$|y^{t}|$ absolute differential cross-section at particle level.

$p_{T}^{t,1}$ absolute differential cross-section at particle level.

$|{y}^{t,1}|$ absolute differential cross-section at particle level.

$p_{T}^{t,2}$ absolute differential cross-section at particle level.

$|{y}^{t,2}|$ absolute differential cross-section at particle level.

$m^{t\bar{t}}$ absolute differential cross-section at particle level.

$p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level.

$|y^{t\bar{t}}|$ absolute differential cross-section at particle level.

$\chi^{t\bar{t}}$ absolute differential cross-section at particle level.

$|y_{B}^{t\bar{t}}|$ absolute differential cross-section at particle level.

$|p_{out}^{t\bar{t}}|$ absolute differential cross-section at particle level.

$|\Delta \phi(t_{1}, t_{2})|$ absolute differential cross-section at particle level.

$H_{T}^{t\bar{t}}$ absolute differential cross-section at particle level.

$|\cos\theta^{*}|$ absolute differential cross-section at particle level.

$p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level, for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV.

$p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level, for 0.55 TeV < $p_{T}^{t,1}$ < 0.6 TeV.

$p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level, for 0.6 TeV < $p_{T}^{t,1}$ < 0.75 TeV.

$p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level, for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.

$|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at particle level, for 0 < $|{y}^{t,1}|$ < 0.2.

$|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at particle level, for 0.2 < $|{y}^{t,1}|$ < 0.5.

$|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at particle level, for 0.5 < $|{y}^{t,1}|$ < 1.

$|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at particle level, for 1 < $|{y}^{t,1}|$ < 2.

$|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level, for 0 < $|{y}^{t,1}|$ < 0.2.

$|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level, for 0.2 < $|{y}^{t,1}|$ < 0.5.

$|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level, for 0.5 < $|{y}^{t,1}|$ < 1.

$|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level, for 1 < $|{y}^{t,1}|$ < 2.

$|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level, for 0 < $|{y}^{t,2}|$ < 0.2.

$|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level, for 0.2 < $|{y}^{t,2}|$ < 0.5.

$|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level, for 0.5 < $|{y}^{t,2}|$ < 1.

$|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level, for 1 < $|{y}^{t,2}|$ < 2.

$p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level, for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV.

$p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level, for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV.

$p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level, for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV.

$p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level, for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.

$p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level, for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV.

$p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level, for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV.

$p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level, for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV.

$p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level, for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.

$|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level, for 0 < $|{y}^{t\bar{t}}|$ < 0.2.

$|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level, for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.

$|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level, for 0.5 < $|{y}^{t\bar{t}}|$ < 1.

$|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level, for 1 < $|{y}^{t\bar{t}}|$ < 2.

$|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at particle level, for 0 < $|{y}^{t\bar{t}}|$ < 0.2.

$|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at particle level, for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.

$|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at particle level, for 0.5 < $|{y}^{t\bar{t}}|$ < 1.

$|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at particle level, for 1 < $|{y}^{t\bar{t}}|$ < 2.

$|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level, for 0 < $|{y}^{t,1}|$ < 0.2.

$|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level, for 0.2 < $|{y}^{t,1}|$ < 0.5.

$|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level, for 0.5 < $|{y}^{t,1}|$ < 1.

$|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level, for 1 < $|{y}^{t,1}|$ < 2.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level, for 0 < $|{y}^{t\bar{t}}|$ < 0.2.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level, for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level, for 0.5 < $|{y}^{t\bar{t}}|$ < 1.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level, for 1 < $|{y}^{t\bar{t}}|$ < 2.

$p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level, for 0 TeV < $p_{T}^{t\bar{t}}$ < 0.1 TeV.

$p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level, for 0.1 TeV < $p_{T}^{t\bar{t}}$ < 0.2 TeV.

$p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level, for 0.2 TeV < $p_{T}^{t\bar{t}}$ < 0.35 TeV.

$p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level, for 0.35 TeV < $p_{T}^{t\bar{t}}$ < 1 TeV.

$|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level, for 0 < $|{y}^{t\bar{t}}|$ < 0.2.

$|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level, for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.

$|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level, for 0.5 < $|{y}^{t\bar{t}}|$ < 1.

$|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level, for 1 < $|{y}^{t\bar{t}}|$ < 2.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level, for 0 < $|{y}^{t\bar{t}}|$ < 0.3 and 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level, for 0 < $|{y}^{t\bar{t}}|$ < 0.3 and 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level, for 0 < $|{y}^{t\bar{t}}|$ < 0.3 and 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level, for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9 and 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level, for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9 and 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level, for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9 and 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level, for 0.9 < $|{y}^{t\bar{t}}|$ < 2 and 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level, for 0.9 < $|{y}^{t\bar{t}}|$ < 2 and 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level, for 0.9 < $|{y}^{t\bar{t}}|$ < 2 and 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.

$p_{T}^{t}$ normalized differential cross-section at particle level.

$|y^{t}|$ normalized differential cross-section at particle level.

$p_{T}^{t,1}$ normalized differential cross-section at particle level.

$|{y}^{t,1}|$ normalized differential cross-section at particle level.

$p_{T}^{t,2}$ normalized differential cross-section at particle level.

$|{y}^{t,2}|$ normalized differential cross-section at particle level.

$m^{t\bar{t}}$ normalized differential cross-section at particle level.

$p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level.

$|y^{t\bar{t}}|$ normalized differential cross-section at particle level.

$\chi^{t\bar{t}}$ normalized differential cross-section at particle level.

$|y_{B}^{t\bar{t}}|$ normalized differential cross-section at particle level.

$|p_{out}^{t\bar{t}}|$ normalized differential cross-section at particle level.

$|\Delta \phi(t_{1}, t_{2})|$ normalized differential cross-section at particle level.

$H_{T}^{t\bar{t}}$ normalized differential cross-section at particle level.

$|\cos\theta^{*}|$ normalized differential cross-section at particle level.

$p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level, for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV.

$p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level, for 0.55 TeV < $p_{T}^{t,1}$ < 0.6 TeV.

$p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level, for 0.6 TeV < $p_{T}^{t,1}$ < 0.75 TeV.

$p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level, for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.

$|{y}^{t,1}|\otimes |{y}^{t,2}|$ normalized differential cross-section at particle level, for 0 < $|{y}^{t,1}|$ < 0.2.

$|{y}^{t,1}|\otimes |{y}^{t,2}|$ normalized differential cross-section at particle level, for 0.2 < $|{y}^{t,1}|$ < 0.5.

$|{y}^{t,1}|\otimes |{y}^{t,2}|$ normalized differential cross-section at particle level, for 0.5 < $|{y}^{t,1}|$ < 1.

$|{y}^{t,1}|\otimes |{y}^{t,2}|$ normalized differential cross-section at particle level, for 1 < $|{y}^{t,1}|$ < 2.

$|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level, for 0 < $|{y}^{t,1}|$ < 0.2.

$|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level, for 0.2 < $|{y}^{t,1}|$ < 0.5.

$|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level, for 0.5 < $|{y}^{t,1}|$ < 1.

$|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level, for 1 < $|{y}^{t,1}|$ < 2.

$|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level, for 0 < $|{y}^{t,2}|$ < 0.2.

$|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level, for 0.2 < $|{y}^{t,2}|$ < 0.5.

$|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level, for 0.5 < $|{y}^{t,2}|$ < 1.

$|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level, for 1 < $|{y}^{t,2}|$ < 2.

$p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level, for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV.

$p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level, for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV.

$p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level, for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV.

$p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level, for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.

$p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level, for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV.

$p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level, for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV.

$p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level, for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV.

$p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level, for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.

$|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level, for 0 < $|{y}^{t\bar{t}}|$ < 0.2.

$|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level, for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.

$|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level, for 0.5 < $|{y}^{t\bar{t}}|$ < 1.

$|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level, for 1 < $|{y}^{t\bar{t}}|$ < 2.

$|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ normalized differential cross-section at particle level, for 0 < $|{y}^{t\bar{t}}|$ < 0.2.

$|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ normalized differential cross-section at particle level, for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.

$|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ normalized differential cross-section at particle level, for 0.5 < $|{y}^{t\bar{t}}|$ < 1.

$|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ normalized differential cross-section at particle level, for 1 < $|{y}^{t\bar{t}}|$ < 2.

$|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level, for 0 < $|{y}^{t,1}|$ < 0.2.

$|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level, for 0.2 < $|{y}^{t,1}|$ < 0.5.

$|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level, for 0.5 < $|{y}^{t,1}|$ < 1.

$|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level, for 1 < $|{y}^{t,1}|$ < 2.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level, for 0 < $|{y}^{t\bar{t}}|$ < 0.2.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level, for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level, for 0.5 < $|{y}^{t\bar{t}}|$ < 1.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level, for 1 < $|{y}^{t\bar{t}}|$ < 2.

$p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level, for 0 TeV < $p_{T}^{t\bar{t}}$ < 0.1 TeV.

$p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level, for 0.1 TeV < $p_{T}^{t\bar{t}}$ < 0.2 TeV.

$p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level, for 0.2 TeV < $p_{T}^{t\bar{t}}$ < 0.35 TeV.

$p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level, for 0.35 TeV < $p_{T}^{t\bar{t}}$ < 1 TeV.

$|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level, for 0 < $|{y}^{t\bar{t}}|$ < 0.2.

$|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level, for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.

$|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level, for 0.5 < $|{y}^{t\bar{t}}|$ < 1.

$|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level, for 1 < $|{y}^{t\bar{t}}|$ < 2.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level, for 0 < $|{y}^{t\bar{t}}|$ < 0.3 and 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level, for 0 < $|{y}^{t\bar{t}}|$ < 0.3 and 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level, for 0 < $|{y}^{t\bar{t}}|$ < 0.3 and 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level, for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9 and 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level, for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9 and 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level, for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9 and 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level, for 0.9 < $|{y}^{t\bar{t}}|$ < 2 and 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level, for 0.9 < $|{y}^{t\bar{t}}|$ < 2 and 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level, for 0.9 < $|{y}^{t\bar{t}}|$ < 2 and 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.

Fiducial phase-space cross-section at parton level.

$p_{T}^{t}$ absolute differential cross-section at parton level.

$|y^{t}|$ absolute differential cross-section at parton level.

$p_{T}^{t,1}$ absolute differential cross-section at parton level.

$|y^{t,1}|$ absolute differential cross-section at parton level.

$p_{T}^{t,2}$ absolute differential cross-section at parton level.

$|{y}^{t,2}|$ absolute differential cross-section at parton level.

$m^{t\bar{t}}$ absolute differential cross-section at parton level.

$p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level.

$|{y}^{t\bar{t}}|$ absolute differential cross-section at parton level.

${\chi}^{t\bar{t}}$ absolute differential cross-section at parton level.

$|y_{B}^{t\bar{t}}|$ absolute differential cross-section at parton level.

$|p_{out}^{t\bar{t}}|$ absolute differential cross-section at parton level.

$|\Delta \phi(t_{1}, t_{2})|$ absolute differential cross-section at parton level.

$H_{T}^{t\bar{t}}$ absolute differential cross-section at parton level.

$|\cos\theta^{*}|$ absolute differential cross-section at parton level.

$p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level, for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV.

$p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level, for 0.55 TeV < $p_{T}^{t,1}$ < 0.6 TeV.

$p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level, for 0.6 TeV < $p_{T}^{t,1}$ < 0.75 TeV.

$p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level, for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.

$|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at parton level, for 0 < $|{y}^{t,1}|$ < 0.2.

$|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at parton level, for 0.2 < $|{y}^{t,1}|$ < 0.5.

$|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at parton level, for 0.5 < $|{y}^{t,1}|$ < 1.

$|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at parton level, for 1 < $|{y}^{t,1}|$ < 2.

$|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level, for 0 < $|{y}^{t,1}|$ < 0.2.

$|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level, for 0.2 < $|{y}^{t,1}|$ < 0.5.

$|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level, for 0.5 < $|{y}^{t,1}|$ < 1.

$|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level, for 1 < $|{y}^{t,1}|$ < 2.

$|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level, for 0 < $|{y}^{t,2}|$ < 0.2.

$|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level, for 0.2 < $|{y}^{t,2}|$ < 0.5.

$|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level, for 0.5 < $|{y}^{t,2}|$ < 1.

$|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level, for 1 < $|{y}^{t,2}|$ < 2.

$p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level, for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV.

$p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level, for 0.5 TeV < $p_{T}^{t,1}$ < 0.625 TeV.

$p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level, for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV.

$p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level, for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.

$p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level, for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV.

$p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level, for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV.

$p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level, for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV.

$p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level, for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.

$|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level, for 0 < $|{y}^{t\bar{t}}|$ < 0.2.

$|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level, for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.

$|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level, for 0.5 < $|{y}^{t\bar{t}}|$ < 1.

$|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level, for 1 < $|{y}^{t\bar{t}}|$ < 2.

$|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at parton level, for 0 < $|{y}^{t\bar{t}}|$ < 0.2.

$|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at parton level, for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.

$|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at parton level, for 0.5 < $|{y}^{t\bar{t}}|$ < 1.

$|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at parton level, for 1 < $|{y}^{t\bar{t}}|$ < 2.

$|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level, for 0 < $|{y}^{t,1}|$ < 0.2.

$|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level, for 0.2 < $|{y}^{t,1}|$ < 0.5.

$|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level, for 0.5 < $|{y}^{t,1}|$ < 1.

$|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level, for 1 < $|{y}^{t,1}|$ < 2.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level, for 0 < $|{y}^{t\bar{t}}|$ < 0.2.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level, for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level, for 0.5 < $|{y}^{t\bar{t}}|$ < 1.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level, for 1 < $|{y}^{t\bar{t}}|$ < 2.

$p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level, for 0 TeV < $p_{T}^{t\bar{t}}$ < 0.1 TeV.

$p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level, for 0.1 TeV < $p_{T}^{t\bar{t}}$ < 0.2 TeV.

$p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level, for 0.2 TeV < $p_{T}^{t\bar{t}}$ < 0.35 TeV.

$p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level, for 0.35 TeV < $p_{T}^{t\bar{t}}$ < 1 TeV.

$|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level, for 0 < $|{y}^{t\bar{t}}|$ < 0.2.

$|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level, for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.

$|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level, for 0.5 < $|{y}^{t\bar{t}}|$ < 1.

$|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level, for 1 < $|{y}^{t\bar{t}}|$ < 2.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level, for 0 < $|{y}^{t\bar{t}}|$ < 0.3 and 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level, for 0 < $|{y}^{t\bar{t}}|$ < 0.3 and 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level, for 0 < $|{y}^{t\bar{t}}|$ < 0.3 and 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level, for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9 and 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level, for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9 and 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level, for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9 and 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level, for 0.9 < $|{y}^{t\bar{t}}|$ < 2 and 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level, for 0.9 < $|{y}^{t\bar{t}}|$ < 2 and 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level, for 0.9 < $|{y}^{t\bar{t}}|$ < 2 and 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.

$p_{T}^{t}$ normalized differential cross-section at parton level.

$|y^{t}|$ normalized differential cross-section at parton level.

$p_{T}^{t,1}$ normalized differential cross-section at parton level.

$|y^{t,1}|$ normalized differential cross-section at parton level.

$p_{T}^{t,2}$ normalized differential cross-section at parton level.

$|{y}^{t,2}|$ normalized differential cross-section at parton level.

$m^{t\bar{t}}$ normalized differential cross-section at parton level.

$p_{T}^{t\bar{t}}$ normalized differential cross-section at parton level.

$|{y}^{t\bar{t}}|$ normalized differential cross-section at parton level.

${\chi}^{t\bar{t}}$ normalized differential cross-section at parton level.

$|y_{B}^{t\bar{t}}|$ normalized differential cross-section at parton level.

$|p_{out}^{t\bar{t}}|$ normalized differential cross-section at parton level.

$|\Delta \phi(t_{1}, t_{2})|$ normalized differential cross-section at parton level.

$H_{T}^{t\bar{t}}$ normalized differential cross-section at parton level.

$|\cos\theta^{*}|$ normalized differential cross-section at parton level.

$p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level, for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV.

$p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level, for 0.55 TeV < $p_{T}^{t,1}$ < 0.6 TeV.

$p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level, for 0.6 TeV < $p_{T}^{t,1}$ < 0.75 TeV.

$p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level, for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.

$|{y}^{t,1}|\otimes |{y}^{t,2}|$ normalized differential cross-section at parton level, for 0 < $|{y}^{t,1}|$ < 0.2.

$|{y}^{t,1}|\otimes |{y}^{t,2}|$ normalized differential cross-section at parton level, for 0.2 < $|{y}^{t,1}|$ < 0.5.

$|{y}^{t,1}|\otimes |{y}^{t,2}|$ normalized differential cross-section at parton level, for 0.5 < $|{y}^{t,1}|$ < 1.

$|{y}^{t,1}|\otimes |{y}^{t,2}|$ normalized differential cross-section at parton level, for 1 < $|{y}^{t,1}|$ < 2.

$|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level, for 0 < $|{y}^{t,1}|$ < 0.2.

$|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level, for 0.2 < $|{y}^{t,1}|$ < 0.5.

$|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level, for 0.5 < $|{y}^{t,1}|$ < 1.

$|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level, for 1 < $|{y}^{t,1}|$ < 2.

$|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level, for 0 < $|{y}^{t,2}|$ < 0.2.

$|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level, for 0.2 < $|{y}^{t,2}|$ < 0.5.

$|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level, for 0.5 < $|{y}^{t,2}|$ < 1.

$|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level, for 1 < $|{y}^{t,2}|$ < 2.

$p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at parton level, for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV.

$p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at parton level, for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV.

$p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at parton level, for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV.

$p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at parton level, for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.

$p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level, for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV.

$p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level, for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV.

$p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level, for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV.

$p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level, for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.

$|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level, for 0 < $|{y}^{t\bar{t}}|$ < 0.2.

$|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level, for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.

$|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level, for 0.5 < $|{y}^{t\bar{t}}|$ < 1.

$|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level, for 1 < $|{y}^{t\bar{t}}|$ < 2.

$|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ normalized differential cross-section at parton level, for 0 < $|{y}^{t\bar{t}}|$ < 0.2.

$|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ normalized differential cross-section at parton level, for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.

$|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ normalized differential cross-section at parton level, for 0.5 < $|{y}^{t\bar{t}}|$ < 1.

$|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ normalized differential cross-section at parton level, for 1 < $|{y}^{t\bar{t}}|$ < 2.

$|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level, for 0 < $|{y}^{t,1}|$ < 0.2.

$|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level, for 0.2 < $|{y}^{t,1}|$ < 0.5.

$|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level, for 0.5 < $|{y}^{t,1}|$ < 1.

$|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level, for 1 < $|{y}^{t,1}|$ < 2.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level, for 0 < $|{y}^{t\bar{t}}|$ < 0.2.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level, for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level, for 0.5 < $|{y}^{t\bar{t}}|$ < 1.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level, for 1 < $|{y}^{t\bar{t}}|$ < 2.

$p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level, for 0 TeV < $p_{T}^{t\bar{t}}$ < 0.1 TeV.

$p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level, for 0.1 TeV < $p_{T}^{t\bar{t}}$ < 0.2 TeV.

$p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level, for 0.2 TeV < $p_{T}^{t\bar{t}}$ < 0.35 TeV.

$p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level, for 0.35 TeV < $p_{T}^{t\bar{t}}$ < 1 TeV.

$|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at parton level, for 0 < $|{y}^{t\bar{t}}|$ < 0.2.

$|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at parton level, for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.

$|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at parton level, for 0.5 < $|{y}^{t\bar{t}}|$ < 1.

Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.

Correlation matrix for the individual sources of systematic uncertainty considered in the analysis, for the combined opposite sign (OS) and same sign (SS) binned-template profile likelihood fit to data. The OS or SS refers to the charge signs of the primary lepton and the soft muon. The gamma parameters are NPs used to describe the effect of the limited statistics of the samples.

Detailed list of the contribution of each source of uncertainty to the total uncertainty on the measured values of $\sigma(tq)$, $\sigma(\bar{t}q)$, $R_t$, and $\sigma(tq+\bar{t}q)$. The evaluation of the systematic uncertainties has a statistical uncertainty of $0.3\,\%$. Uncertainties contributing less than $1.0\,\%$ are marked with "$<1$" in the paper. To provide numerical values for this table in HEPdata, these uncertainties are approximated with $\pm 0.5\,\%$. This approximation is applied to all measurements for the following uncertainties$:$ JES statistical, JES physics modeling, JES mixed detector and modeling, JES close-by-jets, JES pileup, $b$-JES, jet vertex fraction, mistag efficiency and $W+\;$jets shape variation. For the measurement of $\sigma(tq)$ the approximation is applied in addition to the following uncertainties$:$ JES flavor response, $c$-tagging efficiency, $t\bar{t}$ generator + parton shower and $t\bar{t}$ ISR/FSR. For the measurement of $\sigma(\bar{t}q)$ the approximation is applied in addition to these uncertainties$:$ JES flavor response, $b/\bar{b}$ acceptance, and $t\bar{t}$ ISR/FSR. For the measurement of $R_t$ the approximation is applied in addition to these uncertainties$:$ JES detector, $b$-tagging efficiency, $c$-tagging efficiency, $b/\bar{b}$ acceptance and $tq$ scale variations. For the measurement of $\sigma(tq+\bar{t}q)$ the approximation is applied in addition to these uncertainties$:$ JES flavor response, $c$-tagging efficiency, $b/\bar{b}$ acceptance, $t\bar{t}$ generator + parton shower and $t\bar{t}$ ISR/FSR.

Differential t-channel top-quark production cross sections and normalized differential t-channel top-quark production cross sections as functions of ABS(YRAP(T)).

The cross sections for top-quark and top-antiquark production in the t-channel, together with the cross-section ratio.

Differential t-channel top-quark production cross sections and normalized differential t-channel top-quark production cross sections as functions of ABS(YRAP(TBAR)).

Parametrization factors for the $m_{t}$ dependence [see Eq. (4) in the paper] of $\sigma(tq)$, $\sigma(\bar tq)$, and $\sigma(t q+\bar t q)$.

The cross sections for top-quark and top-antiquark production in the t-channel, together with the cross-section ratio.

The value of $|V_{tb}|^{2}$ is extracted by dividing the measured value of $\sigma(t q+\bar t q)$ by the prediction of the approximate NNLO calculation. The experimental and theoretical uncertainties are added in quadrature.

Event yields for the 2-jet-$\ell^{+}$ and 2-jet-$\ell^{-}$ HPR channels. The expectation for the signal and background yields correspond to the result of the binned maximum-likelihood fit described in Sec. $\mathrm{VI~D}$ in the paper. The uncertainty of the expectations is the normalization uncertainty of each process after the fit, as described in Sec. $\mathrm{VII~F}$ in the paper.

Migration matrix relating the parton level $p_{\mathrm{T}}(t)$ shown on the $y$ axis and the reconstruction level $p_{\mathrm{T}}(\ell \nu b)$ shown on the $x$ axis for the top-quark $p_{\mathrm{T}}$ distribution.

Migration matrix relating the parton level $p_{\mathrm{T}}(\bar t)$ shown on the $y$ axis and the reconstruction level $p_{\mathrm{T}}(\ell \nu b)$ shown on the $x$ axis for the top-antiquark $p_{\mathrm{T}}$ distribution.

Migration matrix relating the parton level $|y(t)|$ shown on the $y$ axis and the reconstruction level $|y(\ell \nu b)|$ shown on the $x$ axis for the top-quark $|y|$ distribution.

Migration matrix relating the parton level $|y(\bar t)|$ shown on the $y$ axis and the reconstruction level $|y(\ell \nu b)|$ shown on the $x$ axis for the top-antiquark $|y|$ distribution.

Differential t-channel top-quark production cross section as a function of $p_{\mathrm{T}}(t)$ with the uncertainties for each bin given in percent.

Differential t-channel top-quark production cross section as a function of $p_{\mathrm{T}}(\bar t)$ with the uncertainties for each bin given in percent.

Differential t-channel top-quark production cross section as a function of $|y(t)|$ with the uncertainties for each bin given in percent.

Differential t-channel top-quark production cross section as a function of $|y(\bar t)|$ with the uncertainties for each bin given in percent.

Normalized differential t-channel top-quark production cross section as a function of $p_{\mathrm{T}}(t)$ with the uncertainties for each bin given in percent.

Normalized differential t-channel top-quark production cross section as a function of $p_{\mathrm{T}}(\bar t)$ with the uncertainties for each bin given in percent.

Normalized differential t-channel top-quark production cross section as a function of $|y(t)|$ with the uncertainties for each bin given in percent.

Normalized differential t-channel top-quark production cross section as a function of $|y(\bar t)|$ with the uncertainties for each bin given in percent.

Comparison between the measured differential cross sections and the predictions from the NLO calculation using the MSTW2008 PDF set. For each variable and prediction a $\chi^{2}$ value is calculated with HERAfitter using the covariance matrix of each measured spectrum. The theory uncertainties of the predictions are treated as uncorrelated. The number of degrees of freedom (NDF) is equal to the number of bins in the measured spectrum.

Detailed list of the contribution of each source of uncertainty to the total relative uncertainty on the measured $\dfrac{\mathrm{d}\sigma}{\mathrm{d}p_{\mathrm{T}}(t)}$ distribution given in percent for each bin. The list includes only those uncertainties that contribute with more than $1\%$. The following uncertainties contribute to the total uncertainty with less than $1\%$ to each bin content$:$ JES detector, JES statistical, JES physics modeling, JES mixed detector and modeling, JES close-by jets, JES pileup, JES flavor composition, JES flavor response, jet-vertex fraction, $b/\bar{b}$ acceptance, $E_{\mathrm{T}}^{\mathrm{miss}}$ modeling, $W+$ jets shape variation, and $t \bar{t}$ generator. In cases when the uncertainty is report to be "$<1\%$" in the table of the paper the uncertainty is approximated by a value of $0.5\%$.

Detailed list of the contribution of each source of uncertainty to the total relative uncertainty on the measured $\dfrac{\mathrm{d}\sigma}{\mathrm{d}p_{\mathrm{T}}(\bar t)}$ distribution given in percent for each bin. The list includes only those uncertainties that contribute with more than $1\%$. The following uncertainties contribute to the total uncertainty with less than $1\%$ to each bin content$:$ JES detector, JES statistical, JES physics modeling, JES mixed detector and modeling, JES close-by jets, JES pileup, JES flavor composition, JES flavor response, $b-$JES, jet-vertex fraction, mistag efficiency, $b/\bar{b}$ acceptance, $E_{\mathrm{T}}^{\mathrm{miss}}$ modeling, $W+$ jets shape variation, and $t \bar{t}$ generator. In cases when the uncertainty is report to be "$<1\%$" in the table of the paper the uncertainty is approximated by a value of $0.5\%$.

Detailed list of the contribution of each source of uncertainty to the total relative uncertainty on the measured $\dfrac{\mathrm{d}\sigma}{\mathrm{d}|y(t)|}$ distribution given in percent for each bin. The list includes only those uncertainties that contribute with more than $1\%$. The following uncertainties contribute to the total uncertainty with less than $1\%$ to each bin content$:$ JES detector, JES statistical, JES physics modeling, JES mixed detector and modeling, JES close-by jets, JES pileup, JES flavor composition, JES flavor response, jet-vertex fraction, $b/\bar{b}$ acceptance, $E_{\mathrm{T}}^{\mathrm{miss}}$ modeling, $W+$ jets shape variation, $t \bar{t}$ generator, $t \bar{t}$ ISR/FSR, and unfolding. In cases when the uncertainty is report to be "$<1\%$" in the table of the paper the uncertainty is approximated by a value of $0.5\%$.

Detailed list of the contribution of each source of uncertainty to the total relative uncertainty on the measured $\dfrac{\mathrm{d}\sigma}{\mathrm{d}|y(\bar t)|}$ distribution given in percent for each bin. The list includes only those uncertainties that contribute with more than $1\%$. The following uncertainties contribute to the total uncertainty with less than $1\%$ to each bin content$:$ JES detector, JES statistical, JES physics modeling, JES mixed detector and modeling, JES close-by jets, JES pileup, JES flavor composition, JES flavor response, $b-$JES, jet-vertex fraction, $b/\bar{b}$ acceptance, mistag efficiency, $E_{\mathrm{T}}^{\mathrm{miss}}$ modeling, $W+$ jets shape variation, $t \bar{t}$ generator, $t \bar{t}$ ISR/FSR, and unfolding. In cases when the uncertainty is report to be "$<1\%$" in the table of the paper the uncertainty is approximated by a value of $0.5\%$.

Detailed list of the contribution of each source of uncertainty to the total relative uncertainty on the measured $\dfrac{1}{\sigma}\dfrac{\mathrm{d}\sigma}{\mathrm{d}p_{\mathrm{T}}(t)}$ distribution given in percent for each bin. The list includes only those uncertainties that contribute with more than $1\%$. The JES $\eta$ intercalibration uncertainty has a sign switch from the first to the second bin. For the $tq$ generator $+$ parton shower uncertainty a sign switch is denoted with $\mp$. The following uncertainties contribute to the total uncertainty with less than $1\%$ to each bin content$:$ JES detector, JES statistical, JES physics modeling, JES mixed detector and modeling, JES close-by jets, JES pileup, JES flavor composition, JES flavor response, $b-$JES, jet-vertex fraction, $b/\bar{b}$ acceptance, $c-$tagging efficiency, $E_{\mathrm{T}}^{\mathrm{miss}}$ modeling, lepton uncertainties, $W+$ jets shape variation, and $t \bar{t}$ generator. In cases when the uncertainty is report to be "$<1\%$" in the table of the paper the uncertainty is approximated by a value of $0.5\%$.

Detailed list of the contribution of each source of uncertainty to the total relative uncertainty on the measured $\dfrac{1}{\sigma}\dfrac{\mathrm{d}\sigma}{\mathrm{d}p_{\mathrm{T}}(\bar t)}$ distribution given in percent for each bin. The list includes only those uncertainties that contribute with more than $1\%$. Sign switches within one uncertainty are denoted with $\mp$ and $\pm$. The following uncertainties contribute to the total uncertainty with less than $1\%$ to each bin content$:$ JES detector, JES statistical, JES physics modeling, JES mixed detector and modeling, JES close-by jets, JES pileup, JES flavor composition, JES flavor response, $b-$JES, jet-vertex fraction, $b/\bar{b}$ acceptance, mistag efficiency, $E_{\mathrm{T}}^{\mathrm{miss}}$ modeling, lepton uncertainties, $W+$ jets shape variation, and $t \bar{t}$ generator. In cases when the uncertainty is report to be "$<1\%$" in the table of the paper the uncertainty is approximated by a value of $0.5\%$.

Detailed list of the contribution of each source of uncertainty to the total relative uncertainty on the measured $\dfrac{1}{\sigma}\dfrac{\mathrm{d}\sigma}{\mathrm{d}|y(t)|}$ distribution given in percent for each bin. The list includes only those uncertainties that contribute with more than $1\%$. Sign switches within one uncertainty are denoted with $\mp$ and $\pm$. The following uncertainties contribute to the total uncertainty with less than $1\%$ to each bin content$:$ JES detector, JES statistical, JES physics modeling, JES mixed detector and modeling, JES close-by jets, JES pileup, JES flavor composition, JES flavor response, b-JES, jet-vertex fraction, $b/\bar{b}$ acceptance, $b-$tagging efficiency, $c-$tagging efficiency, mistag efficiency, $E_{\mathrm{T}}^{\mathrm{miss}}$ modeling, lepton uncertainties, $W+$jets shape variation, $t \bar{t}$ generator, $t \bar{t}$ISR/FSR, and unfolding. In cases when the uncertainty is report to be "$<1\%$" in the table of the paper the uncertainty is approximated by a value of $0.5\%$.

Detailed list of the contribution of each source of uncertainty to the total relative uncertainty on the measured $\dfrac{1}{\sigma}\dfrac{\mathrm{d}\sigma}{\mathrm{d}|y(\bar t)|}$ distribution given in percent for each bin. The list includes only those uncertainties that contribute with more than $1\%$. Sign switches within one uncertainty are denoted with $\mp$ and $\pm$. The following uncertainties contribute to the total uncertainty with less than $1\%$ to each bin content $:$ JES detector, JES statistical, JES physics modeling, JES mixed detector and modeling, JES close-by jets, JES pileup, JES flavor composition, JES flavor response, b-JES, jet energy resolution, jet-vertex fraction, $b/\bar{b}$ acceptance, $b-$tagging efficiency, $c-$ tagging efficiency, mistag efficiency, $E_{\mathrm{T}}^{\mathrm{miss}}$ modeling, lepton uncertainties, $W+$ jets shape variation, $t \bar{t}$ generator, $t \bar{t}$ ISR/FSR, and unfolding. In cases when the uncertainty is report to be "$<1\%$" in the table of the paper the uncertainty is approximated by a value of $0.5\%$.

Statistical correlation matrices for the differential cross section as a function of $p_{\mathrm{T}}(t)$.

Statistical correlation matrices for the differential cross section as a function of $p_{\mathrm{T}}(\bar t)$.

Statistical correlation matrices for the differential cross section as a function of $|y(t)|$.

Statistical correlation matrices for the differential cross section as a function of $|y(\bar t)|$.

Statistical correlation matrices for the normalized differential cross section as a function of $p_{\mathrm{T}}(t)$.

Statistical correlation matrices for the normalized differential cross section as a function of $p_{\mathrm{T}}(\bar t)$.

Statistical correlation matrices for the normalized differential cross section as a function of $|y(t)|$.

Statistical correlation matrices for the normalized differential cross section as a function of $|y(\bar t)|$.

Absolute differential cross-section as a function of $\Delta R^{extra1}_{jet1}$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the absolute differential cross-section as function of $\Delta R^{extra1}_{jet1}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $|y^{t,1}|$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the relative differential cross-section as function of $|y^{t,1}|$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $|y^{t,1}|$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the absolute differential cross-section as function of $|y^{t,1}|$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $m^{t\bar{t}}$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the relative differential cross-section as function of $m^{t\bar{t}}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $m^{t\bar{t}}$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the absolute differential cross-section as function of $m^{t\bar{t}}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $|y^{t,2}|$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the relative differential cross-section as function of $|y^{t,2}|$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $|y^{t,2}|$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the absolute differential cross-section as function of $|y^{t,2}|$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $|y^{t\bar{t}}|$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the relative differential cross-section as function of $|y^{t\bar{t}}|$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $|y^{t\bar{t}}|$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the absolute differential cross-section as function of $|y^{t\bar{t}}|$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $p_{T}^{t,1}$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the relative differential cross-section as function of $p_{T}^{t,1}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $p_{T}^{t,1}$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the absolute differential cross-section as function of $p_{T}^{t,1}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $p_{T}^{t,2}$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the relative differential cross-section as function of $p_{T}^{t,2}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $p_{T}^{t,2}$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the absolute differential cross-section as function of $p_{T}^{t,2}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $p_{T}^{t\bar{t}}$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the relative differential cross-section as function of $p_{T}^{t\bar{t}}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $p_{T}^{t\bar{t}}$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $N_{jets}$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the relative differential cross-section as function of $N_{jets}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $N_{jets}$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the absolute differential cross-section as function of $N_{jets}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $\Delta\phi^{t\bar{t}}$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the relative differential cross-section as function of $\Delta\phi^{t\bar{t}}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $\Delta\phi^{t\bar{t}}$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the absolute differential cross-section as function of $\Delta\phi^{t\bar{t}}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $|P_{out}^{t,1}|$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the relative differential cross-section as function of $|P_{out}^{t,1}|$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $|P_{out}^{t,1}|$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the absolute differential cross-section as function of $|P_{out}^{t,1}|$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $|P_{cross}|$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the relative differential cross-section as function of $|P_{cross}|$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $|P_{cross}|$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the absolute differential cross-section as function of $|P_{cross}|$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $Z^{t\bar{t}}$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the relative differential cross-section as function of $Z^{t\bar{t}}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $Z^{t\bar{t}}$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the absolute differential cross-section as function of $Z^{t\bar{t}}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $H_{T}^{t\bar{t}}$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the relative differential cross-section as function of $H_{T}^{t\bar{t}}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $H_{T}^{t\bar{t}}$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $|y_{boost}^{t\bar{t}}|$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the relative differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $|y_{boost}^{t\bar{t}}|$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $\chi^{t\bar{t}}$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the relative differential cross-section as function of $\chi^{t\bar{t}}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $\chi^{t\bar{t}}$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the absolute differential cross-section as function of $\chi^{t\bar{t}}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $R_{Wt}^{leading}$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the relative differential cross-section as function of $R_{Wt}^{leading}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $R_{Wt}^{leading}$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the absolute differential cross-section as function of $R_{Wt}^{leading}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $R_{Wt}^{subleading}$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the relative differential cross-section as function of $R_{Wt}^{subleading}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $R_{Wt}^{subleading}$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the absolute differential cross-section as function of $R_{Wt}^{subleading}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $R_{Wb}^{leading}$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the relative differential cross-section as function of $R_{Wb}^{leading}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $R_{Wb}^{leading}$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the absolute differential cross-section as function of $R_{Wb}^{leading}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $R_{Wb}^{subleading}$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the relative differential cross-section as function of $R_{Wb}^{subleading}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $R_{Wb}^{subleading}$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the absolute differential cross-section as function of $R_{Wb}^{subleading}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $\Delta R^{extra1}_{t,close}$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the relative differential cross-section as function of $\Delta R^{extra1}_{t,close}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $\Delta R^{extra1}_{t,close}$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the absolute differential cross-section as function of $\Delta R^{extra1}_{t,close}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $\Delta R^{extra2}_{t,close}$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the relative differential cross-section as function of $\Delta R^{extra2}_{t,close}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $\Delta R^{extra2}_{t,close}$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the absolute differential cross-section as function of $\Delta R^{extra2}_{t,close}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $\Delta R^{extra3}_{t,close}$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the relative differential cross-section as function of $\Delta R^{extra3}_{t,close}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $\Delta R^{extra3}_{t,close}$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the absolute differential cross-section as function of $\Delta R^{extra3}_{t,close}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $R^{pT, extra1}_{t,1}$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the relative differential cross-section as function of $R^{pT, extra1}_{t,1}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $R^{pT, extra1}_{t,1}$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the absolute differential cross-section as function of $R^{pT, extra1}_{t,1}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $R^{pT, extra2}_{t,1}$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the relative differential cross-section as function of $R^{pT, extra2}_{t,1}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $R^{pT, extra2}_{t,1}$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the absolute differential cross-section as function of $R^{pT, extra2}_{t,1}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $R^{pT, extra3}_{t,1}$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the relative differential cross-section as function of $R^{pT, extra3}_{t,1}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $R^{pT, extra3}_{t,1}$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the absolute differential cross-section as function of $R^{pT, extra3}_{t,1}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $R^{pT, t\bar{t}}_{extra1}$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the relative differential cross-section as function of $R^{pT, t\bar{t}}_{extra1}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $R^{pT, t\bar{t}}_{extra1}$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the absolute differential cross-section as function of $R^{pT, t\bar{t}}_{extra1}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $R^{pT, extra1}_{jet1}$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the relative differential cross-section as function of $R^{pT, extra1}_{jet1}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $R^{pT, extra1}_{jet1}$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the absolute differential cross-section as function of $R^{pT, extra1}_{jet1}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $R^{pT, extra2}_{jet1}$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the relative differential cross-section as function of $R^{pT, extra2}_{jet1}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $R^{pT, extra2}_{jet1}$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the absolute differential cross-section as function of $R^{pT, extra2}_{jet1}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $R^{pT, extra3}_{jet1}$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the relative differential cross-section as function of $R^{pT, extra3}_{jet1}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $R^{pT, extra3}_{jet1}$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the absolute differential cross-section as function of $R^{pT, extra3}_{jet1}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $\Delta R^{extra2}_{extra1}$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the relative differential cross-section as function of $\Delta R^{extra2}_{extra1}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $\Delta R^{extra2}_{extra1}$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the absolute differential cross-section as function of $\Delta R^{extra2}_{extra1}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $\Delta R^{extra3}_{extra1}$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the relative differential cross-section as function of $\Delta R^{extra3}_{extra1}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $\Delta R^{extra3}_{extra1}$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the absolute differential cross-section as function of $\Delta R^{extra3}_{extra1}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $R^{pT, extra2}_{extra1}$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the relative differential cross-section as function of $R^{pT, extra2}_{extra1}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $R^{pT, extra2}_{extra1}$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the absolute differential cross-section as function of $R^{pT, extra2}_{extra1}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $R^{pT, extra3}_{extra1}$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the relative differential cross-section as function of $R^{pT, extra3}_{extra1}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $R^{pT, extra3}_{extra1}$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the absolute differential cross-section as function of $R^{pT, extra3}_{extra1}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Total cross-section at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $p_{T}^{t,1}$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 6. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $p_{T}^{t,1}$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 7. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $p_{T}^{t,1}$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 8. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $p_{T}^{t,1}$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ > 8. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ = 6 and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ = 7 and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ = 7 and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ = 8 and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ = 8 and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ = 8 and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ = 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ > 8 and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ > 8 and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ > 8 and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ = 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ > 8 and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ > 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute double-differential cross-section as a function of $p_{T}^{t,1}$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 6. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $p_{T}^{t,1}$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 7. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $p_{T}^{t,1}$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 8. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $p_{T}^{t,1}$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ > 8. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ = 6 and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ = 7 and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ = 7 and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ = 8 and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ = 8 and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ = 8 and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ = 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ > 8 and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ > 8 and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ > 8 and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ = 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ > 8 and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ > 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative double-differential cross-section as a function of $p_{T}^{t,2}$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 6. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $p_{T}^{t,2}$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 7. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $p_{T}^{t,2}$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 8. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $p_{T}^{t,2}$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ > 8. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ = 6 and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ = 7 and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ = 7 and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ = 8 and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ = 8 and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ = 8 and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ = 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ > 8 and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ > 8 and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ > 8 and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ = 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ > 8 and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ > 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute double-differential cross-section as a function of $p_{T}^{t,2}$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 6. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $p_{T}^{t,2}$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 7. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $p_{T}^{t,2}$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 8. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $p_{T}^{t,2}$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ > 8. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ = 6 and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ = 7 and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ = 7 and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ = 8 and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ = 8 and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ = 8 and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ = 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ > 8 and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ > 8 and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ > 8 and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ = 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ > 8 and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ > 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 6. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 7. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 8. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ > 8. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 6 and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 7 and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 7 and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 8 and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 8 and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 8 and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ > 8 and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ > 8 and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ > 8 and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ > 8 and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ > 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 6. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 7. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 8. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ > 8. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 6 and the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 7 and the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 7 and the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 8 and the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 8 and the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 8 and the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ > 8 and the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ > 8 and the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ > 8 and the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ > 8 and the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ > 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative double-differential cross-section as a function of $|P_{out}^{t,1}|$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 6. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $|P_{out}^{t,1}|$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 7. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $|P_{out}^{t,1}|$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 8. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $|P_{out}^{t,1}|$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ > 8. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix between the relative double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ = 6 and the relative double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ = 7 and the relative double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ = 7 and the relative double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ = 8 and the relative double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ = 8 and the relative double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ = 8 and the relative double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ = 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ > 8 and the relative double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ > 8 and the relative double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ > 8 and the relative double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ = 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ > 8 and the relative double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ > 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute double-differential cross-section as a function of $|P_{out}^{t,1}|$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 6. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $|P_{out}^{t,1}|$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 7. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $|P_{out}^{t,1}|$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 8. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $|P_{out}^{t,1}|$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ > 8. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix between the absolute double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ = 6 and the absolute double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ = 7 and the absolute double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ = 7 and the absolute double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ = 8 and the absolute double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ = 8 and the absolute double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ = 8 and the absolute double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ = 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ > 8 and the absolute double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ > 8 and the absolute double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ > 8 and the absolute double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ = 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ > 8 and the absolute double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ > 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative double-differential cross-section as a function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 6. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 7. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 8. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ > 8. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix between the relative double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 6 and the relative double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 7 and the relative double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 7 and the relative double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 8 and the relative double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 8 and the relative double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 8 and the relative double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ > 8 and the relative double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ > 8 and the relative double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ > 8 and the relative double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ > 8 and the relative double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ > 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute double-differential cross-section as a function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 6. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 7. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 8. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ > 8. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix between the absolute double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 6 and the absolute double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 7 and the absolute double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 7 and the absolute double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 8 and the absolute double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 8 and the absolute double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 8 and the absolute double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ > 8 and the absolute double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ > 8 and the absolute double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ > 8 and the absolute double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ > 8 and the absolute double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ > 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative double-differential cross-section as a function of $|P_{cross}|$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 6. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $|P_{cross}|$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 7. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $|P_{cross}|$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 8. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $|P_{cross}|$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ > 8. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix between the relative double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ = 6 and the relative double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ = 7 and the relative double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ = 7 and the relative double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ = 8 and the relative double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ = 8 and the relative double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ = 8 and the relative double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ = 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ > 8 and the relative double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ > 8 and the relative double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ > 8 and the relative double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ = 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ > 8 and the relative double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ > 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute double-differential cross-section as a function of $|P_{cross}|$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 6. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $|P_{cross}|$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 7. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $|P_{cross}|$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 8. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $|P_{cross}|$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ > 8. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix between the absolute double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ = 6 and the absolute double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ = 7 and the absolute double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ = 7 and the absolute double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ = 8 and the absolute double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ = 8 and the absolute double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ = 8 and the absolute double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ = 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ > 8 and the absolute double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ > 8 and the absolute double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ > 8 and the absolute double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ = 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ > 8 and the absolute double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ > 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative double-differential cross-section as a function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ at particle level in the all hadronic resolved topology in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ at particle level in the all hadronic resolved topology in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ at particle level in the all hadronic resolved topology in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ at particle level in the all hadronic resolved topology in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute double-differential cross-section as a function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ at particle level in the all hadronic resolved topology in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ at particle level in the all hadronic resolved topology in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ at particle level in the all hadronic resolved topology in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ at particle level in the all hadronic resolved topology in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ at particle level in the all hadronic resolved topology in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ at particle level in the all hadronic resolved topology in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ at particle level in the all hadronic resolved topology in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ at particle level in the all hadronic resolved topology in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ at particle level in the all hadronic resolved topology in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ at particle level in the all hadronic resolved topology in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ at particle level in the all hadronic resolved topology in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ at particle level in the all hadronic resolved topology in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative double-differential cross-section as a function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ at particle level in the all hadronic resolved topology in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ at particle level in the all hadronic resolved topology in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ at particle level in the all hadronic resolved topology in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ at particle level in the all hadronic resolved topology in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV and the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV and the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV and the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV and the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV and the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV and the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute double-differential cross-section as a function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ at particle level in the all hadronic resolved topology in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ at particle level in the all hadronic resolved topology in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ at particle level in the all hadronic resolved topology in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ at particle level in the all hadronic resolved topology in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV and the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV and the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV and the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV and the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV and the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV and the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative double-differential cross-section as a function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ at particle level in the all hadronic resolved topology in 0.0 GeV < $p_{T}^{t,2}$ < 175.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ at particle level in the all hadronic resolved topology in 175.0 GeV < $p_{T}^{t,2}$ < 275.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ at particle level in the all hadronic resolved topology in 275.0 GeV < $p_{T}^{t,2}$ < 385.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ at particle level in the all hadronic resolved topology in 385.0 GeV < $p_{T}^{t,2}$ < 1000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 0.0 GeV < $p_{T}^{t,2}$ < 175.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 0.0 GeV < $p_{T}^{t,2}$ < 175.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 175.0 GeV < $p_{T}^{t,2}$ < 275.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 0.0 GeV < $p_{T}^{t,2}$ < 175.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 175.0 GeV < $p_{T}^{t,2}$ < 275.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 175.0 GeV < $p_{T}^{t,2}$ < 275.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 275.0 GeV < $p_{T}^{t,2}$ < 385.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 0.0 GeV < $p_{T}^{t,2}$ < 175.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 275.0 GeV < $p_{T}^{t,2}$ < 385.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 175.0 GeV < $p_{T}^{t,2}$ < 275.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 275.0 GeV < $p_{T}^{t,2}$ < 385.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 275.0 GeV < $p_{T}^{t,2}$ < 385.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 385.0 GeV < $p_{T}^{t,2}$ < 1000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 0.0 GeV < $p_{T}^{t,2}$ < 175.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 385.0 GeV < $p_{T}^{t,2}$ < 1000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 175.0 GeV < $p_{T}^{t,2}$ < 275.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 385.0 GeV < $p_{T}^{t,2}$ < 1000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 275.0 GeV < $p_{T}^{t,2}$ < 385.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 385.0 GeV < $p_{T}^{t,2}$ < 1000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 385.0 GeV < $p_{T}^{t,2}$ < 1000.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute double-differential cross-section as a function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ at particle level in the all hadronic resolved topology in 0.0 GeV < $p_{T}^{t,2}$ < 175.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ at particle level in the all hadronic resolved topology in 175.0 GeV < $p_{T}^{t,2}$ < 275.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ at particle level in the all hadronic resolved topology in 275.0 GeV < $p_{T}^{t,2}$ < 385.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ at particle level in the all hadronic resolved topology in 385.0 GeV < $p_{T}^{t,2}$ < 1000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 0.0 GeV < $p_{T}^{t,2}$ < 175.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 0.0 GeV < $p_{T}^{t,2}$ < 175.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 175.0 GeV < $p_{T}^{t,2}$ < 275.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 0.0 GeV < $p_{T}^{t,2}$ < 175.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 175.0 GeV < $p_{T}^{t,2}$ < 275.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 175.0 GeV < $p_{T}^{t,2}$ < 275.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 275.0 GeV < $p_{T}^{t,2}$ < 385.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 0.0 GeV < $p_{T}^{t,2}$ < 175.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 275.0 GeV < $p_{T}^{t,2}$ < 385.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 175.0 GeV < $p_{T}^{t,2}$ < 275.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 275.0 GeV < $p_{T}^{t,2}$ < 385.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 275.0 GeV < $p_{T}^{t,2}$ < 385.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 385.0 GeV < $p_{T}^{t,2}$ < 1000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 0.0 GeV < $p_{T}^{t,2}$ < 175.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 385.0 GeV < $p_{T}^{t,2}$ < 1000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 175.0 GeV < $p_{T}^{t,2}$ < 275.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 385.0 GeV < $p_{T}^{t,2}$ < 1000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 275.0 GeV < $p_{T}^{t,2}$ < 385.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 385.0 GeV < $p_{T}^{t,2}$ < 1000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 385.0 GeV < $p_{T}^{t,2}$ < 1000.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative double-differential cross-section as a function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ at particle level in the all hadronic resolved topology in 0.0 GeV < $m^{t\bar{t}}$ < 645.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ at particle level in the all hadronic resolved topology in 645.0 GeV < $m^{t\bar{t}}$ < 795.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ at particle level in the all hadronic resolved topology in 795.0 GeV < $m^{t\bar{t}}$ < 1080.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ at particle level in the all hadronic resolved topology in 1080.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 645.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 645.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 645.0 GeV < $m^{t\bar{t}}$ < 795.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 645.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 645.0 GeV < $m^{t\bar{t}}$ < 795.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 645.0 GeV < $m^{t\bar{t}}$ < 795.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 795.0 GeV < $m^{t\bar{t}}$ < 1080.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 645.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 795.0 GeV < $m^{t\bar{t}}$ < 1080.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 645.0 GeV < $m^{t\bar{t}}$ < 795.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 795.0 GeV < $m^{t\bar{t}}$ < 1080.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 795.0 GeV < $m^{t\bar{t}}$ < 1080.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 1080.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 645.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 1080.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 645.0 GeV < $m^{t\bar{t}}$ < 795.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 1080.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 795.0 GeV < $m^{t\bar{t}}$ < 1080.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 1080.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 1080.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute double-differential cross-section as a function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ at particle level in the all hadronic resolved topology in 0.0 GeV < $m^{t\bar{t}}$ < 645.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ at particle level in the all hadronic resolved topology in 645.0 GeV < $m^{t\bar{t}}$ < 795.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ at particle level in the all hadronic resolved topology in 795.0 GeV < $m^{t\bar{t}}$ < 1080.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ at particle level in the all hadronic resolved topology in 1080.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 645.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 645.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 645.0 GeV < $m^{t\bar{t}}$ < 795.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 645.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 645.0 GeV < $m^{t\bar{t}}$ < 795.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 645.0 GeV < $m^{t\bar{t}}$ < 795.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 795.0 GeV < $m^{t\bar{t}}$ < 1080.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 645.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 795.0 GeV < $m^{t\bar{t}}$ < 1080.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 645.0 GeV < $m^{t\bar{t}}$ < 795.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 795.0 GeV < $m^{t\bar{t}}$ < 1080.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 795.0 GeV < $m^{t\bar{t}}$ < 1080.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 1080.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 645.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 1080.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 645.0 GeV < $m^{t\bar{t}}$ < 795.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 1080.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 795.0 GeV < $m^{t\bar{t}}$ < 1080.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 1080.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 1080.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $\chi^{t\bar{t}}$ at parton level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the relative differential cross-section as function of $\chi^{t\bar{t}}$ at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $\chi^{t\bar{t}}$ at parton level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the absolute differential cross-section as function of $\chi^{t\bar{t}}$ at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $p_{T}^{t\bar{t}}$ at parton level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the relative differential cross-section as function of $p_{T}^{t\bar{t}}$ at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $p_{T}^{t\bar{t}}$ at parton level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $\Delta\phi^{t\bar{t}}$ at parton level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the relative differential cross-section as function of $\Delta\phi^{t\bar{t}}$ at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $\Delta\phi^{t\bar{t}}$ at parton level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the absolute differential cross-section as function of $\Delta\phi^{t\bar{t}}$ at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $p_{T}^{t,2}$ at parton level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the relative differential cross-section as function of $p_{T}^{t,2}$ at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $p_{T}^{t,2}$ at parton level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the absolute differential cross-section as function of $p_{T}^{t,2}$ at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the relative differential cross-section as function of $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the absolute differential cross-section as function of $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $|y_{boost}^{t\bar{t}}|$ at parton level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the relative differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $|y_{boost}^{t\bar{t}}|$ at parton level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $p_{T}^{t,1}$ at parton level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the relative differential cross-section as function of $p_{T}^{t,1}$ at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $p_{T}^{t,1}$ at parton level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the absolute differential cross-section as function of $p_{T}^{t,1}$ at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $|y^{t\bar{t}}|$ at parton level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the relative differential cross-section as function of $|y^{t\bar{t}}|$ at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $|y^{t\bar{t}}|$ at parton level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the absolute differential cross-section as function of $|y^{t\bar{t}}|$ at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $|y^{t,2}|$ at parton level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the relative differential cross-section as function of $|y^{t,2}|$ at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $|y^{t,2}|$ at parton level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the absolute differential cross-section as function of $|y^{t,2}|$ at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $H_{T}^{t\bar{t}}$ at parton level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the relative differential cross-section as function of $H_{T}^{t\bar{t}}$ at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $H_{T}^{t\bar{t}}$ at parton level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $|y^{t,1}|$ at parton level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the relative differential cross-section as function of $|y^{t,1}|$ at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $|y^{t,1}|$ at parton level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the absolute differential cross-section as function of $|y^{t,1}|$ at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative double-differential cross-section as a function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute double-differential cross-section as a function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative double-differential cross-section as a function of $|y^{t,2}|$ vs $|y^{t,1}|$ at parton level in the all hadronic resolved topology in 0.0 < $|y^{t,1}|$ < 0.5 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $|y^{t,2}|$ vs $|y^{t,1}|$ at parton level in the all hadronic resolved topology in 0.5 < $|y^{t,1}|$ < 1.0 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $|y^{t,2}|$ vs $|y^{t,1}|$ at parton level in the all hadronic resolved topology in 1.0 < $|y^{t,1}|$ < 1.5 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $|y^{t,2}|$ vs $|y^{t,1}|$ at parton level in the all hadronic resolved topology in 1.5 < $|y^{t,1}|$ < 2.5 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 0.0 < $|y^{t,1}|$ < 0.5 and the relative double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 0.0 < $|y^{t,1}|$ < 0.5 at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 0.5 < $|y^{t,1}|$ < 1.0 and the relative double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 0.0 < $|y^{t,1}|$ < 0.5 at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 0.5 < $|y^{t,1}|$ < 1.0 and the relative double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 0.5 < $|y^{t,1}|$ < 1.0 at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 1.0 < $|y^{t,1}|$ < 1.5 and the relative double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 0.0 < $|y^{t,1}|$ < 0.5 at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 1.0 < $|y^{t,1}|$ < 1.5 and the relative double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 0.5 < $|y^{t,1}|$ < 1.0 at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 1.0 < $|y^{t,1}|$ < 1.5 and the relative double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 1.0 < $|y^{t,1}|$ < 1.5 at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 1.5 < $|y^{t,1}|$ < 2.5 and the relative double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 0.0 < $|y^{t,1}|$ < 0.5 at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 1.5 < $|y^{t,1}|$ < 2.5 and the relative double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 0.5 < $|y^{t,1}|$ < 1.0 at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 1.5 < $|y^{t,1}|$ < 2.5 and the relative double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 1.0 < $|y^{t,1}|$ < 1.5 at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 1.5 < $|y^{t,1}|$ < 2.5 and the relative double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 1.5 < $|y^{t,1}|$ < 2.5 at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute double-differential cross-section as a function of $|y^{t,2}|$ vs $|y^{t,1}|$ at parton level in the all hadronic resolved topology in 0.0 < $|y^{t,1}|$ < 0.5 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $|y^{t,2}|$ vs $|y^{t,1}|$ at parton level in the all hadronic resolved topology in 0.5 < $|y^{t,1}|$ < 1.0 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $|y^{t,2}|$ vs $|y^{t,1}|$ at parton level in the all hadronic resolved topology in 1.0 < $|y^{t,1}|$ < 1.5 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $|y^{t,2}|$ vs $|y^{t,1}|$ at parton level in the all hadronic resolved topology in 1.5 < $|y^{t,1}|$ < 2.5 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 0.0 < $|y^{t,1}|$ < 0.5 and the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 0.0 < $|y^{t,1}|$ < 0.5 at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 0.5 < $|y^{t,1}|$ < 1.0 and the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 0.0 < $|y^{t,1}|$ < 0.5 at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 0.5 < $|y^{t,1}|$ < 1.0 and the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 0.5 < $|y^{t,1}|$ < 1.0 at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 1.0 < $|y^{t,1}|$ < 1.5 and the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 0.0 < $|y^{t,1}|$ < 0.5 at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 1.0 < $|y^{t,1}|$ < 1.5 and the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 0.5 < $|y^{t,1}|$ < 1.0 at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 1.0 < $|y^{t,1}|$ < 1.5 and the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 1.0 < $|y^{t,1}|$ < 1.5 at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 1.5 < $|y^{t,1}|$ < 2.5 and the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 0.0 < $|y^{t,1}|$ < 0.5 at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 1.5 < $|y^{t,1}|$ < 2.5 and the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 0.5 < $|y^{t,1}|$ < 1.0 at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 1.5 < $|y^{t,1}|$ < 2.5 and the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 1.0 < $|y^{t,1}|$ < 1.5 at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 1.5 < $|y^{t,1}|$ < 2.5 and the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 1.5 < $|y^{t,1}|$ < 2.5 at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative double-differential cross-section as a function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 1315.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 1315.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 1315.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 1315.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 1315.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 1315.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute double-differential cross-section as a function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 1315.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 1315.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 1315.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 1315.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 1315.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 1315.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative double-differential cross-section as a function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the relative double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the relative double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the relative double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute double-differential cross-section as a function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the absolute double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the absolute double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the absolute double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative double-differential cross-section as a function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the relative double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the relative double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the relative double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute double-differential cross-section as a function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 1315.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1315.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1315.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1315.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1315.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1315.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 1315.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1315.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1315.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1315.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1315.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1315.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative double-differential cross-section as a function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute double-differential cross-section as a function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative double-differential cross-section as a function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ at parton level in the all hadronic resolved topology in 0.0 GeV < $p_{T}^{t,2}$ < 170.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ at parton level in the all hadronic resolved topology in 170.0 GeV < $p_{T}^{t,2}$ < 290.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ at parton level in the all hadronic resolved topology in 290.0 GeV < $p_{T}^{t,2}$ < 450.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ at parton level in the all hadronic resolved topology in 450.0 GeV < $p_{T}^{t,2}$ < 1000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 0.0 GeV < $p_{T}^{t,2}$ < 170.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 0.0 GeV < $p_{T}^{t,2}$ < 170.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 170.0 GeV < $p_{T}^{t,2}$ < 290.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 0.0 GeV < $p_{T}^{t,2}$ < 170.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 170.0 GeV < $p_{T}^{t,2}$ < 290.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 170.0 GeV < $p_{T}^{t,2}$ < 290.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 290.0 GeV < $p_{T}^{t,2}$ < 450.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 0.0 GeV < $p_{T}^{t,2}$ < 170.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 290.0 GeV < $p_{T}^{t,2}$ < 450.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 170.0 GeV < $p_{T}^{t,2}$ < 290.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 290.0 GeV < $p_{T}^{t,2}$ < 450.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 290.0 GeV < $p_{T}^{t,2}$ < 450.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 450.0 GeV < $p_{T}^{t,2}$ < 1000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 0.0 GeV < $p_{T}^{t,2}$ < 170.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 450.0 GeV < $p_{T}^{t,2}$ < 1000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 170.0 GeV < $p_{T}^{t,2}$ < 290.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 450.0 GeV < $p_{T}^{t,2}$ < 1000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 290.0 GeV < $p_{T}^{t,2}$ < 450.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 450.0 GeV < $p_{T}^{t,2}$ < 1000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 450.0 GeV < $p_{T}^{t,2}$ < 1000.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute double-differential cross-section as a function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ at parton level in the all hadronic resolved topology in 0.0 GeV < $p_{T}^{t,2}$ < 170.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ at parton level in the all hadronic resolved topology in 170.0 GeV < $p_{T}^{t,2}$ < 290.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ at parton level in the all hadronic resolved topology in 290.0 GeV < $p_{T}^{t,2}$ < 450.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ at parton level in the all hadronic resolved topology in 450.0 GeV < $p_{T}^{t,2}$ < 1000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 0.0 GeV < $p_{T}^{t,2}$ < 170.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 0.0 GeV < $p_{T}^{t,2}$ < 170.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 170.0 GeV < $p_{T}^{t,2}$ < 290.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 0.0 GeV < $p_{T}^{t,2}$ < 170.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 170.0 GeV < $p_{T}^{t,2}$ < 290.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 170.0 GeV < $p_{T}^{t,2}$ < 290.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 290.0 GeV < $p_{T}^{t,2}$ < 450.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 0.0 GeV < $p_{T}^{t,2}$ < 170.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 290.0 GeV < $p_{T}^{t,2}$ < 450.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 170.0 GeV < $p_{T}^{t,2}$ < 290.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 290.0 GeV < $p_{T}^{t,2}$ < 450.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 290.0 GeV < $p_{T}^{t,2}$ < 450.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 450.0 GeV < $p_{T}^{t,2}$ < 1000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 0.0 GeV < $p_{T}^{t,2}$ < 170.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 450.0 GeV < $p_{T}^{t,2}$ < 1000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 170.0 GeV < $p_{T}^{t,2}$ < 290.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 450.0 GeV < $p_{T}^{t,2}$ < 1000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 290.0 GeV < $p_{T}^{t,2}$ < 450.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 450.0 GeV < $p_{T}^{t,2}$ < 1000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 450.0 GeV < $p_{T}^{t,2}$ < 1000.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.