Table 8.

Signal selection strategy and cuts imposed in the $4\ell +⧸E_T$ scenario at 14, 27 and 100 TeV. We give the cross-section for background and benchmark scenarios in fb. Statistical significances ${\sigma }_{\mathcal{A}}$ and ${\sigma }_{\mathcal{B}}$ of $4\ell +⧸E_T$ signal are given for each energy

$4\ell +⧸E_T@14\mathrm{T}eV$	Background [fb]	$\mathrm{B}P1[fb]$	$\mathrm{B}P3[fb]$
$\mathrm{N}oCut$	$3.45\times {10}^{-2}$	$1.99\times {10}^{-3}$	$1.86\times {10}^{-3}$
$|{\eta }_i|<2.5,\Delta R_{12}\ge 0.5$	$2.89\times {10}^{-2}$	$5.31\times {10}^{-4}$	$4.63\times {10}^{-4}$
$p_T({\ell }_1)>100$ GeV	$1.7\times {10}^{-2}$	$5.1\times {10}^{-4}$	$4.61\times {10}^{-4}$
$p_T({\ell }_2)>50$ GeV	$1.58\times {10}^{-2}$	$5.02\times {10}^{-4}$	$4.61\times {10}^{-4}$
$p_T({\ell }_3)>25$ GeV	$1.52\times {10}^{-2}$	$4.87\times {10}^{-4}$	$4.59\times {10}^{-4}$
$p_T({\ell }_4)>15$ GeV	$1.4\times {10}^{-2}$	$4.44\times {10}^{-4}$	$4.31\times {10}^{-4}$
$⧸E_T>400\mathrm{G}eV$	$1.0\times {10}^{-4}$	$5.5\times {10}^{-5}$	$1.3\times {10}^{-4}$
$\mathrm{S}ignificance:{\sigma }_{\mathcal{A}}$	$\mathcal{L}=3{\mathrm{ab}}^{-1}$	$0.24\sigma$	$0.46\sigma$
${\sigma }_{\mathcal{B}}$		$0.19\sigma$	$0.38\sigma$
$4\ell +⧸E_T@27\mathrm{T}eV$
$\mathrm{N}oCut$	$9.59\times {10}^{-2}$	$3.03\times {10}^{-2}$	$3.86\times {10}^{-2}$
$|{\eta }_i|<2.5,\Delta R_{12}\ge 0.5$	$7.52\times {10}^{-2}$	$5.9\times {10}^{-3}$	$4.14\times {10}^{-3}$
$p_T({\ell }_1)>100$ GeV	$4.7\times {10}^{-2}$	$5.74\times {10}^{-3}$	$4.13\times {10}^{-3}$
$p_T({\ell }_2)>50$ GeV	$4.39\times {10}^{-2}$	$5.68\times {10}^{-3}$	$4.13\times {10}^{-3}$
$p_T({\ell }_3)>25$ GeV	$4.2\times {10}^{-2}$	$5.52\times {10}^{-3}$	$4.12\times {10}^{-3}$
$p_T({\ell }_4)>15$ GeV	$3.86\times {10}^{-2}$	$5.08\times {10}^{-3}$	$3.9\times {10}^{-3}$
$⧸E_T>350\mathrm{G}eV$	$1.1\times {10}^{-3}$	$1.2\times {10}^{-3}$	$2.2\times {10}^{-3}$
$\mathrm{S}ignificance:{\sigma }_{\mathcal{A}}$	$\mathcal{L}=15{\mathrm{ab}}^{-1}$	$3.1\sigma$	$4.6\sigma$
${\sigma }_{\mathcal{B}}$		$2.6\sigma$	$4.1\sigma$
$4\ell +⧸E_T@100\mathrm{T}eV$
$\mathrm{N}oCut$	2.48	$9.38\times {10}^{-1}$	1.64
$|{\eta }_i|<2.5,\Delta R_{12}\ge 0.5$	$6.56\times {10}^{-1}$	$1.33\times {10}^{-1}$	$1.16\times {10}^{-1}$
$p_T({\ell }_1)>100$ GeV	$4.46\times {10}^{-1}$	$1.3\times {10}^{-1}$	$1.15\times {10}^{-1}$
$p_T({\ell }_2)>50$ GeV	$4.1\times {10}^{-1}$	$1.29\times {10}^{-1}$	$1.14\times {10}^{-1}$
$p_T({\ell }_3)>25$ GeV	$3.83\times {10}^{-1}$	$1.22\times {10}^{-1}$	$1.01\times {10}^{-1}$
$p_T({\ell }_4)>15$ GeV	$3.1\times {10}^{-1}$	$9.9\times {10}^{-2}$	$8.44\times {10}^{-2}$
$⧸E_T>800\mathrm{G}eV$	$7.1\times {10}^{-3}$	$8.0\times {10}^{-3}$	$2.3\times {10}^{-2}$
$\mathrm{S}ignificance:{\sigma }_{\mathcal{A}}$	$\mathcal{L}=30{\mathrm{ab}}^{-1}$	$11.0\sigma$	$23.0\sigma$
${\sigma }_{\mathcal{B}}$		$9.4\sigma$	$22.0\sigma$