momentum and exactly two jets identified as originating from $b$-quarks. No excess above the expected Standard Model background yield is observed. Exclusion limits at 95% confidence level on the mass of the bottom squark are derived in phenomenological supersymmetric $R$-parity-conserving models in which the $\\tilde{b}_1$ is the lightest squark and is assumed to decay exclusively via $\\tilde{b}_1 \\rightarrow b \\tilde{\\chi}_1^0$, where $\\tilde{\\chi}_1^0$ is the lightest neutralino. The limits significantly extend previous results; bottom squark masses up to 800 (840) GeV are excluded for the $\\tilde{\\chi}_1^0$ mass below 360 (100) GeV whilst differences in mass above 100 GeV between the $\\tilde{b}_1$ and the $\\tilde{\\chi}_1^0$ are excluded up to a $\\tilde{b}_1$ mass of 500 GeV.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.74005.v1/t1","@type":"Dataset","description":"Expected exclusion limit at 95% CL in the $m(\\tilde b_1)$-$m(\\tilde\\chi^0_1)$ plane for the sbottom pair production scenario.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.74005.v1/t2","@type":"Dataset","description":"Observed exclusion limit at 95% CL in the $m(\\tilde b_1)$-$m(\\tilde\\chi^0_1)$ plane for the sbottom pair production scenario.","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.74005.v1/t3","@type":"Dataset","description":"Signal region (SR) providing the best expected sensitivity in the $m(\\tilde b_1)$-$m(\\tilde\\chi^0_1)$ plane.","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.74005.v1/t4","@type":"Dataset","description":"Cross-section upper limit in the $m(\\tilde b_1)$-$m(\\tilde\\chi^0_1)$ plane for the best expected signal region.","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.74005.v1/t5","@type":"Dataset","description":"Cross-section upper limit in the $m(\\tilde b_1)$-$m(\\tilde\\chi^0_1)$ plane for the SRA250 signal region.","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.74005.v1/t6","@type":"Dataset","description":"Cross-section upper limit in the $m(\\tilde b_1)$-$m(\\tilde\\chi^0_1)$ plane for the SRA350 signal region.","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.74005.v1/t7","@type":"Dataset","description":"Cross-section upper limit in the $m(\\tilde b_1)$-$m(\\tilde\\chi^0_1)$ plane for the SRA450 signal region.","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.74005.v1/t8","@type":"Dataset","description":"Cross-section upper limit in the $m(\\tilde b_1)$-$m(\\tilde\\chi^0_1)$ plane for the SRB signal region.","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.74005.v1/t9","@type":"Dataset","description":"Expected CLs values in the $m(\\tilde b_1)$-$m(\\tilde\\chi^0_1)$ plane for the best expected signal region.","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.74005.v1/t10","@type":"Dataset","description":"Expected CLs values in the $m(\\tilde b_1)$-$m(\\tilde\\chi^0_1)$ plane for the SRA250 signal region.","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.74005.v1/t11","@type":"Dataset","description":"Expected exclusion limit at 95% CL in the $m(\\tilde b_1)$-$m(\\tilde\\chi^0_1)$ plane for the sbottom pair production scenario, for signal region...","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.74005.v1/t12","@type":"Dataset","description":"Observed exclusion limit at 95% CL in the $m(\\tilde b_1)$-$m(\\tilde\\chi^0_1)$ plane for the sbottom pair production 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b_1)$-$m(\\tilde\\chi^0_1)$ plane for the sbottom pair production scenario, for the SRA250 signal region.","name":"Table 33"},{"@id":"https://doi.org/10.17182/hepdata.74005.v1/t34","@type":"Dataset","description":"Signal acceptance (in %) in the $m(\\tilde b_1)$-$m(\\tilde\\chi^0_1)$ plane for the sbottom pair production scenario, for the SRA350 signal region.","name":"Table 34"},{"@id":"https://doi.org/10.17182/hepdata.74005.v1/t35","@type":"Dataset","description":"Signal acceptance (in %) in the $m(\\tilde b_1)$-$m(\\tilde\\chi^0_1)$ plane for the sbottom pair production scenario, for the SRA450 signal region.","name":"Table 35"},{"@id":"https://doi.org/10.17182/hepdata.74005.v1/t36","@type":"Dataset","description":"Signal acceptance (in %) in the $m(\\tilde b_1)$-$m(\\tilde\\chi^0_1)$ plane for the sbottom pair production scenario, for the SRB signal region.","name":"Table 36"},{"@id":"https://doi.org/10.17182/hepdata.74005.v1/t37","@type":"Dataset","description":"Total experimental systematic uncertainty in percent on the signal efficiency times acceptance in the $m(\\tilde b_1)$-$m(\\tilde\\chi^0_1)$ plane. 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