{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.83011.v3","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1672099"}},{"@id":"https://doi.org/10.1007/JHEP09(2018)050","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2018","description":"A search for supersymmetric partners of top quarks decaying as $\\tilde{t}_1\\rightarrow c\\tilde{\\chi}_1^0$ and supersymmetric partners of charm quarks decaying as $\\tilde{c}_1\\rightarrow c\\tilde{\\chi}_1^0$, where $\\tilde{\\chi}_1^0$ is the lightest neutralino, is presented. The search uses 36.1 fb$^{-1}$ $pp$ collision data at a centre-of-mass energy of 13 TeV collected by the ATLAS experiment at the Large Hadron Collider and is performed in final states with jets identified as containing charm hadrons. Assuming a 100% branching ratio to $c\\tilde{\\chi}_1^0$, top and charm squarks with masses up to 850 GeV are excluded at 95% confidence level     for a massless lightest neutralino. For $m_{\\tilde{t}_1,\\tilde{c}_1}-m_{\\tilde{\\chi}_1^0} < 100$ GeV, top and charm squark masses 1 up to 500 GeV are excluded.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.83011.v3/t1","@type":"Dataset","description":"Acceptance for SR1 in the $\\tilde{t}_1/\\tilde{c}_1-\\tilde{\\chi}_1^0$ mass plane.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.83011.v3/t2","@type":"Dataset","description":"Acceptance for SR2 in the $\\tilde{t}_1/\\tilde{c}_1-\\tilde{\\chi}_1^0$ mass plane.","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.83011.v3/t3","@type":"Dataset","description":"Acceptance for SR3 in the $\\tilde{t}_1/\\tilde{c}_1-\\tilde{\\chi}_1^0$ mass plane.","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.83011.v3/t4","@type":"Dataset","description":"Acceptance for SR4 in the $\\tilde{t}_1/\\tilde{c}_1-\\tilde{\\chi}_1^0$ mass plane.","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.83011.v3/t5","@type":"Dataset","description":"Acceptance for SR5 in the $\\tilde{t}_1/\\tilde{c}_1-\\tilde{\\chi}_1^0$ mass plane.","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.83011.v3/t6","@type":"Dataset","description":"Acceptance for best expected CLS SR in the $\\tilde{t}_1/\\tilde{c}_1-\\tilde{\\chi}_1^0$ mass plane.","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.83011.v3/t7","@type":"Dataset","description":"Detector efficiency for SR1 in the $\\tilde{t}_1/\\tilde{c}_1-\\tilde{\\chi}_1^0$ mass plane.","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.83011.v3/t8","@type":"Dataset","description":"Detector efficiency for SR2 in the $\\tilde{t}_1/\\tilde{c}_1-\\tilde{\\chi}_1^0$ mass plane.","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.83011.v3/t9","@type":"Dataset","description":"Detector efficiency for SR3 in the $\\tilde{t}_1/\\tilde{c}_1-\\tilde{\\chi}_1^0$ mass plane.","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.83011.v3/t10","@type":"Dataset","description":"Detector efficiency for SR4 in the $\\tilde{t}_1/\\tilde{c}_1-\\tilde{\\chi}_1^0$ mass plane.","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.83011.v3/t11","@type":"Dataset","description":"Detector efficiency for SR5 in the $\\tilde{t}_1/\\tilde{c}_1-\\tilde{\\chi}_1^0$ mass plane.","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.83011.v3/t12","@type":"Dataset","description":"Detector efficiency for best expected CLS SR in the $\\tilde{t}_1/\\tilde{c}_1-\\tilde{\\chi}_1^0$ mass plane.","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.83011.v3/t13","@type":"Dataset","description":"Expected exclusion limit at 95% CL in the $m(\\tilde t_1/\\tilde c_1)$-$m(\\tilde\\chi^0_1)$ plane for the stop/scharm pair production scenario.","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.83011.v3/t14","@type":"Dataset","description":"Observed exclusion limit at 95% CL in the $m(\\tilde t_1/\\tilde c_1)$-$m(\\tilde\\chi^0_1)$ plane for the stop/scharm pair production scenario.","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.83011.v3/t15","@type":"Dataset","description":"SR1 expected exclusion limit at 95% CL in the $m(\\tilde t_1/\\tilde c_1)$-$m(\\tilde\\chi^0_1)$ plane for the stop/scharm pair production scenario.","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.83011.v3/t16","@type":"Dataset","description":"SR1 observed exclusion limit at 95% CL in the $m(\\tilde t_1/\\tilde c_1)$-$m(\\tilde\\chi^0_1)$ plane for the stop/scharm pair production scenario.","name":"Table 16"},{"@id":"https://doi.org/10.17182/hepdata.83011.v3/t17","@type":"Dataset","description":"SR2 expected exclusion limit at 95% CL in the $m(\\tilde t_1/\\tilde c_1)$-$m(\\tilde\\chi^0_1)$ plane for the stop/scharm pair production scenario.","name":"Table 17"},{"@id":"https://doi.org/10.17182/hepdata.83011.v3/t18","@type":"Dataset","description":"SR2 observed exclusion limit at 95% CL in the $m(\\tilde t_1/\\tilde c_1)$-$m(\\tilde\\chi^0_1)$ plane for the stop/scharm pair production scenario.","name":"Table 18"},{"@id":"https://doi.org/10.17182/hepdata.83011.v3/t19","@type":"Dataset","description":"SR3 expected exclusion limit at 95% CL in the $m(\\tilde t_1/\\tilde c_1)$-$m(\\tilde\\chi^0_1)$ plane for the stop/scharm pair production scenario.","name":"Table 19"},{"@id":"https://doi.org/10.17182/hepdata.83011.v3/t20","@type":"Dataset","description":"SR3 observed exclusion limit at 95% CL in the $m(\\tilde t_1/\\tilde c_1)$-$m(\\tilde\\chi^0_1)$ plane for the stop/scharm pair production scenario.","name":"Table 20"},{"@id":"https://doi.org/10.17182/hepdata.83011.v3/t21","@type":"Dataset","description":"SR4 expected exclusion limit at 95% CL in the $m(\\tilde t_1/\\tilde c_1)$-$m(\\tilde\\chi^0_1)$ plane for the stop/scharm pair production scenario.","name":"Table 21"},{"@id":"https://doi.org/10.17182/hepdata.83011.v3/t22","@type":"Dataset","description":"SR4 observed exclusion limit at 95% CL in the $m(\\tilde t_1/\\tilde c_1)$-$m(\\tilde\\chi^0_1)$ plane for the stop/scharm pair production scenario.","name":"Table 22"},{"@id":"https://doi.org/10.17182/hepdata.83011.v3/t23","@type":"Dataset","description":"SR5 expected exclusion limit at 95% CL in the $m(\\tilde t_1/\\tilde c_1)$-$m(\\tilde\\chi^0_1)$ plane for the stop/scharm pair production scenario.","name":"Table 23"},{"@id":"https://doi.org/10.17182/hepdata.83011.v3/t24","@type":"Dataset","description":"SR5 observed exclusion limit at 95% CL in the $m(\\tilde t_1/\\tilde c_1)$-$m(\\tilde\\chi^0_1)$ plane for the stop/scharm pair production scenario.","name":"Table 24"},{"@id":"https://doi.org/10.17182/hepdata.83011.v3/t25","@type":"Dataset","description":"Upper limits on signal cross sections and exclusion limits at 95% CL for SR1 in the $m(\\tilde t_1/\\tilde c_1)$-$m(\\tilde\\chi^0_1)$ plane...","name":"Table 25"},{"@id":"https://doi.org/10.17182/hepdata.83011.v3/t26","@type":"Dataset","description":"Upper limits on signal cross sections and exclusion limits at 95% CL for SR2 in the $m(\\tilde t_1/\\tilde c_1)$-$m(\\tilde\\chi^0_1)$ plane...","name":"Table 26"},{"@id":"https://doi.org/10.17182/hepdata.83011.v3/t27","@type":"Dataset","description":"Upper limits on signal cross sections and exclusion limits at 95% CL for SR3 in the $m(\\tilde t_1/\\tilde c_1)$-$m(\\tilde\\chi^0_1)$ plane...","name":"Table 27"},{"@id":"https://doi.org/10.17182/hepdata.83011.v3/t28","@type":"Dataset","description":"Upper limits on signal cross sections and exclusion limits at 95% CL for SR4 in the $m(\\tilde t_1/\\tilde c_1)$-$m(\\tilde\\chi^0_1)$ plane...","name":"Table 28"},{"@id":"https://doi.org/10.17182/hepdata.83011.v3/t29","@type":"Dataset","description":"Upper limits on signal cross sections and exclusion limits at 95% CL for SR5 in the $m(\\tilde t_1/\\tilde c_1)$-$m(\\tilde\\chi^0_1)$ plane...","name":"Table 29"},{"@id":"https://doi.org/10.17182/hepdata.83011.v3/t30","@type":"Dataset","description":"Upper limits on signal cross sections and exclusion limits at 95% CL for the best expected SR in the $m(\\tilde...","name":"Table 30"},{"@id":"https://doi.org/10.17182/hepdata.83011.v3/t31","@type":"Dataset","description":"Minimum branching ratio excluded at 95% CL, assuming no sensitivity for other decay possibilities, in the $m(\\tilde t_1/\\tilde c_1)$-$m(\\tilde\\chi^0_1)$ plane...","name":"Table 31"},{"@id":"https://doi.org/10.17182/hepdata.83011.v3/t32","@type":"Dataset","description":"The signal region with the best expected CLS value for each signal in the $\\tilde{t}_1/\\tilde{c}_1-\\tilde{\\chi}_1^0$ mass plane.","name":"Table 32"},{"@id":"https://doi.org/10.17182/hepdata.83011.v3/t33","@type":"Dataset","description":"Expected exclusion limit at 95% CL in the $m(\\tilde t_1/\\tilde c_1)$-$\\Delta m$ plane for the stop/scharm pair production scenario.","name":"Table 33"},{"@id":"https://doi.org/10.17182/hepdata.83011.v3/t34","@type":"Dataset","description":"Observed exclusion limit at 95% CL in the $m(\\tilde t_1/\\tilde c_1)$-$\\Delta m$ plane for the stop/scharm pair production scenario.","name":"Table 34"},{"@id":"https://doi.org/10.17182/hepdata.83011.v3/t35","@type":"Dataset","description":"Comparison between data and expectation after the background-only fit for the $E_{T}^{miss}$ distribution in SR1. The shaded band indicates detector-related...","name":"Table 35"},{"@id":"https://doi.org/10.17182/hepdata.83011.v3/t36","@type":"Dataset","description":"Comparison between data and expectation after the background-only fit for the $E_{T}^{miss}$ distribution in SR2. The shaded band indicates detector-related...","name":"Table 36"},{"@id":"https://doi.org/10.17182/hepdata.83011.v3/t37","@type":"Dataset","description":"Comparison between data and expectation after the background-only fit for the $E_{T}^{miss}$ distribution in SR3. The shaded band indicates detector-related...","name":"Table 37"},{"@id":"https://doi.org/10.17182/hepdata.83011.v3/t38","@type":"Dataset","description":"Comparison between data and expectation after the background-only fit for the $E_{T}^{miss}$ distribution in SR4. The shaded band indicates detector-related...","name":"Table 38"},{"@id":"https://doi.org/10.17182/hepdata.83011.v3/t39","@type":"Dataset","description":"Comparison between data and expectation after the background-only fit for the $E_{T}^{miss}$ distribution in SR5. The shaded band indicates detector-related...","name":"Table 39"},{"@id":"https://doi.org/10.17182/hepdata.83011.v3/t40","@type":"Dataset","description":"Cutflow for the $(m_{\\tilde{t}}, m_{\\tilde{\\chi}}) = (450,425)$ GeV signal point for signal region SR1.","name":"Table 40"},{"@id":"https://doi.org/10.17182/hepdata.83011.v3/t41","@type":"Dataset","description":"Cutflow for the $(m_{\\tilde{t}}, m_{\\tilde{\\chi}}) = (500,420)$ GeV signal point for signal region SR2.","name":"Table 41"},{"@id":"https://doi.org/10.17182/hepdata.83011.v3/t42","@type":"Dataset","description":"Cutflow for the $(m_{\\tilde{t}}, m_{\\tilde{\\chi}}) = (500,350)$ GeV signal point for signal region SR3.","name":"Table 42"},{"@id":"https://doi.org/10.17182/hepdata.83011.v3/t43","@type":"Dataset","description":"Cutflow for the $(m_{\\tilde{t}}, m_{\\tilde{\\chi}}) = (600,350)$ GeV signal point for signal region SR4.","name":"Table 43"},{"@id":"https://doi.org/10.17182/hepdata.83011.v3/t44","@type":"Dataset","description":"Cutflow for the $(m_{\\tilde{t}}, m_{\\tilde{\\chi}}) = (900,1)$ GeV signal point for signal region SR5.","name":"Table 44"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1672099?version=3"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/83011"}],"inLanguage":"en","name":"Search for supersymmetry in final states with charm jets and missing transverse momentum in 13 TeV $pp$ collisions with the ATLAS detector","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1672099?version=3","version":3}