Figure 14a Expected
Figure 14a
10.17182/hepdata.91374.v5/t1
Expected 95% CL exclusion sensitivity for simplified models of direct higgsino production.
Figure 14a
10.17182/hepdata.91374.v5/t1
Expected 95% CL exclusion sensitivity for simplified models of direct higgsino production.
Figure 14a
10.17182/hepdata.91374.v5/t2
Observed 95% CL exclusion sensitivity for simplified models of direct higgsino production.
Figure 14b
10.17182/hepdata.91374.v5/t3
Expected 95% CL exclusion sensitivity for simplified models of direct wino-bino production, assuming $m(\tilde{\chi}_{2}^{0}) \times m(\tilde{\chi}_{1}^{0})<0$.
Figure 14b
10.17182/hepdata.91374.v5/t4
Observed 95% CL exclusion sensitivity for simplified models of direct wino-bino production, assuming $m(\tilde{\chi}_{2}^{0}) \times m(\tilde{\chi}_{1}^{0})<0$.
Figure 14c
10.17182/hepdata.91374.v5/t5
Expected 95% CL exclusion sensitivity for simplified models of direct wino-bino production, assuming $m(\tilde{\chi}_{2}^{0}) \times m(\tilde{\chi}_{1}^{0})>0$.
Figure 14c
10.17182/hepdata.91374.v5/t6
Observed 95% CL exclusion sensitivity for simplified models of direct wino-bino production, assuming $m(\tilde{\chi}_{2}^{0}) \times m(\tilde{\chi}_{1}^{0})>0$.
Figure 15b
10.17182/hepdata.91374.v5/t7
Expected 95% CL exclusion sensitivity for simplified models of VBF wino-bino production.
Figure 15b
10.17182/hepdata.91374.v5/t8
Observed 95% CL exclusion sensitivity for simplified models of direct wino-bino production.
Figure 16a
10.17182/hepdata.91374.v5/t9
Expected 95% CL exclusion sensitivity for simplified models of direct slepton production.
Figure 16a
10.17182/hepdata.91374.v5/t10
Observed 95% CL exclusion sensitivity for simplified models of direct slepton production.
Figure 2b
10.17182/hepdata.91374.v5/t11
Expected 95% CL exclusion sensitivity for simplified models of direct smuon production.
Figure 2b
10.17182/hepdata.91374.v5/t12
Observed 95% CL exclusion sensitivity for simplified models of direct smuon production.
Figure 2b
10.17182/hepdata.91374.v5/t13
Expected 95% CL exclusion sensitivity for simplified models of direct selectron production.
Figure 2b
10.17182/hepdata.91374.v5/t14
Observed 95% CL exclusion sensitivity for simplified models of direct selectron production.
Figure 2a
10.17182/hepdata.91374.v5/t15
Expected 95% CL exclusion sensitivity for simplified models of direct LH slepton production.
Figure 2a
10.17182/hepdata.91374.v5/t16
Observed 95% CL exclusion sensitivity for simplified models of direct LH slepton production.
Figure 2a
10.17182/hepdata.91374.v5/t17
Expected 95% CL exclusion sensitivity for simplified models of direct RH slepton production.
Figure 2a
10.17182/hepdata.91374.v5/t18
Observed 95% CL exclusion sensitivity for simplified models of direct RH slepton production.
Figure 16b
10.17182/hepdata.91374.v5/t19
Expected 95% CL exclusion sensitivity for simplified models of direct LH smuon production.
Figure 16b
10.17182/hepdata.91374.v5/t20
Observed 95% CL exclusion sensitivity for simplified models of direct LH smuon production.
Figure 16b
10.17182/hepdata.91374.v5/t21
Expected 95% CL exclusion sensitivity for simplified models of direct RH smuon production.
Figure 16b
10.17182/hepdata.91374.v5/t22
Observed 95% CL exclusion sensitivity for simplified models of direct RH smuon production.
Figure 16b
10.17182/hepdata.91374.v5/t23
Expected 95% CL exclusion sensitivity for simplified models of direct LH selectron production.
Figure 16b
10.17182/hepdata.91374.v5/t24
Observed 95% CL exclusion sensitivity for simplified models of direct LH selectron production.
Figure 16b
10.17182/hepdata.91374.v5/t25
Expected 95% CL exclusion sensitivity for simplified models of direct RH selectron production.
Figure 16b
10.17182/hepdata.91374.v5/t26
Observed 95% CL exclusion sensitivity for simplified models of direct RH selectron production.
Figure 28a
10.17182/hepdata.91374.v5/t27
Acceptance (note the $z$-axis is in units of $10^{-4}$) for the C1C1 higgsino process in the SR-E-high region. Truth dilepton...
Figure 28b
10.17182/hepdata.91374.v5/t28
Efficiency for the C1C1 higgsino process in the SR-E-high region. Truth dilepton invariant mass is constrained to be within the...
Figure 28c
10.17182/hepdata.91374.v5/t29
Acceptance (note the $z$-axis is in units of $10^{-4}$) for the C1C1 higgsino process in the SR-E-low region. Truth dilepton...
Figure 28d
10.17182/hepdata.91374.v5/t30
Efficiency for the C1C1 higgsino process in the SR-E-low region. Truth dilepton invariant mass is constrained to be within the...
Figure 28e
10.17182/hepdata.91374.v5/t31
Acceptance (note the $z$-axis is in units of $10^{-4}$) for the C1C1 higgsino process in the SR-E-med region. Truth dilepton...
Figure 28f
10.17182/hepdata.91374.v5/t32
Efficiency for the C1C1 higgsino process in the SR-E-med region. Truth dilepton invariant mass is constrained to be within the...
Figure 29a
10.17182/hepdata.91374.v5/t33
Acceptance (note the $z$-axis is in units of $10^{-4}$) for the N2N1 higgsino process in the SR-E-high region. Truth dilepton...
Figure 29b
10.17182/hepdata.91374.v5/t34
Efficiency for the N2N1 higgsino process in the SR-E-high region. Truth dilepton invariant mass is constrained to be within the...
Figure 29c
10.17182/hepdata.91374.v5/t35
Acceptance (note the $z$-axis is in units of $10^{-4}$) for the N2N1 higgsino process in the SR-E-low region. Truth dilepton...
Figure 29d
10.17182/hepdata.91374.v5/t36
Efficiency for the N2N1 higgsino process in the SR-E-low region. Truth dilepton invariant mass is constrained to be within the...
Figure 29e
10.17182/hepdata.91374.v5/t37
Acceptance (note the $z$-axis is in units of $10^{-4}$) for the N2N1 higgsino process in the SR-E-med region. Truth dilepton...
Figure 29f
10.17182/hepdata.91374.v5/t38
Efficiency for the N2N1 higgsino process in the SR-E-med region. Truth dilepton invariant mass is constrained to be within the...
Figure 29g
10.17182/hepdata.91374.v5/t39
Acceptance (note the $z$-axis is in units of $10^{-4}$) for the N2N1 higgsino process in the SR-E-1l1T region. Truth dilepton...
Figure 29h
10.17182/hepdata.91374.v5/t40
Efficiency for the N2N1 higgsino process in the SR-E-1l1T region. Truth dilepton invariant mass is constrained to be within the...
Figure 30a
10.17182/hepdata.91374.v5/t41
Acceptance (note the $z$-axis is in units of $10^{-4}$) for the N2C1p higgsino process in the SR-E-high region. Truth dilepton...
Figure 30b
10.17182/hepdata.91374.v5/t42
Efficiency for the N2C1p higgsino process in the SR-E-high region. Truth dilepton invariant mass is constrained to be within the...
Figure 30c
10.17182/hepdata.91374.v5/t43
Acceptance (note the $z$-axis is in units of $10^{-4}$) for the N2C1p higgsino process in the SR-E-low region. Truth dilepton...
Figure 30d
10.17182/hepdata.91374.v5/t44
Efficiency for the N2C1p higgsino process in the SR-E-low region. Truth dilepton invariant mass is constrained to be within the...
Figure 30e
10.17182/hepdata.91374.v5/t45
Acceptance (note the $z$-axis is in units of $10^{-4}$) for the N2C1p higgsino process in the SR-E-med region. Truth dilepton...
Figure 30f
10.17182/hepdata.91374.v5/t46
Efficiency for the N2C1p higgsino process in the SR-E-med region. Truth dilepton invariant mass is constrained to be within the...
Figure 30g
10.17182/hepdata.91374.v5/t47
Acceptance (note the $z$-axis is in units of $10^{-4}$) for the N2C1p higgsino process in the SR-E-1l1T region. Truth dilepton...
Figure 30h
10.17182/hepdata.91374.v5/t48
Efficiency for the N2C1p higgsino process in the SR-E-1l1T region. Truth dilepton invariant mass is constrained to be within the...
Figure 31a
10.17182/hepdata.91374.v5/t49
Acceptance (note the $z$-axis is in units of $10^{-4}$) for the N2C1m higgsino process in the SR-E-high region. Truth dilepton...
Figure 31b
10.17182/hepdata.91374.v5/t50
Efficiency for the N2C1m higgsino process in the SR-E-high region. Truth dilepton invariant mass is constrained to be within the...
Figure 31c
10.17182/hepdata.91374.v5/t51
Acceptance (note the $z$-axis is in units of $10^{-4}$) for the N2C1m higgsino process in the SR-E-low region. Truth dilepton...
Figure 31d
10.17182/hepdata.91374.v5/t52
Efficiency for the N2C1m higgsino process in the SR-E-low region. Truth dilepton invariant mass is constrained to be within the...
Figure 31e
10.17182/hepdata.91374.v5/t53
Acceptance (note the $z$-axis is in units of $10^{-4}$) for the N2C1m higgsino process in the SR-E-med region. Truth dilepton...
Figure 31f
10.17182/hepdata.91374.v5/t54
Efficiency for the N2C1m higgsino process in the SR-E-med region. Truth dilepton invariant mass is constrained to be within the...
Figure 31g
10.17182/hepdata.91374.v5/t55
Acceptance (note the $z$-axis is in units of $10^{-4}$) for the N2C1m higgsino process in the SR-E-1l1T region. Truth dilepton...
Figure 31h
10.17182/hepdata.91374.v5/t56
Efficiency for the N2C1m higgsino process in the SR-E-1l1T region. Truth dilepton invariant mass is constrained to be within the...
Figure 32a
10.17182/hepdata.91374.v5/t57
Acceptance (note the $z$-axis is in units of $10^{-3}$) for the slepton process in the SR-S region. Truth stransverse mass...
Figure 32b
10.17182/hepdata.91374.v5/t58
Efficiency for the slepton process in the SR-S region. Truth stransverse mass is constrained to be within the range [100,140]...
Figure 32c
10.17182/hepdata.91374.v5/t59
Acceptance (note the $z$-axis is in units of $10^{-3}$) for the slepton process in the SR-S-high region. Truth stransverse mass...
Figure 32d
10.17182/hepdata.91374.v5/t60
Efficiency for the slepton process in the SR-S-high region. Truth stransverse mass is constrained to be within the range [100,140]...
Figure 32e
10.17182/hepdata.91374.v5/t61
Acceptance (note the $z$-axis is in units of $10^{-3}$) for the slepton process in the SR-S-low region. Truth stransverse mass...
Figure 32f
10.17182/hepdata.91374.v5/t62
Efficiency for the slepton process in the SR-S-low region. Truth stransverse mass is constrained to be within the range [100,140]...
Figure 33a
10.17182/hepdata.91374.v5/t63
Acceptance (note the $z$-axis is in units of $10^{-4}$) for the C1C1 VBF higgsino process in the SR-VBF-high region. Truth...
Figure 33b
10.17182/hepdata.91374.v5/t64
Efficiency for the C1C1 VBF higgsino process in the SR-VBF-high region. Truth dilepton invariant mass is constrained to be within...
Figure 33c
10.17182/hepdata.91374.v5/t65
Acceptance (note the $z$-axis is in units of $10^{-4}$) for the C1C1 VBF higgsino process in the SR-VBF-low region. Truth...
Figure 33d
10.17182/hepdata.91374.v5/t66
Efficiency for the C1C1 VBF higgsino process in the SR-VBF-low region. Truth dilepton invariant mass is constrained to be within...
Figure 33e
10.17182/hepdata.91374.v5/t67
Acceptance (note the $z$-axis is in units of $10^{-4}$) for the C1C1 VBF higgsino process in the SR-VBF region. Truth...
Figure 33f
10.17182/hepdata.91374.v5/t68
Efficiency for the C1C1 VBF higgsino process in the SR-VBF region. Truth dilepton invariant mass is constrained to be within...
Figure 34a
10.17182/hepdata.91374.v5/t69
Acceptance (note the $z$-axis is in units of $10^{-4}$) for the N2N1 VBF higgsino process in the SR-VBF-high region. Truth...
Figure 34b
10.17182/hepdata.91374.v5/t70
Efficiency for the N2N1 VBF higgsino process in the SR-VBF-high region. Truth dilepton invariant mass is constrained to be within...
Figure 34c
10.17182/hepdata.91374.v5/t71
Acceptance (note the $z$-axis is in units of $10^{-4}$) for the N2N1 VBF higgsino process in the SR-VBF-low region. Truth...
Figure 34d
10.17182/hepdata.91374.v5/t72
Efficiency for the N2N1 VBF higgsino process in the SR-VBF-low region. Truth dilepton invariant mass is constrained to be within...
Figure 34e
10.17182/hepdata.91374.v5/t73
Acceptance (note the $z$-axis is in units of $10^{-4}$) for the N2N1 VBF higgsino process in the SR-VBF region. Truth...
Figure 34f
10.17182/hepdata.91374.v5/t74
Efficiency for the N2N1 VBF higgsino process in the SR-VBF region. Truth dilepton invariant mass is constrained to be within...
Figure 35a
10.17182/hepdata.91374.v5/t75
Acceptance (note the $z$-axis is in units of $10^{-4}$) for the N2C1p VBF higgsino process in the SR-VBF-high region. Truth...
Figure 35b
10.17182/hepdata.91374.v5/t76
Efficiency for the N2C1p VBF higgsino process in the SR-VBF-high region. Truth dilepton invariant mass is constrained to be within...
Figure 35c
10.17182/hepdata.91374.v5/t77
Acceptance (note the $z$-axis is in units of $10^{-4}$) for the N2C1p VBF higgsino process in the SR-VBF-low region. Truth...
Figure 35d
10.17182/hepdata.91374.v5/t78
Efficiency for the N2C1p VBF higgsino process in the SR-VBF-low region. Truth dilepton invariant mass is constrained to be within...
Figure 35e
10.17182/hepdata.91374.v5/t79
Acceptance (note the $z$-axis is in units of $10^{-4}$) for the N2C1p VBF higgsino process in the SR-VBF region. Truth...
Figure 35f
10.17182/hepdata.91374.v5/t80
Efficiency for the N2C1p VBF higgsino process in the SR-VBF region. Truth dilepton invariant mass is constrained to be within...
Figure 36a
10.17182/hepdata.91374.v5/t81
Acceptance (note the $z$-axis is in units of $10^{-4}$) for the N2C1m VBF higgsino process in the SR-VBF-high region. Truth...
Figure 36b
10.17182/hepdata.91374.v5/t82
Efficiency for the N2C1m VBF higgsino process in the SR-VBF-high region. Truth dilepton invariant mass is constrained to be within...
Figure 36c
10.17182/hepdata.91374.v5/t83
Acceptance (note the $z$-axis is in units of $10^{-4}$) for the N2C1m VBF higgsino process in the SR-VBF-low region. Truth...
Figure 36d
10.17182/hepdata.91374.v5/t84
Efficiency for the N2C1m VBF higgsino process in the SR-VBF-low region. Truth dilepton invariant mass is constrained to be within...
Figure 36e
10.17182/hepdata.91374.v5/t85
Acceptance (note the $z$-axis is in units of $10^{-4}$) for the N2C1m VBF higgsino process in the SR-VBF region. Truth...
Figure 36f
10.17182/hepdata.91374.v5/t86
Efficiency for the N2C1m VBF higgsino process in the SR-VBF region. Truth dilepton invariant mass is constrained to be within...
Figure 41ab
10.17182/hepdata.91374.v5/t87
Observed and Expected upper cross-section limits for wino-bino scenarios, assuming $m(\tilde{\chi}_{2}^{0}) \times m(\tilde{\chi}_{1}^{0})>0$.
Figure 41cd
10.17182/hepdata.91374.v5/t88
Observed and Expected upper cross-section limits for wino-bino scenarios, assuming $m(\tilde{\chi}_{2}^{0}) \times m(\tilde{\chi}_{1}^{0})<0$.
Figure 42ab
10.17182/hepdata.91374.v5/t89
Observed and Expected upper cross-section limits for higgsino scenarios.
Figure 43ab
10.17182/hepdata.91374.v5/t90
Observed and Expected upper cross-section limits for higgsino scenarios, assuming VBF production..
Figure 44ab
10.17182/hepdata.91374.v5/t91
Observed and Expected upper cross-section limits for direct slepton scenarios.
Figure 44cd
10.17182/hepdata.91374.v5/t92
Observed and Expected upper cross-section limits for direct LH slepton scenarios.
Figure 44ef
10.17182/hepdata.91374.v5/t93
Observed and Expected upper cross-section limits for direct RH slepton scenarios.
Figure 45ab
10.17182/hepdata.91374.v5/t94
Observed and Expected upper cross-section limits for direct smuon scenarios.
Figure 45cd
10.17182/hepdata.91374.v5/t95
Observed and Expected upper cross-section limits for direct LH smuon scenarios.
Figure 45ef
10.17182/hepdata.91374.v5/t96
Observed and Expected upper cross-section limits for direct RH smuon scenarios.
Figure 46ab
10.17182/hepdata.91374.v5/t97
Observed and Expected upper cross-section limits for direct selectron scenarios.
Figure 46cd
10.17182/hepdata.91374.v5/t98
Observed and Expected upper cross-section limits for direct LH selectron scenarios.
Figure 46ef
10.17182/hepdata.91374.v5/t99
Observed and Expected upper cross-section limits for direct RH selectron scenarios.
Table 18
10.17182/hepdata.91374.v5/t100
Number of signal events in SR-E-1L1T for the (m($\tilde{\chi}_{2}^{0}$),m($\tilde{\chi}_{1}^{0}$)) = (155 GeV, 150 GeV) Higgsino signal model at different stages...
Table 19
10.17182/hepdata.91374.v5/t101
Number of signal events in SR-E-high for the (m($\tilde{\chi}_{2}^{0}$),m($\tilde{\chi}_{1}^{0}$)) = (155 GeV, 150 GeV) Higgsino signal model at different stages...
Table 20
10.17182/hepdata.91374.v5/t102
Number of signal events in SR-E-low for the (m($\tilde{\chi}_{2}^{0}$),m($\tilde{\chi}_{1}^{0}$)) = (155 GeV, 150 GeV) Higgsino signal model at different stages...
Table 21
10.17182/hepdata.91374.v5/t103
Number of signal events in SR-E-med for the (m($\tilde{\chi}_{2}^{0}$),m($\tilde{\chi}_{1}^{0}$)) = (155 GeV, 150 GeV) Higgsino signal model at different stages...
Table 22
10.17182/hepdata.91374.v5/t104
Number of signal events in SR-S-high for the (m($\tilde{\ell}$),m($\tilde{\chi}_{1}^{0}$)) = (150 GeV, 140 GeV) Slepton signal model at different stages...
Table 23
10.17182/hepdata.91374.v5/t105
Number of signal events in SR-S-low for the (m($\tilde{\ell}$),m($\tilde{\chi}_{1}^{0}$)) = (150 GeV, 140 GeV) Slepton signal model at different stages...
Table 24
10.17182/hepdata.91374.v5/t106
Number of signal events in SR-VBF for the (m($\tilde{\chi}_{2}^{0}$),m($\tilde{\chi}_{1}^{0}$)) = (100 GeV, 95 GeV) Higgsino signal model at different stages...
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