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The $t\bar{t}$ production cross-section dependence on jet multiplicity and jet transverse momentum is reported for proton--proton collisions at a centre-of-mass energy of 7 TeV in the single-lepton channel. The data were collected with the ATLAS detector at the CERN Large Hadron Collider and comprise the full 2011 data sample corresponding to an integrated luminosity of 4.6 fb$^{-1}$. Differential cross-sections are presented as a function of the jet multiplicity for up to eight jets using jet transverse momentum thresholds of 25, 40, 60, and 80 GeV, and as a function of jet transverse momentum up to the fifth jet. The results are shown after background subtraction and corrections for all detector effects, within a kinematic range closely matched to the experimental acceptance. Several QCD-based Monte Carlo models are compared with the results. Sensitivity to the parton shower modelling is found at the higher jet multiplicities, at high transverse momentum of the leading jet and in the transverse momentum spectrum of the fifth leading jet. The MC@NLO+HERWIG MC is found to predict too few events at higher jet multiplicities.
Measurements of differential cross sections of top quark pair production in association with jets by the ATLAS experiment at the LHC are presented. The measurements are performed as functions of the top quark transverse momentum, the transverse momentum of the top quark-antitop quark system and the out-of-plane transverse momentum using data from $pp$ collisions at $\sqrt{s}=13$ TeV collected by the ATLAS detector at the LHC in 2015 and corresponding to an integrated luminosity of 3.2 fb$^{-1}$. The top quark pair events are selected in the lepton (electron or muon) + jets channel. The measured cross sections, which are compared to several predictions, allow a detailed study of top quark production.
Statistical correlation matrix between $p_{T}^{t\bar{t}}$ in the 4-jet exclusive configuration and $p_{T}^{t,had}$ in the 6-jet inclusive configuration, obtained through the Bootstrap Method.
A search for new particles that decay into top quark pairs is reported. The search is performed with the ATLAS experiment at the LHC using an integrated luminosity of 20.3 fb$^{-1}$ of proton-proton collision data collected at a centre-of-mass energy of $\sqrt{s}=8$ TeV. The lepton-plus-jets final state is used, where the top pair decays to $W^+bW^-\bar{b}$, with one $W$ boson decaying leptonically and the other hadronically. The invariant mass spectrum of top quark pairs is examined for local excesses or deficits that are inconsistent with the Standard Model predictions. No evidence for a top quark pair resonance is found, and 95% confidence-level limits on the production rate are determined for massive states in benchmark models. The upper limits on the cross-section times branching ratio of a narrow $Z'$ boson decaying to top pairs range from 4.2 pb to 0.03 pb for resonance masses from 0.4 TeV to 3.0 TeV. A narrow leptophobic topcolour $Z'$ boson with mass below 1.8 TeV is excluded. Upper limits are set on the cross-section times branching ratio for a broad colour-octet resonance with $\Gamma/m =$ 15% decaying to $t\bar{t}$. These range from 2.5 pb to 0.03 pb for masses from 0.4 TeV to 3.0 TeV. A Kaluza-Klein excitation of the gluon in a Randall-Sundrum model is excluded for masses below 2.2 TeV.
Measurements of differential cross-sections of top-quark pair production in fiducial phase-spaces are presented as a function of top-quark and $t\bar{t}$ system kinematic observables in proton-proton collisions at a centre-of-mass energy of $\sqrt{s}$=13 TeV. The data set corresponds to an integrated luminosity of $3.2$ fb${}^{-1}$, recorded in 2015 with the ATLAS detector at the CERN Large Hadron Collider. Events with exactly one electron or muon and at least two jets in the final state are used for the measurement. Two separate selections are applied that each focus on different top-quark momentum regions, referred to as resolved and boosted topologies of the $t\bar{t}$ final state. The measured spectra are corrected for detector effects and are compared to several Monte Carlo simulations by means of calculated $\chi^2$ and $p$-values.
Table of systematic uncertainties for the relative differential cross-section at particle level for the absolute value of the tt̄ system rapidity in the resolved regime. 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.
Table of systematic uncertainties for the relative differential cross-section at particle level for the absolute value of the tt̄ system rapidity in the resolved regime. 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.
Various differential cross-sections are measured in top-quark pair ($t\bar{t}$) events produced in proton-proton collisions at a centre-of-mass energy of $\sqrt{s} = 7$ TeV at the LHC with the ATLAS detector. These differential cross-sections are presented in a data set corresponding to an integrated luminosity of $4.6$ fb$^{-1}$. The differential cross-sections are presented in terms of kinematic variables, such as momentum, rapidity and invariant mass, of a top-quark proxyreferred to as the pseudo-top-quark as well as the pseudo-top-quark pair system. The dependence of the measurement on theoretical models is minimal. The measurements are performed on $t\bar{t}$ events in the lepton+jets channel, requiring exactly one charged lepton and at least four jets with at least two of them tagged as originating from a $b$-quark. The hadronic and leptonic pseudo-top-quarks are defined via the leptonic or hadronic decay mode of the $W$ boson produced by the top-quark decay in events with a single charged lepton. Differential cross-section measurements of the pseudo-top-quark variables are compared with several Monte Carlo models that implement next-to-leading order or leading-order multi-leg matrix-element calculations.
Ratios of top-quark pair to $Z$-boson cross sections measured from proton--proton collisions at the LHC centre-of-mass energies of $\sqrt s=13$TeV, 8TeV, and 7TeV are presented by the ATLAS Collaboration. Single ratios, at a given $\sqrt s$ for the two processes and at different $\sqrt s$ for each process, as well as double ratios of the two processes at different $\sqrt s$, are evaluated. The ratios are constructed using previously published ATLAS measurements of the $t\overline{t}$ and $Z$-boson production cross sections, corrected to a common phase space where required, and a new analysis of $Z \rightarrow \ell^+ \ell^-$ where $\ell=e,\mu$ at $\sqrt s=13$TeV performed with data collected in 2015 with an integrated luminosity of $3.2$fb$^{-1}$. Correlations of systematic uncertainties are taken into account when evaluating the uncertainties in the ratios. The correlation model is also used to evaluate the combined cross section of the $Z\rightarrow e^+e^-$ and the $Z\rightarrow \mu^+ \mu^-$ channels for each $\sqrt s$ value. The results are compared to calculations performed at next-to-next-to-leading-order accuracy using recent sets of parton distribution functions. The data demonstrate significant power to constrain the gluon distribution function for the Bjorken-$x$ values near 0.1 and the light-quark sea for $x<0.02$.
Differential cross-sections are measured for top-quark pair production in the all-hadronic decay mode, using proton$-$proton collision events collected by the ATLAS experiment in which all six decay jets are separately resolved. Absolute and normalised single- and double-differential cross-sections are measured at particle and parton level as a function of various kinematic variables. Emphasis is placed on well-measured observables in fully reconstructed final states, as well as on the study of correlations between the top-quark pair system and additional jet radiation identified in the event. The study is performed using data from proton$-$proton collisions at $\sqrt{s}=13~\mbox{TeV}$ collected by the ATLAS detector at CERN's Large Hadron Collider in 2015 and 2016, corresponding to an integrated luminosity of $\mbox{36.1 fb}^{-1}$. The rapidities of the individual top quarks and of the top-quark pair are well modelled by several independent event generators. Significant mismodelling is observed in the transverse momenta of the leading three jet emissions, while the leading top-quark transverse momentum and top-quark pair transverse momentum are both found to be incompatible with several theoretical predictions.
Covariance matrix of the relative 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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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 $N_{jets}$ > 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 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 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 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 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 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 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 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 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 $p_{T}^{t,1}$ 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.
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 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.
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.
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.
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 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 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 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 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 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 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 $|y^{t,2}|$ 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 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 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 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 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 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 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.
A measurement of jet shapes in top-quark pair events using 1.8 fb$^{-1}$ of $\sqrt{s}$ = 7 TeV pp collision data recorded by the ATLAS detector is presented. Samples of top-quark pair events are selected in both the single-lepton and dilepton final states. The differential and integrated shapes of the jets initiated by bottom-quarks from the top-quark decays are compared with those of the jets originated by light-quarks from the hadronic W-boson decays $W \to q\bar{q}'$ in the single-lepton channel. The light-quark jets are found to have a narrower distribution of the momentum flow inside the jet area than b-quark jets.
Single- and double-differential cross-section measurements are presented for the production of top-quark pairs, in the lepton + jets channel at particle and parton level. Two topologies, resolved and boosted, are considered and the results are presented as a function of several kinematic variables characterising the top and $t\bar{t}$ system and jet multiplicities. The study was performed using data from $pp$ collisions at centre-of-mass energy of 13 TeV collected in 2015 and 2016 by the ATLAS detector at the CERN Large Hadron Collider (LHC), corresponding to an integrated luminosity of $36~\mathrm{fb}^{-1}$. Due to the large $t\bar{t}$ cross-section at the LHC, such measurements allow a detailed study of the properties of top-quark production and decay, enabling precision tests of several Monte Carlo generators and fixed-order Standard Model predictions. Overall, there is good agreement between the theoretical predictions and the data.
Covariance matrix of the Relative differential cross-section as function of $p_{T}^{t,had}$ at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Relative differential cross-section as function of $|y^{t,had}|$ at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Absolute differential cross-section as function of $|y^{t,had}|$ at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Relative differential cross-section as function of $p_{T}^{t,1}$ at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Absolute differential cross-section as function of $p_{T}^{t,1}$ at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Relative differential cross-section as function of $p_{T}^{t,2}$ at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Absolute differential cross-section as function of $p_{T}^{t,2}$ at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Relative differential cross-section as function of $m^{t\bar{t}}$ at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Absolute differential cross-section as function of $m^{t\bar{t}}$ at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Relative differential cross-section as function of $p_{T}^{t\bar{t}}$ at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Relative differential cross-section as function of $|p_{out}^{t,had}|$ at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Absolute differential cross-section as function of $|p_{out}^{t,had}|$ at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Relative differential cross-section as function of $|\Delta\phi(t,\bar{t})|$ at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Absolute differential cross-section as function of $|\Delta\phi(t,\bar{t})|$ at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Relative differential cross-section as function of $H_{T}^{t\bar{t}}$ at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Relative differential cross-section as function of $N^{extra jets}$ at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Absolute differential cross-section as function of $N^{extra jets}$ at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Relative differential cross-section as function of $|y^{t\bar{t}}|$ at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Absolute differential cross-section as function of $|y^{t\bar{t}}|$ at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Relative differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Relative differential cross-section as function of $\chi^{t\bar{t}}$ at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Absolute differential cross-section as function of $\chi^{t\bar{t}}$ at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 200.0 GeV < $m^{t\bar{t}}$ < 400.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 200.0 GeV < $m^{t\bar{t}}$ < 400.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 400.0 GeV < $m^{t\bar{t}}$ < 550.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 200.0 GeV < $m^{t\bar{t}}$ < 400.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 400.0 GeV < $m^{t\bar{t}}$ < 550.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 400.0 GeV < $m^{t\bar{t}}$ < 550.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 550.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 200.0 GeV < $m^{t\bar{t}}$ < 400.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 550.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 400.0 GeV < $m^{t\bar{t}}$ < 550.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 550.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 550.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 200.0 GeV < $m^{t\bar{t}}$ < 400.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 400.0 GeV < $m^{t\bar{t}}$ < 550.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 550.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 200.0 GeV < $m^{t\bar{t}}$ < 400.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 400.0 GeV < $m^{t\bar{t}}$ < 550.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 550.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 200.0 GeV < $m^{t\bar{t}}$ < 400.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 200.0 GeV < $m^{t\bar{t}}$ < 400.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 400.0 GeV < $m^{t\bar{t}}$ < 550.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 200.0 GeV < $m^{t\bar{t}}$ < 400.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 400.0 GeV < $m^{t\bar{t}}$ < 550.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 400.0 GeV < $m^{t\bar{t}}$ < 550.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 550.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 200.0 GeV < $m^{t\bar{t}}$ < 400.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 550.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 400.0 GeV < $m^{t\bar{t}}$ < 550.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 550.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 550.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 200.0 GeV < $m^{t\bar{t}}$ < 400.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 400.0 GeV < $m^{t\bar{t}}$ < 550.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 550.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 200.0 GeV < $m^{t\bar{t}}$ < 400.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 400.0 GeV < $m^{t\bar{t}}$ < 550.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 550.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV at particle level in the 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 200.0 GeV < $m^{t\bar{t}}$ < 400.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 200.0 GeV < $m^{t\bar{t}}$ < 400.0 GeV at particle level in the 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 400.0 GeV < $m^{t\bar{t}}$ < 550.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 200.0 GeV < $m^{t\bar{t}}$ < 400.0 GeV at particle level in the 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 400.0 GeV < $m^{t\bar{t}}$ < 550.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 400.0 GeV < $m^{t\bar{t}}$ < 550.0 GeV at particle level in the 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 550.0 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 200.0 GeV < $m^{t\bar{t}}$ < 400.0 GeV at particle level in the 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 550.0 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 400.0 GeV < $m^{t\bar{t}}$ < 550.0 GeV at particle level in the 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 550.0 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 550.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at particle level in the 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 < $m^{t\bar{t}}$ < 1000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 200.0 GeV < $m^{t\bar{t}}$ < 400.0 GeV at particle level in the 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 < $m^{t\bar{t}}$ < 1000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 400.0 GeV < $m^{t\bar{t}}$ < 550.0 GeV at particle level in the 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 < $m^{t\bar{t}}$ < 1000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 550.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at particle level in the 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 < $m^{t\bar{t}}$ < 1000.0 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 < $m^{t\bar{t}}$ < 1000.0 GeV at particle level in the 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 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 200.0 GeV < $m^{t\bar{t}}$ < 400.0 GeV at particle level in the 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 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 400.0 GeV < $m^{t\bar{t}}$ < 550.0 GeV at particle level in the 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 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 550.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at particle level in the 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 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 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 < $m^{t\bar{t}}$ < 1000.0 GeV at particle level in the 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 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV at particle level in the 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 200.0 GeV < $m^{t\bar{t}}$ < 400.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 200.0 GeV < $m^{t\bar{t}}$ < 400.0 GeV at particle level in the 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 400.0 GeV < $m^{t\bar{t}}$ < 550.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 200.0 GeV < $m^{t\bar{t}}$ < 400.0 GeV at particle level in the 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 400.0 GeV < $m^{t\bar{t}}$ < 550.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 400.0 GeV < $m^{t\bar{t}}$ < 550.0 GeV at particle level in the 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 550.0 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 200.0 GeV < $m^{t\bar{t}}$ < 400.0 GeV at particle level in the 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 550.0 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 400.0 GeV < $m^{t\bar{t}}$ < 550.0 GeV at particle level in the 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 550.0 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 550.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at particle level in the 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 < $m^{t\bar{t}}$ < 1000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 200.0 GeV < $m^{t\bar{t}}$ < 400.0 GeV at particle level in the 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 < $m^{t\bar{t}}$ < 1000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 400.0 GeV < $m^{t\bar{t}}$ < 550.0 GeV at particle level in the 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 < $m^{t\bar{t}}$ < 1000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 550.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at particle level in the 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 < $m^{t\bar{t}}$ < 1000.0 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 < $m^{t\bar{t}}$ < 1000.0 GeV at particle level in the 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 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 200.0 GeV < $m^{t\bar{t}}$ < 400.0 GeV at particle level in the 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 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 400.0 GeV < $m^{t\bar{t}}$ < 550.0 GeV at particle level in the 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 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 550.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at particle level in the 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 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 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 < $m^{t\bar{t}}$ < 1000.0 GeV at particle level in the 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 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 0.0 GeV < $p_{T}^{t,had}$ < 60.0 GeV and the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 0.0 GeV < $p_{T}^{t,had}$ < 60.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 60.0 GeV < $p_{T}^{t,had}$ < 120.0 GeV and the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 0.0 GeV < $p_{T}^{t,had}$ < 60.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 60.0 GeV < $p_{T}^{t,had}$ < 120.0 GeV and the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 60.0 GeV < $p_{T}^{t,had}$ < 120.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 120.0 GeV < $p_{T}^{t,had}$ < 200.0 GeV and the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 0.0 GeV < $p_{T}^{t,had}$ < 60.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 120.0 GeV < $p_{T}^{t,had}$ < 200.0 GeV and the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 60.0 GeV < $p_{T}^{t,had}$ < 120.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 120.0 GeV < $p_{T}^{t,had}$ < 200.0 GeV and the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 120.0 GeV < $p_{T}^{t,had}$ < 200.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 200.0 GeV < $p_{T}^{t,had}$ < 300.0 GeV and the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 0.0 GeV < $p_{T}^{t,had}$ < 60.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 200.0 GeV < $p_{T}^{t,had}$ < 300.0 GeV and the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 60.0 GeV < $p_{T}^{t,had}$ < 120.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 200.0 GeV < $p_{T}^{t,had}$ < 300.0 GeV and the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 120.0 GeV < $p_{T}^{t,had}$ < 200.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 200.0 GeV < $p_{T}^{t,had}$ < 300.0 GeV and the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 200.0 GeV < $p_{T}^{t,had}$ < 300.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 300.0 GeV < $p_{T}^{t,had}$ < 1000.0 GeV and the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 0.0 GeV < $p_{T}^{t,had}$ < 60.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 300.0 GeV < $p_{T}^{t,had}$ < 1000.0 GeV and the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 60.0 GeV < $p_{T}^{t,had}$ < 120.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 300.0 GeV < $p_{T}^{t,had}$ < 1000.0 GeV and the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 120.0 GeV < $p_{T}^{t,had}$ < 200.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 300.0 GeV < $p_{T}^{t,had}$ < 1000.0 GeV and the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 200.0 GeV < $p_{T}^{t,had}$ < 300.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 300.0 GeV < $p_{T}^{t,had}$ < 1000.0 GeV and the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 300.0 GeV < $p_{T}^{t,had}$ < 1000.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 0.0 GeV < $p_{T}^{t,had}$ < 60.0 GeV and the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 0.0 GeV < $p_{T}^{t,had}$ < 60.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 60.0 GeV < $p_{T}^{t,had}$ < 120.0 GeV and the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 0.0 GeV < $p_{T}^{t,had}$ < 60.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 60.0 GeV < $p_{T}^{t,had}$ < 120.0 GeV and the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 60.0 GeV < $p_{T}^{t,had}$ < 120.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 120.0 GeV < $p_{T}^{t,had}$ < 200.0 GeV and the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 0.0 GeV < $p_{T}^{t,had}$ < 60.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 120.0 GeV < $p_{T}^{t,had}$ < 200.0 GeV and the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 60.0 GeV < $p_{T}^{t,had}$ < 120.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 120.0 GeV < $p_{T}^{t,had}$ < 200.0 GeV and the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 120.0 GeV < $p_{T}^{t,had}$ < 200.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 200.0 GeV < $p_{T}^{t,had}$ < 300.0 GeV and the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 0.0 GeV < $p_{T}^{t,had}$ < 60.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 200.0 GeV < $p_{T}^{t,had}$ < 300.0 GeV and the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 60.0 GeV < $p_{T}^{t,had}$ < 120.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 200.0 GeV < $p_{T}^{t,had}$ < 300.0 GeV and the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 120.0 GeV < $p_{T}^{t,had}$ < 200.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 200.0 GeV < $p_{T}^{t,had}$ < 300.0 GeV and the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 200.0 GeV < $p_{T}^{t,had}$ < 300.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 300.0 GeV < $p_{T}^{t,had}$ < 1000.0 GeV and the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 0.0 GeV < $p_{T}^{t,had}$ < 60.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 300.0 GeV < $p_{T}^{t,had}$ < 1000.0 GeV and the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 60.0 GeV < $p_{T}^{t,had}$ < 120.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 300.0 GeV < $p_{T}^{t,had}$ < 1000.0 GeV and the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 120.0 GeV < $p_{T}^{t,had}$ < 200.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 300.0 GeV < $p_{T}^{t,had}$ < 1000.0 GeV and the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 200.0 GeV < $p_{T}^{t,had}$ < 300.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 300.0 GeV < $p_{T}^{t,had}$ < 1000.0 GeV and the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 300.0 GeV < $p_{T}^{t,had}$ < 1000.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 6.0 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 6.0 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 6.0 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 6.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 6.0 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 6.0 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 6.0 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 6.0 at particle level in the 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 $N^{jets}$ = 4.0 and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the 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 $N^{jets}$ = 5.0 and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the 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 $N^{jets}$ = 5.0 and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the 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 $N^{jets}$ = 6.0 and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the 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 $N^{jets}$ = 6.0 and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the 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 $N^{jets}$ = 6.0 and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 at particle level in the 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 $N^{jets}$ $\geq$ 7.0 and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the 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 $N^{jets}$ $\geq$ 7.0 and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the 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 $N^{jets}$ $\geq$ 7.0 and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 at particle level in the 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 $N^{jets}$ $\geq$ 7.0 and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 at particle level in the 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 $N^{jets}$ = 4.0 and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the 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 $N^{jets}$ = 5.0 and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the 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 $N^{jets}$ = 5.0 and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the 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 $N^{jets}$ = 6.0 and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the 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 $N^{jets}$ = 6.0 and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the 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 $N^{jets}$ = 6.0 and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 at particle level in the 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 $N^{jets}$ $\geq$ 7.0 and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the 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 $N^{jets}$ $\geq$ 7.0 and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the 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 $N^{jets}$ $\geq$ 7.0 and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 at particle level in the 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 $N^{jets}$ $\geq$ 7.0 and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 and the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 5.0 and the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 5.0 and the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 6.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 6.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 and the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 5.0 and the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 5.0 and the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 6.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 6.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 at particle level in the 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 3.5 < $N^{jets}$ < 4.5 and the Relative double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 3.5 < $N^{jets}$ < 4.5 at particle level in the 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 4.5 < $N^{jets}$ < 5.5 and the Relative double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 3.5 < $N^{jets}$ < 4.5 at particle level in the 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 4.5 < $N^{jets}$ < 5.5 and the Relative double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 4.5 < $N^{jets}$ < 5.5 at particle level in the 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 5.5 < $N^{jets}$ < 6.5 and the Relative double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 3.5 < $N^{jets}$ < 4.5 at particle level in the 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 5.5 < $N^{jets}$ < 6.5 and the Relative double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 4.5 < $N^{jets}$ < 5.5 at particle level in the 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 5.5 < $N^{jets}$ < 6.5 and the Relative double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 5.5 < $N^{jets}$ < 6.5 at particle level in the 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 6.5 < $N^{jets}$ < 7.5 and the Relative double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 3.5 < $N^{jets}$ < 4.5 at particle level in the 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 6.5 < $N^{jets}$ < 7.5 and the Relative double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 4.5 < $N^{jets}$ < 5.5 at particle level in the 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 6.5 < $N^{jets}$ < 7.5 and the Relative double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 5.5 < $N^{jets}$ < 6.5 at particle level in the 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 6.5 < $N^{jets}$ < 7.5 and the Relative double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 6.5 < $N^{jets}$ < 7.5 at particle level in the 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 3.5 < $N^{jets}$ < 4.5 and the Absolute double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 3.5 < $N^{jets}$ < 4.5 at particle level in the 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 4.5 < $N^{jets}$ < 5.5 and the Absolute double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 3.5 < $N^{jets}$ < 4.5 at particle level in the 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 4.5 < $N^{jets}$ < 5.5 and the Absolute double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 4.5 < $N^{jets}$ < 5.5 at particle level in the 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 5.5 < $N^{jets}$ < 6.5 and the Absolute double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 3.5 < $N^{jets}$ < 4.5 at particle level in the 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 5.5 < $N^{jets}$ < 6.5 and the Absolute double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 4.5 < $N^{jets}$ < 5.5 at particle level in the 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 5.5 < $N^{jets}$ < 6.5 and the Absolute double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 5.5 < $N^{jets}$ < 6.5 at particle level in the 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 6.5 < $N^{jets}$ < 7.5 and the Absolute double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 3.5 < $N^{jets}$ < 4.5 at particle level in the 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 6.5 < $N^{jets}$ < 7.5 and the Absolute double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 4.5 < $N^{jets}$ < 5.5 at particle level in the 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 6.5 < $N^{jets}$ < 7.5 and the Absolute double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 5.5 < $N^{jets}$ < 6.5 at particle level in the 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 6.5 < $N^{jets}$ < 7.5 and the Absolute double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 6.5 < $N^{jets}$ < 7.5 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 and the Relative double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 and the Relative double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 and the Relative double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Relative double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Relative double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Relative double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Relative double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Relative double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Relative double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Relative double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 and the Absolute double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 and the Absolute double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 and the Absolute double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Absolute double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Absolute double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Absolute double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Absolute double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Absolute double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Absolute double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Absolute double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 and the Relative double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 5.0 and the Relative double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 5.0 and the Relative double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Relative double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Relative double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Relative double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 6.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Relative double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Relative double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Relative double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 6.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Relative double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 and the Absolute double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 5.0 and the Absolute double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 5.0 and the Absolute double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Absolute double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Absolute double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Absolute double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 6.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Absolute double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Absolute double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Absolute double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 6.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Absolute double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 at particle level in the 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 $N^{jets}$ in $N^{jets}$ = 4.0 and the Relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the 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 $N^{jets}$ in $N^{jets}$ = 5.0 and the Relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the 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 $N^{jets}$ in $N^{jets}$ = 5.0 and the Relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the 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 $N^{jets}$ in $N^{jets}$ = 6.0 and the Relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the 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 $N^{jets}$ in $N^{jets}$ = 6.0 and the Relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the 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 $N^{jets}$ in $N^{jets}$ = 6.0 and the Relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ = 6.0 at particle level in the 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 $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the 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 $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the 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 $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ = 6.0 at particle level in the 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 $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 at particle level in the 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 $N^{jets}$ in $N^{jets}$ = 4.0 and the Absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the 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 $N^{jets}$ in $N^{jets}$ = 5.0 and the Absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the 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 $N^{jets}$ in $N^{jets}$ = 5.0 and the Absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the 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 $N^{jets}$ in $N^{jets}$ = 6.0 and the Absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the 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 $N^{jets}$ in $N^{jets}$ = 6.0 and the Absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the 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 $N^{jets}$ in $N^{jets}$ = 6.0 and the Absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ = 6.0 at particle level in the 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 $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the 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 $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the 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 $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ = 6.0 at particle level in the 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 $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 and the Relative double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 and the Relative double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 and the Relative double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Relative double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Relative double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Relative double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Relative double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Relative double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Relative double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Relative double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 and the Absolute double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 and the Absolute double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 and the Absolute double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Absolute double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Absolute double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Absolute double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Absolute double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Absolute double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Absolute double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Absolute double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 0.0 < $|y^{t,had}|$ < 0.7 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 0.0 < $|y^{t,had}|$ < 0.7 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 0.7 < $|y^{t,had}|$ < 1.4 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 0.0 < $|y^{t,had}|$ < 0.7 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 0.7 < $|y^{t,had}|$ < 1.4 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 0.7 < $|y^{t,had}|$ < 1.4 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 1.4 < $|y^{t,had}|$ < 2.5 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 0.0 < $|y^{t,had}|$ < 0.7 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 1.4 < $|y^{t,had}|$ < 2.5 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 0.7 < $|y^{t,had}|$ < 1.4 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 1.4 < $|y^{t,had}|$ < 2.5 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 1.4 < $|y^{t,had}|$ < 2.5 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 0.0 < $|y^{t,had}|$ < 0.7 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 0.0 < $|y^{t,had}|$ < 0.7 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 0.7 < $|y^{t,had}|$ < 1.4 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 0.0 < $|y^{t,had}|$ < 0.7 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 0.7 < $|y^{t,had}|$ < 1.4 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 0.7 < $|y^{t,had}|$ < 1.4 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 1.4 < $|y^{t,had}|$ < 2.5 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 0.0 < $|y^{t,had}|$ < 0.7 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 1.4 < $|y^{t,had}|$ < 2.5 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 0.7 < $|y^{t,had}|$ < 1.4 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 1.4 < $|y^{t,had}|$ < 2.5 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 1.4 < $|y^{t,had}|$ < 2.5 at particle level in the 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 $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.4 and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.4 at particle level in the 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 $|y^{t\bar{t}}|$ in 0.4 < $|y^{t\bar{t}}|$ < 0.8 and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.4 at particle level in the 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 $|y^{t\bar{t}}|$ in 0.4 < $|y^{t\bar{t}}|$ < 0.8 and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.4 < $|y^{t\bar{t}}|$ < 0.8 at particle level in the 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 $|y^{t\bar{t}}|$ in 0.8 < $|y^{t\bar{t}}|$ < 1.2 and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.4 at particle level in the 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 $|y^{t\bar{t}}|$ in 0.8 < $|y^{t\bar{t}}|$ < 1.2 and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.4 < $|y^{t\bar{t}}|$ < 0.8 at particle level in the 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 $|y^{t\bar{t}}|$ in 0.8 < $|y^{t\bar{t}}|$ < 1.2 and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.8 < $|y^{t\bar{t}}|$ < 1.2 at particle level in the 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 $|y^{t\bar{t}}|$ in 1.2 < $|y^{t\bar{t}}|$ < 2.5 and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.4 at particle level in the 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 $|y^{t\bar{t}}|$ in 1.2 < $|y^{t\bar{t}}|$ < 2.5 and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.4 < $|y^{t\bar{t}}|$ < 0.8 at particle level in the 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 $|y^{t\bar{t}}|$ in 1.2 < $|y^{t\bar{t}}|$ < 2.5 and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.8 < $|y^{t\bar{t}}|$ < 1.2 at particle level in the 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 $|y^{t\bar{t}}|$ in 1.2 < $|y^{t\bar{t}}|$ < 2.5 and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.2 < $|y^{t\bar{t}}|$ < 2.5 at particle level in the 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 $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.4 and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.4 at particle level in the 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 $|y^{t\bar{t}}|$ in 0.4 < $|y^{t\bar{t}}|$ < 0.8 and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.4 at particle level in the 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 $|y^{t\bar{t}}|$ in 0.4 < $|y^{t\bar{t}}|$ < 0.8 and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.4 < $|y^{t\bar{t}}|$ < 0.8 at particle level in the 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 $|y^{t\bar{t}}|$ in 0.8 < $|y^{t\bar{t}}|$ < 1.2 and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.4 at particle level in the 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 $|y^{t\bar{t}}|$ in 0.8 < $|y^{t\bar{t}}|$ < 1.2 and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.4 < $|y^{t\bar{t}}|$ < 0.8 at particle level in the 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 $|y^{t\bar{t}}|$ in 0.8 < $|y^{t\bar{t}}|$ < 1.2 and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.8 < $|y^{t\bar{t}}|$ < 1.2 at particle level in the 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 $|y^{t\bar{t}}|$ in 1.2 < $|y^{t\bar{t}}|$ < 2.5 and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.4 at particle level in the 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 $|y^{t\bar{t}}|$ in 1.2 < $|y^{t\bar{t}}|$ < 2.5 and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.4 < $|y^{t\bar{t}}|$ < 0.8 at particle level in the 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 $|y^{t\bar{t}}|$ in 1.2 < $|y^{t\bar{t}}|$ < 2.5 and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.8 < $|y^{t\bar{t}}|$ < 1.2 at particle level in the 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 $|y^{t\bar{t}}|$ in 1.2 < $|y^{t\bar{t}}|$ < 2.5 and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.2 < $|y^{t\bar{t}}|$ < 2.5 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.4 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.4 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.4 < $|y^{t\bar{t}}|$ < 0.8 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.4 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.4 < $|y^{t\bar{t}}|$ < 0.8 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.4 < $|y^{t\bar{t}}|$ < 0.8 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.8 < $|y^{t\bar{t}}|$ < 1.2 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.4 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.8 < $|y^{t\bar{t}}|$ < 1.2 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.4 < $|y^{t\bar{t}}|$ < 0.8 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.8 < $|y^{t\bar{t}}|$ < 1.2 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.8 < $|y^{t\bar{t}}|$ < 1.2 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.2 < $|y^{t\bar{t}}|$ < 2.5 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.4 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.2 < $|y^{t\bar{t}}|$ < 2.5 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.4 < $|y^{t\bar{t}}|$ < 0.8 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.2 < $|y^{t\bar{t}}|$ < 2.5 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.8 < $|y^{t\bar{t}}|$ < 1.2 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.2 < $|y^{t\bar{t}}|$ < 2.5 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.2 < $|y^{t\bar{t}}|$ < 2.5 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.4 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.4 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.4 < $|y^{t\bar{t}}|$ < 0.8 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.4 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.4 < $|y^{t\bar{t}}|$ < 0.8 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.4 < $|y^{t\bar{t}}|$ < 0.8 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.8 < $|y^{t\bar{t}}|$ < 1.2 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.4 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.8 < $|y^{t\bar{t}}|$ < 1.2 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.4 < $|y^{t\bar{t}}|$ < 0.8 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.8 < $|y^{t\bar{t}}|$ < 1.2 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.8 < $|y^{t\bar{t}}|$ < 1.2 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.2 < $|y^{t\bar{t}}|$ < 2.5 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.4 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.2 < $|y^{t\bar{t}}|$ < 2.5 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.4 < $|y^{t\bar{t}}|$ < 0.8 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.2 < $|y^{t\bar{t}}|$ < 2.5 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.8 < $|y^{t\bar{t}}|$ < 1.2 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.2 < $|y^{t\bar{t}}|$ < 2.5 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.2 < $|y^{t\bar{t}}|$ < 2.5 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 30.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 30.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 30.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 30.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 30.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 30.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 80.0 GeV < $p_{T}^{t\bar{t}}$ < 190.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 30.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 80.0 GeV < $p_{T}^{t\bar{t}}$ < 190.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 30.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 80.0 GeV < $p_{T}^{t\bar{t}}$ < 190.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 80.0 GeV < $p_{T}^{t\bar{t}}$ < 190.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 190.0 GeV < $p_{T}^{t\bar{t}}$ < 800.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 30.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 190.0 GeV < $p_{T}^{t\bar{t}}$ < 800.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 30.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 190.0 GeV < $p_{T}^{t\bar{t}}$ < 800.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 80.0 GeV < $p_{T}^{t\bar{t}}$ < 190.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 190.0 GeV < $p_{T}^{t\bar{t}}$ < 800.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 190.0 GeV < $p_{T}^{t\bar{t}}$ < 800.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 30.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 30.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 30.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 30.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 30.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 30.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 80.0 GeV < $p_{T}^{t\bar{t}}$ < 190.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 30.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 80.0 GeV < $p_{T}^{t\bar{t}}$ < 190.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 30.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 80.0 GeV < $p_{T}^{t\bar{t}}$ < 190.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 80.0 GeV < $p_{T}^{t\bar{t}}$ < 190.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 190.0 GeV < $p_{T}^{t\bar{t}}$ < 800.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 30.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 190.0 GeV < $p_{T}^{t\bar{t}}$ < 800.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 30.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 190.0 GeV < $p_{T}^{t\bar{t}}$ < 800.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 80.0 GeV < $p_{T}^{t\bar{t}}$ < 190.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 190.0 GeV < $p_{T}^{t\bar{t}}$ < 800.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 190.0 GeV < $p_{T}^{t\bar{t}}$ < 800.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t,had}$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t,had}|$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t,had}|$ and the absolute differential cross-section as function of $|y^{t,had}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t,1}$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t,1}$ and the absolute differential cross-section as function of $|y^{t,had}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t,1}$ and the absolute differential cross-section as function of $p_{T}^{t,1}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t,2}$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t,2}$ and the absolute differential cross-section as function of $|y^{t,had}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t,2}$ and the absolute differential cross-section as function of $p_{T}^{t,1}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t,2}$ and the absolute differential cross-section as function of $p_{T}^{t,2}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $m^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $m^{t\bar{t}}$ and the absolute differential cross-section as function of $|y^{t,had}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $m^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,1}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $m^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,2}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $m^{t\bar{t}}$ and the absolute differential cross-section as function of $m^{t\bar{t}}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $|y^{t,had}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,1}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,2}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $m^{t\bar{t}}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|p_{out}^{t,had}|$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|p_{out}^{t,had}|$ and the absolute differential cross-section as function of $|y^{t,had}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|p_{out}^{t,had}|$ and the absolute differential cross-section as function of $p_{T}^{t,1}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|p_{out}^{t,had}|$ and the absolute differential cross-section as function of $p_{T}^{t,2}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|p_{out}^{t,had}|$ and the absolute differential cross-section as function of $m^{t\bar{t}}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|p_{out}^{t,had}|$ and the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|p_{out}^{t,had}|$ and the absolute differential cross-section as function of $|p_{out}^{t,had}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|\Delta\phi(t,\bar{t})|$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|\Delta\phi(t,\bar{t})|$ and the absolute differential cross-section as function of $|y^{t,had}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|\Delta\phi(t,\bar{t})|$ and the absolute differential cross-section as function of $p_{T}^{t,1}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|\Delta\phi(t,\bar{t})|$ and the absolute differential cross-section as function of $p_{T}^{t,2}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|\Delta\phi(t,\bar{t})|$ and the absolute differential cross-section as function of $m^{t\bar{t}}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|\Delta\phi(t,\bar{t})|$ and the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|\Delta\phi(t,\bar{t})|$ and the absolute differential cross-section as function of $|p_{out}^{t,had}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|\Delta\phi(t,\bar{t})|$ and the absolute differential cross-section as function of $|\Delta\phi(t,\bar{t})|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $|y^{t,had}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,1}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,2}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $m^{t\bar{t}}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $|p_{out}^{t,had}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $|\Delta\phi(t,\bar{t})|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{extra jets}$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{extra jets}$ and the absolute differential cross-section as function of $|y^{t,had}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{extra jets}$ and the absolute differential cross-section as function of $p_{T}^{t,1}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{extra jets}$ and the absolute differential cross-section as function of $p_{T}^{t,2}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{extra jets}$ and the absolute differential cross-section as function of $m^{t\bar{t}}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{extra jets}$ and the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{extra jets}$ and the absolute differential cross-section as function of $|p_{out}^{t,had}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{extra jets}$ and the absolute differential cross-section as function of $|\Delta\phi(t,\bar{t})|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{extra jets}$ and the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{extra jets}$ and the absolute differential cross-section as function of $N^{extra jets}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $|y^{t,had}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $p_{T}^{t,1}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $p_{T}^{t,2}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $m^{t\bar{t}}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $|p_{out}^{t,had}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $|\Delta\phi(t,\bar{t})|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $N^{extra jets}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $|y^{t\bar{t}}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ and the absolute differential cross-section as function of $|y^{t,had}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ and the absolute differential cross-section as function of $p_{T}^{t,1}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ and the absolute differential cross-section as function of $p_{T}^{t,2}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ and the absolute differential cross-section as function of $m^{t\bar{t}}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ and the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ and the absolute differential cross-section as function of $|p_{out}^{t,had}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ and the absolute differential cross-section as function of $|\Delta\phi(t,\bar{t})|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ and the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ and the absolute differential cross-section as function of $N^{extra jets}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ and the absolute differential cross-section as function of $|y^{t\bar{t}}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ and the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi^{t\bar{t}}$ and the absolute differential cross-section as function of $|y^{t,had}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,1}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,2}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi^{t\bar{t}}$ and the absolute differential cross-section as function of $m^{t\bar{t}}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi^{t\bar{t}}$ and the absolute differential cross-section as function of $|p_{out}^{t,had}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi^{t\bar{t}}$ and the absolute differential cross-section as function of $|\Delta\phi(t,\bar{t})|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi^{t\bar{t}}$ and the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi^{t\bar{t}}$ and the absolute differential cross-section as function of $N^{extra jets}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi^{t\bar{t}}$ and the absolute differential cross-section as function of $|y^{t\bar{t}}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi^{t\bar{t}}$ and the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi^{t\bar{t}}$ and the absolute differential cross-section as function of $\chi^{t\bar{t}}$ at particle level in the resolved topology.
Covariance matrix of the Relative differential cross-section as function of $p_{T}^{t}$ at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Absolute differential cross-section as function of $p_{T}^{t}$ at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Relative differential cross-section as function of $|y^{t}|$ at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Absolute differential cross-section as function of $|y^{t}|$ at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Relative differential cross-section as function of $m^{t\bar{t}}$ at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Absolute differential cross-section as function of $m^{t\bar{t}}$ at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Relative differential cross-section as function of $p_{T}^{t\bar{t}}$ at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Relative differential cross-section as function of $|y^{t\bar{t}}|$ at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Absolute differential cross-section as function of $|y^{t\bar{t}}|$ at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Relative differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Relative differential cross-section as function of $H_{T}^{t\bar{t}}$ at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Relative differential cross-section as function of $\chi_{tt}$ at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Absolute differential cross-section as function of $\chi_{tt}$ at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 0.0 < $|y^{t}|$ < 0.75 and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 0.0 < $|y^{t}|$ < 0.75 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 0.75 < $|y^{t}|$ < 1.5 and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 0.0 < $|y^{t}|$ < 0.75 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 0.75 < $|y^{t}|$ < 1.5 and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 0.75 < $|y^{t}|$ < 1.5 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 1.5 < $|y^{t}|$ < 2.5 and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 0.0 < $|y^{t}|$ < 0.75 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 1.5 < $|y^{t}|$ < 2.5 and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 0.75 < $|y^{t}|$ < 1.5 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 1.5 < $|y^{t}|$ < 2.5 and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 1.5 < $|y^{t}|$ < 2.5 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 0.0 < $|y^{t}|$ < 0.75 and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 0.0 < $|y^{t}|$ < 0.75 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 0.75 < $|y^{t}|$ < 1.5 and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 0.0 < $|y^{t}|$ < 0.75 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 0.75 < $|y^{t}|$ < 1.5 and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 0.75 < $|y^{t}|$ < 1.5 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 1.5 < $|y^{t}|$ < 2.5 and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 0.0 < $|y^{t}|$ < 0.75 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 1.5 < $|y^{t}|$ < 2.5 and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 0.75 < $|y^{t}|$ < 1.5 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 1.5 < $|y^{t}|$ < 2.5 and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 1.5 < $|y^{t}|$ < 2.5 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 80.0 GeV < $p_{T}^{t\bar{t}}$ < 180.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 80.0 GeV < $p_{T}^{t\bar{t}}$ < 180.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 80.0 GeV < $p_{T}^{t\bar{t}}$ < 180.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 180.0 GeV < $p_{T}^{t\bar{t}}$ < 330.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 180.0 GeV < $p_{T}^{t\bar{t}}$ < 330.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 80.0 GeV < $p_{T}^{t\bar{t}}$ < 180.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 180.0 GeV < $p_{T}^{t\bar{t}}$ < 330.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 180.0 GeV < $p_{T}^{t\bar{t}}$ < 330.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 330.0 GeV < $p_{T}^{t\bar{t}}$ < 800.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 330.0 GeV < $p_{T}^{t\bar{t}}$ < 800.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 80.0 GeV < $p_{T}^{t\bar{t}}$ < 180.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 330.0 GeV < $p_{T}^{t\bar{t}}$ < 800.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 180.0 GeV < $p_{T}^{t\bar{t}}$ < 330.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 330.0 GeV < $p_{T}^{t\bar{t}}$ < 800.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 330.0 GeV < $p_{T}^{t\bar{t}}$ < 800.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 80.0 GeV < $p_{T}^{t\bar{t}}$ < 180.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 80.0 GeV < $p_{T}^{t\bar{t}}$ < 180.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 80.0 GeV < $p_{T}^{t\bar{t}}$ < 180.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 180.0 GeV < $p_{T}^{t\bar{t}}$ < 330.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 180.0 GeV < $p_{T}^{t\bar{t}}$ < 330.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 80.0 GeV < $p_{T}^{t\bar{t}}$ < 180.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 180.0 GeV < $p_{T}^{t\bar{t}}$ < 330.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 180.0 GeV < $p_{T}^{t\bar{t}}$ < 330.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 330.0 GeV < $p_{T}^{t\bar{t}}$ < 800.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 330.0 GeV < $p_{T}^{t\bar{t}}$ < 800.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 80.0 GeV < $p_{T}^{t\bar{t}}$ < 180.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 330.0 GeV < $p_{T}^{t\bar{t}}$ < 800.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 180.0 GeV < $p_{T}^{t\bar{t}}$ < 330.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 330.0 GeV < $p_{T}^{t\bar{t}}$ < 800.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 330.0 GeV < $p_{T}^{t\bar{t}}$ < 800.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 500.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 500.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 500.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 500.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 500.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 500.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 500.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 500.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 500.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 500.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV at parton level in the 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 $|y^{t\bar{t}}|$ in 0.0 GeV < $|y^{t\bar{t}}|$ < 0.5 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 GeV < $|y^{t\bar{t}}|$ < 0.5 GeV at parton level in the 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 $|y^{t\bar{t}}|$ in 0.5 GeV < $|y^{t\bar{t}}|$ < 1.1 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 GeV < $|y^{t\bar{t}}|$ < 0.5 GeV at parton level in the 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 $|y^{t\bar{t}}|$ in 0.5 GeV < $|y^{t\bar{t}}|$ < 1.1 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.5 GeV < $|y^{t\bar{t}}|$ < 1.1 GeV at parton level in the 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 $|y^{t\bar{t}}|$ in 1.1 GeV < $|y^{t\bar{t}}|$ < 1.7 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 GeV < $|y^{t\bar{t}}|$ < 0.5 GeV at parton level in the 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 $|y^{t\bar{t}}|$ in 1.1 GeV < $|y^{t\bar{t}}|$ < 1.7 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.5 GeV < $|y^{t\bar{t}}|$ < 1.1 GeV at parton level in the 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 $|y^{t\bar{t}}|$ in 1.1 GeV < $|y^{t\bar{t}}|$ < 1.7 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.1 GeV < $|y^{t\bar{t}}|$ < 1.7 GeV at parton level in the 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 $|y^{t\bar{t}}|$ in 1.7 GeV < $|y^{t\bar{t}}|$ < 2.5 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 GeV < $|y^{t\bar{t}}|$ < 0.5 GeV at parton level in the 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 $|y^{t\bar{t}}|$ in 1.7 GeV < $|y^{t\bar{t}}|$ < 2.5 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.5 GeV < $|y^{t\bar{t}}|$ < 1.1 GeV at parton level in the 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 $|y^{t\bar{t}}|$ in 1.7 GeV < $|y^{t\bar{t}}|$ < 2.5 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.1 GeV < $|y^{t\bar{t}}|$ < 1.7 GeV at parton level in the 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 $|y^{t\bar{t}}|$ in 1.7 GeV < $|y^{t\bar{t}}|$ < 2.5 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.7 GeV < $|y^{t\bar{t}}|$ < 2.5 GeV at parton level in the 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 $|y^{t\bar{t}}|$ in 0.0 GeV < $|y^{t\bar{t}}|$ < 0.5 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 GeV < $|y^{t\bar{t}}|$ < 0.5 GeV at parton level in the 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 $|y^{t\bar{t}}|$ in 0.5 GeV < $|y^{t\bar{t}}|$ < 1.1 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 GeV < $|y^{t\bar{t}}|$ < 0.5 GeV at parton level in the 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 $|y^{t\bar{t}}|$ in 0.5 GeV < $|y^{t\bar{t}}|$ < 1.1 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.5 GeV < $|y^{t\bar{t}}|$ < 1.1 GeV at parton level in the 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 $|y^{t\bar{t}}|$ in 1.1 GeV < $|y^{t\bar{t}}|$ < 1.7 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 GeV < $|y^{t\bar{t}}|$ < 0.5 GeV at parton level in the 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 $|y^{t\bar{t}}|$ in 1.1 GeV < $|y^{t\bar{t}}|$ < 1.7 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.5 GeV < $|y^{t\bar{t}}|$ < 1.1 GeV at parton level in the 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 $|y^{t\bar{t}}|$ in 1.1 GeV < $|y^{t\bar{t}}|$ < 1.7 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.1 GeV < $|y^{t\bar{t}}|$ < 1.7 GeV at parton level in the 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 $|y^{t\bar{t}}|$ in 1.7 GeV < $|y^{t\bar{t}}|$ < 2.5 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 GeV < $|y^{t\bar{t}}|$ < 0.5 GeV at parton level in the 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 $|y^{t\bar{t}}|$ in 1.7 GeV < $|y^{t\bar{t}}|$ < 2.5 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.5 GeV < $|y^{t\bar{t}}|$ < 1.1 GeV at parton level in the 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 $|y^{t\bar{t}}|$ in 1.7 GeV < $|y^{t\bar{t}}|$ < 2.5 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.1 GeV < $|y^{t\bar{t}}|$ < 1.7 GeV at parton level in the 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 $|y^{t\bar{t}}|$ in 1.7 GeV < $|y^{t\bar{t}}|$ < 2.5 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.7 GeV < $|y^{t\bar{t}}|$ < 2.5 GeV at parton level in the 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 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV at parton level in the 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 500.0 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 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV at parton level in the 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 500.0 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 500.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the 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 < $m^{t\bar{t}}$ < 1000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV at parton level in the 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 < $m^{t\bar{t}}$ < 1000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 500.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the 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 < $m^{t\bar{t}}$ < 1000.0 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 < $m^{t\bar{t}}$ < 1000.0 GeV at parton level in the 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 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV at parton level in the 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 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 500.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the 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 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 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 < $m^{t\bar{t}}$ < 1000.0 GeV at parton level in the 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 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV at parton level in the 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 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV at parton level in the 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 500.0 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 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV at parton level in the 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 500.0 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 500.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the 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 < $m^{t\bar{t}}$ < 1000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV at parton level in the 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 < $m^{t\bar{t}}$ < 1000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 500.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the 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 < $m^{t\bar{t}}$ < 1000.0 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 < $m^{t\bar{t}}$ < 1000.0 GeV at parton level in the 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 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV at parton level in the 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 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 500.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the 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 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 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 < $m^{t\bar{t}}$ < 1000.0 GeV at parton level in the 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 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.5 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.5 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.5 < $|y^{t\bar{t}}|$ < 1.1 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.5 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.5 < $|y^{t\bar{t}}|$ < 1.1 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.5 < $|y^{t\bar{t}}|$ < 1.1 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.1 < $|y^{t\bar{t}}|$ < 1.7 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.5 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.1 < $|y^{t\bar{t}}|$ < 1.7 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.5 < $|y^{t\bar{t}}|$ < 1.1 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.1 < $|y^{t\bar{t}}|$ < 1.7 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.1 < $|y^{t\bar{t}}|$ < 1.7 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.7 < $|y^{t\bar{t}}|$ < 2.5 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.5 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.7 < $|y^{t\bar{t}}|$ < 2.5 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.5 < $|y^{t\bar{t}}|$ < 1.1 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.7 < $|y^{t\bar{t}}|$ < 2.5 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.1 < $|y^{t\bar{t}}|$ < 1.7 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.7 < $|y^{t\bar{t}}|$ < 2.5 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.7 < $|y^{t\bar{t}}|$ < 2.5 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.5 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.5 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.5 < $|y^{t\bar{t}}|$ < 1.1 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.5 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.5 < $|y^{t\bar{t}}|$ < 1.1 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.5 < $|y^{t\bar{t}}|$ < 1.1 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.1 < $|y^{t\bar{t}}|$ < 1.7 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.5 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.1 < $|y^{t\bar{t}}|$ < 1.7 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.5 < $|y^{t\bar{t}}|$ < 1.1 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.1 < $|y^{t\bar{t}}|$ < 1.7 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.1 < $|y^{t\bar{t}}|$ < 1.7 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.7 < $|y^{t\bar{t}}|$ < 2.5 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.5 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.7 < $|y^{t\bar{t}}|$ < 2.5 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.5 < $|y^{t\bar{t}}|$ < 1.1 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.7 < $|y^{t\bar{t}}|$ < 2.5 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.1 < $|y^{t\bar{t}}|$ < 1.7 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.7 < $|y^{t\bar{t}}|$ < 2.5 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.7 < $|y^{t\bar{t}}|$ < 2.5 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t}$ and the absolute differential cross-section as function of $p_{T}^{t}$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t}|$ and the absolute differential cross-section as function of $p_{T}^{t}$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t}|$ and the absolute differential cross-section as function of $|y^{t}|$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $m^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t}$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $m^{t\bar{t}}$ and the absolute differential cross-section as function of $|y^{t}|$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $m^{t\bar{t}}$ and the absolute differential cross-section as function of $m^{t\bar{t}}$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t}$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $|y^{t}|$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $m^{t\bar{t}}$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $p_{T}^{t}$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $|y^{t}|$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $m^{t\bar{t}}$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $|y^{t\bar{t}}|$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ and the absolute differential cross-section as function of $p_{T}^{t}$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ and the absolute differential cross-section as function of $|y^{t}|$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ and the absolute differential cross-section as function of $m^{t\bar{t}}$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ and the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ and the absolute differential cross-section as function of $|y^{t\bar{t}}|$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ and the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t}$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $|y^{t}|$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $m^{t\bar{t}}$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $|y^{t\bar{t}}|$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi_{tt}$ and the absolute differential cross-section as function of $p_{T}^{t}$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi_{tt}$ and the absolute differential cross-section as function of $|y^{t}|$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi_{tt}$ and the absolute differential cross-section as function of $m^{t\bar{t}}$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi_{tt}$ and the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi_{tt}$ and the absolute differential cross-section as function of $|y^{t\bar{t}}|$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi_{tt}$ and the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi_{tt}$ and the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi_{tt}$ and the absolute differential cross-section as function of $\chi_{tt}$ at parton level in the resolved topology.
Covariance matrix of the Relative differential cross-section as function of $p_{T}^{t,had}$ at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Relative differential cross-section as function of $|y^{t,had}|$ at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Absolute differential cross-section as function of $|y^{t,had}|$ at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Relative differential cross-section as function of $p_{T}^{t,1}$ at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Absolute differential cross-section as function of $p_{T}^{t,1}$ at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Relative differential cross-section as function of $p_{T}^{t,2}$ at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Absolute differential cross-section as function of $p_{T}^{t,2}$ at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Relative differential cross-section as function of $p_{T}^{t\bar{t}}$ at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Relative differential cross-section as function of $|y^{t\bar{t}}|$ at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Absolute differential cross-section as function of $|y^{t\bar{t}}|$ at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Relative differential cross-section as function of $m^{t\bar{t}}$ at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Absolute differential cross-section as function of $m^{t\bar{t}}$ at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Relative differential cross-section as function of $\chi^{t\bar{t}}$ at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Absolute differential cross-section as function of $\chi^{t\bar{t}}$ at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Relative differential cross-section as function of $|p_{out}^{t,lep}|$ at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Absolute differential cross-section as function of $|p_{out}^{t,lep}|$ at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Relative differential cross-section as function of $H_{T}^{t\bar{t}}$ at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Relative differential cross-section as function of $N^{extra jets}$ at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Absolute differential cross-section as function of $N^{extra jets}$ at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Relative differential cross-section as function of $N^{subjets}$ at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Absolute differential cross-section as function of $N^{subjets}$ at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 40.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 40.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 40.0 GeV < $p_{T}^{t\bar{t}}$ < 150.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 40.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 40.0 GeV < $p_{T}^{t\bar{t}}$ < 150.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 40.0 GeV < $p_{T}^{t\bar{t}}$ < 150.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 150.0 GeV < $p_{T}^{t\bar{t}}$ < 1000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 40.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 150.0 GeV < $p_{T}^{t\bar{t}}$ < 1000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 40.0 GeV < $p_{T}^{t\bar{t}}$ < 150.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 150.0 GeV < $p_{T}^{t\bar{t}}$ < 1000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 150.0 GeV < $p_{T}^{t\bar{t}}$ < 1000.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 40.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 40.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 40.0 GeV < $p_{T}^{t\bar{t}}$ < 150.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 40.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 40.0 GeV < $p_{T}^{t\bar{t}}$ < 150.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 40.0 GeV < $p_{T}^{t\bar{t}}$ < 150.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 150.0 GeV < $p_{T}^{t\bar{t}}$ < 1000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 40.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 150.0 GeV < $p_{T}^{t\bar{t}}$ < 1000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 40.0 GeV < $p_{T}^{t\bar{t}}$ < 150.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 150.0 GeV < $p_{T}^{t\bar{t}}$ < 1000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 150.0 GeV < $p_{T}^{t\bar{t}}$ < 1000.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 1.0 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 1.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t\bar{t}}|$ in 1.0 < $|y^{t\bar{t}}|$ < 2.0 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 1.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t\bar{t}}|$ in 1.0 < $|y^{t\bar{t}}|$ < 2.0 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t\bar{t}}|$ in 1.0 < $|y^{t\bar{t}}|$ < 2.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 1.0 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 1.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t\bar{t}}|$ in 1.0 < $|y^{t\bar{t}}|$ < 2.0 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 1.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t\bar{t}}|$ in 1.0 < $|y^{t\bar{t}}|$ < 2.0 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t\bar{t}}|$ in 1.0 < $|y^{t\bar{t}}|$ < 2.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 0.0 < $|y^{t,had}|$ < 1.0 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 0.0 < $|y^{t,had}|$ < 1.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 1.0 < $|y^{t,had}|$ < 2.0 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 0.0 < $|y^{t,had}|$ < 1.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 1.0 < $|y^{t,had}|$ < 2.0 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 1.0 < $|y^{t,had}|$ < 2.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 0.0 < $|y^{t,had}|$ < 1.0 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 0.0 < $|y^{t,had}|$ < 1.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 1.0 < $|y^{t,had}|$ < 2.0 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 0.0 < $|y^{t,had}|$ < 1.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 1.0 < $|y^{t,had}|$ < 2.0 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 1.0 < $|y^{t,had}|$ < 2.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 490.0 GeV < $m^{t\bar{t}}$ < 1160.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 490.0 GeV < $m^{t\bar{t}}$ < 1160.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 1160.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 490.0 GeV < $m^{t\bar{t}}$ < 1160.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 1160.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 1160.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 490.0 GeV < $m^{t\bar{t}}$ < 1160.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 490.0 GeV < $m^{t\bar{t}}$ < 1160.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 1160.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 490.0 GeV < $m^{t\bar{t}}$ < 1160.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 1160.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 1160.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $H_{T}^{t\bar{t}}$ in 350.0 GeV < $H_{T}^{t\bar{t}}$ < 780.0 GeV and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $H_{T}^{t\bar{t}}$ in 350.0 GeV < $H_{T}^{t\bar{t}}$ < 780.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $H_{T}^{t\bar{t}}$ in 780.0 GeV < $H_{T}^{t\bar{t}}$ < 2500.0 GeV and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $H_{T}^{t\bar{t}}$ in 350.0 GeV < $H_{T}^{t\bar{t}}$ < 780.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $H_{T}^{t\bar{t}}$ in 780.0 GeV < $H_{T}^{t\bar{t}}$ < 2500.0 GeV and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $H_{T}^{t\bar{t}}$ in 780.0 GeV < $H_{T}^{t\bar{t}}$ < 2500.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $H_{T}^{t\bar{t}}$ in 350.0 GeV < $H_{T}^{t\bar{t}}$ < 780.0 GeV and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $H_{T}^{t\bar{t}}$ in 350.0 GeV < $H_{T}^{t\bar{t}}$ < 780.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $H_{T}^{t\bar{t}}$ in 780.0 GeV < $H_{T}^{t\bar{t}}$ < 2500.0 GeV and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $H_{T}^{t\bar{t}}$ in 350.0 GeV < $H_{T}^{t\bar{t}}$ < 780.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $H_{T}^{t\bar{t}}$ in 780.0 GeV < $H_{T}^{t\bar{t}}$ < 2500.0 GeV and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $H_{T}^{t\bar{t}}$ in 780.0 GeV < $H_{T}^{t\bar{t}}$ < 2500.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 40.0 GeV and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 40.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 40.0 GeV < $p_{T}^{t\bar{t}}$ < 150.0 GeV and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 40.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 40.0 GeV < $p_{T}^{t\bar{t}}$ < 150.0 GeV and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 40.0 GeV < $p_{T}^{t\bar{t}}$ < 150.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 150.0 GeV < $p_{T}^{t\bar{t}}$ < 1000.0 GeV and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 40.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 150.0 GeV < $p_{T}^{t\bar{t}}$ < 1000.0 GeV and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 40.0 GeV < $p_{T}^{t\bar{t}}$ < 150.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 150.0 GeV < $p_{T}^{t\bar{t}}$ < 1000.0 GeV and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 150.0 GeV < $p_{T}^{t\bar{t}}$ < 1000.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 40.0 GeV and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 40.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 40.0 GeV < $p_{T}^{t\bar{t}}$ < 150.0 GeV and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 40.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 40.0 GeV < $p_{T}^{t\bar{t}}$ < 150.0 GeV and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 40.0 GeV < $p_{T}^{t\bar{t}}$ < 150.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 150.0 GeV < $p_{T}^{t\bar{t}}$ < 1000.0 GeV and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 40.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 150.0 GeV < $p_{T}^{t\bar{t}}$ < 1000.0 GeV and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 40.0 GeV < $p_{T}^{t\bar{t}}$ < 150.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 150.0 GeV < $p_{T}^{t\bar{t}}$ < 1000.0 GeV and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 150.0 GeV < $p_{T}^{t\bar{t}}$ < 1000.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.65 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.65 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.65 < $|y^{t\bar{t}}|$ < 1.3 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.65 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.65 < $|y^{t\bar{t}}|$ < 1.3 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.65 < $|y^{t\bar{t}}|$ < 1.3 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.3 < $|y^{t\bar{t}}|$ < 2.0 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.65 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.3 < $|y^{t\bar{t}}|$ < 2.0 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.65 < $|y^{t\bar{t}}|$ < 1.3 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.3 < $|y^{t\bar{t}}|$ < 2.0 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.3 < $|y^{t\bar{t}}|$ < 2.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.65 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.65 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.65 < $|y^{t\bar{t}}|$ < 1.3 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.65 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.65 < $|y^{t\bar{t}}|$ < 1.3 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.65 < $|y^{t\bar{t}}|$ < 1.3 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.3 < $|y^{t\bar{t}}|$ < 2.0 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.65 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.3 < $|y^{t\bar{t}}|$ < 2.0 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.65 < $|y^{t\bar{t}}|$ < 1.3 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.3 < $|y^{t\bar{t}}|$ < 2.0 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.3 < $|y^{t\bar{t}}|$ < 2.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 0.5 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 0.5 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 2.0 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 0.5 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 2.0 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 2.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 3.0 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 0.5 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 3.0 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 2.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 3.0 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 3.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 0.5 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 0.5 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 2.0 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 0.5 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 2.0 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 2.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 3.0 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 0.5 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 3.0 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 2.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 3.0 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 3.0 at particle level in the boosted 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 $N^{extra jets}$ in $N^{extra jets}$ = 0.5 and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 0.5 at particle level in the boosted 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 $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 2.5 and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 0.5 at particle level in the boosted 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 $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 2.5 and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 2.5 at particle level in the boosted 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 $N^{extra jets}$ in $N^{extra jets}$ = 0.5 and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 0.5 at particle level in the boosted 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 $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 2.5 and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 0.5 at particle level in the boosted 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 $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 2.5 and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 2.5 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 0.0 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 0.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 1.0 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 0.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 1.0 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 1.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 2.0 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 0.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 2.0 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 1.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 2.0 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 2.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 0.0 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 0.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 1.0 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 0.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 1.0 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 1.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 2.0 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 0.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 2.0 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 1.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 2.0 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 2.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t,had}$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t,had}|$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t,had}|$ and the absolute differential cross-section as function of $|y^{t,had}|$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t,1}$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t,1}$ and the absolute differential cross-section as function of $|y^{t,had}|$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t,1}$ and the absolute differential cross-section as function of $p_{T}^{t,1}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t,2}$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t,2}$ and the absolute differential cross-section as function of $|y^{t,had}|$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t,2}$ and the absolute differential cross-section as function of $p_{T}^{t,1}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t,2}$ and the absolute differential cross-section as function of $p_{T}^{t,2}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $|y^{t,had}|$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,1}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,2}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $|y^{t,had}|$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $p_{T}^{t,1}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $p_{T}^{t,2}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $|y^{t\bar{t}}|$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $m^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $m^{t\bar{t}}$ and the absolute differential cross-section as function of $|y^{t,had}|$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $m^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,1}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $m^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,2}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $m^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $m^{t\bar{t}}$ and the absolute differential cross-section as function of $|y^{t\bar{t}}|$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $m^{t\bar{t}}$ and the absolute differential cross-section as function of $m^{t\bar{t}}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi^{t\bar{t}}$ and the absolute differential cross-section as function of $|y^{t,had}|$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,1}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,2}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi^{t\bar{t}}$ and the absolute differential cross-section as function of $|y^{t\bar{t}}|$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi^{t\bar{t}}$ and the absolute differential cross-section as function of $m^{t\bar{t}}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi^{t\bar{t}}$ and the absolute differential cross-section as function of $\chi^{t\bar{t}}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|p_{out}^{t,lep}|$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|p_{out}^{t,lep}|$ and the absolute differential cross-section as function of $|y^{t,had}|$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|p_{out}^{t,lep}|$ and the absolute differential cross-section as function of $p_{T}^{t,1}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|p_{out}^{t,lep}|$ and the absolute differential cross-section as function of $p_{T}^{t,2}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|p_{out}^{t,lep}|$ and the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|p_{out}^{t,lep}|$ and the absolute differential cross-section as function of $|y^{t\bar{t}}|$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|p_{out}^{t,lep}|$ and the absolute differential cross-section as function of $m^{t\bar{t}}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|p_{out}^{t,lep}|$ and the absolute differential cross-section as function of $\chi^{t\bar{t}}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|p_{out}^{t,lep}|$ and the absolute differential cross-section as function of $|p_{out}^{t,lep}|$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $|y^{t,had}|$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,1}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,2}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $|y^{t\bar{t}}|$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $m^{t\bar{t}}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $\chi^{t\bar{t}}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $|p_{out}^{t,lep}|$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{extra jets}$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{extra jets}$ and the absolute differential cross-section as function of $|y^{t,had}|$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{extra jets}$ and the absolute differential cross-section as function of $p_{T}^{t,1}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{extra jets}$ and the absolute differential cross-section as function of $p_{T}^{t,2}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{extra jets}$ and the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{extra jets}$ and the absolute differential cross-section as function of $|y^{t\bar{t}}|$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{extra jets}$ and the absolute differential cross-section as function of $m^{t\bar{t}}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{extra jets}$ and the absolute differential cross-section as function of $\chi^{t\bar{t}}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{extra jets}$ and the absolute differential cross-section as function of $|p_{out}^{t,lep}|$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{extra jets}$ and the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{extra jets}$ and the absolute differential cross-section as function of $N^{extra jets}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{subjets}$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{subjets}$ and the absolute differential cross-section as function of $|y^{t,had}|$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{subjets}$ and the absolute differential cross-section as function of $p_{T}^{t,1}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{subjets}$ and the absolute differential cross-section as function of $p_{T}^{t,2}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{subjets}$ and the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{subjets}$ and the absolute differential cross-section as function of $|y^{t\bar{t}}|$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{subjets}$ and the absolute differential cross-section as function of $m^{t\bar{t}}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{subjets}$ and the absolute differential cross-section as function of $\chi^{t\bar{t}}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{subjets}$ and the absolute differential cross-section as function of $|p_{out}^{t,lep}|$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{subjets}$ and the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{subjets}$ and the absolute differential cross-section as function of $N^{extra jets}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{subjets}$ and the absolute differential cross-section as function of $N^{subjets}$ at particle level in the boosted topology.
Covariance matrix of the Relative differential cross-section as function of $m^{t\bar{t}}$ at parton level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Absolute differential cross-section as function of $m^{t\bar{t}}$ at parton level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Relative differential cross-section as function of $p_{T}^{t}$ at parton level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix of the Absolute differential cross-section as function of $p_{T}^{t}$ at parton level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t}$ in 350.0 GeV < $p_{T}^{t}$ < 550.0 GeV and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t}$ in 350.0 GeV < $p_{T}^{t}$ < 550.0 GeV at parton level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t}$ in 550.0 GeV < $p_{T}^{t}$ < 2000.0 GeV and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t}$ in 350.0 GeV < $p_{T}^{t}$ < 550.0 GeV at parton level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t}$ in 550.0 GeV < $p_{T}^{t}$ < 2000.0 GeV and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t}$ in 550.0 GeV < $p_{T}^{t}$ < 2000.0 GeV at parton level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t}$ in 350.0 GeV < $p_{T}^{t}$ < 550.0 GeV and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t}$ in 350.0 GeV < $p_{T}^{t}$ < 550.0 GeV at parton level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t}$ in 550.0 GeV < $p_{T}^{t}$ < 2000.0 GeV and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t}$ in 350.0 GeV < $p_{T}^{t}$ < 550.0 GeV at parton level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t}$ in 550.0 GeV < $p_{T}^{t}$ < 2000.0 GeV and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t}$ in 550.0 GeV < $p_{T}^{t}$ < 2000.0 GeV at parton level in the boosted topology, accounting for the statistical and systematic uncertainties.
Statistical correlation matrix between the absolute differential cross-section as function of $m^{t\bar{t}}$ and the absolute differential cross-section as function of $m^{t\bar{t}}$ at parton level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t}$ and the absolute differential cross-section as function of $m^{t\bar{t}}$ at parton level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t}$ and the absolute differential cross-section as function of $p_{T}^{t}$ at parton level in the boosted topology.
The distribution and orientation of energy inside jets is predicted to be an experimental handle on colour connections between the hard--scatter quarks and gluons initiating the jets. This Letter presents a measurement of the distribution of one such variable, the jet pull angle. The pull angle is measured for jets produced in $t\bar{t}$ events with one $W$ boson decaying leptonically and the other decaying to jets using 20.3 fb$^{-1}$ of data recorded with the ATLAS detector at a centre-of-mass energy of $\sqrt{s}=8$ TeV at the LHC. The jet pull angle distribution is corrected for detector resolution and acceptance effects and is compared to various models.
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