. 2021 May 27;81(5):466. doi: 10.1140/epjc/s10052-021-09218-1

Table 6.

The set of kinematical cuts used to isolate signal events from background

$@ 14 T e V$	$@ 27 T e V$	$@ 100 T e V$
$2 ℓ + ⧸ E_{T}$
$\| η \| < 2.5$	$\| η \| < 2.5$	$\| η \| < 2.5$
$Δ R_{ℓ ℓ} \geq 0.5$	$Δ R_{ℓ ℓ} \geq 0.5$	$Δ R_{ℓ ℓ} \geq 0.5$
$p_{T} (ℓ_{1}) > 475$ GeV	$p_{T} (ℓ_{1}) > 500$ GeV	$p_{T} (ℓ_{1}) > 2000$ GeV
$p_{T} (ℓ_{2}) > 50$ GeV	$p_{T} (ℓ_{2}) > 300$ GeV	$p_{T} (ℓ_{2}) > 1000$ GeV
$⧸ E_{T} > 50$ GeV	$⧸ E_{T} > 400$ GeV	$⧸ E_{T} > 2300$ GeV
$4 ℓ + ⧸ E_{T}$
$\| η \| < 2.5$	$\| η \| < 2.5$	$\| η \| < 2.5$
$Δ R_{ℓ ℓ} \geq 0.5$	$Δ R_{ℓ ℓ} \geq 0.5$	$Δ R_{ℓ ℓ} \geq 0.5$
$p_{T} (ℓ_{1}) > 100$ GeV	$p_{T} (ℓ_{1}) > 100$ GeV	$p_{T} (ℓ_{1}) > 100$ GeV
$p_{T} (ℓ_{2}) > 50$ GeV	$p_{T} (ℓ_{2}) > 50$ GeV	$p_{T} (ℓ_{2}) > 50$ GeV
$p_{T} (ℓ_{3}) > 25$ GeV	$p_{T} (ℓ_{3}) > 25$ GeV	$p_{T} (ℓ_{3}) > 25$ GeV
$p_{T} (ℓ_{4}) > 15$ GeV	$p_{T} (ℓ_{4}) > 15$ GeV	$p_{T} (ℓ_{4}) > 15$ GeV
$⧸ E_{T} >$ 400 GeV	$⧸ E_{T} > 350$ GeV	$⧸ E_{T} > 800$ GeV
$6 ℓ + ⧸ E_{T}$
$\| η \| < 2.5$	$\| η \| < 2.5$	$\| η \| < 2.5$
$Δ R_{ℓ ℓ} \geq 0.2$	$Δ R_{ℓ ℓ} \geq 0.2$	$Δ R_{ℓ ℓ} \geq 0.2$
$p_{T} (ℓ_{1}) > 50$ GeV	$p_{T} (ℓ_{1}) > 50$ GeV	$p_{T} (ℓ_{1}) > 100$ GeV
$p_{T} (ℓ_{2}) > 20$ GeV	$p_{T} (ℓ_{2}) > 20$ GeV	$p_{T} (ℓ_{2}) > 50$ GeV
$p_{T} (ℓ_{3}) > 20$ GeV	$p_{T} (ℓ_{3}) > 20$ GeV	$p_{T} (ℓ_{3}) > 20$ GeV
$p_{T} (ℓ_{4}) > 20$ GeV	$p_{T} (ℓ_{4}) > 20$ GeV	$p_{T} (ℓ_{4}) > 20$ GeV
$p_{T} (ℓ_{5}) > 10$ GeV	$p_{T} (ℓ_{5}) > 10$ GeV	$p_{T} (ℓ_{5}) > 15$ GeV
$p_{T} (ℓ_{6}) > 5$ GeV	$p_{T} (ℓ_{6}) > 5$ GeV	$p_{T} (ℓ_{6}) > 5$ GeV
$⧸ E_{T} > 100$ GeV	$⧸ E_{T} > 100$ GeV	$⧸ E_{T} > 100$ GeV