{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.68163.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1304456"}},{"@id":"https://doi.org/10.1007/JHEP11(2014)118","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2015","description":"CERN-LHC.  The results of a search for top squark (stop) pair production in final states with one isolated lepton, jets, and missing transverse momentum are reported. The analysis is performed with proton-proton collision data at $\\sqrt{s}=$ 8 TeV collected with the ATLAS detector at the LHC in 2012 corresponding to an integrated luminosity of 20 fb$^{-1}$. The lightest supersymmetric particle (LSP) is taken to be the lightest neutralino which only interacts weakly and is assumed to be stable. The stop decay scenarios considered are those to a top quark and the LSP as well as to a bottom quark and the lightest chargino, where the chargino decays to the LSP by emitting a W boson. A wide range of scenarios with different mass splittings between the stop, the lightest neutralino and the lightest chargino are considered, including cases where the W bosons or the top quarks are off-shell. Decay scenarios involving the heavier charginos and neutralinos are addressed using a set of phenomenological models of supersymmetry. No significant excess over the Standard Model prediction is observed. A stop with a mass between 210 and 640 GeV decaying directly to a top quark and a massless LSP is excluded at 95% confidence level, and in models where the mass of the lightest chargino is twice that of the LSP, stops are excluded at 95% confidence level up to a mass of 500 GeV for an LSP mass in the range of 100 to 150 GeV. Stringent exclusion limits are also derived for all other considered stop decay scenarios, and generic upper limits are set on the visible cross-section for processes beyond the Standard Model.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t1","@type":"Dataset","description":"Expected and observed $H_{T,sig}^{miss}$ distribution for tN_med SR, before applying the $H_{T,sig}^{miss}>12$ requirement. The uncertainty includes statistical and all experimental...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t2","@type":"Dataset","description":"Expected and observed large-R jet mass distribution for tN_boost SR, before applying the large-R jet mass$>75$ GeV requirement. The uncertainty...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t3","@type":"Dataset","description":"Expected and observed b-jet multiplicity distribution for bCc_diag SR, before applying the b-jet multiplicity$=0$ requirement. The uncertainty includes statistical and...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t4","@type":"Dataset","description":"Expected and observed $am_{T2}$ distribution for bCd_high1 SR, before applying the $am_{T2}>200$ GeV requirement. The uncertainty includes statistical and all...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t5","@type":"Dataset","description":"Expected and observed leading b-jet $p_T$ distribution for bCd_high2 SR, before applying the leading b-jet $p_T>170$ GeV requirement. The uncertainty...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t6","@type":"Dataset","description":"Expected and observed $E_T^{miss}$ distribution for tNbC_mix SR, before applying the $E_T^{miss}>270$ GeV requirement. The uncertainty includes statistical and all...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t7","@type":"Dataset","description":"Expected and observed lepton $p_T$ distribution for bCa_low SR. The uncertainty includes statistical and all experimental systematic uncertainties. The last...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t8","@type":"Dataset","description":"Expected and observed lepton $p_T$ distribution for bCa_med SR. The uncertainty includes statistical and all experimental systematic uncertainties. The last...","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t9","@type":"Dataset","description":"Expected and observed $am_T2$ distribution for bCb_med1 SR. The uncertainty includes statistical and all experimental systematic uncertainties. The last bin...","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t10","@type":"Dataset","description":"Expected and observed $am_T2$ distribution for bCb_high SR. The uncertainty includes statistical and all experimental systematic uncertainties. The last bin...","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t11","@type":"Dataset","description":"Best expected signal region for the $\\tilde t_1\\to t\\chi^0_1$ scenario with $m_{\\tilde t_1}>m_t+m_{\\chi^0_1}$. This mapping is used for the final...","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t12","@type":"Dataset","description":"Best expected signal region for the $\\tilde t_1$ three-body scenario ($\\tilde t_1\\to bW\\chi^0_1$). This mapping is used for the final...","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t13","@type":"Dataset","description":"Best expected signal region for the $\\tilde t_1$ four-body scenario ($\\tilde t_1\\to bff'\\chi^0_1$). This mapping is used for the final...","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t14","@type":"Dataset","description":"Best expected signal region for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=2\\times m_{\\chi^0_1}$. This mapping is used for the final...","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t15","@type":"Dataset","description":"Best expected signal region for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=150$ GeV. This mapping is used for the final...","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t16","@type":"Dataset","description":"Best expected signal region for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=106$ GeV. This mapping is used for the final...","name":"Table 16"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t17","@type":"Dataset","description":"Best expected signal region for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=m_{\\chi^0_1}+5$ GeV. This mapping is used for the final...","name":"Table 17"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t18","@type":"Dataset","description":"Best expected signal region for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=m_{\\chi^0_1}+20$ GeV. This mapping is used for the final...","name":"Table 18"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t19","@type":"Dataset","description":"Best expected signal region for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=m_{\\tilde t_1}-10$ GeV. This mapping is used for the...","name":"Table 19"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t20","@type":"Dataset","description":"Best expected signal region for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\tilde t_1}=300$ GeV. This mapping is used for the...","name":"Table 20"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t21","@type":"Dataset","description":"Upper limits on the model cross-section for the $\\tilde t_1\\to t\\chi^0_1$ scenario with $m_{\\tilde t_1}>m_t+m_{\\chi^0_1}$.","name":"Table 21"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t22","@type":"Dataset","description":"Observed exclusion contour for the $\\tilde t_1\\to t\\chi^0_1$ scenario with $m_{\\tilde t_1}>m_t+m_{\\chi^0_1}$.","name":"Table 22"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t23","@type":"Dataset","description":"Expected exclusion contour for the $\\tilde t_1\\to t\\chi^0_1$ scenario with $m_{\\tilde t_1}>m_t+m_{\\chi^0_1}$.","name":"Table 23"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t24","@type":"Dataset","description":"Upper limit on signal events for the $\\tilde t_1$ three-body scenario ($\\tilde t_1\\to bW\\chi^0_1$).","name":"Table 24"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t25","@type":"Dataset","description":"Observed exclusion contour for the $\\tilde t_1$ three-body scenario ($\\tilde t_1\\to bW\\chi^0_1$).","name":"Table 25"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t26","@type":"Dataset","description":"Expected exclusion contour for the $\\tilde t_1$ three-body scenario ($\\tilde t_1\\to bW\\chi^0_1$).","name":"Table 26"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t27","@type":"Dataset","description":"Upper limit on signal events for the $\\tilde t_1$ four-body scenario ($\\tilde t_1\\to bff'\\chi^0_1$).","name":"Table 27"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t28","@type":"Dataset","description":"Observed exclusion contour for the $\\tilde t_1$ four-body scenario ($\\tilde t_1\\to bff'\\chi^0_1$).","name":"Table 28"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t29","@type":"Dataset","description":"Expected exclusion contour for the $\\tilde t_1$ four-body scenario ($\\tilde t_1\\to bff'\\chi^0_1$).","name":"Table 29"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t30","@type":"Dataset","description":"Upper limit on signal events for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=2\\times m_{\\chi^0_1}$.","name":"Table 30"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t31","@type":"Dataset","description":"Observed exclusion contour for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=2\\times m_{\\chi^0_1}$.","name":"Table 31"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t32","@type":"Dataset","description":"Expected exclusion contour for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=2\\times m_{\\chi^0_1}$.","name":"Table 32"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t33","@type":"Dataset","description":"Upper limit on signal events for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=150$ GeV.","name":"Table 33"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t34","@type":"Dataset","description":"Observed exclusion contour for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=150$ GeV.","name":"Table 34"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t35","@type":"Dataset","description":"Expected exclusion contour for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=150$ GeV.","name":"Table 35"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t36","@type":"Dataset","description":"Upper limit on signal events for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=106$ GeV.","name":"Table 36"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t37","@type":"Dataset","description":"Observed exclusion contour for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=106$ GeV.","name":"Table 37"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t38","@type":"Dataset","description":"Expected exclusion contour for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=106$ GeV.","name":"Table 38"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t39","@type":"Dataset","description":"Upper limit on signal events for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=m_{\\chi^0_1}+5$ GeV.","name":"Table 39"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t40","@type":"Dataset","description":"Observed exclusion contour for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=m_{\\chi^0_1}+5$ GeV.","name":"Table 40"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t41","@type":"Dataset","description":"Expected exclusion contour for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=m_{\\chi^0_1}+5$ GeV.","name":"Table 41"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t42","@type":"Dataset","description":"Upper limit on signal events for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=m_{\\chi^0_1}+20$ GeV.","name":"Table 42"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t43","@type":"Dataset","description":"Observed exclusion contour for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=m_{\\chi^0_1}+20$ GeV.","name":"Table 43"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t44","@type":"Dataset","description":"Expected exclusion contour for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=m_{\\chi^0_1}+20$ GeV.","name":"Table 44"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t45","@type":"Dataset","description":"Upper limit on signal events for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=m_{\\tilde t_1}-10$ GeV.","name":"Table 45"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t46","@type":"Dataset","description":"Observed exclusion contour for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=m_{\\tilde t_1}-10$ GeV.","name":"Table 46"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t47","@type":"Dataset","description":"Expected exclusion contour for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=m_{\\tilde t_1}-10$ GeV.","name":"Table 47"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t48","@type":"Dataset","description":"Upper limit on signal events for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\tilde t_1}=300$ GeV.","name":"Table 48"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t49","@type":"Dataset","description":"Observed exclusion contour for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\tilde t_1}=300$ GeV.","name":"Table 49"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t50","@type":"Dataset","description":"Expected exclusion contour for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\tilde t_1}=300$ GeV.","name":"Table 50"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t51","@type":"Dataset","description":"Acceptance of tN_diag SR ($E_T^{miss}>150$ GeV, $m_T>140$ GeV) for the $\\tilde t_1\\to t\\chi^0_1$ scenario with $m_{\\tilde t_1}>m_t+m_{\\chi^0_1}$. The acceptance is...","name":"Table 51"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t52","@type":"Dataset","description":"Acceptance of tN_med SR for the $\\tilde t_1\\to t\\chi^0_1$ scenario with $m_{\\tilde t_1}>m_t+m_{\\chi^0_1}$. The acceptance is defined as the fraction...","name":"Table 52"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t53","@type":"Dataset","description":"Acceptance of tN_boost SR for the $\\tilde t_1\\to t\\chi^0_1$ scenario with $m_{\\tilde t_1}>m_t+m_{\\chi^0_1}$. The acceptance is defined as the fraction...","name":"Table 53"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t54","@type":"Dataset","description":"Acceptance of bCb_med2 SR ($am_{T2}>250$ GeV, $m_T>60$ GeV) for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=2\\times m_{\\chi^0_1}$. The acceptance is...","name":"Table 54"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t55","@type":"Dataset","description":"Acceptance of bCc_diag SR for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=2\\times m_{\\chi^0_1}$. The acceptance is defined as the fraction...","name":"Table 55"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t56","@type":"Dataset","description":"Acceptance of bCd_bulk SR ($am_{T2}>175$ GeV, $m_T>120$ GeV) for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=2\\times m_{\\chi^0_1}$. The acceptance is...","name":"Table 56"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t57","@type":"Dataset","description":"Acceptance of bCd_high1 SR for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=2\\times m_{\\chi^0_1}$. The acceptance is defined as the fraction...","name":"Table 57"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t58","@type":"Dataset","description":"Acceptance of bCd_high2 SR for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=2\\times m_{\\chi^0_1}$. The acceptance is defined as the fraction...","name":"Table 58"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t59","@type":"Dataset","description":"Acceptance of bCa_med for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=m_{\\chi^0_1}+20$ GeV. The acceptance is defined as the fraction of...","name":"Table 59"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t60","@type":"Dataset","description":"Acceptance of bCa_low for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=m_{\\chi^0_1}+20$ GeV. The acceptance is defined as the fraction of...","name":"Table 60"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t61","@type":"Dataset","description":"Acceptance of bCb_med1 for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=m_{\\chi^0_1}+20$ GeV. The acceptance is defined as the fraction of...","name":"Table 61"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t62","@type":"Dataset","description":"Acceptance of bCb_high for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=m_{\\chi^0_1}+20$ GeV. The acceptance is defined as the fraction of...","name":"Table 62"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t63","@type":"Dataset","description":"Acceptance of 3-body SR ($80<am_{T2}<90$ GeV, $m_T>120$ GeV) for the 3-body scenario ($\\tilde t_1\\to b W\\chi^0_1$). The acceptance is defined...","name":"Table 63"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t64","@type":"Dataset","description":"Acceptance of tNbC_mix SR for the asymmetric scenario ($\\tilde t_1$, $\\tilde t_1\\to t\\chi^0_1$, b $\\chi^\\pm_1$) with $m_{\\chi^\\pm_1}=2\\times m_{\\chi^0_1}$. The acceptance...","name":"Table 64"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t65","@type":"Dataset","description":"Efficiency of tN_diag SR ($E_T^{miss}>150$ GeV, $m_T>140$ GeV) for the $\\tilde t_1\\to t\\chi^0_1$ scenario with $m_{\\tilde t_1}>m_t+m_{\\chi^0_1}$. The efficiency is...","name":"Table 65"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t66","@type":"Dataset","description":"Efficiency of tN_med SR for the $\\tilde t_1\\to t\\chi^0_1$ scenario with $m_{\\tilde t_1}>m_t+m_{\\chi^0_1}$. The efficiency is the ratio between the...","name":"Table 66"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t67","@type":"Dataset","description":"Efficiency of tN_boost SR for the $\\tilde t_1\\to t\\chi^0_1$ scenario with $m_{\\tilde t_1}>m_t+m_{\\chi^0_1}$. The efficiency is the ratio between the...","name":"Table 67"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t68","@type":"Dataset","description":"Efficiency of bCb_med2 SR ($am_{T2}>250$ GeV, $m_T>60$ GeV) for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=2\\times m_{\\chi^0_1}$. The efficiency is...","name":"Table 68"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t69","@type":"Dataset","description":"Efficiency of bCc_diag SR for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=2\\times m_{\\chi^0_1}$. The efficiency is the ratio between the...","name":"Table 69"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t70","@type":"Dataset","description":"Efficiency of bCd_bulk SR ($am_{T2}>175$ GeV, $m_T>120$ GeV) for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=2\\times m_{\\chi^0_1}$. The efficiency is...","name":"Table 70"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t71","@type":"Dataset","description":"Efficiency of bCd_high1 SR for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=2\\times m_{\\chi^0_1}$. The efficiency is the ratio between the...","name":"Table 71"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t72","@type":"Dataset","description":"Efficiency of bCd_high2 SR for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=2\\times m_{\\chi^0_1}$. The efficiency is the ratio between the...","name":"Table 72"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t73","@type":"Dataset","description":"Efficiency of bCa_med for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=m_{\\chi^0_1}+20$ GeV. The efficiency is the ratio between the expected...","name":"Table 73"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t74","@type":"Dataset","description":"Efficiency of bCa_low for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=m_{\\chi^0_1}+20$ GeV. The efficiency is the ratio between the expected...","name":"Table 74"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t75","@type":"Dataset","description":"Efficiency of bCb_med1 for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=m_{\\chi^0_1}+20$ GeV. The efficiency is the ratio between the expected...","name":"Table 75"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t76","@type":"Dataset","description":"Efficiency of bCb_high for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=m_{\\chi^0_1}+20$ GeV. The efficiency is the ratio between the expected...","name":"Table 76"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t77","@type":"Dataset","description":"Efficiency of 3-body SR ($80<am_{T2}<90$ GeV, $m_T>120$ GeV) for the 3-body scenario ($\\tilde t_1\\to b W\\chi^0_1$). The efficiency is the...","name":"Table 77"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t78","@type":"Dataset","description":"Efficiency of tNbC_mix SR for the asymmetric scenario ($\\tilde t_1$, $\\tilde t_1\\to t\\chi^0_1$, b $\\chi^\\pm_1$) with $m_{\\chi^\\pm_1}=2\\times m_{\\chi^0_1}$. The efficiency...","name":"Table 78"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t79","@type":"Dataset","description":"Number of generated events for the $\\tilde t_1\\to t\\chi^0_1$ scenario with $m_{\\tilde t_1}>m_t+m_{\\chi^0_1}$.","name":"Table 79"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t80","@type":"Dataset","description":"Number of generated events for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=2\\times m_{\\chi^0_1}$.","name":"Table 80"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t81","@type":"Dataset","description":"Number of generated events for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=m_{\\chi^0_1}+20$ GeV; $E_T^{miss}$(gen)$>60$ GeV.","name":"Table 81"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t82","@type":"Dataset","description":"Number of generated events for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=m_{\\chi^0_1}+20$ GeV; $E_T^{miss}$(gen)$>250$ GeV.","name":"Table 82"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t83","@type":"Dataset","description":"Number of generated events for the 3-body scenario ($\\tilde t_1\\to b W\\chi^0_1$).","name":"Table 83"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t84","@type":"Dataset","description":"Number of generated events for the asymmetric scenario ($\\tilde t_1$, $\\tilde t_1\\to t\\chi^0_1$, b $\\chi^\\pm_1$) with $m_{\\chi^\\pm_1}=2\\times m_{\\chi^0_1}$.","name":"Table 84"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t85","@type":"Dataset","description":"Cross-section for the $\\tilde t_1\\to t\\chi^0_1$ scenario with $m_{\\tilde t_1}>m_t+m_{\\chi^0_1}$.","name":"Table 85"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t86","@type":"Dataset","description":"Cross-section for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=2\\times m_{\\chi^0_1}$.","name":"Table 86"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t87","@type":"Dataset","description":"Cross-section for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=m_{\\chi^0_1}+20$ GeV.","name":"Table 87"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t88","@type":"Dataset","description":"Cross-section for the 3-body scenario ($\\tilde t_1\\to b W\\chi^0_1$).","name":"Table 88"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t89","@type":"Dataset","description":"Cross-section for the asymmetric scenario ($\\tilde t_1$, $\\tilde t_1\\to t\\chi^0_1$, b $\\chi^\\pm_1$) with $m_{\\chi^\\pm_1}=2\\times m_{\\chi^0_1}$.","name":"Table 89"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t90","@type":"Dataset","description":"Combined experimental systematic uncertainty of expected tN_diag SR yields for the $\\tilde t_1\\to t\\chi^0_1$ scenario with $m_{\\tilde t_1}>m_t+m_{\\chi^0_1}$, using the...","name":"Table 90"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t91","@type":"Dataset","description":"Combined experimental systematic uncertainty of expected tN_med SR yields for the $\\tilde t_1\\to t\\chi^0_1$ scenario with $m_{\\tilde t_1}>m_t+m_{\\chi^0_1}$.","name":"Table 91"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t92","@type":"Dataset","description":"Combined experimental systematic uncertainty of expected tN_boost SR yields for the $\\tilde t_1\\to t\\chi^0_1$ scenario with $m_{\\tilde t_1}>m_t+m_{\\chi^0_1}$.","name":"Table 92"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t93","@type":"Dataset","description":"Combined experimental systematic uncertainty of expected bCb_med2 SR yields for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=2\\times m_{\\chi^0_1}$, using the...","name":"Table 93"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t94","@type":"Dataset","description":"Combined experimental systematic uncertainty of expected bCc_diag SR yields for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=2\\times m_{\\chi^0_1}$.","name":"Table 94"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t95","@type":"Dataset","description":"Combined experimental systematic uncertainty of expected bCd_bulk SR yields for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=2\\times m_{\\chi^0_1}$, using the...","name":"Table 95"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t96","@type":"Dataset","description":"Combined experimental systematic uncertainty of expected bCd_high1 SR yields for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=2\\times m_{\\chi^0_1}$.","name":"Table 96"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t97","@type":"Dataset","description":"Combined experimental systematic uncertainty of expected bCd_high2 SR yields for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=2\\times m_{\\chi^0_1}$.","name":"Table 97"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t98","@type":"Dataset","description":"Combined experimental systematic uncertainty of expected bCa_med SR yields for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=m_{\\chi^0_1}+20$ GeV.","name":"Table 98"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t99","@type":"Dataset","description":"Combined experimental systematic uncertainty of expected bCa_low SR yields for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=m_{\\chi^0_1}+20$ GeV.","name":"Table 99"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t100","@type":"Dataset","description":"Combined experimental systematic uncertainty of expected bCb_med1 SR yields for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=m_{\\chi^0_1}+20$ GeV.","name":"Table 100"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t101","@type":"Dataset","description":"Combined experimental systematic uncertainty of expected bCb_high SR yields for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=m_{\\chi^0_1}+20$ GeV.","name":"Table 101"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t102","@type":"Dataset","description":"Combined experimental systematic uncertainty of expected 3-body SR yields for the 3-body scenario ($\\tilde t_1\\to b W\\chi^0_1$), using the 2...","name":"Table 102"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t103","@type":"Dataset","description":"Combined experimental systematic uncertainty of expected tNbC_mix SR yields for the asymmetric scenario ($\\tilde t_1$, $\\tilde t_1\\to t\\chi^0_1$, b $\\chi^\\pm_1$)...","name":"Table 103"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t104","@type":"Dataset","description":"Observed CLs in tN_diag SR for the $\\tilde t_1\\to t\\chi^0_1$ scenario with $m_{\\tilde t_1}>m_t+m_{\\chi^0_1}$.","name":"Table 104"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t105","@type":"Dataset","description":"Observed CLs in tN_med SR for the $\\tilde t_1\\to t\\chi^0_1$ scenario with $m_{\\tilde t_1}>m_t+m_{\\chi^0_1}$.","name":"Table 105"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t106","@type":"Dataset","description":"Observed CLs in tN_boost SR for the $\\tilde t_1\\to t\\chi^0_1$ scenario with $m_{\\tilde t_1}>m_t+m_{\\chi^0_1}$.","name":"Table 106"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t107","@type":"Dataset","description":"Observed CLs in bCb_med2 SR for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=2\\times m_{\\chi^0_1}$.","name":"Table 107"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t108","@type":"Dataset","description":"Observed CLs in bCc_diag SR for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=2\\times m_{\\chi^0_1}$.","name":"Table 108"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t109","@type":"Dataset","description":"Observed CLs in bCd_bulk SR for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=2\\times m_{\\chi^0_1}$.","name":"Table 109"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t110","@type":"Dataset","description":"Observed CLs in bCd_high1 SR for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=2\\times m_{\\chi^0_1}$.","name":"Table 110"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t111","@type":"Dataset","description":"Observed CLs in bCd_high2 SR for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=2\\times m_{\\chi^0_1}$.","name":"Table 111"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t112","@type":"Dataset","description":"Observed CLs in bCa_med SR for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=m_{\\chi^0_1}+20$ GeV.","name":"Table 112"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t113","@type":"Dataset","description":"Observed CLs in bCa_low SR for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=m_{\\chi^0_1}+20$ GeV.","name":"Table 113"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t114","@type":"Dataset","description":"Observed CLs in bCb_med1 SR for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=m_{\\chi^0_1}+20$ GeV.","name":"Table 114"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t115","@type":"Dataset","description":"Observed CLs in bCb_high SR for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=m_{\\chi^0_1}+20$ GeV.","name":"Table 115"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t116","@type":"Dataset","description":"Observed CLs in 3-body SR for the 3-body scenario ($\\tilde t_1\\to b W\\chi^0_1$).","name":"Table 116"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t117","@type":"Dataset","description":"Observed CLs in tNbC_mix SR for the mixed scenario (50% $\\tilde t_1\\to t\\chi^0_1$, 50% $\\tilde t_1\\to b\\chi^0_1$).","name":"Table 117"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t118","@type":"Dataset","description":"Expected CLs in tN_diag SR for the $\\tilde t_1\\to t\\chi^0_1$ scenario with $m_{\\tilde t_1}>m_t+m_{\\chi^0_1}$.","name":"Table 118"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t119","@type":"Dataset","description":"Expected CLs in tN_med SR for the $\\tilde t_1\\to t\\chi^0_1$ scenario with $m_{\\tilde t_1}>m_t+m_{\\chi^0_1}$.","name":"Table 119"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t120","@type":"Dataset","description":"Expected CLs in tN_boost SR for the $\\tilde t_1\\to t\\chi^0_1$ scenario with $m_{\\tilde t_1}>m_t+m_{\\chi^0_1}$.","name":"Table 120"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t121","@type":"Dataset","description":"Expected CLs in bCb_med2 SR for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=2\\times m_{\\chi^0_1}$.","name":"Table 121"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t122","@type":"Dataset","description":"Expected CLs in bCc_diag SR for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=2\\times m_{\\chi^0_1}$.","name":"Table 122"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t123","@type":"Dataset","description":"Expected CLs in bCd_bulk SR for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=2\\times m_{\\chi^0_1}$.","name":"Table 123"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t124","@type":"Dataset","description":"Expected CLs in bCd_high1 SR for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=2\\times m_{\\chi^0_1}$.","name":"Table 124"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t125","@type":"Dataset","description":"Expected CLs in bCd_high2 SR for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=2\\times m_{\\chi^0_1}$.","name":"Table 125"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t126","@type":"Dataset","description":"Expected CLs in bCa_med SR for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=m_{\\chi^0_1}+20$ GeV.","name":"Table 126"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t127","@type":"Dataset","description":"Expected CLs in bCa_low SR for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=m_{\\chi^0_1}+20$ GeV.","name":"Table 127"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t128","@type":"Dataset","description":"Expected CLs in bCb_med1 SR for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=m_{\\chi^0_1}+20$ GeV.","name":"Table 128"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t129","@type":"Dataset","description":"Expected CLs in bCb_high SR for the $\\tilde t_1\\to b\\chi^\\pm_1$ scenario with $m_{\\chi^\\pm_1}=m_{\\chi^0_1}+20$ GeV.","name":"Table 129"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t130","@type":"Dataset","description":"Expected CLs in 3-body SR for the 3-body scenario ($\\tilde t_1\\to b W\\chi^0_1$).","name":"Table 130"},{"@id":"https://doi.org/10.17182/hepdata.68163.v1/t131","@type":"Dataset","description":"Expected CLs in tNbC_mix SR for the mixed scenario (50% $\\tilde t_1\\to t\\chi^0_1$, 50% $\\tilde t_1\\to b\\chi^\\pm_1$).","name":"Table 131"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1304456?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/68163"}],"inLanguage":"en","name":"Search for top squark pair production in final states with one isolated lepton, jets, and missing transverse momentum in $\\sqrt{s}=$ 8 TeV pp collisions with the ATLAS detector","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1304456?version=1","version":1}