. 2016 Dec 2;76(12):664. doi: 10.1140/epjc/s10052-016-4489-7

Table 9.

Expected and observed 95% CL cross-section times branching ratio upper limits as a function of $m_{h^{0}}$ , for LLP masses of 40, 48, 55, and 60 $Ge V / c^{2}$ , $τ_{LLP} = 10 ps$ , estimated by the fast simulation

Model	Expected upper limit (pb)	Observed upper limit (pb)
BV40 10ps mH90	3.57 $_{- 1.18}^{+ 2.23}$	3.04
BV40 10ps mH95	3.52 $_{- 1.17}^{+ 2.18}$	2.96
BV40 10ps mH100	3.55 $_{- 1.16}^{+ 2.12}$	2.86
BV40 10ps mH105	3.49 $_{- 1.18}^{+ 2.19}$	2.77
BV40 10ps mH110	3.59 $_{- 1.21}^{+ 2.32}$	2.93
BV40 10ps mH114	3.76 $_{- 1.30}^{+ 2.38}$	2.99
BV40 10ps mH120	4.07 $_{- 1.42}^{+ 2.63}$	3.20
BV40 10ps mH125	4.04 $_{- 1.43}^{+ 2.66}$	3.07
BV40 10ps mH130	4.55 $_{- 1.61}^{+ 2.98}$	3.63
BV40 10ps mH140	4.71 $_{- 1.69}^{+ 3.14}$	3.79
BV48 10ps mH100	2.78 $_{- 0.95}^{+ 1.75}$	2.23
BV48 10ps mH105	2.17 $_{- 0.74}^{+ 1.36}$	1.73
BV48 10ps mH110	1.99 $_{- 0.69}^{+ 1.24}$	1.56
BV48 10ps mH114	2.02 $_{- 0.70}^{+ 1.29}$	1.65
BV48 10ps mH120	2.07 $_{- 0.71}^{+ 1.34}$	1.68
BV48 10ps mH125	2.12 $_{- 0.74}^{+ 1.38}$	1.74
BV48 10ps mH130	2.22 $_{- 0.78}^{+ 1.45}$	1.80
BV48 10ps mH140	2.49 $_{- 0.89}^{+ 1.65}$	1.98
BV55 10ps mH130	1.94 $_{- 0.69}^{+ 1.27}$	1.76
BV55 10ps mH140	1.93 $_{- 0.69}^{+ 1.26}$	1.75
BV60 10ps mH130	1.79 $_{- 0.63}^{+ 1.16}$	1.52
BV60 10ps mH140	1.86 $_{- 0.66}^{+ 1.21}$	1.48