The ratio of pPb to pp $\eta_{\mathrm{dijet}}$ spectra for dijets in the range $75 < p_{\mathrm{T}}^{\mathrm{ave}} < 95$ GeV.

The ratio of pPb to pp $\eta_{\mathrm{dijet}}$ spectra for dijets in the range $95 < p_{\mathrm{T}}^{\mathrm{ave}} < 115$ GeV.

The ratio of pPb to pp $\eta_{\mathrm{dijet}}$ spectra for dijets in the range $95 < p_{\mathrm{T}}^{\mathrm{ave}} < 115$ GeV.

The ratio of pPb to pp $\eta_{\mathrm{dijet}}$ spectra for dijets in the range $115 < p_{\mathrm{T}}^{\mathrm{ave}} < 150$ GeV.

The ratio of pPb to pp $\eta_{\mathrm{dijet}}$ spectra for dijets in the range $115 < p_{\mathrm{T}}^{\mathrm{ave}} < 150$ GeV.

The ratio of pPb to pp $\eta_{\mathrm{dijet}}$ spectra for dijets in the range $p_{\mathrm{T}}^{\mathrm{ave}} > 150$ GeV.

The ratio of pPb to pp $\eta_{\mathrm{dijet}}$ spectra for dijets in the range $p_{\mathrm{T}}^{\mathrm{ave}} > 150$ GeV.

The ratio of theory to data, for the ratio of the pPb to pp $\eta_{\mathrm{dijet}}$ spectra for $115 < p_{\mathrm{T}}^{\mathrm{ave}} < 150$ GeV. The total uncertainties on the data points are provided in the column entitled 'DATA UNCERTAINTIES'. The theory points are from the NLO pQCD calculations of DSSZ, EPS09, nCTEQ15, and EPPS16 nPDFs, using CT14 as the baseline PDF.

The ratio of theory to data, for the ratio of the pPb to pp $\eta_{\mathrm{dijet}}$ spectra for $115 < p_{\mathrm{T}}^{\mathrm{ave}} < 150$ GeV. The total uncertainties on the data points are provided in the column entitled 'DATA UNCERTAINTIES'. The theory points are from the NLO pQCD calculations of DSSZ, EPS09, nCTEQ15, and EPPS16 nPDFs, using CT14 as the baseline PDF.

The measured pp dijet pseudorapidity spectra, shifted to match the $\eta_{\mathrm{dijet}}$ range of the pPb collisions, for $55 < p_{\mathrm{T}}^{\mathrm{ave}} < 75$ GeV.

The measured pp dijet pseudorapidity spectra, shifted to match the $\eta_{\mathrm{dijet}}$ range of the pPb collisions, for $55 < p_{\mathrm{T}}^{\mathrm{ave}} < 75$ GeV.

The measured pp dijet pseudorapidity spectra, shifted to match the $\eta_{\mathrm{dijet}}$ range of the pPb collisions, for $75 < p_{\mathrm{T}}^{\mathrm{ave}} < 95$ GeV.

The measured pp dijet pseudorapidity spectra, shifted to match the $\eta_{\mathrm{dijet}}$ range of the pPb collisions, for $75 < p_{\mathrm{T}}^{\mathrm{ave}} < 95$ GeV.

The measured pp dijet pseudorapidity spectra, shifted to match the $\eta_{\mathrm{dijet}}$ range of the pPb collisions, for $95 < p_{\mathrm{T}}^{\mathrm{ave}} < 115$ GeV.

The measured pp dijet pseudorapidity spectra, shifted to match the $\eta_{\mathrm{dijet}}$ range of the pPb collisions, for $95 < p_{\mathrm{T}}^{\mathrm{ave}} < 115$ GeV.

The measured pp dijet pseudorapidity spectra, shifted to match the $\eta_{\mathrm{dijet}}$ range of the pPb collisions, for $115 < p_{\mathrm{T}}^{\mathrm{ave}} < 150$ GeV.

The measured pp dijet pseudorapidity spectra, shifted to match the $\eta_{\mathrm{dijet}}$ range of the pPb collisions, for $115 < p_{\mathrm{T}}^{\mathrm{ave}} < 150$ GeV.

The measured pp dijet pseudorapidity spectra, shifted to match the $\eta_{\mathrm{dijet}}$ range of the pPb collisions, for $55 < p_{\mathrm{T}}^{\mathrm{ave}} < 75$ GeV.

The measured pp dijet pseudorapidity spectra, shifted to match the $\eta_{\mathrm{dijet}}$ range of the pPb collisions, for $55 < p_{\mathrm{T}}^{\mathrm{ave}} < 75$ GeV.

The measured pPb dijet pseudorapidity spectra for $55 < p_{\mathrm{T}}^{\mathrm{ave}} < 75$ GeV using the CT14 as the baseline PDF.

The measured pPb dijet pseudorapidity spectra for $55 < p_{\mathrm{T}}^{\mathrm{ave}} < 75$ GeV using the CT14 as the baseline PDF.

The measured pPb dijet pseudorapidity spectra for $75 < p_{\mathrm{T}}^{\mathrm{ave}} < 95$ GeV using the CT14 as the baseline PDF.

The measured pPb dijet pseudorapidity spectra for $75 < p_{\mathrm{T}}^{\mathrm{ave}} < 95$ GeV using the CT14 as the baseline PDF.

The measured pPb dijet pseudorapidity spectra for $95 < p_{\mathrm{T}}^{\mathrm{ave}} < 115$ GeV using the CT14 as the baseline PDF.

The measured pPb dijet pseudorapidity spectra for $95 < p_{\mathrm{T}}^{\mathrm{ave}} < 115$ GeV using the CT14 as the baseline PDF.

The measured pPb dijet pseudorapidity spectra for $115 < p_{\mathrm{T}}^{\mathrm{ave}} < 150$ GeV using the CT14 as the baseline PDF.

The measured pPb dijet pseudorapidity spectra for $115 < p_{\mathrm{T}}^{\mathrm{ave}} < 150$ GeV using the CT14 as the baseline PDF.

The measured pPb dijet pseudorapidity spectra for $p_{\mathrm{T}}^{\mathrm{ave}} > 150$ GeV using the CT14 as the baseline PDF.

The measured pPb dijet pseudorapidity spectra for $p_{\mathrm{T}}^{\mathrm{ave}} > 150$ GeV using the CT14 as the baseline PDF.

The measured pPb dijet pseudorapidity spectra for $55 < p_{\mathrm{T}}^{\mathrm{ave}} < 75$ GeV using the MMHT14 as the baseline PDF.

The measured pPb dijet pseudorapidity spectra for $55 < p_{\mathrm{T}}^{\mathrm{ave}} < 75$ GeV using the MMHT14 as the baseline PDF.

The measured pPb dijet pseudorapidity spectra for $75 < p_{\mathrm{T}}^{\mathrm{ave}} < 95$ GeV using the MMHT14 as the baseline PDF.

The measured pPb dijet pseudorapidity spectra for $75 < p_{\mathrm{T}}^{\mathrm{ave}} < 95$ GeV using the MMHT14 as the baseline PDF.

The measured pPb dijet pseudorapidity spectra for $95 < p_{\mathrm{T}}^{\mathrm{ave}} < 115$ GeV using the MMHT14 as the baseline PDF.

The measured pPb dijet pseudorapidity spectra for $95 < p_{\mathrm{T}}^{\mathrm{ave}} < 115$ GeV using the MMHT14 as the baseline PDF.

The measured pPb dijet pseudorapidity spectra for $115 < p_{\mathrm{T}}^{\mathrm{ave}} < 150$ GeV using the MMHT14 as the baseline PDF.

The measured pPb dijet pseudorapidity spectra for $115 < p_{\mathrm{T}}^{\mathrm{ave}} < 150$ GeV using the MMHT14 as the baseline PDF.

The measured pPb dijet pseudorapidity spectra for $p_{\mathrm{T}}^{\mathrm{ave}} > 150$ GeV using the MMHT14 as the baseline PDF.

The measured pPb dijet pseudorapidity spectra for $p_{\mathrm{T}}^{\mathrm{ave}} > 150$ GeV using the MMHT14 as the baseline PDF.

Differential cross section (multiplied by the dimuon branching fraction) of prompt $\psi$(2S) mesons in pPb collisions at $\sqrt(s_{\textrm{NN}})=5.02 $ TeV, as a function of $p_{\textrm{T}}$, for three forward $y_{\mathrm{CM}}$ regions. The fully correlated luminosity uncertainty of 3.5% is not included in the point-by-point uncertainty. NOTE- The cross section unit is nb (nano barn); the y-axes of the figures in the publication show pb (pico barn) by mistake.

Differential cross section (multiplied by the dimuon branching fraction) of prompt $\psi$(2S) mesons in pp collisions at $\sqrt(s_{\textrm{NN}})=5.02 $ TeV, as a function of $p_{\textrm{T}}$, for four $y_{\mathrm{CM}}$ regions. The fully correlated luminosity uncertainty of 2.3% is not inlcuded in the point-by-point uncertainty.

Differential cross section (multiplied by the dimuon branching fraction) of prompt $\psi$(2S) mesons in pp collisions at $\sqrt(s)=5.02 $ TeV, as a function of $p_{\textrm{T}}$, for four $y_{\mathrm{CM}}$ regions. The fully correlated luminosity uncertainty of 2.3% is not included in the point-by-point uncertainty. NOTE- The cross section unit is nb (nano barn); the y-axes of the figures in the publication show pb (pico barn) by mistake.

Rapidity dependence of $R_{\mathrm{pPb}}$ for prompt $\psi$(2S) mesons at $\sqrt(s_{\textrm{NN}})=5.02 $ TeV, in three $p_{\mathrm{T}}$ ranges. The fully correlated global uncertainty of 4.2% is not inlcuded in the point-by-point uncertainty.

Rapidity dependence of $R_{\mathrm{pPb}}$ for prompt $\psi$(2S) mesons at $\sqrt(s_{\textrm{NN}})=5.02 $ TeV, in three $p_{\mathrm{T}}$ ranges. The fully correlated global uncertainty of 4.2% is not included in the point-by-point uncertainty.

Transverse momentum dependence of $R_{\mathrm{pPb}}$ for prompt $\psi$(2S) mesons at $\sqrt(s_{\textrm{NN}})=5.02 $ TeV, in seven $y_{\mathrm{CM}}$ ranges. The fully correlated global uncertainty of 4.2% is not inlcuded in the point-by-point uncertainty.

Transverse momentum dependence of $R_{\mathrm{pPb}}$ for prompt $\psi$(2S) mesons at $\sqrt(s_{\textrm{NN}})=5.02 $ TeV, in seven $y_{\mathrm{CM}}$ ranges. The fully correlated global uncertainty of 4.2% is not incuded in the point-by-point uncertainty.

Bin-to-bin correlation in the measured cross section for Z+jets as a function of inclusive jet multiplicity, $N_{\text{jets}}^{\text{min}}$.

Measured cross section for Z+jets as a function of the transverse momementum of the Z boson, $p_{\text{T}}(\text{Z})$, for events with at least one jet and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured cross section for Z+jets as a function of the transverse momementum of the Z boson, $p_{\text{T}}(\text{Z})$, for events with at least one jet.

Measured cross section for Z+jets as a function of the transverse momenum of the first jet, $p_{\text{T}}(\text{j}_1)$, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured cross section for Z+jets as a function of the transverse momenum of the first jet, $p_{\text{T}}(\text{j}_1)$.

Measured cross section for Z+jets as a function of the transverse momenum of the second jet, $p_{\text{T}}(\text{j}_2)$, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured cross section for Z+jets as a function of the transverse momenum of the second jet, $p_{\text{T}}(\text{j}_2)$.

Measured cross section for Z+jets as a function of the transverse momenum of the third jet, $p_{\text{T}}(\text{j}_3)$, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured cross section for Z+jets as a function of the transverse momenum of the third jet, $p_{\text{T}}(\text{j}_3)$.

Measured cross section for Z+jets as a function of the absolute rapidity of the first jet, $|y(\text{j}_1)|$, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured cross section for Z+jets as a function of the absolute rapidity of the first jet, $|y(\text{j}_1)|$.

Measured cross section for Z+jets as a function of the absolute rapidity of the second jet, $|y(\text{j}_2)|$, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured cross section for Z+jets as a function of the absolute rapidity of the second jet, $|y(\text{j}_2)|$.

Measured cross section for Z+jets as a function of the absolute rapidity of the third jet, $|y(\text{j}_3)|$, and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured cross section for Z+jets as a function of the absolute rapidity of the third jet, $|y(\text{j}_3)|$.

Measured cross section for Z+jets as a function of the $H_{\text{T}}$ observable for event with at least one jet and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured cross section for Z+jets as a function of the $H_{\text{T}}$ observable for event with at least one jet.

Measured cross section for Z+jets as a function of the $H_{\text{T}}$ observable for event with at least two jets and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured cross section for Z+jets as a function of the $H_{\text{T}}$ observable for event with at least two jets.

Measured cross section for Z+jets as a function of the $H_{\text{T}}$ observable for event with at least three jets and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured cross section for Z+jets as a function of the $H_{\text{T}}$ observable for event with at least three jets.

Measured cross section for Z+jets as a function of the transverse momentum balance between the Z boson and the accompanying jets, $p_{\text{T}}^{\text{bal}}$, for events with at least one jet and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured cross section for Z+jets as a function of the transverse momentum balance between the Z boson and the accompanying jets, $p_{\text{T}}^{\text{bal}}$, for events with at least one jet.

Measured cross section for Z+jets as a function of the transverse momentum balance between the Z boson and the accompanying jets, $p_{\text{T}}^{\text{bal}}$, for events with at least two jets and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured cross section for Z+jets as a function of the transverse momentum balance between the Z boson and the accompanying jets, $p_{\text{T}}^{\text{bal}}$, for events with at least two jets.

Measured cross section for Z+jets as a function of the transverse momentum balance between the Z boson and the accompanying jets, $p_{\text{T}}^{\text{bal}}$, for events with at least three jets and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured cross section for Z+jets as a function of the transverse momentum balance between the Z boson and the accompanying jets, $p_{\text{T}}^{\text{bal}}$, for events with at least three jets.

Measured cross section for Z+jets as a function of the JZB variable with no restriction on $p_{\text{T}}(\text{Z})$ and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured cross section for Z+jets as a function of the JZB variable with no restriction on $p_{\text{T}}(\text{Z})$.

Measured cross section for Z+jets as a function of the JZB variable for $p_{\text{T}}(\text{Z})\leq50\,$GeV) and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured cross section for Z+jets as a function of the JZB variable for $p_{\text{T}}(\text{Z})\leq50\,$GeV).

Measured cross section for Z+jets as a function of the JZB variable for $p_{\text{T}}(\text{Z})>50\,$GeV and breakdown of the relative uncertainty.

Bin-to-bin correlation in the measured cross section for Z+jets as a function of the JZB variable for $p_{\text{T}}(\text{Z})>50\,$GeV.

Expected and observed upper limits at the 95% CL on the pp --> X --> ZZ cross section as a function of $m_X$ with $\Gamma_X$=10 GeV in VBF production mode.

Expected and observed upper limits at the 95% CL on the pp --> X --> ZZ cross section as a function of $m_X$ with $\Gamma_X$=100 GeV with VBF fraction profiled.

Expected and observed upper limits at the 95% CL on the pp --> X --> ZZ cross section as a function of $m_X$ with $\Gamma_X$=100 GeV in VBF production mode.

Observed upper limits at the 95% CL on the pp --> X --> ZZ cross section as a function of $m_X$ and $\Gamma_X$ values when VBF fraction is profiled.

Observed upper limits at the 95% CL on the pp --> X --> ZZ cross section as a function of $m_X$ and $\Gamma_X$ values in VBF production mode.

Distribution of $m_{jj}$ in data and simulation for events in the signal regions of the low-mass search. The points show the data while the filled histograms show the background contributions. The gray band shows the statistical and systematic uncertainties in the background, while the dashed vertical region ("Higgs") shows the expected SM Higgs boson mass range, which is excluded from this analysis. A 600 GeV bulk graviton signal prediction is represented by the black dashed histogram; for visibility, the signal cross-section is increased by a factor of 50. The background normalization is derived from the final fit to the $m_{VZ}$ observable in data.

The m$_{j}$ distributions of the events in data, compared to the expected background shape, for the high-mass analysis in the electron channel, for the high-purity category. The expected background shape is extracted from a fit to the data sidebands (Z+jets) or derived from simulation ("top quark" and "VV"). The dashed region around the background sum represents the uncertainty in the Z+jets distribution, while the dashed vertical region ("Higgs") shows the expected SM Higgs boson mass range, excluded from the analysis.

The m$_{j}$ distributions of the events in data, compared to the expected background shape, for the high-mass analysis in the electron channel, for the low-purity category. The expected background shape is extracted from a fit to the data sidebands (Z+jets) or derived from simulation ("top quark" and "VV"). The dashed region around the background sum represents the uncertainty in the Z+jets distribution, while the dashed vertical region ("Higgs") shows the expected SM Higgs boson mass range, excluded from the analysis.

The m$_{j}$ distributions of the events in data, compared to the expected background shape, for the high-mass analysis in the muon channel, for the high-purity category. The expected background shape is extracted from a fit to the data sidebands (Z+jets) or derived from simulation ("top quark" and "VV"). The dashed region around the background sum represents the uncertainty in the Z+jets distribution, while the dashed vertical region ("Higgs") shows the expected SM Higgs boson mass range, excluded from the analysis.

The m$_{j}$ distributions of the events in data, compared to the expected background shape, for the high-mass analysis in the muon channel, for the low-purity category. The expected background shape is extracted from a fit to the data sidebands (Z+jets) or derived from simulation ("top quark" and "VV"). The dashed region around the background sum represents the uncertainty in the Z+jets distribution, while the dashed vertical region ("Higgs") shows the expected SM Higgs boson mass range, excluded from the analysis.

Expected and observed distributions of the resonance candidate mass $m_{\text{VZ}}$ in the high-mass analysis, in the electron channel, high-purity category. The shaded area represents the post-fit uncertainty in the background. The expected contribution from W' signal candidates with mass $m_{\text{X}} = 2000$ GeV, normalized to a cross section of 100 fb$^{-1}$, is also shown.

Expected and observed distributions of the resonance candidate mass $m_{\text{VZ}}$ in the high-mass analysis, in the electron channel, low-purity category. The shaded area represents the post-fit uncertainty in the background. The expected contribution from W' signal candidates with mass $m_{\text{X}} = 2000$ GeV, normalized to a cross section of 100 fb$^{-1}$, is also shown.

Expected and observed distributions of the resonance candidate mass $m_{\text{VZ}}$ in the high-mass analysis, in the muon channel, high-purity category. The shaded area represents the post-fit uncertainty in the background. The expected contribution from W' signal candidates with mass $m_{\text{X}} = 2000$ GeV, normalized to a cross section of 100 fb$^{-1}$, is also shown.

Expected and observed distributions of the resonance candidate mass $m_{\text{VZ}}$ in the high-mass analysis, in the muon channel, low-purity category. The shaded area represents the post-fit uncertainty in the background. The expected contribution from W' signal candidates with mass $m_{\text{X}} = 2000$ GeV, normalized to a cross section of 100 fb$^{-1}$, is also shown.

Sideband $m_{ZV}$ distribution for the low-mass search in the merged V, untagged category, after fitting the sideband data alone. The points show the data while the filled histograms show the background contributions. Electron and muon categories are combined. The gray band indicates the statistical and post-fit systematic uncertainties in the normalization and shape of the background. Larger bin widths are used at higher values of $m_{ZV}$; the bin widths are indicated by the horizontal error bars.

Sideband $m_{ZV}$ distribution for the low-mass search in the merged V, tagged category, after fitting the sideband data alone. The points show the data while the filled histograms show the background contributions. Electron and muon categories are combined. The gray band indicates the statistical and post-fit systematic uncertainties in the normalization and shape of the background. Larger bin widths are used at higher values of $m_{ZV}$; the bin widths are indicated by the horizontal error bars.

Sideband $m_{ZV}$ distribution for the low-mass search in the resolved V, untagged category, after fitting the sideband data alone. The points show the data while the filled histograms show the background contributions. Electron and muon categories are combined. The gray band indicates the statistical and post-fit systematic uncertainties in the normalization and shape of the background. Larger bin widths are used at higher values of $m_{ZV}$; the bin widths are indicated by the horizontal error bars.

Sideband $m_{ZV}$ distribution for the low-mass search in the resolved V, tagged category, after fitting the sideband data alone. The points show the data while the filled histograms show the background contributions. Electron and muon categories are combined. The gray band indicates the statistical and post-fit systematic uncertainties in the normalization and shape of the background. Larger bin widths are used at higher values of $m_{ZV}$; the bin widths are indicated by the horizontal error bars.

The signal region $m_{VZ}$ distribution for the low-mass search, in the the merged V, untagged category, after fitting the signal and sideband regions. Electron and muon categories are combined. A 600 GeV bulk graviton signal prediction is represented by the black dashed histogram. The gray band indicates the statistical and post-fit systematic uncertainties in the normalization and shape of the background. Larger bin widths are used at higher values of $m_{VZ}$; the bin widths are indicated by the horizontal error bars.

The signal region $m_{VZ}$ distribution for the low-mass search, in the the merged V, tagged category, after fitting the signal and sideband regions. Electron and muon categories are combined. A 600 GeV bulk graviton signal prediction is represented by the black dashed histogram. The gray band indicates the statistical and post-fit systematic uncertainties in the normalization and shape of the background. Larger bin widths are used at higher values of $m_{VZ}$; the bin widths are indicated by the horizontal error bars.

The signal region $m_{VZ}$ distribution for the low-mass search, in the the resolved V, untagged category, after fitting the signal and sideband regions. Electron and muon categories are combined. A 600 GeV bulk graviton signal prediction is represented by the black dashed histogram. The gray band indicates the statistical and post-fit systematic uncertainties in the normalization and shape of the background. Larger bin widths are used at higher values of $m_{VZ}$; the bin widths are indicated by the horizontal error bars.

The signal region $m_{VZ}$ distribution for the low-mass search, in the the resolved V, tagged category, after fitting the signal and sideband regions. Electron and muon categories are combined. A 600 GeV bulk graviton signal prediction is represented by the black dashed histogram. The gray band indicates the statistical and post-fit systematic uncertainties in the normalization and shape of the background. Larger bin widths are used at higher values of $m_{VZ}$; the bin widths are indicated by the horizontal error bars.

Observed and expected 95% CL upper limit on $\sigma_{W'} Br(W' \to ZW)$ as a function of the resonance mass, taking into account all statistical and systematic uncertainties. The electron and muon channels and the various categories used in the analysis are combined together. The green (inner) and yellow (outer) bands represent the 68% and 95% coverage of the expected limit in the background-only hypothesis.

Observed and expected 95% CL upper limit on $\sigma_{G} Br(G \to ZZ)$ as a function of the resonance mass, taking into account all statistical and systematic uncertainties. The electron and muon channels and the various categories used in the analysis are combined together. The green (inner) and yellow (outer) bands represent the 68% and 95% coverage of the expected limit in the background-only hypothesis.

Observed local p-values for W' narrow resonances as a function of the resonance mass.

Observed local p-values for G narrow resonances as a function of the resonance mass.

Covariance matrix of absolute cross section at particle level as a function of $|y(\text{t}_\text{h})|$.

Absolute cross section at particle level as a function of $p_\text{T}(\text{t}_\text{l})$.

Covariance matrix of absolute cross section at particle level as a function of $p_\text{T}(\text{t}_\text{l})$.

Absolute cross section at particle level as a function of $|y(\text{t}_\text{l})|$.

Covariance matrix of absolute cross section at particle level as a function of $|y(\text{t}_\text{l})|$.

Absolute cross section at particle level as a function of $M(\text{t}\bar{\text{t}})$.

Covariance matrix of absolute cross section at particle level as a function of $M(\text{t}\bar{\text{t}})$.

Absolute cross section at particle level as a function of $p_\text{T}(\text{t}\bar{\text{t}})$.

Covariance matrix of absolute cross section at particle level as a function of $p_\text{T}(\text{t}\bar{\text{t}})$.

Absolute cross section at particle level as a function of $|y(\text{t}\bar{\text{t}})|$.

Covariance matrix of absolute cross section at particle level as a function of $|y(\text{t}\bar{\text{t}})|$.

Absolute cross section at particle level as a function of Additional jets.

Covariance matrix of absolute cross section at particle level as a function of Additional jets.

Absolute cross section at particle level as a function of Additional jets vs. $M(\text{t}\bar{\text{t}})$.

Absolute cross section at particle level as a function of Additional jets vs. $M(\text{t}\bar{\text{t}})$.

Absolute cross section at particle level as a function of Additional jets vs. $M(\text{t}\bar{\text{t}})$.

Absolute cross section at particle level as a function of Additional jets vs. $M(\text{t}\bar{\text{t}})$.

Covariance matrix of absolute cross section at particle level as a function of Additional jets vs. $M(\text{t}\bar{\text{t}})$.

Absolute cross section at particle level as a function of Additional jets vs. $p_\text{T}(\text{t}_\text{h})$.

Absolute cross section at particle level as a function of Additional jets vs. $p_\text{T}(\text{t}_\text{h})$.

Absolute cross section at particle level as a function of Additional jets vs. $p_\text{T}(\text{t}_\text{h})$.

Absolute cross section at particle level as a function of Additional jets vs. $p_\text{T}(\text{t}_\text{h})$.

Covariance matrix of absolute cross section at particle level as a function of Additional jets vs. $p_\text{T}(\text{t}_\text{h})$.

Absolute cross section at particle level as a function of Additional jets vs. $p_\text{T}(\text{t}\bar{\text{t}})$.

Absolute cross section at particle level as a function of Additional jets vs. $p_\text{T}(\text{t}\bar{\text{t}})$.

Absolute cross section at particle level as a function of Additional jets vs. $p_\text{T}(\text{t}\bar{\text{t}})$.

Absolute cross section at particle level as a function of Additional jets vs. $p_\text{T}(\text{t}\bar{\text{t}})$.

Covariance matrix of absolute cross section at particle level as a function of Additional jets vs. $p_\text{T}(\text{t}\bar{\text{t}})$.

Absolute cross section at particle level as a function of $|y(\text{t}_\text{h})|$ vs. $p_\text{T}(\text{t}_\text{h})$.

Absolute cross section at particle level as a function of $|y(\text{t}_\text{h})|$ vs. $p_\text{T}(\text{t}_\text{h})$.

Absolute cross section at particle level as a function of $|y(\text{t}_\text{h})|$ vs. $p_\text{T}(\text{t}_\text{h})$.

Absolute cross section at particle level as a function of $|y(\text{t}_\text{h})|$ vs. $p_\text{T}(\text{t}_\text{h})$.

Covariance matrix of absolute cross section at particle level as a function of $|y(\text{t}_\text{h})|$ vs. $p_\text{T}(\text{t}_\text{h})$.

Absolute cross section at particle level as a function of $M(\text{t}\bar{\text{t}})$ vs. $|y(\text{t}\bar{\text{t}})|$.

Absolute cross section at particle level as a function of $M(\text{t}\bar{\text{t}})$ vs. $|y(\text{t}\bar{\text{t}})|$.

Absolute cross section at particle level as a function of $M(\text{t}\bar{\text{t}})$ vs. $|y(\text{t}\bar{\text{t}})|$.

Absolute cross section at particle level as a function of $M(\text{t}\bar{\text{t}})$ vs. $|y(\text{t}\bar{\text{t}})|$.

Covariance matrix of absolute cross section at particle level as a function of $M(\text{t}\bar{\text{t}})$ vs. $|y(\text{t}\bar{\text{t}})|$.

Absolute cross section at particle level as a function of $p_\text{T}(\text{t}_\text{h})$ vs. $M(\text{t}\bar{\text{t}})$.

Absolute cross section at particle level as a function of $p_\text{T}(\text{t}_\text{h})$ vs. $M(\text{t}\bar{\text{t}})$.

Absolute cross section at particle level as a function of $p_\text{T}(\text{t}_\text{h})$ vs. $M(\text{t}\bar{\text{t}})$.

Absolute cross section at particle level as a function of $p_\text{T}(\text{t}_\text{h})$ vs. $M(\text{t}\bar{\text{t}})$.

Covariance matrix of absolute cross section at particle level as a function of $p_\text{T}(\text{t}_\text{h})$ vs. $M(\text{t}\bar{\text{t}})$.

Absolute cross section at particle level as a function of $p_\text{T}(b_\text{l})$.

Absolute cross section at particle level as a function of $p_\text{T}(b_\text{h})$.

Absolute cross section at particle level as a function of $p_\text{T}(j_\text{W1})$.

Absolute cross section at particle level as a function of $p_\text{T}(j_\text{W2})$.

Absolute cross section at particle level as a function of $p_\text{T}(j_\text{1})$.

Absolute cross section at particle level as a function of $p_\text{T}(j_\text{2})$.

Absolute cross section at particle level as a function of $p_\text{T}(j_\text{3})$.

Absolute cross section at particle level as a function of $p_\text{T}(j_\text{4})$.

Covariance matrix of absolute cross section at particle level as a function of Jet type vs. $p_\text{T}(\mathrm{jet})$.

Absolute cross section at particle level as a function of $|\eta(b_\text{l})|$.

Absolute cross section at particle level as a function of $|\eta(b_\text{h})|$.

Absolute cross section at particle level as a function of $|\eta(j_\text{W1})|$.

Absolute cross section at particle level as a function of $|\eta(j_\text{W2})|$.

Absolute cross section at particle level as a function of $|\eta(j_\text{1})|$.

Absolute cross section at particle level as a function of $|\eta(j_\text{2})|$.

Absolute cross section at particle level as a function of $|\eta(j_\text{3})|$.

Absolute cross section at particle level as a function of $|\eta(j_\text{4})|$.

Covariance matrix of absolute cross section at particle level as a function of Jet type vs. $|\eta(\text{jet})|$.

Absolute cross section at particle level as a function of $\Delta R_{\text{j}_\text{t}}(b_\text{l})$.

Absolute cross section at particle level as a function of $\Delta R_{\text{j}_\text{t}}(b_\text{h})$.

Absolute cross section at particle level as a function of $\Delta R_{\text{j}_\text{t}}(j_\text{W1})$.

Absolute cross section at particle level as a function of $\Delta R_{\text{j}_\text{t}}(j_\text{W2})$.

Absolute cross section at particle level as a function of $\Delta R_{\text{j}_\text{t}}(j_\text{1})$.

Absolute cross section at particle level as a function of $\Delta R_{\text{j}_\text{t}}(j_\text{2})$.

Absolute cross section at particle level as a function of $\Delta R_{\text{j}_\text{t}}(j_\text{3})$.

Absolute cross section at particle level as a function of $\Delta R_{\text{j}_\text{t}}(j_\text{4})$.

Covariance matrix of absolute cross section at particle level as a function of Jet type vs. $\Delta R_{\text{j}_\text{t}}$.

Absolute cross section at particle level as a function of $\Delta R_\text{t}(b_\text{l})$.

Absolute cross section at particle level as a function of $\Delta R_\text{t}(b_\text{h})$.

Absolute cross section at particle level as a function of $\Delta R_\text{t}(j_\text{W1})$.

Absolute cross section at particle level as a function of $\Delta R_\text{t}(j_\text{W2})$.

Absolute cross section at particle level as a function of $\Delta R_\text{t}(j_\text{1})$.

Absolute cross section at particle level as a function of $\Delta R_\text{t}(j_\text{2})$.

Absolute cross section at particle level as a function of $\Delta R_\text{t}(j_\text{3})$.

Absolute cross section at particle level as a function of $\Delta R_\text{t}(j_\text{4})$.

Covariance matrix of absolute cross section at particle level as a function of Jet type vs. $\Delta R_\text{t}$.

Normalized cross section at particle level as a function of $p_\text{T}(\text{t}_\text{h})$.

Covariance matrix of normalized cross section at particle level as a function of $p_\text{T}(\text{t}_\text{h})$.

Normalized cross section at particle level as a function of $|y(\text{t}_\text{h})|$.

Covariance matrix of normalized cross section at particle level as a function of $|y(\text{t}_\text{h})|$.

Normalized cross section at particle level as a function of $p_\text{T}(\text{t}_\text{l})$.

Covariance matrix of normalized cross section at particle level as a function of $p_\text{T}(\text{t}_\text{l})$.

Normalized cross section at particle level as a function of $|y(\text{t}_\text{l})|$.

Covariance matrix of normalized cross section at particle level as a function of $|y(\text{t}_\text{l})|$.

Normalized cross section at particle level as a function of $M(\text{t}\bar{\text{t}})$.

Covariance matrix of normalized cross section at particle level as a function of $M(\text{t}\bar{\text{t}})$.

Normalized cross section at particle level as a function of $p_\text{T}(\text{t}\bar{\text{t}})$.

Covariance matrix of normalized cross section at particle level as a function of $p_\text{T}(\text{t}\bar{\text{t}})$.

Normalized cross section at particle level as a function of $|y(\text{t}\bar{\text{t}})|$.

Covariance matrix of normalized cross section at particle level as a function of $|y(\text{t}\bar{\text{t}})|$.

Normalized cross section at particle level as a function of Additional jets.

Covariance matrix of normalized cross section at particle level as a function of Additional jets.

Normalized cross section at particle level as a function of Additional jets vs. $M(\text{t}\bar{\text{t}})$.

Normalized cross section at particle level as a function of Additional jets vs. $M(\text{t}\bar{\text{t}})$.

Normalized cross section at particle level as a function of Additional jets vs. $M(\text{t}\bar{\text{t}})$.

Normalized cross section at particle level as a function of Additional jets vs. $M(\text{t}\bar{\text{t}})$.

Covariance matrix of normalized cross section at particle level as a function of Additional jets vs. $M(\text{t}\bar{\text{t}})$.

Normalized cross section at particle level as a function of Additional jets vs. $p_\text{T}(\text{t}_\text{h})$.

Normalized cross section at particle level as a function of Additional jets vs. $p_\text{T}(\text{t}_\text{h})$.

Normalized cross section at particle level as a function of Additional jets vs. $p_\text{T}(\text{t}_\text{h})$.

Normalized cross section at particle level as a function of Additional jets vs. $p_\text{T}(\text{t}_\text{h})$.

Covariance matrix of normalized cross section at particle level as a function of Additional jets vs. $p_\text{T}(\text{t}_\text{h})$.

Normalized cross section at particle level as a function of Additional jets vs. $p_\text{T}(\text{t}\bar{\text{t}})$.

Normalized cross section at particle level as a function of Additional jets vs. $p_\text{T}(\text{t}\bar{\text{t}})$.

Normalized cross section at particle level as a function of Additional jets vs. $p_\text{T}(\text{t}\bar{\text{t}})$.

Normalized cross section at particle level as a function of Additional jets vs. $p_\text{T}(\text{t}\bar{\text{t}})$.

Covariance matrix of normalized cross section at particle level as a function of Additional jets vs. $p_\text{T}(\text{t}\bar{\text{t}})$.

Normalized cross section at particle level as a function of $|y(\text{t}_\text{h})|$ vs. $p_\text{T}(\text{t}_\text{h})$.

Normalized cross section at particle level as a function of $|y(\text{t}_\text{h})|$ vs. $p_\text{T}(\text{t}_\text{h})$.

Normalized cross section at particle level as a function of $|y(\text{t}_\text{h})|$ vs. $p_\text{T}(\text{t}_\text{h})$.

Normalized cross section at particle level as a function of $|y(\text{t}_\text{h})|$ vs. $p_\text{T}(\text{t}_\text{h})$.

Covariance matrix of normalized cross section at particle level as a function of $|y(\text{t}_\text{h})|$ vs. $p_\text{T}(\text{t}_\text{h})$.

Normalized cross section at particle level as a function of $M(\text{t}\bar{\text{t}})$ vs. $|y(\text{t}\bar{\text{t}})|$.

Normalized cross section at particle level as a function of $M(\text{t}\bar{\text{t}})$ vs. $|y(\text{t}\bar{\text{t}})|$.

Normalized cross section at particle level as a function of $M(\text{t}\bar{\text{t}})$ vs. $|y(\text{t}\bar{\text{t}})|$.

Normalized cross section at particle level as a function of $M(\text{t}\bar{\text{t}})$ vs. $|y(\text{t}\bar{\text{t}})|$.

Covariance matrix of normalized cross section at particle level as a function of $M(\text{t}\bar{\text{t}})$ vs. $|y(\text{t}\bar{\text{t}})|$.

Normalized cross section at particle level as a function of $p_\text{T}(\text{t}_\text{h})$ vs. $M(\text{t}\bar{\text{t}})$.

Normalized cross section at particle level as a function of $p_\text{T}(\text{t}_\text{h})$ vs. $M(\text{t}\bar{\text{t}})$.

Normalized cross section at particle level as a function of $p_\text{T}(\text{t}_\text{h})$ vs. $M(\text{t}\bar{\text{t}})$.

Normalized cross section at particle level as a function of $p_\text{T}(\text{t}_\text{h})$ vs. $M(\text{t}\bar{\text{t}})$.

Covariance matrix of normalized cross section at particle level as a function of $p_\text{T}(\text{t}_\text{h})$ vs. $M(\text{t}\bar{\text{t}})$.

Normalized cross section at particle level as a function of $p_\text{T}(b_\text{l})$.

Normalized cross section at particle level as a function of $p_\text{T}(b_\text{h})$.

Normalized cross section at particle level as a function of $p_\text{T}(j_\text{W1})$.

Normalized cross section at particle level as a function of $p_\text{T}(j_\text{W2})$.

Normalized cross section at particle level as a function of $p_\text{T}(j_\text{1})$.

Normalized cross section at particle level as a function of $p_\text{T}(j_\text{2})$.

Normalized cross section at particle level as a function of $p_\text{T}(j_\text{3})$.

Normalized cross section at particle level as a function of $p_\text{T}(j_\text{4})$.

Covariance matrix of normalized cross section at particle level as a function of Jet type vs. $p_\text{T}(\mathrm{jet})$.

Normalized cross section at particle level as a function of $|\eta(b_\text{l})|$.

Normalized cross section at particle level as a function of $|\eta(b_\text{h})|$.

Normalized cross section at particle level as a function of $|\eta(j_\text{W1})|$.

Normalized cross section at particle level as a function of $|\eta(j_\text{W2})|$.

Normalized cross section at particle level as a function of $|\eta(j_\text{1})|$.

Normalized cross section at particle level as a function of $|\eta(j_\text{2})|$.

Normalized cross section at particle level as a function of $|\eta(j_\text{3})|$.

Normalized cross section at particle level as a function of $|\eta(j_\text{4})|$.

Covariance matrix of normalized cross section at particle level as a function of Jet type vs. $|\eta(\text{jet})|$.

Normalized cross section at particle level as a function of $\Delta R_{\text{j}_\text{t}}(b_\text{l})$.

Normalized cross section at particle level as a function of $\Delta R_{\text{j}_\text{t}}(b_\text{h})$.

Normalized cross section at particle level as a function of $\Delta R_{\text{j}_\text{t}}(j_\text{W1})$.

Normalized cross section at particle level as a function of $\Delta R_{\text{j}_\text{t}}(j_\text{W2})$.

Normalized cross section at particle level as a function of $\Delta R_{\text{j}_\text{t}}(j_\text{1})$.

Normalized cross section at particle level as a function of $\Delta R_{\text{j}_\text{t}}(j_\text{2})$.

Normalized cross section at particle level as a function of $\Delta R_{\text{j}_\text{t}}(j_\text{3})$.

Normalized cross section at particle level as a function of $\Delta R_{\text{j}_\text{t}}(j_\text{4})$.

Covariance matrix of normalized cross section at particle level as a function of Jet type vs. $\Delta R_{\text{j}_\text{t}}$.

Normalized cross section at particle level as a function of $\Delta R_\text{t}(b_\text{l})$.

Normalized cross section at particle level as a function of $\Delta R_\text{t}(b_\text{h})$.

Normalized cross section at particle level as a function of $\Delta R_\text{t}(j_\text{W1})$.

Normalized cross section at particle level as a function of $\Delta R_\text{t}(j_\text{W2})$.

Normalized cross section at particle level as a function of $\Delta R_\text{t}(j_\text{1})$.

Normalized cross section at particle level as a function of $\Delta R_\text{t}(j_\text{2})$.

Normalized cross section at particle level as a function of $\Delta R_\text{t}(j_\text{3})$.

Normalized cross section at particle level as a function of $\Delta R_\text{t}(j_\text{4})$.

Covariance matrix of normalized cross section at particle level as a function of Jet type vs. $\Delta R_\text{t}$.

gap fraction at particle level.

Covariance matrix of gap fraction at particle level.

gap fraction at particle level.

Covariance matrix of gap fraction at particle level.

jet multiplicities for $p_{T}(jet) > 30.0$ GeV.

jet multiplicities for $p_{T}(jet) > 50.0$ GeV.

jet multiplicities for $p_{T}(jet) > 75.0$ GeV.

jet multiplicities for $p_{T}(jet) > 100.0$ GeV.

Covariance matrix of jet multiplicities with different pT(jet) thresholds.

Absolute cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{high})$.

Covariance matrix of absolute cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{high})$.

Absolute cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{low})$.

Covariance matrix of absolute cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{low})$.

Absolute cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{h})$.

Covariance matrix of absolute cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{h})$.

Absolute cross section at the parton level as a function of $|y(\text{t}_\text{h})|$.

Covariance matrix of absolute cross section at the parton level as a function of $|y(\text{t}_\text{h})|$.

Absolute cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{l})$.

Covariance matrix of absolute cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{l})$.

Absolute cross section at the parton level as a function of $|y(\text{t}_\text{l})|$.

Covariance matrix of absolute cross section at the parton level as a function of $|y(\text{t}_\text{l})|$.

Absolute cross section at the parton level as a function of $M(\text{t}\bar{\text{t}})$.

Covariance matrix of absolute cross section at the parton level as a function of $M(\text{t}\bar{\text{t}})$.

Absolute cross section at the parton level as a function of $p_\text{T}(\text{t}\bar{\text{t}})$.

Covariance matrix of absolute cross section at the parton level as a function of $p_\text{T}(\text{t}\bar{\text{t}})$.

Absolute cross section at the parton level as a function of $|y(\text{t}\bar{\text{t}})|$.

Covariance matrix of absolute cross section at the parton level as a function of $|y(\text{t}\bar{\text{t}})|$.

Absolute cross section at the parton level as a function of $|y(\text{t}_\text{h})|$ vs. $p_\text{T}(\text{t}_\text{h})$.

Absolute cross section at the parton level as a function of $|y(\text{t}_\text{h})|$ vs. $p_\text{T}(\text{t}_\text{h})$.

Absolute cross section at the parton level as a function of $|y(\text{t}_\text{h})|$ vs. $p_\text{T}(\text{t}_\text{h})$.

Absolute cross section at the parton level as a function of $|y(\text{t}_\text{h})|$ vs. $p_\text{T}(\text{t}_\text{h})$.

Covariance matrix of absolute cross section at the parton level as a function of $|y(\text{t}_\text{h})|$ vs. $p_\text{T}(\text{t}_\text{h})$.

Absolute cross section at the parton level as a function of $M(\text{t}\bar{\text{t}})$ vs. $|y(\text{t}\bar{\text{t}})|$.

Absolute cross section at the parton level as a function of $M(\text{t}\bar{\text{t}})$ vs. $|y(\text{t}\bar{\text{t}})|$.

Absolute cross section at the parton level as a function of $M(\text{t}\bar{\text{t}})$ vs. $|y(\text{t}\bar{\text{t}})|$.

Absolute cross section at the parton level as a function of $M(\text{t}\bar{\text{t}})$ vs. $|y(\text{t}\bar{\text{t}})|$.

Covariance matrix of absolute cross section at the parton level as a function of $M(\text{t}\bar{\text{t}})$ vs. $|y(\text{t}\bar{\text{t}})|$.

Absolute cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{h})$ vs. $M(\text{t}\bar{\text{t}})$.

Absolute cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{h})$ vs. $M(\text{t}\bar{\text{t}})$.

Absolute cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{h})$ vs. $M(\text{t}\bar{\text{t}})$.

Absolute cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{h})$ vs. $M(\text{t}\bar{\text{t}})$.

Covariance matrix of absolute cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{h})$ vs. $M(\text{t}\bar{\text{t}})$.

Normalized cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{high})$.

Covariance matrix of normalized cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{high})$.

Normalized cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{low})$.

Covariance matrix of normalized cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{low})$.

Normalized cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{h})$.

Covariance matrix of normalized cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{h})$.

Normalized cross section at the parton level as a function of $|y(\text{t}_\text{h})|$.

Covariance matrix of normalized cross section at the parton level as a function of $|y(\text{t}_\text{h})|$.

Normalized cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{l})$.

Covariance matrix of normalized cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{l})$.

Normalized cross section at the parton level as a function of $|y(\text{t}_\text{l})|$.

Covariance matrix of normalized cross section at the parton level as a function of $|y(\text{t}_\text{l})|$.

Normalized cross section at the parton level as a function of $M(\text{t}\bar{\text{t}})$.

Covariance matrix of normalized cross section at the parton level as a function of $M(\text{t}\bar{\text{t}})$.

Normalized cross section at the parton level as a function of $p_\text{T}(\text{t}\bar{\text{t}})$.

Covariance matrix of normalized cross section at the parton level as a function of $p_\text{T}(\text{t}\bar{\text{t}})$.

Normalized cross section at the parton level as a function of $|y(\text{t}\bar{\text{t}})|$.

Covariance matrix of normalized cross section at the parton level as a function of $|y(\text{t}\bar{\text{t}})|$.

Normalized cross section at the parton level as a function of $|y(\text{t}_\text{h})|$ vs. $p_\text{T}(\text{t}_\text{h})$.

Normalized cross section at the parton level as a function of $|y(\text{t}_\text{h})|$ vs. $p_\text{T}(\text{t}_\text{h})$.

Normalized cross section at the parton level as a function of $|y(\text{t}_\text{h})|$ vs. $p_\text{T}(\text{t}_\text{h})$.

Normalized cross section at the parton level as a function of $|y(\text{t}_\text{h})|$ vs. $p_\text{T}(\text{t}_\text{h})$.

Covariance matrix of normalized cross section at the parton level as a function of $|y(\text{t}_\text{h})|$ vs. $p_\text{T}(\text{t}_\text{h})$.

Normalized cross section at the parton level as a function of $M(\text{t}\bar{\text{t}})$ vs. $|y(\text{t}\bar{\text{t}})|$.

Normalized cross section at the parton level as a function of $M(\text{t}\bar{\text{t}})$ vs. $|y(\text{t}\bar{\text{t}})|$.

Normalized cross section at the parton level as a function of $M(\text{t}\bar{\text{t}})$ vs. $|y(\text{t}\bar{\text{t}})|$.

Normalized cross section at the parton level as a function of $M(\text{t}\bar{\text{t}})$ vs. $|y(\text{t}\bar{\text{t}})|$.

Covariance matrix of normalized cross section at the parton level as a function of $M(\text{t}\bar{\text{t}})$ vs. $|y(\text{t}\bar{\text{t}})|$.

Normalized cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{h})$ vs. $M(\text{t}\bar{\text{t}})$.

Normalized cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{h})$ vs. $M(\text{t}\bar{\text{t}})$.

Normalized cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{h})$ vs. $M(\text{t}\bar{\text{t}})$.

Normalized cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{h})$ vs. $M(\text{t}\bar{\text{t}})$.

Covariance matrix of normalized cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{h})$ vs. $M(\text{t}\bar{\text{t}})$.

Normalized dijet angular distribution for events with 4.2 < dijet mass < 4.8 TeV.

Normalized dijet angular distribution for events with 3.6 < dijet mass < 4.2 TeV.

Normalized dijet angular distribution for events with 3.0 < dijet mass < 3.6 TeV.

Normalized dijet angular distribution for events with 2.4 < dijet mass < 3.0 TeV.

The 95% CL upper limits on the quark coupling gq, as a function of mass, for an axialvector or vector DM mediator with gDM = 1.0 and mDM = 1 GeV.

Electroweak correction factors for events with dijet mass > 6.0 TeV computed by the authors of JHEP 11 (2012) 095 (arXiv:1210.0438).

Electroweak correction factors for events with 5.4 < dijet mass < 6.0 TeV computed by the authors of JHEP 11 (2012) 095 (arXiv:1210.0438).

Electroweak correction factors for events with 4.8 < dijet mass < 5.4 TeV computed by the authors of JHEP 11 (2012) 095 (arXiv:1210.0438).

Electroweak correction factors for events with 4.2 < dijet mass < 4.8 TeV computed by the authors of JHEP 11 (2012) 095 (arXiv:1210.0438).

Electroweak correction factors for events with 3.6 < dijet mass < 4.2 TeV computed by the authors of JHEP 11 (2012) 095 (arXiv:1210.0438).

Electroweak correction factors for events with 3.0 < dijet mass < 3.6 TeV computed by the authors of JHEP 11 (2012) 095 (arXiv:1210.0438).

Electroweak correction factors for events with 2.4 < dijet mass < 3.0 TeV computed by the authors of JHEP 11 (2012) 095 (arXiv:1210.0438).

Covariance matrix for 1 < CHI < 2.

Covariance matrix for 2 < CHI < 3.

Covariance matrix for 3 < CHI < 4.

Covariance matrix for 4 < CHI < 5.

Covariance matrix for 5 < CHI < 6.

Covariance matrix for 6 < CHI < 7.

Covariance matrix for 7 < CHI < 8.

Covariance matrix for 8 < CHI < 9.

Covariance matrix for 9 < CHI < 10.

Covariance matrix for 10 < CHI < 12.

Covariance matrix for 12 < CHI < 14.

Covariance matrix for 14 < CHI < 16.

NLO QCD+EW prediction and benchmark signal predictions for dijet mass > 6.0 TeV.

NLO QCD+EW prediction and benchmark signal predictions for 5.4 < dijet mass < 6.0 TeV.

NLO QCD+EW prediction and benchmark signal predictions for 4.8 < dijet mass < 5.4 TeV.

NLO QCD+EW prediction and benchmark signal predictions for 4.2 < dijet mass < 4.8 TeV.

NLO QCD+EW prediction and benchmark signal predictions for 3.6 < dijet mass < 4.2 TeV.

NLO QCD+EW prediction and benchmark signal predictions for 3.0 < dijet mass < 3.6 TeV.

NLO QCD+EW prediction and benchmark signal predictions for 2.4 < dijet mass < 3.0 TeV.