"Table 637" of "Differential $t\bar{t}$ cross-section measurements using boosted top quarks in the all-hadronic final state with 139 fb$^{-1}$ of ATLAS data"

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.

两组粒子层面归一化微分截面之间的协方差矩阵：第一组截面以$|y^{t\bar{t}}|otimes m^{t\bar{t}}otimes p_{T}^{t,1}$为联合变量，对应的运动学区间为$0.3 < |y^{t\bar{t}}| < 0.9$且$1.2\ ext{TeV} < m^{t\bar{t}} < 1.5\ ext{TeV}$；第二组截面同样以$|y^{t\bar{t}}|otimes m^{t\bar{t}}otimes p_{T}^{t,1}$为联合变量，对应的运动学区间为$0.3 < |y^{t\bar{t}}| < 0.9$且$1.5\ ext{TeV} < m^{t\bar{t}} < 4\ ext{TeV}$。