Distributions of reconstructed VLQ mass for expected postfit background (blue histogram), signal plus background (colored lines), and observed data (black points) for events in the hadronic 5-jet bHbH channel.

Distributions of reconstructed VLQ mass for expected postfit background (blue histogram), signal plus background (colored lines), and observed data (black points) for events in the hadronic 5-jet bHbZ channel.

Distributions of reconstructed VLQ mass for expected postfit background (blue histogram), signal plus background (colored lines), and observed data (black points) for events in the hadronic 5-jet bZbZ channel.

Distributions of reconstructed VLQ mass for expected postfit background (blue histogram), signal plus background (colored lines), and observed data (black points) for events in the hadronic 5-jet bHtW channel.

Distributions of reconstructed VLQ mass for expected postfit background (blue histogram), signal plus background (colored lines), and observed data (black points) for events in the hadronic 5-jet bZtW channel.

Distributions of reconstructed VLQ mass for expected postfit background (blue histogram), signal plus background (colored lines), and observed data (black points) for events in the hadronic 6-jet bHbH channel.

Distributions of reconstructed VLQ mass for expected postfit background (blue histogram), signal plus background (colored lines), and observed data (black points) for events in the hadronic 6-jet bHbZ channel.

Distributions of reconstructed VLQ mass for expected postfit background (blue histogram), signal plus background (colored lines), and observed data (black points) for events in the hadronic 6-jet bZbZ channel.

Distributions of reconstructed VLQ mass for expected postfit background (blue histogram), signal plus background (colored lines), and observed data (black points) for events in the hadronic 6-jet bHtW channel.

Distributions of reconstructed VLQ mass for expected postfit background (blue histogram), signal plus background (colored lines), and observed data (black points) for events in the hadronic 6-jet bZtW channel.

Distributions of reconstructed VLQ mass for expected postfit background (blue histogram), signal plus background (colored lines), and observed data (black points) for events in the semileptonic 3-jet bHbZ channel.

Distributions of reconstructed VLQ mass for expected postfit background (blue histogram), signal plus background (colored lines), and observed data (black points) for events in the semileptonic 3-jet bZbZ channel.

Distributions of reconstructed VLQ mass for expected postfit background (blue histogram), signal plus background (colored lines), and observed data (black points) for events in the semileptonic 4-jet bHbZ channel.

Distributions of reconstructed VLQ mass for expected postfit background (blue histogram), signal plus background (colored lines), and observed data (black points) for events in the semileptonic 4-jet bZbZ channel.

The limit at 95% CL on the cross section for VLQ pair production for the branching fraction hypothesis 0% $\mathcal{B}(B \to bH)$, 100% $\mathcal{B}(B \to bH)$, and 0% $\mathcal{B}(B \to bH)$

The limit at 95% CL on the cross section for VLQ pair production for the branching fraction hypothesis 25% $\mathcal{B}(B \to bH)$, 25% $\mathcal{B}(B \to bH)$, and 50% $\mathcal{B}(B \to bH)$

The limit at 95% CL on the cross section for VLQ pair production for the branching fraction hypothesis 50% $\mathcal{B}(B \to bH)$, 50% $\mathcal{B}(B \to bH)$, and 0% $\mathcal{B}(B \to bH)$

The limit at 95% CL on the cross section for VLQ pair production for the branching fraction hypothesis 100% $\mathcal{B}(B \to bH)$, 0% $\mathcal{B}(B \to bH)$, and 0% $\mathcal{B}(B \to bH)$

Median expected exclusion limits on the VLQ mass at 95% CL as a function of the branching fractions $\mathcal{B}(B \to bH)$ and $\mathcal{B}(B \to tW)$, with $\mathcal{B}(B \to tW) = 1 - \mathcal{B}(B \to bH) - \mathcal{B}(B \to bZ)$. The grey area corresponds to the region where the exclusion limit is less than 1000 GeV.

Median observed exclusion limits on the VLQ mass at 95% CL as a function of the branching fractions $\mathcal{B}(B \to bH)$ and $\mathcal{B}(B \to tW)$, with $\mathcal{B}(B \to tW) = 1 - \mathcal{B}(B \to bH) - \mathcal{B}(B \to bZ)$. The grey area corresponds to the region where the exclusion limit is less than 1000 GeV.

Observed upper limits at 95% CL on B($\text{H} \rightarrow \text{a}_{1}\text{a}_{1}$) in percent, obtained from the combination of the $\mu\mu$bb and $\tau\tau$bb channels. The results are obtained as functions of $m_{\text{a}_{1}}$ for 2HDM+S Type I (independent of tan$\beta$), Type II (tan$\beta$=2.0), Type III (tan$\beta$=2.0), and Type IV (tan$\beta$=0.6), respectively.

Postfit distributions of $S_\mathrm{T}^\mathrm{MET}$ in the $\mathrm{e}\mu$ channel of the $\geq$1b category for the combined 2016-2018 data set after a simultaneous fit of the background and vector LQ signal to the data. The number of events in each bin are divided by the respective bin width. The last bin includes the overflow.

Postfit distributions of $S_\mathrm{T}^\mathrm{MET}$ in the $\ell\tau_\mathrm{h}$ channel of the 0b category for the combined 2016-2018 data set after a simultaneous fit of the background and vector LQ signal to the data. The number of events in each bin are divided by the respective bin width. The last bin includes the overflow.

Postfit distributions of $S_\mathrm{T}^\mathrm{MET}$ in the $\ell\tau_\mathrm{h}$ channel of the $\geq$1b category for the combined 2016-2018 data set after a simultaneous fit of the background and vector LQ signal to the data. The number of events in each bin are divided by the respective bin width. The last bin includes the overflow.

Postfit distributions of $S_\mathrm{T}^\mathrm{MET}$ in the $\tau_\mathrm{h}\tau_\mathrm{h}$ channel of the 0b category for the combined 2016-2018 data set after a simultaneous fit of the background and vector LQ signal to the data. The number of events in each bin are divided by the respective bin width. The last bin includes the overflow.

Postfit distributions of $S_\mathrm{T}^\mathrm{MET}$ in the $\tau_\mathrm{h}\tau_\mathrm{h}$ channel of the $\geq$1b category for the combined 2016-2018 data set after a simultaneous fit of the background and vector LQ signal to the data. The number of events in each bin are divided by the respective bin width. The last bin includes the overflow.

Postfit distributions of $\chi$ in the $\mathrm{e}\mu$ channel of the 0j, $400 < m_\mathrm{vis} < 600\,\mathrm{GeV}$ category for the combined 2016-2018 data set after a simultaneous fit of the background and vector LQ signal to the data. The number of events in each bin are divided by the respective bin width.

Postfit distributions of $\chi$ in the $\mathrm{e}\mu$ channel of the 0j, $m_\mathrm{vis} > 600\,\mathrm{GeV}$ category for the combined 2016-2018 data set after a simultaneous fit of the background and vector LQ signal to the data. The number of events in each bin are divided by the respective bin width.

Postfit distributions of $\chi$ in the $\ell\tau_\mathrm{h}$ channel of the 0j, $400 < m_\mathrm{vis} < 600\,\mathrm{GeV}$ category for the combined 2016-2018 data set after a simultaneous fit of the background and vector LQ signal to the data. The number of events in each bin are divided by the respective bin width.

Postfit distributions of $\chi$ in the $\ell\tau_\mathrm{h}$ channel of the 0j, $m_\mathrm{vis} > 600\,\mathrm{GeV}$ category for the combined 2016-2018 data set after a simultaneous fit of the background and vector LQ signal to the data. The number of events in each bin are divided by the respective bin width.

Postfit distributions of $\chi$ in the $\tau_\mathrm{h}\tau_\mathrm{h}$ channel of the 0j, $400 < m_\mathrm{vis} < 600\,\mathrm{GeV}$ category for the combined 2016-2018 data set after a simultaneous fit of the background and vector LQ signal to the data. The number of events in each bin are divided by the respective bin width.

Postfit distributions of $\chi$ in the $\tau_\mathrm{h}\tau_\mathrm{h}$ channel of the 0j, $m_\mathrm{vis} > 600\,\mathrm{GeV}$ category for the combined 2016-2018 data set after a simultaneous fit of the background and vector LQ signal to the data. The number of events in each bin are divided by the respective bin width.

Exclusion limits on the total cross section of a scalar LQ as a function of LQ mass under the assumption of exclusive LQ couplings to b quarks and $\tau$ leptons.

Exclusion limits on the total cross section of a vector LQ as a function of LQ mass under the assumption of exclusive LQ couplings to b quarks and $\tau$ leptons.

Exclusion limits on the mass of a scalar LQ as a function of the coupling strength $\lambda$ under the assumption of exclusive LQ couplings to b quarks and $\tau$ leptons.

Exclusion limits on the mass of a vector LQ as a function of the coupling strength $\lambda$ under the assumption of exclusive LQ couplings to b quarks and $\tau$ leptons.

Exclusion limits on the coupling strength $\lambda$ of a scalar LQ as a function of the LQ mass under the assumption of exclusive LQ couplings to b quarks and $\tau$ leptons.

Exclusion limits on the coupling strength $\lambda$ of a vector LQ as a function of the LQ mass under the assumption of exclusive LQ couplings to b quarks and $\tau$ leptons.

Measured min-$d_{xy}$ distribution in the 2-match category, after requiring the $d_{xy}$ muon to pass the isolation requirement $I_{\mathrm{rel}}^{\mathrm{PF}} <0.25$ (i. e., the B and D bins of the ABCD plane). Overlaid with a red histogram is the background predicted from the region of the ABCD plane failing the same requirement (the A and C bins), as well as three signal benchmark hypotheses (as defined in the legends), assuming $\alpha_D = \alpha_{\mathrm{EM}}$ (the fine-structure constant). The red hatched bands correspond to the background prediction uncertainty. The last bin includes the overflow.

Two-dimensional exclusion surfaces for $\Delta = 0.1 \, m_1$ as a function of the DM mass $m_1$ and the signal strength $y$, with $m_{A'} = 3 \, m_1$. Filled histograms denote observed limits on $\sigma(\mathrm{pp} \to A' \to \chi_2 \chi_1) \, \mathcal{B}(\chi_2 \to \chi_1 \mu^+ \mu^-)$. Solid (dashed) curves denote the observed (expected) exclusion limits at 95% CL, with 68% CL uncertainty bands around the expectation. Regions above the curves are excluded, depending on the $\alpha_D$ hypothesis: $\alpha_{\mathrm{D}} = \alpha_{\mathrm{EM}}$ (dark blue) or 0.1 (light magenta).

Two-dimensional exclusion surfaces for $\Delta = 0.4 \, m_1$ as a function of the DM mass $m_1$ and the signal strength $y$, with $m_{A'} = 3 \, m_1$. Filled histograms denote observed limits on $\sigma(\mathrm{pp} \to A' \to \chi_2 \chi_1) \, \mathcal{B}(\chi_2 \to \chi_1 \mu^+ \mu^-)$. Solid (dashed) curves denote the observed (expected) exclusion limits at 95% CL, with 68% CL uncertainty bands around the expectation. Regions above the curves are excluded, depending on the $\alpha_D$ hypothesis: $\alpha_{\mathrm{D}} = \alpha_{\mathrm{EM}}$ (dark blue) or 0.1 (light magenta).

The signal cross-sections values of the signal QBH RS1 with n=1 extra dimensions, as a function of threshold mass

The product of acceptance and selection efficiency for QBH ADD model, as a function of threshold mass of the signal.

The product of acceptance and selection efficiency for QBH RS1 models, as a function of threshold mass of the signal.

The product of acceptance and selection efficiency for q* signal, as a function of resonance mass

The product of acceptance and selection efficiency for b* signal, as a function of resonance mass of the signal.

Distributions of the γ+jet invariant mass generated from various signal samples for reconstructed mass 4 TeV

Fitting distribution of data with expected q*, and QBH signal events, and fit parameters p0= 3.05674e+00, p1 = 10.5343, p3 = 4.15163 and p4 = 0.107405

Fitting distribution of data with expected b* events, and fit parameters p0= 1.45055e+03, p1 = 2.04830e+01, p3 = -4.16760e-01 and p4 = -5.07768e-01

Fitting distribution of data with expected b* events for 0btag category, and fit parameters p0= 2.44120e+00, p1 = 1.08886e+01, p3 = 4.23198e+00 and p4 = 1.16300e-01

Exclusion limits on the product of cross section and branching fraction for q* signal coupling f = 1.0, as a function of the resonance mass hypothesis.

Theoretical cross-section of q* signal for coupling multiplier f =1.0

Exclusion limits on the product of cross section and branching fraction for the q* signal coupling f = 0.5, as a function of the resonance mass hypothesis.

Theoretical cross-section of q* signal for coupling multiplier f =0.5

Exclusion limits on the product of cross section and branching fraction for q* coupling f = 0.1, as a function of the resonance mass hypothesis.

Theoretical cross-section of q* signal for coupling multiplier f =0.1

Exclusion limits on the product of cross section and branching fraction for b* signal coupling f = 1.0, as a function of the resonance mass hypothesis.

Theoretical cross-section of b* signal for coupling multiplier f =1.0

Exclusion limits on the product of cross section and branching fraction for b* signal coupling f = 0.5, as a function of the resonance mass hypothesis.

Theoretical cross-section of b* signal for coupling multiplier f =0.5

Exclusion limits on the product of cross section and branching fraction for b* signal coupling f = 0.1, as a function of the resonance mass hypothesis.

Theoretical cross-section of b* signal for coupling multiplier f =0.1

Exclusion limits on the product of cross section and branching fraction for QBH ADD signal, as a function of the mass hypothesis.

Theoretical cross-section of ADD signal

Exclusion limits on the product of cross section and branching fraction for QBH RS1 signal, as a function of the mass hypothesis.

Theoretical cross-section of RS1 signal

The expected and observed exclusion mass limits for q* and b* signals, as a function coupling multiplier

The observed exclusion mass limits for b* signal, as a function of threshold mass of the signal.

The total coherent $\mathrm{J}/\psi$ photoproduction cross section as a function of photon-nuclear center-of-mass energy per nucleon $W_{\gamma \mathrm{N}}^{\mathrm{Pb}}$, measured in PbPb ultra-peripheral collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV. The $W_{\gamma \mathrm{N}}^{\mathrm{Pb}}$ values used correspond to the center of each rapidity range. The theoretical uncertainties is due to the uncertainties in the photon flux.

The nuclear gluon suppression factor $R_{\mathrm{g}}^{\mathrm{Pb}}$ as a function of Bjorken $x$ extracted from the CMS measurement of the coherent $\mathrm{J}/\psi$ photoproduction in PbPb ultra-peripheral collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV. The $x$ values are evaluated at the centers of their corresponding rapidity ranges. The theoretical uncertainties are due to the uncertainties in the photon flux and the impulse approximation model.

The nuclear gluon suppression factor $R_{\mathrm{g}}^{\mathrm{Pb}}$ as a function of Bjorken $x$ extracted from the CMS measurement of the coherent $\mathrm{J}/\psi$ photoproduction in PbPb ultra-peripheral collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV. The $x$ values are evaluated at the centers of their corresponding rapidity ranges. The theoretical uncertainties are due to the uncertainties in the photon flux and the impulse approximation model.

The total covariance matrix of the total coherent photoproduction cross section as a function of photon-nuclear center-of-mass energy per nucleon $W_{\gamma \mathrm{N}}^{\mathrm{Pb}}$. The covariance matrix includes both the experimental and theoretical (photon flux) uncertainties. The bins are ordered as increasing in $W_{\gamma \mathrm{N}}^{\mathrm{Pb}}$.

The photon flux values from STARLight as a function of rapidity, in different neutron multiplicity classes: 0n0n, 0nXn, and XnXn.

The experimental covariance matrix of the total coherent photoproduction cross section as a function of photon-nuclear center-of-mass energy per nucleon $W_{\gamma \mathrm{N}}^{\mathrm{Pb}}$. The bins are ordered as increasing in $W_{\gamma \mathrm{N}}^{\mathrm{Pb}}$.

The covariance matrix for the flux in the 0n0n neutron multiplicity class.

The theoretical (photon flux) covariance matrix of the total coherent photoproduction cross section as a function of photon-nuclear center-of-mass energy per nucleon $W_{\gamma \mathrm{N}}^{\mathrm{Pb}}$. The bins are ordered as increasing in $W_{\gamma \mathrm{N}}^{\mathrm{Pb}}$.

The covariance matrix for the flux in the 0nXn neutron multiplicity class.

The covariance matrix for the flux in the XnXn neutron multiplicity class.

The total covariance matrix of the total coherent photoproduction cross section as a function of photon-nuclear center-of-mass energy per nucleon $W_{\gamma \mathrm{N}}^{\mathrm{Pb}}$. The covariance matrix includes both the experimental and theoretical (photon flux) uncertainties. The bins are ordered as increasing in $W_{\gamma \mathrm{N}}^{\mathrm{Pb}}$.

The experimental covariance matrix of the total coherent photoproduction cross section as a function of photon-nuclear center-of-mass energy per nucleon $W_{\gamma \mathrm{N}}^{\mathrm{Pb}}$. The bins are ordered as increasing in $W_{\gamma \mathrm{N}}^{\mathrm{Pb}}$.

The theoretical (photon flux) covariance matrix of the total coherent photoproduction cross section as a function of photon-nuclear center-of-mass energy per nucleon $W_{\gamma \mathrm{N}}^{\mathrm{Pb}}$. The bins are ordered as increasing in $W_{\gamma \mathrm{N}}^{\mathrm{Pb}}$.

Observed and expected 95% CL upper limits on the product of the production cross section ($\sigma$) and the branching fraction, obtained after combining all categories with 138 $\mathrm{fb}^{−1}$ of data at $\sqrt{s}$ = 13 TeV for $\mathrm{V'}$ to $VV$ + $VH$ signal in HVT model C.

Total signal efficiency including all event categories as a function of the resonance mass $M_X$ for all DY/ggF signal models under consideration. The estimates from MC simulation (markers) are interpolated with a functional form (lines).

Total signal efficiency including all event categories as a function of the resonance mass $M_X$ for all VBF signal models under consideration. The estimates from MC simulation (markers) are interpolated with a functional form (lines).

Distribution of the MLP W+jets score in the CRs for the $T\overline{T}$ search. The observed data, predicted $T\overline{T}$ signal with mass of 1.2 (1.5) TeV in the singlet scenario, and the background are all shown. Statistical and systematic uncertainties in the background prediction before performing the fit to data are also shown.

Distribution of DeepAK8 jet tags in the DeepAK8 CR of the $T\overline{T}$ search. The observed data are shown using black markers, $T\overline{T}$ signals using solid lines, and background using filled histograms. Statistical and systematic uncertainties in the background prediction before performing the fit to data are shown by the hatched region.

Distribution of HT in the W+jets CR of the $T\overline{T}$ search. The observed data are shown using black markers, $T\overline{T}$ signals using solid lines, and background using filled histograms. Statistical and systematic uncertainties in the background prediction before performing the fit to data are shown by the hatched region.

Distribution of HT in the $T\overline{T}$ CR of the $T\overline{T}$ search. The observed data are shown using black markers, $T\overline{T}$ signals using solid lines, and background using filled histograms. Statistical and systematic uncertainties in the background prediction before performing the fit to data are shown by the hatched region.

Numbers of predicted and observed CR events in 2016--2018 data for the $T\overline{T}$ signal hypotheses in the single-lepton channel, after a background-only fit to data. Predicted numbers of signal events before the fit to data are included for comparison, using the singlet branching fraction scenario. Uncertainties include statistical and systematic components, and lepton flavor categories are combined with their uncertainties added in quadrature. Values in the DeepAK8 CR represent the number of large-radius jets rather than number of events.

Numbers of predicted and observed CR events in 2016--2018 data for the $B\overline{B}$ signal hypotheses in the single-lepton channel, after a background-only fit to data. Predicted numbers of signal events before the fit to data are included for comparison, using the singlet branching fraction scenario. Uncertainties include statistical and systematic components, and lepton flavor categories are combined with their uncertainties added in quadrature. Values in the DeepAK8 CR represent the number of large-radius jets rather than number of events.

Numbers of predicted and observed CR events in 2017--2018 data in the same-sign dilepton channel, after a background-only fit to data. Predicted numbers of signal events before the fit to data are included for comparison, using the singlet branching fraction scenario. Uncertainties include statistical and systematic components. Predictions for 2017 and 2018 are combined with their uncertainties added in quadrature.

Distribution of lepton $p_T$ in 2017 in the multilepton channel nonprompt lepton control region for all flavor categories, evaluated with the best-fit nonprompt rates. The uncertainty shown is the quadratic sum of statistical and systematics uncertainties.

Distribution of lepton $p_T$ in 2018 in the multilepton channel nonprompt lepton control region for all flavor categories, evaluated with the best-fit nonprompt rates. The uncertainty shown is the quadratic sum of statistical and systematics uncertainties.

Numbers of predicted and observed CR events in 2017--2018 data in the multilepton channel, after a background-only fit to data. Predicted numbers of signal events before the fit to data are included for comparison, using the singlet branching fraction scenario. Uncertainties include statistical and systematic components. Predictions for 2017 and 2018 are combined with their uncertainties added in quadrature.

Numbers of predicted and observed $T\overline{T}$ SR events in 2016--2018 data in the single-lepton channel, after a background-only fit to data. Predicted numbers of signal events before the fit to data are included for comparison, using the singlet branching fraction scenario. Uncertainties include statistical and systematic components, and lepton flavor categories are combined with their uncertainties added in quadrature.

Distribution of the VLQ score in single-lepton category 1. Observed data is shown using black markers, $T\overline{T}$ signal with mass of 1.2 (1.5) TeV in the singlet scenario using solid (dashed) lines, and post-fit background using filled histograms. Statistical and systematic uncertainties in the background prediction after performing the fit to data are shown by the hatched region. Electron and muon categories have been combined with their uncertainties added in quadrature.

Distribution of the VLQ score in single-lepton category 2. Observed data is shown using black markers, $T\overline{T}$ signal with mass of 1.2 (1.5) TeV in the singlet scenario using solid (dashed) lines, and post-fit background using filled histograms. Statistical and systematic uncertainties in the background prediction after performing the fit to data are shown by the hatched region. Electron and muon categories have been combined with their uncertainties added in quadrature.

Distribution of the VLQ score in single-lepton category 3. Observed data is shown using black markers, $T\overline{T}$ signal with mass of 1.2 (1.5) TeV in the singlet scenario using solid (dashed) lines, and post-fit background using filled histograms. Statistical and systematic uncertainties in the background prediction after performing the fit to data are shown by the hatched region. Electron and muon categories have been combined with their uncertainties added in quadrature.

Distribution of the VLQ score in single-lepton category 4. Observed data is shown using black markers, $T\overline{T}$ signal with mass of 1.2 (1.5) TeV in the singlet scenario using solid (dashed) lines, and post-fit background using filled histograms. Statistical and systematic uncertainties in the background prediction after performing the fit to data are shown by the hatched region. Electron and muon categories have been combined with their uncertainties added in quadrature.

Distribution of the VLQ score in single-lepton category 5. Observed data is shown using black markers, $T\overline{T}$ signal with mass of 1.2 (1.5) TeV in the singlet scenario using solid (dashed) lines, and post-fit background using filled histograms. Statistical and systematic uncertainties in the background prediction after performing the fit to data are shown by the hatched region. Electron and muon categories have been combined with their uncertainties added in quadrature.

Distribution of the VLQ score in single-lepton category 6. Observed data is shown using black markers, $T\overline{T}$ signal with mass of 1.2 (1.5) TeV in the singlet scenario using solid (dashed) lines, and post-fit background using filled histograms. Statistical and systematic uncertainties in the background prediction after performing the fit to data are shown by the hatched region. Electron and muon categories have been combined with their uncertainties added in quadrature.

Distribution of the VLQ score in single-lepton category 7. Observed data is shown using black markers, $T\overline{T}$ signal with mass of 1.2 (1.5) TeV in the singlet scenario using solid (dashed) lines, and post-fit background using filled histograms. Statistical and systematic uncertainties in the background prediction after performing the fit to data are shown by the hatched region. Electron and muon categories have been combined with their uncertainties added in quadrature.

Distribution of the VLQ score in single-lepton category 8. Observed data is shown using black markers, $T\overline{T}$ signal with mass of 1.2 (1.5) TeV in the singlet scenario using solid (dashed) lines, and post-fit background using filled histograms. Statistical and systematic uncertainties in the background prediction after performing the fit to data are shown by the hatched region. Electron and muon categories have been combined with their uncertainties added in quadrature.

Distribution of the VLQ score in single-lepton category 9. Observed data is shown using black markers, $T\overline{T}$ signal with mass of 1.2 (1.5) TeV in the singlet scenario using solid (dashed) lines, and post-fit background using filled histograms. Statistical and systematic uncertainties in the background prediction after performing the fit to data are shown by the hatched region. Electron and muon categories have been combined with their uncertainties added in quadrature.

Distribution of the VLQ score in single-lepton category 10. Observed data is shown using black markers, $T\overline{T}$ signal with mass of 1.2 (1.5) TeV in the singlet scenario using solid (dashed) lines, and post-fit background using filled histograms. Statistical and systematic uncertainties in the background prediction after performing the fit to data are shown by the hatched region. Electron and muon categories have been combined with their uncertainties added in quadrature.

Distribution of the VLQ score in single-lepton category 11. Observed data is shown using black markers, $T\overline{T}$ signal with mass of 1.2 (1.5) TeV in the singlet scenario using solid (dashed) lines, and post-fit background using filled histograms. Statistical and systematic uncertainties in the background prediction after performing the fit to data are shown by the hatched region. Electron and muon categories have been combined with their uncertainties added in quadrature.

Distribution of the VLQ score in single-lepton category 12. Observed data is shown using black markers, $T\overline{T}$ signal with mass of 1.2 (1.5) TeV in the singlet scenario using solid (dashed) lines, and post-fit background using filled histograms. Statistical and systematic uncertainties in the background prediction after performing the fit to data are shown by the hatched region. Electron and muon categories have been combined with their uncertainties added in quadrature.

Distribution of $H_T^{\mathrm{lep}}$ in the same-sign dilepton signal region for $ee$ category. Data from 2017 and 2018 is shown using black markers, $T\overline{T}$ signals with mass of 1.2 (1.5) TeV in the singlet scenario using solid (dashed) lines, and post-fit background using filled histograms. Statistical and systematic uncertainties in the background prediction after performing the fit to data are shown by the hatched region.

Distribution of $H_T^{\mathrm{lep}}$ in the same-sign dilepton signal region for $e\mu$ category. Data from 2017 and 2018 is shown using black markers, $T\overline{T}$ signals with mass of 1.2 (1.5) TeV in the singlet scenario using solid (dashed) lines, and post-fit background using filled histograms. Statistical and systematic uncertainties in the background prediction after performing the fit to data are shown by the hatched region.

Distribution of $H_T^{\mathrm{lep}}$ in the same-sign dilepton signal region for $\mu\mu$ category. Data from 2017 and 2018 is shown using black markers, $T\overline{T}$ signals with mass of 1.2 (1.5) TeV in the singlet scenario using solid (dashed) lines, and post-fit background using filled histograms. Statistical and systematic uncertainties in the background prediction after performing the fit to data are shown by the hatched region.

Distribution of $S_T$ in the multilepton signal region for $eee$ category. Data from 2017 and 2018 is shown using black markers, $T\overline{T}$ signals with mass of 1.2 (1.5) TeV in the singlet scenario using solid (dashed) lines, and post-fit background using filled histograms. Statistical and systematic uncertainties in the background prediction after performing the fit to data are shown by the hatched region.

Distribution of $S_T$ in the multilepton signal region for $ee\mu$ category. Data from 2017 and 2018 is shown using black markers, $T\overline{T}$ signals with mass of 1.2 (1.5) TeV in the singlet scenario using solid (dashed) lines, and post-fit background using filled histograms. Statistical and systematic uncertainties in the background prediction after performing the fit to data are shown by the hatched region.

Distribution of $S_T$ in the multilepton signal region for $e\mu\mu$ category. Data from 2017 and 2018 is shown using black markers, $T\overline{T}$ signals with mass of 1.2 (1.5) TeV in the singlet scenario using solid (dashed) lines, and post-fit background using filled histograms. Statistical and systematic uncertainties in the background prediction after performing the fit to data are shown by the hatched region.

Distribution of $S_T$ in the multilepton signal region for $\mu\mu\mu$ category. Data from 2017 and 2018 is shown using black markers, $T\overline{T}$ signals with mass of 1.2 (1.5) TeV in the singlet scenario using solid (dashed) lines, and post-fit background using filled histograms. Statistical and systematic uncertainties in the background prediction after performing the fit to data are shown by the hatched region.

Numbers of predicted and observed $B\overline{B}$ SR events in 2016--2018 data in the single-lepton channel, after a background-only fit to data. Predicted numbers of signal events before the fit to data are included for comparison, using the singlet branching fraction scenario. Uncertainties include statistical and systematic components, and lepton flavor categories are combined with their uncertainties added in quadrature.

Numbers of predicted and observed SR events in 2017--2018 data in the same-sign dilepton channel, after a background-only fit to data. Predicted numbers of signal events before the fit to data are included for comparison, using the singlet branching fraction scenario. Uncertainties include statistical and systematic components. Predictions for 2017 and 2018 are combined with their uncertainties added in quadrature.

Numbers of predicted and observed SR events in 2017--2018 data in the multilepton channel, after a background-only fit to data. Predicted numbers of signal events before the fit to data are included for comparison, using the singlet branching fraction scenario. Uncertainties include statistical and systematic components. Predictions for 2017 and 2018 are combined with their uncertainties added in quadrature.

Expected and observed lower limits on the VLT quark masses.

Expected and observed lower limits on the VLB quark masses.

Expected 95% CL upper limits on $T\overline{T}$ production cross sections for the singlet combination.

Expected 95% CL upper limits on $T\overline{T}$ production cross sections for the doublet combination.

Expected 95% CL upper limits on $B\overline{B}$ production cross sections for the singlet combination.

Expected 95% CL upper limits on $B\overline{B}$ production cross sections for the doublet combination.

The 95% CL expected lower mass limits on pair-produced T quark masses as functions of their branching ratios to W and H bosons.

The 95% CL observed lower mass limits on pair-produced T quark masses as functions of their branching ratios to W and H bosons.

The 95% CL expected lower mass limits on pair-produced B quark masses as functions of their branching ratios to W and H bosons.

The 95% CL observed lower mass limits on pair-produced B quark masses as functions of their branching ratios to W and H bosons.

Distribution of an input to the BDT classifier in the $3\ell$ category: The linear discrimminant $p_{T}^{miss,LD}$. The discriminant is defined by the relation $p_{T}^{miss,LD} = 0.6 p_{T}^{miss} + 0.4 H_{T}^{miss}$, where $H_{T}^{miss}$ corresponds to the magnitude of the vector $p_{T}$ sum of all electrons, muons, taus and small radius jets passing the selection critertia, and $p_{T}^{miss}$ represents the missing transverse momentum vector computed as the negative vector $p_{T}$ sum of all the particles reconstructed by the PF algorithm in the event.

Distributions of the transverse mass $m_{T}$ of the lepton that is not originating from the Z boson decay and the missing transverse momentum in the $3\ell$/WZ control region. The distributions expected for the WZ and ZZ as well as for other background processes are shown for the values of nuisance parameters obtained from the ML fit used in the signal extraction.

Distributions of the four lepton invariant mass $m_{4\ell}$ in the $4\ell$/ZZ control region. The distributions expected for the ZZ as well as for other background processes are shown for the values of nuisance parameters obtained from the ML fit used in the signal extraction.

Distributions of the transverse mass $m_{T}$ of the leading lepton and the missing transverse momentum in the $2\ell$(ss) control region. The distributions expected for the misidentified $\ell$ background as well as for other background processes is shown for the values of nuisance parameters obtained from the background-only ML fit, in which the HH signal is constrained to be zero.

Distributions of the reconstructed HH mass $m_{HH}$ in the $2\ell+2 au_{h}$ control region. The distributions expected for the misidentified $\ell/ au_{h}$ background as well as for other background processes is shown for the values of nuisance parameters obtained from the background-only ML fit, in which the HH signal is constrained to be zero.

Distribution in the output of the BDT trained for nonresonant HH production and evaluated for the benchmark scenario JHEP04 BM7 for the $2\ell$(ss) category. The SM HH signal is shown for a cross section amounting to $30$ times the value predicted in the SM. The distributions expected for the background processes are shown for the values of nuisance parameters obtained from the ML fit of the signal+background hypothesis to the data. The binning is chosen to approximate signal quantiles.

Distribution in the output of the BDT trained for nonresonant HH production and evaluated for the benchmark scenario JHEP04 BM7 for the $3\ell$ category. The SM HH signal is shown for a cross section amounting to $30$ times the value predicted in the SM. The distributions expected for the background processes are shown for the values of nuisance parameters obtained from the ML fit of the signal+background hypothesis to the data. The binning is chosen to approximate signal quantiles.

Distribution in the output of the BDT trained for nonresonant HH production and evaluated for the benchmark scenario JHEP04 BM7 for the $4\ell$ category. The SM HH signal is shown for a cross section amounting to $30$ times the value predicted in the SM. The distributions expected for the background processes are shown for the values of nuisance parameters obtained from the ML fit of the signal+background hypothesis to the data. The binning is chosen to approximate signal quantiles.

Distribution in the output of the BDT trained for nonresonant HH production and evaluated for the benchmark scenario JHEP04 BM7 for the $3\ell+1 au_{h}$ category. The SM HH signal is shown for a cross section amounting to $30$ times the value predicted in the SM. The distributions expected for the background processes are shown for the values of nuisance parameters obtained from the ML fit of the signal+background hypothesis to the data. The binning is chosen to approximate background quantiles.

Distribution in the output of the BDT trained for nonresonant HH production and evaluated for the benchmark scenario JHEP04 BM7 for the $2\ell+2 au_{h}$ category. The SM HH signal is shown for a cross section amounting to $30$ times the value predicted in the SM. The distributions expected for the background processes are shown for the values of nuisance parameters obtained from the ML fit of the signal+background hypothesis to the data. The binning is chosen to approximate background quantiles.

Distribution in the output of the BDT trained for nonresonant HH production and evaluated for the benchmark scenario JHEP04 BM7 for the $1\ell+3 au_{h}$ category. The SM HH signal is shown for a cross section amounting to $30$ times the value predicted in the SM. The distributions expected for the background processes are shown for the values of nuisance parameters obtained from the ML fit of the signal+background hypothesis to the data. The binning is chosen to approximate background quantiles.

Distribution in the output of the BDT trained for nonresonant HH production and evaluated for the benchmark scenario JHEP04 BM7 for the $4 au_{h}$ category. The SM HH signal is shown for a cross section amounting to $30$ times the value predicted in the SM. The distributions expected for the background processes are shown for the values of nuisance parameters obtained from the ML fit of the signal+background hypothesis to the data. The binning is chosen to approximate background quantiles.

Observed and expected $95\%$ CL upper limits on the SM HH production cross section, obtained for both individual search categories and from a simultaneous fit of all seven categories combined.

Observed and expected $95\%$ CL upper limits on the HH production cross section as a function of the Higgs boson self-coupling strength modifier $\kappa_\lambda$ for the combination of all seven categories. All Higgs boson couplings other than $\lambda$ are assumed to have the values predicted in the SM.

Observed and expected $95\%$ CL upper limits on the HH production cross section as a function of the Higgs boson self-coupling strength modifier $\kappa_\lambda$ for the seven different categories as well as their combination. All Higgs boson couplings other than $\lambda$ are assumed to have the values predicted in the SM.

Observed and expected $95\%$ CL upper limits on the HH production cross section for the twelve benchmark scenarios from doi:10.1007/JHEP04(2016)126, the additional benchmark scenario 8a from doi:10.1007/JHEP09(2018)057, the seven benchmark scenarios from doi:10.1007/JHEP03(2020)091, and for the SM.

Observed and expected $95\%$ CL upper limits on the HH production cross section for the twelve benchmark scenarios from doi:10.1007/JHEP04(2016)126, the additional benchmark scenario 8a from doi:10.1007/JHEP09(2018)057, the seven benchmark scenarios from doi:10.1007/JHEP03(2020)091, and for the SM. The limits are shown for all seven search categories as well as for their combination.

Observed and expected $95\%$ CL upper limits on the HH production cross section as a function of the effective coupling $c_{2}$ for the combination of all seven categories. All Higgs boson couplings other than $c_{2}$ are assumed to have the values predicted in the SM.

Observed and expected $95\%$ CL upper limits on the HH production cross section as a function of the effective coupling $c_{2}$ and the top Yukawa coupling modifier $\kappa_{t}$ for the combination of all seven categories. All Higgs boson couplings other than $c_{2}$ and $\kappa_{t}$ are assumed to have the values predicted in the SM. The position of the SM in the ($c_{2}-\kappa_{t}$) plane, as well as the best fit value of $(c_{2},\kappa_{t})=(1.05, 1.74)$ together with contours for the theory cross section are shown as well.

Observed and expected $95\%$ CL upper limits on the HH production cross section as a function of the Higgs boson self-coupling modifier $\kappa_{\lambda}$ and the top Yukawa coupling modifier $\kappa_{t}$ for the combination of all seven categories. All Higgs boson couplings other than $\kappa_{\lambda}$ and $\kappa_{t}$ are assumed to have the values predicted in the SM. The position of the SM in the ($\kappa_{\lambda}-\kappa_{t}$) plane, as well as the best fit value of $(\kappa_{\lambda},\kappa_{t})=(-3.54, -1.70)$ together with contours for the theory cross section are shown as well.

Observed and expected $95\%$ CL upper limits on the HH production cross section as a function of the effective coupling $c_{2}$ and the Higgs boson self-coupling modifier $\kappa_{\lambda}$ for the combination of all seven categories. All Higgs boson couplings other than $c_{2}$ and $\kappa_{\lambda}$ are assumed to have the values predicted in the SM. The position of the SM in the ($c_{2}-\kappa_{\lambda}$) plane, as well as the best fit value of $(c_{2},\kappa_{\lambda})=(-0.66, 5.33)$ together with contours for the theory cross section are shown as well.

Observed and expected $95\%$ CL upper limits on the production of new particles X of spin $0$ and mass $m_{X}$ in the range $250$-$1000$ GeV, which decay to Higgs boson pairs.

Observed and expected $95\%$ CL upper limits on the production of new particles X of spin $0$ and mass $m_{X}$ in the range $250$-$1000$ GeV, which decay to Higgs boson pairs. The Limit is shown for the seven different search categories as well as their combination.

Observed and expected $95\%$ CL upper limits on the production of new particles X of spin $2$ and mass $m_{X}$ in the range $250$-$1000$ GeV, which decay to Higgs boson pairs.

Observed and expected $95\%$ CL upper limits on the production of new particles X of spin $2$ and mass $m_{X}$ in the range $250$-$1000$ GeV, which decay to Higgs boson pairs. The Limit is shown for the seven different search categories as well as their combination.

Distribution in the output of the BDT trained for resonances of spin 2 and mass $750\,$GeV production for the $2\ell$(ss) category. The resonant HH signal is shown for a cross section amounting to $1\,$pb. The distributions expected for the background processes are shown for the values of nuisance parameters obtained from the ML fit of the signal+background hypothesis to the data. The binning is chosen to approximate signal quantiles.

Distribution in the output of the BDT trained for resonances of spin 2 and mass $750\,$GeV production for the $3\ell$ category. The resonant HH signal is shown for a cross section amounting to $1\,$pb. The distributions expected for the background processes are shown for the values of nuisance parameters obtained from the ML fit of the signal+background hypothesis to the data. The binning is chosen to approximate signal quantiles.

$|y^{t}|$ 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.

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

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized 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.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized 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.

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

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized 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.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized 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.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized 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.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized 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.

$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized 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.

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

$p_{T}^{t}$ covariance matrix for the absolute differential cross-section at particle level.

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level for 0.55 TeV < $p_{T}^{t,1}$ < 0.6 TeV.

Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level for 0.6 TeV < $p_{T}^{t,1}$ < 0.75 TeV.

Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.

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

Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level for 0.55 TeV < $p_{T}^{t,1}$ < 0.6 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level for 0.6 TeV < $p_{T}^{t,1}$ < 0.75 TeV.

Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level for 0.55 TeV < $p_{T}^{t,1}$ < 0.6 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.

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

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

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

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

Covariance matrix between the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at particle level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at particle level for 0.2 < $|{y}^{t,1}|$ < 0.5.

Covariance matrix between the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at particle level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at particle level for 0.5 < $|{y}^{t,1}|$ < 1.

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

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

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

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

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

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

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

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

Covariance matrix between the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.2 < $|{y}^{t,1}|$ < 0.5.

Covariance matrix between the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.5 < $|{y}^{t,1}|$ < 1.

Covariance matrix between the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 1 < $|{y}^{t,1}|$ < 2.

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

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

Covariance matrix between the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.2 < $|{y}^{t,1}|$ < 0.5 and the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 1 < $|{y}^{t,1}|$ < 2.

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

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

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

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

Covariance matrix between the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level for 0 < $|{y}^{t,2}|$ < 0.2 and the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level for 0.2 < $|{y}^{t,2}|$ < 0.5.

Covariance matrix between the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level for 0 < $|{y}^{t,2}|$ < 0.2 and the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level for 0.5 < $|{y}^{t,2}|$ < 1.

Covariance matrix between the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level for 0 < $|{y}^{t,2}|$ < 0.2 and the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level for 1 < $|{y}^{t,2}|$ < 2.

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

Covariance matrix between the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level for 0.2 < $|{y}^{t,2}|$ < 0.5 and the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level for 0.5 < $|{y}^{t,2}|$ < 1.

Covariance matrix between the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level for 0.2 < $|{y}^{t,2}|$ < 0.5 and the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level for 1 < $|{y}^{t,2}|$ < 2.

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

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

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

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

Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV.

Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV.

Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.

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

Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV.

Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.

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

Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.

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

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

Covariance matrix between the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV.

Covariance matrix between the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV.

Covariance matrix between the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.

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

Covariance matrix between the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV and the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV.

Covariance matrix between the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV and the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.

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

Covariance matrix between the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV and the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.

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

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

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.5 < $|{y}^{t\bar{t}}|$ < 1.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 1 < $|{y}^{t\bar{t}}|$ < 2.

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

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

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 1 < $|{y}^{t\bar{t}}|$ < 2.

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

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

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

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

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at particle level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at particle level for 0.5 < $|{y}^{t\bar{t}}|$ < 1.

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

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

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

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

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

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

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

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

Covariance matrix between the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.2 < $|{y}^{t,1}|$ < 0.5.

Covariance matrix between the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.5 < $|{y}^{t,1}|$ < 1.

Covariance matrix between the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 1 < $|{y}^{t,1}|$ < 2.

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

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

Covariance matrix between the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.2 < $|{y}^{t,1}|$ < 0.5 and the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 1 < $|{y}^{t,1}|$ < 2.

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

Covariance matrix between the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.5 < $|{y}^{t,1}|$ < 1 and the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 1 < $|{y}^{t,1}|$ < 2.

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

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

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.5 < $|{y}^{t\bar{t}}|$ < 1.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 1 < $|{y}^{t\bar{t}}|$ < 2.

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

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

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5 and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 1 < $|{y}^{t\bar{t}}|$ < 2.

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

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.5 < $|{y}^{t\bar{t}}|$ < 1 and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 1 < $|{y}^{t\bar{t}}|$ < 2.

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

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

Covariance matrix between the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0 TeV < $p_{T}^{t\bar{t}}$ < 0.1 TeV and the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.1 TeV < $p_{T}^{t\bar{t}}$ < 0.2 TeV.

Covariance matrix between the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0 TeV < $p_{T}^{t\bar{t}}$ < 0.1 TeV and the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.2 TeV < $p_{T}^{t\bar{t}}$ < 0.35 TeV.

Covariance matrix between the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0 TeV < $p_{T}^{t\bar{t}}$ < 0.1 TeV and the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.35 TeV < $p_{T}^{t\bar{t}}$ < 1 TeV.

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

Covariance matrix between the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.1 TeV < $p_{T}^{t\bar{t}}$ < 0.2 TeV and the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.2 TeV < $p_{T}^{t\bar{t}}$ < 0.35 TeV.

Covariance matrix between the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.1 TeV < $p_{T}^{t\bar{t}}$ < 0.2 TeV and the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.35 TeV < $p_{T}^{t\bar{t}}$ < 1 TeV.

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

Covariance matrix between the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.2 TeV < $p_{T}^{t\bar{t}}$ < 0.35 TeV and the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.35 TeV < $p_{T}^{t\bar{t}}$ < 1 TeV.

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

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

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level for 0.5 < $|{y}^{t\bar{t}}|$ < 1.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level for 1 < $|{y}^{t\bar{t}}|$ < 2.

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

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

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level for 1 < $|{y}^{t\bar{t}}|$ < 2.

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

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level for 0.5 < $|{y}^{t\bar{t}}|$ < 1 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level for 1 < $|{y}^{t\bar{t}}|$ < 2.

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

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

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.

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

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.

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

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.

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

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.

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

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.

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

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

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

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.

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

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

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.

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

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.

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

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

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.

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

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level for 0.55 TeV < $p_{T}^{t,1}$ < 0.6 TeV.

Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level for 0.6 TeV < $p_{T}^{t,1}$ < 0.75 TeV.

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

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

Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level for 0.55 TeV < $p_{T}^{t,1}$ < 0.6 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level for 0.6 TeV < $p_{T}^{t,1}$ < 0.75 TeV.

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

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

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

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.

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

Covariance matrix between the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ normalized differential cross-section at particle level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute normalized cross-section at particle level for 0.2 < $|{y}^{t,1}|$ < 0.5.

Covariance matrix between the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ normalized differential cross-section at particle level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ normalized differential cross-section at particle level for 0.5 < $|{y}^{t,1}|$ < 1.

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

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

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

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

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

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

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

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

Covariance matrix between the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.2 < $|{y}^{t,1}|$ < 0.5.

Covariance matrix between the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.5 < $|{y}^{t,1}|$ < 1.

Covariance matrix between the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 1 < $|{y}^{t,1}|$ < 2.

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

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

Covariance matrix between the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.2 < $|{y}^{t,1}|$ < 0.5 and the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 1 < $|{y}^{t,1}|$ < 2.

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

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

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

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

Covariance matrix between the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level for 0 < $|{y}^{t,2}|$ < 0.2 and the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level for 0.2 < $|{y}^{t,2}|$ < 0.5.

Covariance matrix between the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level for 0 < $|{y}^{t,2}|$ < 0.2 and the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level for 0.5 < $|{y}^{t,2}|$ < 1.

Covariance matrix between the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level for 0 < $|{y}^{t,2}|$ < 0.2 and the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level for 1 < $|{y}^{t,2}|$ < 2.

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

Covariance matrix between the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level for 0.2 < $|{y}^{t,2}|$ < 0.5 and the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level for 0.5 < $|{y}^{t,2}|$ < 1.

Covariance matrix between the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level for 0.2 < $|{y}^{t,2}|$ < 0.5 and the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level for 1 < $|{y}^{t,2}|$ < 2.

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

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

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

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

Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV.

Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV.

Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.

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

Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV.

Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.

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

Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.

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

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

Covariance matrix between the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV.

Covariance matrix between the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV.

Covariance matrix between the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.

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

Covariance matrix between the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV and the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV.

Covariance matrix between the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV and the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.

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

Covariance matrix between the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV and the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.

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

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

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.5 < $|{y}^{t\bar{t}}|$ < 1.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 1 < $|{y}^{t\bar{t}}|$ < 2.

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

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

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 1 < $|{y}^{t\bar{t}}|$ < 2.

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

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

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

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

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ normalized differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ normalized differential cross-section at particle level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ normalized differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ normalized differential cross-section at particle level for 0.5 < $|{y}^{t\bar{t}}|$ < 1.

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

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

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

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

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

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

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

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

Covariance matrix between the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.2 < $|{y}^{t,1}|$ < 0.5.

Covariance matrix between the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.5 < $|{y}^{t,1}|$ < 1.

Covariance matrix between the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 1 < $|{y}^{t,1}|$ < 2.

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

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

Covariance matrix between the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.2 < $|{y}^{t,1}|$ < 0.5 and the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 1 < $|{y}^{t,1}|$ < 2.

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

Covariance matrix between the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.5 < $|{y}^{t,1}|$ < 1 and the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 1 < $|{y}^{t,1}|$ < 2.

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

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

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.5 < $|{y}^{t\bar{t}}|$ < 1.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 1 < $|{y}^{t\bar{t}}|$ < 2.

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

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

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5 and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 1 < $|{y}^{t\bar{t}}|$ < 2.

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

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.5 < $|{y}^{t\bar{t}}|$ < 1 and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 1 < $|{y}^{t\bar{t}}|$ < 2.

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

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

Covariance matrix between the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0 TeV < $p_{T}^{t\bar{t}}$ < 0.1 TeV and the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.1 TeV < $p_{T}^{t\bar{t}}$ < 0.2 TeV.

Covariance matrix between the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0 TeV < $p_{T}^{t\bar{t}}$ < 0.1 TeV and the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.2 TeV < $p_{T}^{t\bar{t}}$ < 0.35 TeV.

Covariance matrix between the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0 TeV < $p_{T}^{t\bar{t}}$ < 0.1 TeV and the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.35 TeV < $p_{T}^{t\bar{t}}$ < 1 TeV.

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

Covariance matrix between the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.1 TeV < $p_{T}^{t\bar{t}}$ < 0.2 TeV and the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.2 TeV < $p_{T}^{t\bar{t}}$ < 0.35 TeV.

Covariance matrix between the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.1 TeV < $p_{T}^{t\bar{t}}$ < 0.2 TeV and the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.35 TeV < $p_{T}^{t\bar{t}}$ < 1 TeV.

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

Covariance matrix between the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.2 TeV < $p_{T}^{t\bar{t}}$ < 0.35 TeV and the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.35 TeV < $p_{T}^{t\bar{t}}$ < 1 TeV.

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

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

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level for 0.5 < $|{y}^{t\bar{t}}|$ < 1.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level for 1 < $|{y}^{t\bar{t}}|$ < 2.

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

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

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level for 1 < $|{y}^{t\bar{t}}|$ < 2.

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

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level for 0.5 < $|{y}^{t\bar{t}}|$ < 1 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level for 1 < $|{y}^{t\bar{t}}|$ < 2.

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

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 < $|{y}^{t\bar{t}}|$ < 0.3, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 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 < $|{y}^{t\bar{t}}|$ < 0.3, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.

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 < $|{y}^{t\bar{t}}|$ < 0.3, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 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 < $|{y}^{t\bar{t}}|$ < 0.3, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.

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 < $|{y}^{t\bar{t}}|$ < 0.3, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 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 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.

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 < $|{y}^{t\bar{t}}|$ < 0.3, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 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, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.

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 < $|{y}^{t\bar{t}}|$ < 0.3, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 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, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.

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 < $|{y}^{t\bar{t}}|$ < 0.3, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 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.

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 < $|{y}^{t\bar{t}}|$ < 0.3, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 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, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.

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 < $|{y}^{t\bar{t}}|$ < 0.3, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 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, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.

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 < $|{y}^{t\bar{t}}|$ < 0.3, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 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.

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 < $|{y}^{t\bar{t}}|$ < 0.3, 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 < $|{y}^{t\bar{t}}|$ < 0.3, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.

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 < $|{y}^{t\bar{t}}|$ < 0.3, 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 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.

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 < $|{y}^{t\bar{t}}|$ < 0.3, 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, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.

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 < $|{y}^{t\bar{t}}|$ < 0.3, 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, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.

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 < $|{y}^{t\bar{t}}|$ < 0.3, 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.

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 < $|{y}^{t\bar{t}}|$ < 0.3, 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, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.

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 < $|{y}^{t\bar{t}}|$ < 0.3, 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, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.

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 < $|{y}^{t\bar{t}}|$ < 0.3, 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.

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 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 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 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.

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 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 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, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.

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 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 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, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.

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 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 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.

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 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 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, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.

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 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 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, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.

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 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 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.

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, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 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, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.

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, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 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, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.

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, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 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.

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, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 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, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.

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, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 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, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.

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, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 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, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.

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, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.

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.

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 0.9 < $|{y}^{t\bar{t}}|$ < 2, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.

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 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.

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

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, 1.5 TeV < $m^{t\bar{t}}$ < 4 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.

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, 1.5 TeV < $m^{t\bar{t}}$ < 4 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, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.

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, 1.5 TeV < $m^{t\bar{t}}$ < 4 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, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.

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, 1.5 TeV < $m^{t\bar{t}}$ < 4 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.

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, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 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, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.

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, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 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, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.

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, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 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.

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, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.

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.

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, 1.5 TeV < $m^{t\bar{t}}$ < 4 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.

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level for 0.55 TeV < $p_{T}^{t,1}$ < 0.6 TeV.

Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level for 0.6 TeV < $p_{T}^{t,1}$ < 0.75 TeV.

Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.

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

Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level for 0.55 TeV < $p_{T}^{t,1}$ < 0.6 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level for 0.6 TeV < $p_{T}^{t,1}$ < 0.75 TeV.

Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level for 0.55 TeV < $p_{T}^{t,1}$ < 0.6 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.

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

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

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

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

Covariance matrix between the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at parton level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at parton level for 0.2 < $|{y}^{t,1}|$ < 0.5.

Covariance matrix between the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at parton level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at parton level for 0.5 < $|{y}^{t,1}|$ < 1.

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

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

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

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

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

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

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

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

Covariance matrix between the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.2 < $|{y}^{t,1}|$ < 0.5.

Covariance matrix between the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.5 < $|{y}^{t,1}|$ < 1.

Covariance matrix between the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 1 < $|{y}^{t,1}|$ < 2.

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

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

Covariance matrix between the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.2 < $|{y}^{t,1}|$ < 0.5 and the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 1 < $|{y}^{t,1}|$ < 2.

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

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

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

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

Covariance matrix between the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level for 0 < $|{y}^{t,2}|$ < 0.2 and the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level for 0.2 < $|{y}^{t,2}|$ < 0.5.

Covariance matrix between the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level for 0 < $|{y}^{t,2}|$ < 0.2 and the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level for 0.5 < $|{y}^{t,2}|$ < 1.

Covariance matrix between the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level for 0 < $|{y}^{t,2}|$ < 0.2 and the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level for 1 < $|{y}^{t,2}|$ < 2.

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

Covariance matrix between the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level for 0.2 < $|{y}^{t,2}|$ < 0.5 and the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level for 0.5 < $|{y}^{t,2}|$ < 1.

Covariance matrix between the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level for 0.2 < $|{y}^{t,2}|$ < 0.5 and the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level for 1 < $|{y}^{t,2}|$ < 2.

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

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

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

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

Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV.

Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV.

Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.

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

Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV.

Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.

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

Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.

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

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

Covariance matrix between the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV.

Covariance matrix between the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV.

Covariance matrix between the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.

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

Covariance matrix between the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV and the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV.

Covariance matrix between the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV and the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.

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

Covariance matrix between the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV and the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.

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

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

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.5 < $|{y}^{t\bar{t}}|$ < 1.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 1 < $|{y}^{t\bar{t}}|$ < 2.

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

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

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 1 < $|{y}^{t\bar{t}}|$ < 2.

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

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

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

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

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at parton level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at parton level for 0.5 < $|{y}^{t\bar{t}}|$ < 1.

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

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

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

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

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

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

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

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

Covariance matrix between the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.2 < $|{y}^{t,1}|$ < 0.5.

Covariance matrix between the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.5 < $|{y}^{t,1}|$ < 1.

Covariance matrix between the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 1 < $|{y}^{t,1}|$ < 2.

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

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

Covariance matrix between the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.2 < $|{y}^{t,1}|$ < 0.5 and the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 1 < $|{y}^{t,1}|$ < 2.

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

Covariance matrix between the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.5 < $|{y}^{t,1}|$ < 1 and the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 1 < $|{y}^{t,1}|$ < 2.

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

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

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.5 < $|{y}^{t\bar{t}}|$ < 1.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 1 < $|{y}^{t\bar{t}}|$ < 2.

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

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

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5 and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 1 < $|{y}^{t\bar{t}}|$ < 2.

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

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.5 < $|{y}^{t\bar{t}}|$ < 1 and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 1 < $|{y}^{t\bar{t}}|$ < 2.

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

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

Covariance matrix between the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0 TeV < $p_{T}^{t\bar{t}}$ < 0.1 TeV and the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.1 TeV < $p_{T}^{t\bar{t}}$ < 0.2 TeV.

Covariance matrix between the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0 TeV < $p_{T}^{t\bar{t}}$ < 0.1 TeV and the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.2 TeV < $p_{T}^{t\bar{t}}$ < 0.35 TeV.

Covariance matrix between the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0 TeV < $p_{T}^{t\bar{t}}$ < 0.1 TeV and the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.35 TeV < $p_{T}^{t\bar{t}}$ < 1 TeV.

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

Covariance matrix between the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.1 TeV < $p_{T}^{t\bar{t}}$ < 0.2 TeV and the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.2 TeV < $p_{T}^{t\bar{t}}$ < 0.35 TeV.

Covariance matrix between the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.1 TeV < $p_{T}^{t\bar{t}}$ < 0.2 TeV and the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.35 TeV < $p_{T}^{t\bar{t}}$ < 1 TeV.

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

Covariance matrix between the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.2 TeV < $p_{T}^{t\bar{t}}$ < 0.35 TeV and the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.35 TeV < $p_{T}^{t\bar{t}}$ < 1 TeV.

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

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

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level for 0.5 < $|{y}^{t\bar{t}}|$ < 1.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level for 1 < $|{y}^{t\bar{t}}|$ < 2.

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

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

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level for 1 < $|{y}^{t\bar{t}}|$ < 2.

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

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level for 0.5 < $|{y}^{t\bar{t}}|$ < 1 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level for 1 < $|{y}^{t\bar{t}}|$ < 2.

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

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

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.

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

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.

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

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.

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

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.

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

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

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

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.

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

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

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.

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

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.

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

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

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.

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

Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level for 0.55 TeV < $p_{T}^{t,1}$ < 0.6 TeV.

Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level for 0.6 TeV < $p_{T}^{t,1}$ < 0.75 TeV.

Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.

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

Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level for 0.55 TeV < $p_{T}^{t,1}$ < 0.6 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level for 0.6 TeV < $p_{T}^{t,1}$ < 0.75 TeV.

Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level for 0.55 TeV < $p_{T}^{t,1}$ < 0.6 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.

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

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

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