"Table 649" 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 0.9 < $|{y}^{t\bar{t}}|$ < 2, 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 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.

两组粒子级（particle level）归一化微分截面（normalized differential cross-section）之间的协方差矩阵（covariance matrix），第一组截面的观测变量为|y^{tar{t}}|⊗m^{tar{t}}⊗p_{T}^{t,1}，运动学区间为0.9 < |y^{tar{t}}| < 2、1.2 太电子伏特（TeV） < m^{tar{t}} < 1.5 太电子伏特（TeV）；第二组截面的观测变量同样为|y^{tar{t}}|⊗m^{tar{t}}⊗p_{T}^{t,1}，运动学区间为0.9 < |y^{tar{t}}| < 2、1.5 太电子伏特（TeV） < m^{tar{t}} < 4 太电子伏特（TeV）。