Distribution of $E^{miss}_T$ in data and for the expected SM background in the Single-Muon CR after performing the 'simplified shape fit'. Overflows are included in the fourth bin of each distribution. The $E^{miss}_T$ calculation in this CR does not include the muon contribution. The error bars are statistical, and the dashed band includes statistical and systematic uncertainties determined by the fit. The lower panel shows the ratio of data to expected background event yields.

Distribution of $E^{miss}_T$ in data and for the expected SM background in the Two-Muon CR after performing the 'simplified shape fit'. The $E^{miss}_T$ calculation in this CR does not include the muon contribution. The error bars are statistical, and the dashed band includes statistical and systematic uncertainties determined by the fit. The lower panel shows the ratio of data to expected background event yields.

Distribution of $E^{miss}_T$ in data and for the expected SM background in the Two-Muon CR after performing the 'simplified shape fit'. Overflows are included in the fourth bin of each distribution. The $E^{miss}_T$ calculation in this CR does not include the muon contribution. The error bars are statistical, and the dashed band includes statistical and systematic uncertainties determined by the fit. The lower panel shows the ratio of data to expected background event yields.

Distribution of $E^{miss}_T$ in data and for the expected SM background in the Two-Electron CR after performing the 'simplified shape fit'. The $E^{miss}_$ calculation in this CR does not include electron contribution. The error bars are statistical, and the dashed band includes statistical and systematic uncertainties determined by the fit. The lower panel shows the ratio of data to expected background event yields.

Distribution of $E^{miss}_T$ in data and for the expected SM background in the Two-Electron CR after performing the 'simplified shape fit'. Overflows are included in the fourth bin of each distribution. The $E^{miss}_T$ calculation in this CR does not include electron contribution. The error bars are statistical, and the dashed band includes statistical and systematic uncertainties determined by the fit. The lower panel shows the ratio of data to expected background event yields.

The observed exclusion contours on the $m_{\chi} - m_{med}$ plane for a simplified DM model involving an axial-vector mediator with couplings $g_{\chi}$ = 1, $g_q$ = 0.25 and $g_l$ = 0.

The observed exclusion contours on the $m_{\chi} - m_{med}$ plane for a simplified DM model involving an axial-vector mediator with couplings $g_{\chi}$ = 1, $g_q$ = 0.25 and $g_l$ = 0.

The expected exclusion contours on the $m_{\chi} - m_{med}$ plane for a simplified DM model involving an axial-vector mediator with couplings $g_{\chi}$ = 1, $g_q$ = 0.25 and $g_l$ = 0.

The expected exclusion contours on the $m_{\chi} - m_{med}$ plane for a simplified DM model involving an axial-vector mediator with couplings $g_{\chi}$ = 1, $g_q$ = 0.25 and $g_l$ = 0.

The expected + 1 sigma exclusion contours on the $m_{\chi} - m_{med}$ plane for a simplified DM model involving an axial-vector mediator with couplings $g_{\chi}$ = 1, $g_q$ = 0.25 and $g_l$ = 0.

The expected + 1 sigma exclusion contours on the $m_{\chi} - m_{med}$ plane for a simplified DM model involving an axial-vector mediator with couplings $g_{\chi}$ = 1, $g_q$ = 0.25 and $g_l$ = 0.

The expected - 1 sigma exclusion contours on the $m_{\chi} - m_{med}$ plane for a simplified DM model involving an axial-vector mediator with couplings $g_{\chi}$ = 1, $g_q$ = 0.25 and $g_l$ = 0.

The expected - 1 sigma exclusion contours on the $m_{\chi} - m_{med}$ plane for a simplified DM model involving an axial-vector mediator with couplings $g_{\chi}$ = 1, $g_q$ = 0.25 and $g_l$ = 0.

The observed exclusion contours on the $m_{\chi} - m_{med}$ plane for a simplified DM model involving an axial-vector mediator with couplings $g_{\chi}$ = 1, $g_q$ = 0.1 and $g_l$ = 0.1.

The observed exclusion contours on the $m_{\chi} - m_{med}$ plane for a simplified DM model involving an axial-vector mediator with couplings $g_{\chi}$ = 1, $g_q$ = 0.1 and $g_l$ = 0.1.

The expected exclusion contours on the $m_{\chi} - m_{med}$ plane for a simplified DM model involving an axial-vector mediator with couplings $g_{\chi}$ = 1, $g_q$ = 0.1 and $g_l$ = 0.1.

The expected exclusion contours on the $m_{\chi} - m_{med}$ plane for a simplified DM model involving an axial-vector mediator with couplings $g_{\chi}$ = 1, $g_q$ = 0.1 and $g_l$ = 0.1.

The expected + 1 sigma exclusion contours on the $m_{\chi} - m_{med}$ plane for a simplified DM model involving an axial-vector mediator with couplings $g_{\chi}$ = 1, $g_q$ = 0.1 and $g_l$ = 0.1.

The expected + 1 sigma exclusion contours on the $m_{\chi} - m_{med}$ plane for a simplified DM model involving an axial-vector mediator with couplings $g_{\chi}$ = 1, $g_q$ = 0.1 and $g_l$ = 0.1.

The expected - 1 sigma exclusion contours on the $m_{\chi} - m_{med}$ plane for a simplified DM model involving an axial-vector mediator with couplings $g_{\chi}$ = 1, $g_q$ = 0.1 and $g_l$ = 0.1.

The expected - 1 sigma exclusion contours on the $m_{\chi} - m_{med}$ plane for a simplified DM model involving an axial-vector mediator with couplings $g_{\chi}$ = 1, $g_q$ = 0.1 and $g_l$ = 0.1.

The observed exclusion contours on the $m_{\chi} - m_{med}$ plane for a vector mediator with couplings $g_{\chi}$ = 1, $g_q$ = 0.25 and $g_l$ = 0.

The observed exclusion contours on the $m_{\chi} - m_{med}$ plane for a vector mediator with couplings $g_{\chi}$ = 1, $g_q$ = 0.25 and $g_l$ = 0.

The expected exclusion contours on the $m_{\chi} - m_{med}$ plane for a vector mediator with couplings $g_{\chi}$ = 1, $g_q$ = 0.25 and $g_l$ = 0.

The expected exclusion contours on the $m_{\chi} - m_{med}$ plane for a vector mediator with couplings $g_{\chi}$ = 1, $g_q$ = 0.25 and $g_l$ = 0.

The expected + 1 sigma exclusion contours on the $m_{\chi} - m_{med}$ plane for a vector mediator with couplings $g_{\chi}$ = 1, $g_q$ = 0.25 and $g_l$ = 0.

The expected + 1 sigma exclusion contours on the $m_{\chi} - m_{med}$ plane for a vector mediator with couplings $g_{\chi}$ = 1, $g_q$ = 0.25 and $g_l$ = 0.

The expected - 1 sigma exclusion contours on the $m_{\chi} - m_{med}$ plane for a vector mediator with couplings $g_{\chi}$ = 1, $g_q$ = 0.25 and $g_l$ = 0.

The expected - 1 sigma exclusion contours on the $m_{\chi} - m_{med}$ plane for a vector mediator with couplings $g_{\chi}$ = 1, $g_q$ = 0.25 and $g_l$ = 0.

The observed exclusion contours on the $m_{\chi} - m_{med}$ plane for a vector mediator with couplings and $g_{\chi}$ = 1, $g_q$ = 0.1 and $g_l$ = 0.01

The observed exclusion contours on the $m_{\chi} - m_{med}$ plane for a vector mediator with couplings and $g_{\chi}$ = 1, $g_q$ = 0.1 and $g_l$ = 0.01

The expected exclusion contours on the $m_{\chi} - m_{med}$ plane for a vector mediator with couplings $g_{\chi}$ = 1, $g_q$ = 0.1 and $g_l$ = 0.01.

The expected exclusion contours on the $m_{\chi} - m_{med}$ plane for a vector mediator with couplings $g_{\chi}$ = 1, $g_q$ = 0.1 and $g_l$ = 0.01.

The expected + 1 sigma exclusion contours on the $m_{\chi} - m_{med}$ plane for a vector mediator with couplings $g_{\chi}$ = 1, $g_q$ = 0.1 and $g_l$ = 0.01.

The expected + 1 sigma exclusion contours on the $m_{\chi} - m_{med}$ plane for a vector mediator with couplings $g_{\chi}$ = 1, $g_q$ = 0.1 and $g_l$ = 0.01.

The expected - 1 sigma exclusion contours on the $m_{\chi} - m_{med}$ plane for a vector mediator with couplings $g_{\chi}$ = 1, $g_q$ = 0.1 and $g_l$ = 0.01.

The expected - 1 sigma exclusion contours on the $m_{\chi} - m_{med}$ plane for a vector mediator with couplings $g_{\chi}$ = 1, $g_q$ = 0.1 and $g_l$ = 0.01.

The 90% CL exclusion limit on $\chi$-proton spin-dependent scattering cross section in an axial-vector model with couplings $g_{\chi}$ = 1, $g_q$ = 0.25 and $g_l$ = 0 as a function of the dark-matter mass $m_{\chi}$.

The 90% CL exclusion limit on $\chi$-proton spin-dependent scattering cross section in an axial-vector model with couplings $g_{\chi}$ = 1, $g_q$ = 0.25 and $g_l$ = 0 as a function of the dark-matter mass $m_{\chi}$. The 90% CL exclusion limit is displayed only in the regime where the theory is perturbative.

The 90% CL exclusion limit on $\chi$-neutron spin-dependent scattering cross section in an axial-vector model with couplings $g_{\chi}$ = 1, $g_q$ = 0.25 and $g_l$ = 0 as a function of the dark-matter mass $m_{\chi}$.

The 90% CL exclusion limit on $\chi$-neutron spin-dependent scattering cross section in an axial-vector model with couplings $g_{\chi}$ = 1, $g_q$ = 0.25 and $g_l$ = 0 as a function of the dark-matter mass $m_{\chi}$. The 90% CL exclusion limit is displayed only in the regime where the theory is perturbative.

The 90% CL exclusion limit on $\chi$-nucleon spin-independent scattering cross section in a vector model with couplings $g_{\chi}$ = 1, $g_q$ = 0.25 and $g_l$ = 0 as a function of the dark-matter mass $m_{\chi}$.

The 90% CL exclusion limit on $\chi$-nucleon spin-independent scattering cross section in a vector model with couplings $g_{\chi}$ = 1, $g_q$ = 0.25 and $g_l$ = 0 as a function of the dark-matter mass $m_{\chi}$.

Observed and expected exclusion at 95% CL on the coupling $c_W$ as a function of the effective scale $f_a$ for an ALP mass of 1 MeV.

Observed and expected exclusion at 95% CL on the coupling $c_W$ as a function of the effective scale $f_a$ for an ALP mass of 1 MeV.

The observed 95% CL upper limits on signal strength $\mu$, the ratio of the experimental limit to the predicted signal cross section, for a simplified model of dark matter production involving an axial-vector operator and couplings $g_{\chi}$ = 1, $g_q$ = 0.25 and $g_l$ = 0 as a function of the mass of the dark matter, $m_{\chi}$ and the mass of the axial-vector mediator, $m_{med}$.

The observed 95% CL upper limits on signal strength $\mu$, the ratio of the experimental limit to the predicted signal cross section, for a simplified model of dark matter production involving an axial-vector operator and couplings $g_{\chi}$ = 1, $g_q$ = 0.25 and $g_l$ = 0 as a function of the mass of the dark matter, $m_{\chi}$ and the mass of the axial-vector mediator, $m_{med}$.

The observed 95% CL upper limits on cross section for a simplified model of dark matter production involving an axial-vector operator and couplings $g_{\chi}$ = 1, $g_q$ = 0.25 and $g_l$ = 0 as a function of the mass of the dark matter, $m_{\chi}$ and the mass of the axial-vector mediator, $m_{med}$.

The observed 95% CL upper limits on cross section for a simplified model of dark matter production involving an axial-vector operator and couplings $g_{\chi}$ = 1, $g_q$ = 0.25 and $g_l$ = 0 as a function of the mass of the dark matter, $m_{\chi}$ and the mass of the axial-vector mediator, $m_{med}$.

Acceptance in % for a simplified model of dark matter production involving an axial-vector operator with couplings $g_{\chi}$ = 1, $g_q$ = 0.25 and $g_l$ = 0 for different values of $m_{\chi}$ and $m_{med}$ in the four inclusive signal regions.

Acceptance in % for a simplified model of dark matter production involving an axial-vector operator with couplings $g_{\chi}$ = 1, $g_q$ = 0.25 and $g_l$ = 0 for different values of $m_{\chi}$ and $m_{med}$ in the four inclusive signal regions.

Acceptance in % for a simplified model of dark matter production involving an axial-vector operator with couplings $g_{\chi}$ = 1, $g_q$ = 0.25 and $g_l$ = 0 for different values of $m_{\chi}$ and $m_{med}$ in the three exclusive signal regions.

Acceptance in % for a simplified model of dark matter production involving an axial-vector operator with couplings $g_{\chi}$ = 1, $g_q$ = 0.25 and $g_l$ = 0 for different values of $m_{\chi}$ and $m_{med}$ in the three exclusive signal regions.

Efficiencies for a simplified model of dark matter production involving an axial-vector operator with couplings $g_{\chi}$ = 1, $g_q$ = 0.25 and $g_l$ = 0 for different values of $m_{\chi}$ and $m_{med}$ in the four inclusive signal regions.

Efficiencies for a simplified model of dark matter production involving an axial-vector operator with couplings $g_{\chi}$ = 1, $g_q$ = 0.25 and $g_l$ = 0 for different values of $m_{\chi}$ and $m_{med}$ in the four inclusive signal regions.

Efficiencies for a simplified model of dark matter production involving an axial-vector operator with couplings $g_{\chi}$ = 1, $g_q$ = 0.25 and $g_l$ = 0 for different values of $m_{\chi}$ and $m_{med}$ in the three exclusive signal regions.

Efficiencies for a simplified model of dark matter production involving an axial-vector operator with couplings $g_{\chi}$ = 1, $g_q$ = 0.25 and $g_l$ = 0 for different values of $m_{\chi}$ and $m_{med}$ in the three exclusive signal regions.

Expected signal yields after each of the analysis selection cuts for the 800 GeV mass point. Total expected events represents all type-III seesaw events expected for integrated luminosity 139 fb$^{-1}$. Only events with at least two leptons were generated for this analysis.

Distribution of $H_\text{T} + E_\text{T}^\text{miss}$ in the opposite-sign electron-electron signal region after the background-only fit.

Distribution of $H_\text{T} + E_\text{T}^\text{miss}$ in the opposite-sign electron-muon signal region after the background-only fit.

Distribution of $H_\text{T} + E_\text{T}^\text{miss}$ in the opposite-sign muon-muon signal region after the background-only fit.

Distribution of $H_\text{T} + E_\text{T}^\text{miss}$ in the same-sign electron-electron signal region after the background-only fit.

Distribution of $H_\text{T} + E_\text{T}^\text{miss}$ in the same-sign electron-muon signal region after the background-only fit.

Distribution of $H_\text{T} + E_\text{T}^\text{miss}$ in the same-sign muon-muon signal region after the background-only fit.

Acceptance x efficiency versus $\kappa_{2V}$ for non-resonant signal of $HH$.

Acceptance x efficiency versus resonance mass for both narrow and broad resonance $X$ to $HH$.

Acceptance x efficiency versus resonance mass for both narrow and broad resonance $X$ to $HH$.

Acceptance x efficiency versus resonance mass for both narrow and broad resonance $X$ to $HH$.

Acceptance x efficiency versus resonance mass for both narrow and broad resonance $X$ to $HH$.

Post-fit mass distribution of the $HH$ candidates in the signal region. The expected background is shown after the profile-likelihood fit to data with the background-only hypothesis; the narrow-width resonant signal at 800 GeV and the non-resonant signal at $\kappa_{2V}$ = 3 are overlaid, both normalised to the corresponding observed upper limits on the cross-section.

Post-fit mass distribution of the $HH$ candidates in the signal region. The expected background is shown after the profile-likelihood fit to data with the background-only hypothesis; the narrow-width resonant signal at 800 GeV and the non-resonant signal at $\kappa_{2V}$ = 3 are overlaid, both normalised to the corresponding observed upper limits on the cross-section.

Post-fit mass distribution of the $HH$ candidates in the signal region. The expected background is shown after the profile-likelihood fit to data with the background-only hypothesis; the narrow-width resonant signal at 800 GeV and the non-resonant signal at $\kappa_{2V}$ = 3 are overlaid, both normalised to the corresponding observed upper limits on the cross-section.

Post-fit mass distribution of the $HH$ candidates in the signal region. The expected background is shown after the profile-likelihood fit to data with the background-only hypothesis; the narrow-width resonant signal at 800 GeV and the non-resonant signal at $\kappa_{2V}$ = 3 are overlaid, both normalised to the corresponding observed upper limits on the cross-section.

Observed and expected limits at 95% CL on the cross-sections of narrow resonance $X$ to $HH$ as a function of the mass $m_{X}$.

Observed and expected limits at 95% CL on the cross-sections of narrow resonance $X$ to $HH$ as a function of the mass $m_{X}$.

Observed and expected limits at 95% CL on the cross-sections of narrow resonance $X$ to $HH$ as a function of the mass $m_{X}$.

Observed and expected limits at 95% CL on the cross-section of narrow resonance $X$ to $HH$ as a function of the mass $m_{X}$.

Observed and expected limits at 95% CL on the cross-sections of broad resonance $X$ to $HH$ as a function of the mass $m_{X}$.

Observed and expected limits at 95% CL on the cross-sections of broad resonance $X$ to $HH$ as a function of the mass $m_{X}$.

Observed and expected limits at 95% CL on the cross-sections of broad resonance $X$ to $HH$ as a function of the mass $m_{X}$.

Observed and expected limits at 95% CL on the cross-section of broad resonance $X$ to $HH$ as a function of the mass $m_{X}$.

Observed and expected limits at 95% CL on the cross-sections of non-resonant $HH$ production via VBF as a function of the di-vector-boson-di-Higgs-boson coupling modifier $\kappa_{2V}$. The theory prediction of the cross-section as a function of $\kappa_{2V}$ is also shown. The minimum theory cross-section is 1.37 fb at $\kappa_{2V}=1.17$.

Observed and expected limits at 95% CL on the cross-sections of non-resonant $HH$ production via VBF as a function of the di-vector-boson-di-Higgs-boson coupling modifier $\kappa_{2V}$. The theory prediction of the cross-section as a function of $\kappa_{2V}$ is also shown. The minimum theory cross-section is 1.37 fb at $\kappa_{2V}=1.17$.

Observed and expected limits at 95% CL on the cross-sections of non-resonant $HH$ production via VBF as a function of the di-vector-boson-di-Higgs-boson coupling modifier $\kappa_{2V}$. The theory prediction of the cross-section as a function of $\kappa_{2V}$ is also shown. The minimum theory cross-section is 1.37 fb at $\kappa_{2V}=1.17$.

Observed and expected limits at 95% CL on the cross-sections of non-resonant $HH$ production via VBF as a function of the di-vector-boson-di-Higgs-boson coupling modifier $\kappa_{2V}$. The theory prediction of the cross-section as a function of $\kappa_{2V}$ is also shown. The minimum theory cross-section is 1.37 fb at $\kappa_{2V}=1.17$.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.

Fit correlations between the physical parameters of interest, obtained from the fit for solution (b).

Values of the physical parameters extracted in the combination of solution (a) of 13 TeV results with those obtained from 7 TeV and 8 TeV data.

Values of the physical parameters extracted in the combination of solution (b) of 13 TeV results with those obtained from 7 TeV and 8 TeV data.

Correlation matrix of the BLUE combination of the 7 TeV and 8 TeV results and the solution (a) of the 13 TeV result.

Correlation matrix of the BLUE combination of the 7 TeV and 8 TeV results and the solution (b) of the 13 TeV result.

Summary of systematic uncertainties assigned to the physical parameters of interest.

Distribution of $m^{vis}_{HH}$ after applying all the event selection that define the $HH$ SR, except the requirement on $m^{vis}_{HH}$. The background labelled as "Others" contains $W$+jets, diboson, $t\bar{t}$ and single-top-quark processes. The $X\rightarrow HH \rightarrow b\bar{b}\tau^{+}\tau^{-}$ signal is overlaid for two resonance mass hypotheses with a cross-section set to the expected limit, while all backgrounds are pre-fit. The first and the last bins contains the under-flow and over-flow bin entries, respectively. The hatched bands represent combined statistical and systematic uncertainties.

Event yields of the various estimated backgrounds and data, computed in the signal region of the search for $X\rightarrow HH \rightarrow b\bar{b}\tau^{+}\tau^{-}$. The background labelled as "Others" contains $W$+jets, diboson, $t\bar{t}$ and single-top-quark processes. Statistical and systematic uncertainties are quoted. The background yields and uncertainties are pre-fit and are found to be similar to those post-fit.

Event yields of the various estimated backgrounds and data, computed in the signal region of the search for $X\rightarrow HH \rightarrow b\bar{b}\tau^{+}\tau^{-}$. The background labelled as "Others" contains $W$+jets, diboson, $t\bar{t}$ and single-top-quark processes. Statistical and systematic uncertainties are quoted. The background yields and uncertainties are pre-fit and are found to be similar to those post-fit.

Expected and observed 95% CL upper limits on the production of a heavy, narrow-width, scalar resonance decaying to a pair of Higgs bosons ($X\rightarrow HH$). The final state used in the search consists of a boosted $b\bar{b}$ pair and a boosted hadronically decaying $\tau^{+}\tau^{-}$ pair, and the SM braching ratio of the Higgs boson are assumed. The $\pm 1\sigma$ and $\pm 2\sigma$ variations about the expected limit are indicated by the error bands. Two different requirements are applied on the visible mass of the two boosted Higgs boson candidates for the resonance mass hypotheses of 1.6 TeV and 2.5 TeV, leading to discontinuities in the limits (at 1.6 TeV, the difference between imposing no requirement and $m^{vis}_{HH}>900$ GeV is less than 1% though).

Expected and observed 95% CL upper limits on the production of a heavy, narrow-width, scalar resonance decaying to a pair of Higgs bosons ($X\rightarrow HH$). The final state used in the search consists of a boosted $b\bar{b}$ pair and a boosted hadronically decaying $\tau^{+}\tau^{-}$ pair, and the SM braching ratio of the Higgs boson are assumed. The $\pm 1\sigma$ and $\pm 2\sigma$ variations about the expected limit are indicated by the error bands. Two different requirements are applied on the visible mass of the two boosted Higgs boson candidates for the resonance mass hypotheses of 1.6 TeV and 2.5 TeV, leading to discontinuities in the limits (at 1.6 TeV, the difference between imposing no requirement and $m^{vis}_{HH}>900$ GeV is less than 1% though).

Limit Plot

Limit Plot

Limit Plot

Limit Plot

Limit Plot

Limit Plot

Limit Plot

Limit Plot

Limit Plot

HVT WW Acceptance times Efficiency

HVT WW Acceptance times Efficiency

HVT WZ Acceptance times Efficiency

HVT WZ Acceptance times Efficiency

RS Graviton WW Acceptance times Efficiency

RS Graviton WW Acceptance times Efficiency

RS Graviton ZZ Acceptance times Efficiency

RS Graviton ZZ Acceptance times Efficiency

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

Relative double-differential cross-section as a function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute double-differential cross-section as a function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative double-differential cross-section as a function of $|y^{t,2}|$ vs $|y^{t,1}|$ at parton level in the all hadronic resolved topology in 0.0 < $|y^{t,1}|$ < 0.5 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $|y^{t,2}|$ vs $|y^{t,1}|$ at parton level in the all hadronic resolved topology in 0.5 < $|y^{t,1}|$ < 1.0 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $|y^{t,2}|$ vs $|y^{t,1}|$ at parton level in the all hadronic resolved topology in 1.0 < $|y^{t,1}|$ < 1.5 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $|y^{t,2}|$ vs $|y^{t,1}|$ at parton level in the all hadronic resolved topology in 1.5 < $|y^{t,1}|$ < 2.5 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 0.0 < $|y^{t,1}|$ < 0.5 and the relative double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 0.0 < $|y^{t,1}|$ < 0.5 at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 0.5 < $|y^{t,1}|$ < 1.0 and the relative double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 0.0 < $|y^{t,1}|$ < 0.5 at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 0.5 < $|y^{t,1}|$ < 1.0 and the relative double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 0.5 < $|y^{t,1}|$ < 1.0 at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 1.0 < $|y^{t,1}|$ < 1.5 and the relative double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 0.0 < $|y^{t,1}|$ < 0.5 at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 1.0 < $|y^{t,1}|$ < 1.5 and the relative double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 0.5 < $|y^{t,1}|$ < 1.0 at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 1.0 < $|y^{t,1}|$ < 1.5 and the relative double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 1.0 < $|y^{t,1}|$ < 1.5 at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 1.5 < $|y^{t,1}|$ < 2.5 and the relative double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 0.0 < $|y^{t,1}|$ < 0.5 at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 1.5 < $|y^{t,1}|$ < 2.5 and the relative double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 0.5 < $|y^{t,1}|$ < 1.0 at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 1.5 < $|y^{t,1}|$ < 2.5 and the relative double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 1.0 < $|y^{t,1}|$ < 1.5 at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 1.5 < $|y^{t,1}|$ < 2.5 and the relative double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 1.5 < $|y^{t,1}|$ < 2.5 at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute double-differential cross-section as a function of $|y^{t,2}|$ vs $|y^{t,1}|$ at parton level in the all hadronic resolved topology in 0.0 < $|y^{t,1}|$ < 0.5 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $|y^{t,2}|$ vs $|y^{t,1}|$ at parton level in the all hadronic resolved topology in 0.5 < $|y^{t,1}|$ < 1.0 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $|y^{t,2}|$ vs $|y^{t,1}|$ at parton level in the all hadronic resolved topology in 1.0 < $|y^{t,1}|$ < 1.5 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $|y^{t,2}|$ vs $|y^{t,1}|$ at parton level in the all hadronic resolved topology in 1.5 < $|y^{t,1}|$ < 2.5 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 0.0 < $|y^{t,1}|$ < 0.5 and the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 0.0 < $|y^{t,1}|$ < 0.5 at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 0.5 < $|y^{t,1}|$ < 1.0 and the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 0.0 < $|y^{t,1}|$ < 0.5 at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 0.5 < $|y^{t,1}|$ < 1.0 and the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 0.5 < $|y^{t,1}|$ < 1.0 at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 1.0 < $|y^{t,1}|$ < 1.5 and the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 0.0 < $|y^{t,1}|$ < 0.5 at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 1.0 < $|y^{t,1}|$ < 1.5 and the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 0.5 < $|y^{t,1}|$ < 1.0 at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 1.0 < $|y^{t,1}|$ < 1.5 and the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 1.0 < $|y^{t,1}|$ < 1.5 at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 1.5 < $|y^{t,1}|$ < 2.5 and the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 0.0 < $|y^{t,1}|$ < 0.5 at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 1.5 < $|y^{t,1}|$ < 2.5 and the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 0.5 < $|y^{t,1}|$ < 1.0 at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 1.5 < $|y^{t,1}|$ < 2.5 and the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 1.0 < $|y^{t,1}|$ < 1.5 at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 1.5 < $|y^{t,1}|$ < 2.5 and the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 1.5 < $|y^{t,1}|$ < 2.5 at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative double-differential cross-section as a function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 1315.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 1315.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 1315.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 1315.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 1315.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 1315.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute double-differential cross-section as a function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 1315.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 1315.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 1315.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 1315.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 1315.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 1315.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative double-differential cross-section as a function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the relative double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the relative double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the relative double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute double-differential cross-section as a function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the absolute double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the absolute double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the absolute double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative double-differential cross-section as a function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the relative double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the relative double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the relative double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute double-differential cross-section as a function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 1315.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1315.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1315.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1315.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1315.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1315.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 1315.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1315.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1315.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1315.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1315.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1315.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative double-differential cross-section as a function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute double-differential cross-section as a function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative double-differential cross-section as a function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ at parton level in the all hadronic resolved topology in 0.0 GeV < $p_{T}^{t,2}$ < 170.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ at parton level in the all hadronic resolved topology in 170.0 GeV < $p_{T}^{t,2}$ < 290.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ at parton level in the all hadronic resolved topology in 290.0 GeV < $p_{T}^{t,2}$ < 450.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ at parton level in the all hadronic resolved topology in 450.0 GeV < $p_{T}^{t,2}$ < 1000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 0.0 GeV < $p_{T}^{t,2}$ < 170.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 0.0 GeV < $p_{T}^{t,2}$ < 170.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 170.0 GeV < $p_{T}^{t,2}$ < 290.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 0.0 GeV < $p_{T}^{t,2}$ < 170.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 170.0 GeV < $p_{T}^{t,2}$ < 290.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 170.0 GeV < $p_{T}^{t,2}$ < 290.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 290.0 GeV < $p_{T}^{t,2}$ < 450.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 0.0 GeV < $p_{T}^{t,2}$ < 170.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 290.0 GeV < $p_{T}^{t,2}$ < 450.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 170.0 GeV < $p_{T}^{t,2}$ < 290.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 290.0 GeV < $p_{T}^{t,2}$ < 450.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 290.0 GeV < $p_{T}^{t,2}$ < 450.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 450.0 GeV < $p_{T}^{t,2}$ < 1000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 0.0 GeV < $p_{T}^{t,2}$ < 170.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 450.0 GeV < $p_{T}^{t,2}$ < 1000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 170.0 GeV < $p_{T}^{t,2}$ < 290.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 450.0 GeV < $p_{T}^{t,2}$ < 1000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 290.0 GeV < $p_{T}^{t,2}$ < 450.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 450.0 GeV < $p_{T}^{t,2}$ < 1000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 450.0 GeV < $p_{T}^{t,2}$ < 1000.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute double-differential cross-section as a function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ at parton level in the all hadronic resolved topology in 0.0 GeV < $p_{T}^{t,2}$ < 170.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ at parton level in the all hadronic resolved topology in 170.0 GeV < $p_{T}^{t,2}$ < 290.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ at parton level in the all hadronic resolved topology in 290.0 GeV < $p_{T}^{t,2}$ < 450.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ at parton level in the all hadronic resolved topology in 450.0 GeV < $p_{T}^{t,2}$ < 1000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 0.0 GeV < $p_{T}^{t,2}$ < 170.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 0.0 GeV < $p_{T}^{t,2}$ < 170.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 170.0 GeV < $p_{T}^{t,2}$ < 290.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 0.0 GeV < $p_{T}^{t,2}$ < 170.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 170.0 GeV < $p_{T}^{t,2}$ < 290.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 170.0 GeV < $p_{T}^{t,2}$ < 290.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 290.0 GeV < $p_{T}^{t,2}$ < 450.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 0.0 GeV < $p_{T}^{t,2}$ < 170.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 290.0 GeV < $p_{T}^{t,2}$ < 450.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 170.0 GeV < $p_{T}^{t,2}$ < 290.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 290.0 GeV < $p_{T}^{t,2}$ < 450.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 290.0 GeV < $p_{T}^{t,2}$ < 450.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 450.0 GeV < $p_{T}^{t,2}$ < 1000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 0.0 GeV < $p_{T}^{t,2}$ < 170.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 450.0 GeV < $p_{T}^{t,2}$ < 1000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 170.0 GeV < $p_{T}^{t,2}$ < 290.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 450.0 GeV < $p_{T}^{t,2}$ < 1000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 290.0 GeV < $p_{T}^{t,2}$ < 450.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 450.0 GeV < $p_{T}^{t,2}$ < 1000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 450.0 GeV < $p_{T}^{t,2}$ < 1000.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Post-fit background and signal yields in the full signal region. The total systematic uncertainty differs from the sum in quadrature of the different uncertainties due to correlations. Q mis-id refers to the charge misassignment background. Mat. Conv. and Low $m_{\gamma^*}$ refer respectively to events with one non-prompt electron originating from photon conversion in the detector material and to events with a virtual photon leading to an $e^+e^-$ pair. HF $e$ (HF $\mu$) refers to events with one non-prompt electron (muon) from heavy-flavour hadron decay, LF refers to events with a lepton originating from light-meson decay, and 'Other $t\bar{t}X$' includes events coming from $t\bar{t}WZ$, $t\bar{t}Z$+jets, $t\bar{t}WH$, $t\bar{t}HH$.

Ranking of the nuisance parameters included in the fit according to their impact on the signal strength $\mu$. Only the 20 most highly ranked nuisance parameters are shown in the thumbnail figure. The empty blue rectangles correspond to the pre-fit impact on $\mu$ and the filled blue ones to the post-fit impact on $\mu$, both referring to the upper $x$-axis scale. The impact of each nuisance parameter, $\Delta\mu$, is computed by comparing the nominal best-fit value of $\mu$ with the result of the fit when fixing the nuisance parameter to its best-fit value, $\hat{\theta}$, shifted by its pre-fit (post-fit) uncertainties $\pm \Delta\theta$ ($\pm \Delta\hat{\theta}$). The black points show the pulls of the parameter relative to their nominal values, $\theta_0$. The nominal value for all parameters is $\theta_0 = 0$. The pulls of the most impactful parameters and their relative post-fit errors, $\Delta\hat{\theta}/\Delta\theta$, are referenced to the lower $x$-axis scale. In the table, POI means Parameter of Interest.

Comparison between data and prediction before the fit ('Pre-Fit') for the 'HF e' control region. Mat. Conv. and Low $m_{\gamma^*}$ refer respectively to events with one non-prompt electron originating from photon conversion in the detector material and to events with a virtual photon leading to an $e^+e^-$ pair.

Comparison between data and prediction before the fit ('Pre-Fit') for the 'HF mu' control region. Mat. Conv. and Low $m_{\gamma^*}$ refer respectively to events with one non-prompt electron originating from photon conversion in the detector material and to events with a virtual photon leading to an $e^+e^-$ pair.

Comparison between data and prediction before the fit ('Pre-Fit') for the $m_{ee}^{PV}$ variable in the 'Conv.' control region. The first and last bins contain underflow and overflow events, respectively. Q mis-id refers to the charge misassignment background. Mat. Conv. and Low $m_{\gamma^*}$ refer respectively to events with one non-prompt electron originating from photon conversion in the detector material and to events with a virtual photon leading to an $e^+e^-$ pair.

Comparison between data and prediction before the fit ('Pre-Fit') for the $\Sigma p_{T}^{l}$ variable in the 'ttW' control region. The first and last bins contain underflow and overflow events, respectively. Q mis-id refers to the charge misassignment background. Mat. Conv. and Low $m_{\gamma^*}$ refer respectively to events with one non-prompt electron originating from photon conversion in the detector material and to events with a virtual photon leading to an $e^+e^-$ pair.

Comparison between data and prediction after the fit ('Post-Fit') for the 'HF e' control region. Mat. Conv. and Low $m_{\gamma^*}$ refer respectively to events with one non-prompt electron originating from photon conversion in the detector material and to events with a virtual photon leading to an $e^+e^-$ pair.

Comparison between data and prediction after the fit ('Post-Fit') for the 'HF mu' control region. Mat. Conv. and Low $m_{\gamma^*}$ refer respectively to events with one non-prompt electron originating from photon conversion in the detector material and to events with a virtual photon leading to an $e^+e^-$ pair.

Comparison between data and prediction after the fit ('Post-Fit') for the $m_{ee}^{PV}$ variable in the 'Conv.' control region. The first and last bins contain underflow and overflow events, respectively. Q mis-id refers to the charge misassignment background. Mat. Conv. and Low $m_{\gamma^*}$ refer respectively to events with one non-prompt electron originating from photon conversion in the detector material and to events with a virtual photon leading to an $e^+e^-$ pair.

Comparison between data and prediction after the fit ('Post-Fit') for the $\Sigma p_{T}^{l}$ variable in the in 'ttW' control region. The first and last bins contain underflow and overflow events, respectively. Q mis-id refers to the charge misassignment background. Mat. Conv. and Low $m_{\gamma^*}$ refer respectively to events with one non-prompt electron originating from photon conversion in the detector material and to events with a virtual photon leading to an $e^+e^-$ pair.

Comparison between data and prediction before the fit ('Pre-Fit') for the BDT score in the signal region. The first and last bins contain underflow and overflow events, respectively. Q mis-id refers to the charge misassignment background. Mat. Conv. and Low $m_{\gamma^*}$ refer respectively to events with one non-prompt electron originating from photon conversion in the detector material and to events with a virtual photon leading to an $e^+e^-$ pair.

Comparison between data and prediction after the fit ('Post-Fit') for the BDT score in the signal region. The first and last bins contain underflow and overflow events, respectively. Q mis-id refers to the charge misassignment background. Mat. Conv. and Low $m_{\gamma^*}$ refer respectively to events with one non-prompt electron originating from photon conversion in the detector material and to events with a virtual photon leading to an $e^+e^-$ pair.

Correlation matrix of the total uncertainties in the measured fiducial cross section for the observable $p_{\mathrm{T}}^{\mathrm{lead.~lep.}}$

Measured fiducial cross section for $pp\rightarrow W^+W^-$+jets production for the observable $p_{\mathrm{T}}^{\mathrm{sub-lead.~lep.}}$. The second column contains the results obtained with a fiducial particle phase space that includes a veto on $b$-jets. This alternative result is obtained from the nominal result by the application of bin-wise correction that is calculated as the ratio of the predicted differential cross-section in the nominal analysis phase space and the predicted cross-section for a phase space that includes a veto on events with $b$-jets with $p_{\mathrm{T}} > 20$ GeV. Also shown are the Standard Model predictions for $q\bar{q} \rightarrow WW$, obtained from Sherpa 2.2.2, MadGraph 2.3.3 + Pythia 8.212 using FxFx merging, and Powheg MiNLO + Pythia 8.244. These predictions are supplemented by the Sherpa 2.2.2 + OpenLoops simulation of $gg\rightarrow WW$. Finally, the prediction from MATRIX is given, which includes nNLO QCD and NLO EW corrections to $WW$+jet production. Overflow events are included in the last bin. The largest observed value is 609 GeV.

Correlation matrix of the statistical uncertainties in the measured fiducial cross section for the observable $p_{\mathrm{T}}^{\mathrm{sub-lead.~lep.}}$

Correlation matrix of the total uncertainties in the measured fiducial cross section for the observable $p_{\mathrm{T}}^{\mathrm{sub-lead.~lep.}}$

Measured fiducial cross section for $pp\rightarrow W^+W^-$+jets production for the observable $p_{\mathrm{T}}^{\mathrm{lead.~jet}}$. The second column contains the results obtained with a fiducial particle phase space that includes a veto on $b$-jets. This alternative result is obtained from the nominal result by the application of bin-wise correction that is calculated as the ratio of the predicted differential cross-section in the nominal analysis phase space and the predicted cross-section for a phase space that includes a veto on events with $b$-jets with $p_{\mathrm{T}} > 20$ GeV. Also shown are the Standard Model predictions for $q\bar{q} \rightarrow WW$, obtained from Sherpa 2.2.2, MadGraph 2.3.3 + Pythia 8.212 using FxFx merging, and Powheg MiNLO + Pythia 8.244. These predictions are supplemented by the Sherpa 2.2.2 + OpenLoops simulation of $gg\rightarrow WW$. Finally, the prediction from MATRIX is given, which includes nNLO QCD and NLO EW corrections to $WW$+jet production. Overflow events are included in the last bin. The largest observed value is 1485 GeV.

Correlation matrix of the statistical uncertainties in the measured fiducial cross section for the observable $p_{\mathrm{T}}^{\mathrm{lead.~jet}}$

Correlation matrix of the total uncertainties in the measured fiducial cross section for the observable $p_{\mathrm{T}}^{\mathrm{lead.~jet}}$

Measured fiducial cross section for $pp\rightarrow W^+W^-$+jets production for the observable $H_{\mathrm{T}}$. The second column contains the results obtained with a fiducial particle phase space that includes a veto on $b$-jets. This alternative result is obtained from the nominal result by the application of bin-wise correction that is calculated as the ratio of the predicted differential cross-section in the nominal analysis phase space and the predicted cross-section for a phase space that includes a veto on events with $b$-jets with $p_{\mathrm{T}} > 20$ GeV. Also shown are the Standard Model predictions for $q\bar{q} \rightarrow WW$, obtained from Sherpa 2.2.2, MadGraph 2.3.3 + Pythia 8.212 using FxFx merging, and Powheg MiNLO + Pythia 8.244. These predictions are supplemented by the Sherpa 2.2.2 + OpenLoops simulation of $gg\rightarrow WW$. Finally, the prediction from MATRIX is given, which includes nNLO QCD and NLO EW corrections to $WW$+jet production. Overflow events are included in the last bin. The largest observed value is 2969 GeV.

Correlation matrix of the statistical uncertainties in the measured fiducial cross section for the observable $H_{\mathrm{T}}$

Correlation matrix of the total uncertainties in the measured fiducial cross section for the observable $H_{\mathrm{T}}$

Measured fiducial cross section for $pp\rightarrow W^+W^-$+jets production for the observable $S_{\mathrm{T}}$. The second column contains the results obtained with a fiducial particle phase space that includes a veto on $b$-jets. This alternative result is obtained from the nominal result by the application of bin-wise correction that is calculated as the ratio of the predicted differential cross-section in the nominal analysis phase space and the predicted cross-section for a phase space that includes a veto on events with $b$-jets with $p_{\mathrm{T}} > 20$ GeV. Also shown are the Standard Model predictions for $q\bar{q} \rightarrow WW$, obtained from Sherpa 2.2.2, MadGraph 2.3.3 + Pythia 8.212 using FxFx merging, and Powheg MiNLO + Pythia 8.244. These predictions are supplemented by the Sherpa 2.2.2 + OpenLoops simulation of $gg\rightarrow WW$. Finally, the prediction from MATRIX is given, which includes nNLO QCD and NLO EW corrections to $WW$+jet production. Overflow events are included in the last bin. The largest observed value is 3296 GeV.

Correlation matrix of the statistical uncertainties in the measured fiducial cross section for the observable $S_{\mathrm{T}}$

Correlation matrix of the total uncertainties in the measured fiducial cross section for the observable $S_{\mathrm{T}}$

Measured fiducial cross section for $pp\rightarrow W^+W^-$+jets production for the observable $m_{\mathrm{T},e\mu}$. The second column contains the results obtained with a fiducial particle phase space that includes a veto on $b$-jets. This alternative result is obtained from the nominal result by the application of bin-wise correction that is calculated as the ratio of the predicted differential cross-section in the nominal analysis phase space and the predicted cross-section for a phase space that includes a veto on events with $b$-jets with $p_{\mathrm{T}} > 20$ GeV. Also shown are the Standard Model predictions for $q\bar{q} \rightarrow WW$, obtained from Sherpa 2.2.2, MadGraph 2.3.3 + Pythia 8.212 using FxFx merging, and Powheg MiNLO + Pythia 8.244. These predictions are supplemented by the Sherpa 2.2.2 + OpenLoops simulation of $gg\rightarrow WW$. Finally, the prediction from MATRIX is given, which includes nNLO QCD and NLO EW corrections to $WW$+jet production. Overflow events are included in the last bin. The largest observed value is 4130 GeV.

Correlation matrix of the statistical uncertainties in the measured fiducial cross section for the observable $m_{\mathrm{T},e\mu}$

Correlation matrix of the total uncertainties in the measured fiducial cross section for the observable $m_{\mathrm{T},e\mu}$

Measured fiducial cross section for $pp\rightarrow W^+W^-$+jets production for the observable $m_{e\mu}$. The second column contains the results obtained with a fiducial particle phase space that includes a veto on $b$-jets. This alternative result is obtained from the nominal result by the application of bin-wise correction that is calculated as the ratio of the predicted differential cross-section in the nominal analysis phase space and the predicted cross-section for a phase space that includes a veto on events with $b$-jets with $p_{\mathrm{T}} > 20$ GeV. Also shown are the Standard Model predictions for $q\bar{q} \rightarrow WW$, obtained from Sherpa 2.2.2, MadGraph 2.3.3 + Pythia 8.212 using FxFx merging, and Powheg MiNLO + Pythia 8.244. These predictions are supplemented by the Sherpa 2.2.2 + OpenLoops simulation of $gg\rightarrow WW$. Finally, the prediction from MATRIX is given, which includes nNLO QCD and NLO EW corrections to $WW$+jet production. Overflow events are included in the last bin. The largest observed value is 3519 GeV.

Correlation matrix of the statistical uncertainties in the measured fiducial cross section for the observable $m_{e\mu}$

Correlation matrix of the total uncertainties in the measured fiducial cross section for the observable $m_{e\mu}$

Measured fiducial cross section for $pp\rightarrow W^+W^-$+jets production for the observable $p_{\mathrm{T},e\mu}$. The second column contains the results obtained with a fiducial particle phase space that includes a veto on $b$-jets. This alternative result is obtained from the nominal result by the application of bin-wise correction that is calculated as the ratio of the predicted differential cross-section in the nominal analysis phase space and the predicted cross-section for a phase space that includes a veto on events with $b$-jets with $p_{\mathrm{T}} > 20$ GeV. Also shown are the Standard Model predictions for $q\bar{q} \rightarrow WW$, obtained from Sherpa 2.2.2, MadGraph 2.3.3 + Pythia 8.212 using FxFx merging, and Powheg MiNLO + Pythia 8.244. These predictions are supplemented by the Sherpa 2.2.2 + OpenLoops simulation of $gg\rightarrow WW$. Finally, the prediction from MATRIX is given, which includes nNLO QCD and NLO EW corrections to $WW$+jet production. Overflow events are included in the last bin. The largest observed value is 1067 GeV.

Correlation matrix of the statistical uncertainties in the measured fiducial cross section for the observable $p_{\mathrm{T},e\mu}$

Correlation matrix of the total uncertainties in the measured fiducial cross section for the observable $p_{\mathrm{T},e\mu}$

Measured fiducial cross section for $pp\rightarrow W^+W^-$+jets production for the observable $\Delta\phi(e,\mu)$. The second column contains the results obtained with a fiducial particle phase space that includes a veto on $b$-jets. This alternative result is obtained from the nominal result by the application of bin-wise correction that is calculated as the ratio of the predicted differential cross-section in the nominal analysis phase space and the predicted cross-section for a phase space that includes a veto on events with $b$-jets with $p_{\mathrm{T}} > 20$ GeV. Also shown are the Standard Model predictions for $q\bar{q} \rightarrow WW$, obtained from Sherpa 2.2.2, MadGraph 2.3.3 + Pythia 8.212 using FxFx merging, and Powheg MiNLO + Pythia 8.244. These predictions are supplemented by the Sherpa 2.2.2 + OpenLoops simulation of $gg\rightarrow WW$. Finally, the prediction from MATRIX is given, which includes nNLO QCD and NLO EW corrections to $WW$+jet production.

Correlation matrix of the statistical uncertainties in the measured fiducial cross section for the observable $\Delta\phi(e,\mu)$

Correlation matrix of the total uncertainties in the measured fiducial cross section for the observable $\Delta\phi(e,\mu)$

Measured fiducial cross section for $pp\rightarrow W^+W^-$+jets production for the observable $y_{e\mu}$. The second column contains the results obtained with a fiducial particle phase space that includes a veto on $b$-jets. This alternative result is obtained from the nominal result by the application of bin-wise correction that is calculated as the ratio of the predicted differential cross-section in the nominal analysis phase space and the predicted cross-section for a phase space that includes a veto on events with $b$-jets with $p_{\mathrm{T}} > 20$ GeV. Also shown are the Standard Model predictions for $q\bar{q} \rightarrow WW$, obtained from Sherpa 2.2.2, MadGraph 2.3.3 + Pythia 8.212 using FxFx merging, and Powheg MiNLO + Pythia 8.244. These predictions are supplemented by the Sherpa 2.2.2 + OpenLoops simulation of $gg\rightarrow WW$. Finally, the prediction from MATRIX is given, which includes nNLO QCD and NLO EW corrections to $WW$+jet production.

Correlation matrix of the statistical uncertainties in the measured fiducial cross section for the observable $y_{e\mu}$

Correlation matrix of the total uncertainties in the measured fiducial cross section for the observable $y_{e\mu}$

Measured fiducial cross section for $pp\rightarrow W^+W^-$+jets production for the observable $\cos\theta^*$. The second column contains the results obtained with a fiducial particle phase space that includes a veto on $b$-jets. This alternative result is obtained from the nominal result by the application of bin-wise correction that is calculated as the ratio of the predicted differential cross-section in the nominal analysis phase space and the predicted cross-section for a phase space that includes a veto on events with $b$-jets with $p_{\mathrm{T}} > 20$ GeV. Also shown are the Standard Model predictions for $q\bar{q} \rightarrow WW$, obtained from Sherpa 2.2.2, MadGraph 2.3.3 + Pythia 8.212 using FxFx merging, and Powheg MiNLO + Pythia 8.244. These predictions are supplemented by the Sherpa 2.2.2 + OpenLoops simulation of $gg\rightarrow WW$. Finally, the prediction from MATRIX is given, which includes nNLO QCD and NLO EW corrections to $WW$+jet production.

Correlation matrix of the statistical uncertainties in the measured fiducial cross section for the observable $\cos\theta^*$

Correlation matrix of the total uncertainties in the measured fiducial cross section for the observable $\cos\theta^*$

Measured fiducial cross section for $pp\rightarrow W^+W^-$+jets production for the observable $n_{\mathrm{jet}}$. The second column contains the results obtained with a fiducial particle phase space that includes a veto on $b$-jets. This alternative result is obtained from the nominal result by the application of bin-wise correction that is calculated as the ratio of the predicted differential cross-section in the nominal analysis phase space and the predicted cross-section for a phase space that includes a veto on events with $b$-jets with $p_{\mathrm{T}} > 20$ GeV. Also shown are the Standard Model predictions for $q\bar{q} \rightarrow WW$, obtained from Sherpa 2.2.2, MadGraph 2.3.3 + Pythia 8.212 using FxFx merging, and Powheg MiNLO + Pythia 8.244. These predictions are supplemented by the Sherpa 2.2.2 + OpenLoops simulation of $gg\rightarrow WW$. Finally, the prediction from MATRIX is given, which includes nNLO QCD and NLO EW corrections to $WW$+jet production.

Correlation matrix of the statistical uncertainties in the measured fiducial cross section for the observable $n_{\mathrm{jet}}$

Correlation matrix of the total uncertainties in the measured fiducial cross section for the observable $n_{\mathrm{jet}}$

Measured fiducial cross section for $pp\rightarrow W^+W^-$+jets production for the observable $m_{e\mu}$ for $p_{\mathrm{T}}^{\mathrm{lead.~jet}} > 200$ GeV. The second column contains the results obtained with a fiducial particle phase space that includes a veto on $b$-jets. This alternative result is obtained from the nominal result by the application of bin-wise correction that is calculated as the ratio of the predicted differential cross-section in the nominal analysis phase space and the predicted cross-section for a phase space that includes a veto on events with $b$-jets with $p_{\mathrm{T}} > 20$ GeV. Also shown are the Standard Model predictions for $q\bar{q} \rightarrow WW$, obtained from Sherpa 2.2.2, MadGraph 2.3.3 + Pythia 8.212 using FxFx merging, and Powheg MiNLO + Pythia 8.244. These predictions are supplemented by the Sherpa 2.2.2 + OpenLoops simulation of $gg\rightarrow WW$. Finally, the prediction from MATRIX is given, which includes nNLO QCD and NLO EW corrections to $WW$+jet production. Overflow events are included in the last bin. The largest observed value is 3519 GeV.

Correlation matrix of the statistical uncertainties in the measured fiducial cross section for the observable $m_{e\mu}$

Correlation matrix of the total uncertainties in the measured fiducial cross section for the observable $m_{e\mu}$

Measured fiducial cross section for $pp\rightarrow W^+W^-$+jets production for the observable $\Delta\phi(e,\mu)$ for $p_{\mathrm{T}}^{\mathrm{lead.~jet}} > 200$ GeV. The second column contains the results obtained with a fiducial particle phase space that includes a veto on $b$-jets. This alternative result is obtained from the nominal result by the application of bin-wise correction that is calculated as the ratio of the predicted differential cross-section in the nominal analysis phase space and the predicted cross-section for a phase space that includes a veto on events with $b$-jets with $p_{\mathrm{T}} > 20$ GeV. Also shown are the Standard Model predictions for $q\bar{q} \rightarrow WW$, obtained from Sherpa 2.2.2, MadGraph 2.3.3 + Pythia 8.212 using FxFx merging, and Powheg MiNLO + Pythia 8.244. These predictions are supplemented by the Sherpa 2.2.2 + OpenLoops simulation of $gg\rightarrow WW$. Finally, the prediction from MATRIX is given, which includes nNLO QCD and NLO EW corrections to $WW$+jet production.

Correlation matrix of the statistical uncertainties in the measured fiducial cross section for the observable $\Delta\phi(e,\mu)$

Correlation matrix of the total uncertainties in the measured fiducial cross section for the observable $\Delta\phi(e,\mu)$

Measured fiducial cross section for $pp\rightarrow W^+W^-$+jets production for the observable $\Delta\phi(\mathrm{sub-lead.~lep.}, \mathrm{lead.~jet})$ for $p_{\mathrm{T}}^{\mathrm{lead.~lep.}} > 200$ GeV. The second column contains the results obtained with a fiducial particle phase space that includes a veto on $b$-jets. This alternative result is obtained from the nominal result by the application of bin-wise correction that is calculated as the ratio of the predicted differential cross-section in the nominal analysis phase space and the predicted cross-section for a phase space that includes a veto on events with $b$-jets with $p_{\mathrm{T}} > 20$ GeV. Also shown are the Standard Model predictions for $q\bar{q} \rightarrow WW$, obtained from Sherpa 2.2.2, MadGraph 2.3.3 + Pythia 8.212 using FxFx merging, and Powheg MiNLO + Pythia 8.244. These predictions are supplemented by the Sherpa 2.2.2 + OpenLoops simulation of $gg\rightarrow WW$. Finally, the prediction from MATRIX is given, which includes nNLO QCD and NLO EW corrections to $WW$+jet production.

Correlation matrix of the statistical uncertainties in the measured fiducial cross section for the observable $\Delta\phi(\mathrm{sub-lead.~lep.}, \mathrm{lead.~jet})$

Correlation matrix of the total uncertainties in the measured fiducial cross section for the observable $\Delta\phi(\mathrm{sub-lead.~lep.}, \mathrm{lead.~jet})$

Measured fiducial cross section for $pp\rightarrow W^+W^-$+jets production for the observable $\Delta R(\mathrm{sub-lead.~lep.}, \mathrm{lead.~jet})$ for $p_{\mathrm{T}}^{\mathrm{lead.~lep.}} > 200$ GeV. The second column contains the results obtained with a fiducial particle phase space that includes a veto on $b$-jets. This alternative result is obtained from the nominal result by the application of bin-wise correction that is calculated as the ratio of the predicted differential cross-section in the nominal analysis phase space and the predicted cross-section for a phase space that includes a veto on events with $b$-jets with $p_{\mathrm{T}} > 20$ GeV. Also shown are the Standard Model predictions for $q\bar{q} \rightarrow WW$, obtained from Sherpa 2.2.2, MadGraph 2.3.3 + Pythia 8.212 using FxFx merging, and Powheg MiNLO + Pythia 8.244. These predictions are supplemented by the Sherpa 2.2.2 + OpenLoops simulation of $gg\rightarrow WW$. Finally, the prediction from MATRIX is given, which includes nNLO QCD and NLO EW corrections to $WW$+jet production.

Correlation matrix of the statistical uncertainties in the measured fiducial cross section for the observable $\Delta R(\mathrm{sub-lead.~lep.}, \mathrm{lead.~jet})$

Correlation matrix of the total uncertainties in the measured fiducial cross section for the observable $\Delta R(\mathrm{sub-lead.~lep.}, \mathrm{lead.~jet})$

Measured fiducial cross section for $pp\rightarrow W^+W^-$+jets production for the observable $p_{\mathrm{T}}^{\mathrm{sub-lead.~lep.}} / p_{\mathrm{T}}^{\mathrm{lead.~lep.}}$ for $p_{\mathrm{T}}^{\mathrm{lead.~lep.}} > 200$ GeV. The second column contains the results obtained with a fiducial particle phase space that includes a veto on $b$-jets. This alternative result is obtained from the nominal result by the application of bin-wise correction that is calculated as the ratio of the predicted differential cross-section in the nominal analysis phase space and the predicted cross-section for a phase space that includes a veto on events with $b$-jets with $p_{\mathrm{T}} > 20$ GeV. Also shown are the Standard Model predictions for $q\bar{q} \rightarrow WW$, obtained from Sherpa 2.2.2, MadGraph 2.3.3 + Pythia 8.212 using FxFx merging, and Powheg MiNLO + Pythia 8.244. These predictions are supplemented by the Sherpa 2.2.2 + OpenLoops simulation of $gg\rightarrow WW$. Finally, the prediction from MATRIX is given, which includes nNLO QCD and NLO EW corrections to $WW$+jet production.

Correlation matrix of the statistical uncertainties in the measured fiducial cross section for the observable $p_{\mathrm{T}}^{\mathrm{sub-lead.~lep.}} / p_{\mathrm{T}}^{\mathrm{lead.~lep.}}$

Correlation matrix of the total uncertainties in the measured fiducial cross section for the observable $p_{\mathrm{T}}^{\mathrm{sub-lead.~lep.}} / p_{\mathrm{T}}^{\mathrm{lead.~lep.}}$

Measured fiducial cross section for $pp\rightarrow W^+W^-$+jets production for the observable $p_{\mathrm{T}}^{\mathrm{sub-lead.~lep.}} / p_{\mathrm{T}}^{\mathrm{lead.~jet}}$ for $p_{\mathrm{T}}^{\mathrm{lead.~lep.}} > 200$ GeV. The second column contains the results obtained with a fiducial particle phase space that includes a veto on $b$-jets. This alternative result is obtained from the nominal result by the application of bin-wise correction that is calculated as the ratio of the predicted differential cross-section in the nominal analysis phase space and the predicted cross-section for a phase space that includes a veto on events with $b$-jets with $p_{\mathrm{T}} > 20$ GeV. Also shown are the Standard Model predictions for $q\bar{q} \rightarrow WW$, obtained from Sherpa 2.2.2, MadGraph 2.3.3 + Pythia 8.212 using FxFx merging, and Powheg MiNLO + Pythia 8.244. These predictions are supplemented by the Sherpa 2.2.2 + OpenLoops simulation of $gg\rightarrow WW$. Finally, the prediction from MATRIX is given, which includes nNLO QCD and NLO EW corrections to $WW$+jet production. The largest observed value is 19.6.

Correlation matrix of the statistical uncertainties in the measured fiducial cross section for the observable $p_{\mathrm{T}}^{\mathrm{sub-lead.~lep.}} / p_{\mathrm{T}}^{\mathrm{lead.~jet}}$

Correlation matrix of the total uncertainties in the measured fiducial cross section for the observable $p_{\mathrm{T}}^{\mathrm{sub-lead.~lep.}} / p_{\mathrm{T}}^{\mathrm{lead.~jet}}$