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This paper presents for the first time a precise measurement of the production properties of the Z boson in the full phase space of the decay leptons. The measurement is obtained from proton-proton collision data collected by the ATLAS experiment in 2012 at $\sqrt s$ = 8 TeV at the LHC and corresponding to an integrated luminosity of 20.2 fb$^{-1}$. The results, based on a total of 15.3 million Z-boson decays to electron and muon pairs, extend and improve a previous measurement of the full set of angular coefficients describing Z-boson decay. The double-differential cross-section distributions in Z-boson transverse momentum p$_T$ and rapidity y are measured in the pole region, defined as 80 $<$ m $<$ 100 GeV, over the range $|y| <$ 3.6. The total uncertainty of the normalised cross-section measurements in the peak region of the p$_T$ distribution is dominated by statistical uncertainties over the full range and increases as a function of rapidity from 0.5-1.0% for $|y| <$ 2.0 to 2-7% at higher rapidities. The results for the rapidity-dependent transverse momentum distributions are compared to state-of-the-art QCD predictions, which combine in the best cases approximate N$^4$LL resummation with N$^3$LO fixed-order perturbative calculations. The differential rapidity distributions integrated over p$_T$ are even more precise, with accuracies from 0.2-0.3% for $|y| <$ 2.0 to 0.4-0.9% at higher rapidities, and are compared to fixed-order QCD predictions using the most recent parton distribution functions. The agreement between data and predictions is quite good in most cases.
A measurement of single top-quark production in the s-channel is performed in proton$-$proton collisions at a centre-of-mass energy of 13 TeV with the ATLAS detector at the CERN Large Hadron Collider. The dataset corresponds to an integrated luminosity of 139 fb$^{-1}$. The analysis is performed on events with an electron or muon, missing transverse momentum and exactly two $b$-tagged jets in the final state. A discriminant based on matrix element calculations is used to separate single-top-quark s-channel events from the main background contributions, which are top-quark pair production and $W$-boson production in association with jets. The observed (expected) signal significance over the background-only hypothesis is 3.3 (3.9) standard deviations, and the measured cross-section is $\sigma=8.2^{+3.5}_{-2.9}$ pb, consistent with the Standard Model prediction of $\sigma^{\mathrm{SM}}=10.32^{+0.40}_{-0.36}$ pb.
Distribution of ${E}_{T}^{miss}$ after the fit of the multijet backgrounds, in the electron channel, in the signal region, without applying the cut on ${E}_{T}^{miss}$. Simulated events are normalised to the expected number of events given the integrated luminosity, after applying the normalisation factors obtained in the multijet fit. The last bin includes the overflow. The uncertainty band indicates the simulation's statistical uncertainty, the normalisation uncertainties for different processes ($40$ % for $W$+jets production, $30$ % for multijet background and $6$ % for top-quark processes) and the multijet background shape uncertainty in each bin, summed in quadrature. The lower panel of the figure shows the ratio of the data to the prediction.
Distribution of ${E}_{T}^{miss}$ after the fit of the multijet backgrounds, in the electron channel, in the $W$+jets VR, without applying the cut on ${E}_{T}^{miss}$. Simulated events are normalised to the expected number of events given the integrated luminosity, after applying the normalisation factors obtained in the multijet fit. The last bin includes the overflow. The uncertainty band indicates the simulation's statistical uncertainty, the normalisation uncertainties for different processes ($40$ % for $W$+jets production, $30$ % for multijet background and $6$ % for top-quark processes) and the multijet background shape uncertainty in each bin, summed in quadrature. The lower panel of the figure shows the ratio of the data to the prediction.
Distribution of ${E}_{T}^{miss}$ after the fit of the multijet backgrounds, in the electron channel, in the $t\bar{t}$ 3-jets VR, without applying the cut on ${E}_{T}^{miss}$. Simulated events are normalised to the expected number of events given the integrated luminosity, after applying the normalisation factors obtained in the multijet fit. The last bin includes the overflow. The uncertainty band indicates the simulation's statistical uncertainty, the normalisation uncertainties for different processes ($40$ % for $W$+jets production, $30$ % for multijet background and $6$ % for top-quark processes) and the multijet background shape uncertainty in each bin, summed in quadrature. The lower panel of the figure shows the ratio of the data to the prediction.
Distribution of ${E}_{T}^{miss}$ after the fit of the multijet backgrounds, in the electron channel, in the $t\bar{t}$ 4-jets VR, without applying the cut on ${E}_{T}^{miss}$. Simulated events are normalised to the expected number of events given the integrated luminosity, after applying the normalisation factors obtained in the multijet fit. The last bin includes the overflow. The uncertainty band indicates the simulation's statistical uncertainty, the normalisation uncertainties for different processes ($40$ % for $W$+jets production, $30$ % for multijet background and $6$ % for top-quark processes) and the multijet background shape uncertainty in each bin, summed in quadrature. The lower panel of the figure shows the ratio of the data to the prediction.
Distribution of $m_{T}^{W}$ after the fit of the multijet backgrounds, in the muon channel, in the signal region, without applying the cut on $m_{T}^{W}$. Simulated events are normalised to the expected number of events given the integrated luminosity, after applying the normalisation factors obtained in the multijet fit. The last bin includes the overflow. The uncertainty band indicates the simulation's statistical uncertainty, the normalisation uncertainties for different processes ($40$ % for $W$+jets production, $30$ % for multijet background and $6$ % for top-quark processes) and the multijet background shape uncertainty in each bin, summed in quadrature. The lower panel of the figure shows the ratio of the data to the prediction.
Distribution of $m_{T}^{W}$ after the fit of the multijet backgrounds, in the muon channel, in the $W$+jets VR, without applying the cut on $m_{T}^{W}$. Simulated events are normalised to the expected number of events given the integrated luminosity, after applying the normalisation factors obtained in the multijet fit. The last bin includes the overflow. The uncertainty band indicates the simulation's statistical uncertainty, the normalisation uncertainties for different processes ($40$ % for $W$+jets production, $30$ % for multijet background and $6$ % for top-quark processes) and the multijet background shape uncertainty in each bin, summed in quadrature. The lower panel of the figure shows the ratio of the data to the prediction.
Distribution of $m_{T}^{W}$ after the fit of the multijet backgrounds, in the muon channel, in the $t\bar{t}$ 3-jets VR, without applying the cut on $m_{T}^{W}$. Simulated events are normalised to the expected number of events given the integrated luminosity, after applying the normalisation factors obtained in the multijet fit. The last bin includes the overflow. The uncertainty band indicates the simulation's statistical uncertainty, the normalisation uncertainties for different processes ($40$ % for $W$+jets production, $30$ % for multijet background and $6$ % for top-quark processes) and the multijet background shape uncertainty in each bin, summed in quadrature. The lower panel of the figure shows the ratio of the data to the prediction.
Distribution of $m_{T}^{W}$ after the fit of the multijet backgrounds, in the muon channel, in the $t\bar{t}$ 4-jets VR, without applying the cut on $m_{T}^{W}$. Simulated events are normalised to the expected number of events given the integrated luminosity, after applying the normalisation factors obtained in the multijet fit. The last bin includes the overflow. The uncertainty band indicates the simulation's statistical uncertainty, the normalisation uncertainties for different processes ($40$ % for $W$+jets production, $30$ % for multijet background and $6$ % for top-quark processes) and the multijet background shape uncertainty in each bin, summed in quadrature. The lower panel of the figure shows the ratio of the data to the prediction.
Expected distributions of the MEM discriminant $P(S|X)$ in the SR, for the s-channel single-top signal, and for the $t\bar{t}$ and $W$+jets backgrounds, for MEM discriminant values larger than $2.0\times10^{-4}$. Each distribution is normalised to unity. The binning is the same as the optimised binning used in the signal extraction fit, resulting in a non-linear horizontal scale.
Distribution of the MEM discriminant $P(S|X)$ in the $W$+jets VR. Simulated events are normalised to the expected number of events given the integrated luminosity, after applying the normalisation factors obtained in the multijet fit presented in Section 5 in the paper. The uncertainty band indicates the simulation's statistical uncertainty and the normalisation uncertainties for the various processes in each bin, summed in quadrature. The ratio of the observed number to the predicted number of events in each bin is shown in the lower panel of the figure, with different vertical axis ranges. The binning is the same as the optimised binning used in the signal extraction fit described in Section 8 in the paper, resulting in a non-linear horizontal scale.
Distribution of the MEM discriminant $P(S|X)$ in the $t\bar{t}$ 3-jets VR. Simulated events are normalised to the expected number of events given the integrated luminosity, after applying the normalisation factors obtained in the multijet fit presented in Section 5 in the paper. The uncertainty band indicates the simulation's statistical uncertainty and the normalisation uncertainties for the various processes in each bin, summed in quadrature. The ratio of the observed number to the predicted number of events in each bin is shown in the lower panel of the figure, with different vertical axis ranges. The binning is the same as the optimised binning used in the signal extraction fit described in Section 8 in the paper, resulting in a non-linear horizontal scale.
Distribution of the MEM discriminant $P(S|X)$ in the $t\bar{t}$ 4-jets VR. Simulated events are normalised to the expected number of events given the integrated luminosity, after applying the normalisation factors obtained in the multijet fit presented in Section 5 in the paper. The uncertainty bands indicate the simulation's statistical uncertainty and the normalisation uncertainties for the various processes in each bin, summed in quadrature. The ratio of the observed number to the predicted number of events in each bin is shown in the lower panel of the figure, with different vertical axis ranges. The binning is the same as the optimised binning used in the signal extraction fit described in Section 8 in the paper, resulting in a non-linear horizontal scale.
Distribution of the MEM discriminant $P(S|X)$ in the SR before the fit to data, for MEM discriminant values larger than $2.0\times10^{-4}$. The lower panel of the figure shows the ratio of the data to the prediction, with different vertical axis ranges. The uncertainty band indicates the total uncertainties and their correlations in each bin. The uncertainties in the $t\bar{t}$ and $W$+jets normalisation factors, as well as in the s-channel signal cross-section, are not defined pre-fit and therefore not included. The binning is the same as the optimised binning used in the fit, resulting in a non-linear horizontal scale.
Distribution of the MEM discriminant $P(S|X)$ in the SR after the fit to data, for MEM discriminant values larger than $2.0\times10^{-4}$. The lower panel of the figure shows the ratio of the data to the prediction, with different vertical axis ranges. The uncertainty band indicates the total uncertainties and their correlations in each bin. The binning is the same as the optimised binning used in the fit, resulting in a non-linear horizontal scale.
Distribution of the MEM discriminant $P(S|X)$ in the SR after the fit to data, for MEM discriminant values larger than $2.0\times10^{-4}$, after subtraction of all backgrounds. The fitted distribution for the simulation of the signal is shown together with the post-fit uncertainty in the backgrounds. The binning is the same as the optimised binning used in the fit, resulting in a non-linear horizontal scale.
Observed impact of the different sources of uncertainty on the measured s-channel signal cross-section, grouped by categories. The impact of each category is obtained by repeating the fit after having fixed the set of nuisance parameters corresponding to that category, subtracting the square of the resulting uncertainty from the square of the uncertainty found in the full fit, and calculating the square root. The 'Systematic uncertainties' category combines all sources of systematic uncertainties. The statistical uncertainty is obtained by repeating the fit after having fixed all nuisance parameters, including the $t\bar{t}$ and $W$+jets normalisation factors. 'Total' gives the total uncertainty on the measurement.
Observed impact of the different sources of $t\bar{t}$ modelling uncertainty on the measured s-channel signal cross-section. The impact of each category is obtained by repeating the fit after having fixed the set of nuisance parameters corresponding to that category, subtracting the square of the resulting uncertainty from the square of the uncertainty found in the full fit, and calculating the square root. 'PS & had.' refers to the parton shower and hadronisation model, and 'ME/PS matching' to the matching of the ME to the parton shower.
Observed impact of the different sources of s-channel modelling uncertainty on the measured s-channel signal cross-section. The impact of each category is obtained by repeating the fit after having fixed the set of nuisance parameters corresponding to that category, subtracting the square of the resulting uncertainty from the square of the uncertainty found in the full fit, and calculating the square root. 'PS & had.' refers to the parton shower and hadronisation model, as described in Section 7 in the paper.
Observed impact of the different sources of t-channel modelling uncertainty on the measured s-channel signal cross-section. The impact of each category is obtained by repeating the fit after having fixed the set of nuisance parameters corresponding to that category, subtracting the square of the resulting uncertainty from the square of the uncertainty found in the full fit, and calculating the square root. 'PS & had.' refers to the parton shower and hadronisation model, as described in Section 7 in the paper.
Observed impact of the different sources of $tW$ modelling uncertainty on the measured s-channel signal cross-section, grouped by categories. The impact of each category is obtained by repeating the fit after having fixed the set of nuisance parameters corresponding to that category, subtracting the square of the resulting uncertainty from the square of the uncertainty found in the full fit, and calculating the square root. 'PS & had.' refers to the parton shower and hadronisation model, and '$t\bar{t}$ overlap' to the algorithm removing the overlap between $tW$ and $t\bar{t}$ production at NLO, as described in Section 7 in the paper.
Observed impact of the different sources of PDF uncertainties on the measured s-channel signal cross-section, grouped by categories. The impact of each category is obtained by repeating the fit after having fixed the set of nuisance parameters corresponding to that category, subtracting the square of the resulting uncertainty from the square of the uncertainty found in the full fit, and calculating the square root.
Comparison between data and prediction after the fit to data in the signal region for the leading-jet $p_{T}$. The last bin includes the overflow. The uncertainty band includes all uncertainties and their correlations. The lower panel of the figure shows the ratio of the data to the prediction.
Comparison between data and prediction after the fit to data in the signal region for the leading-jet $\eta$. The uncertainty band includes all uncertainties and their correlations. The lower panel of the figure shows the ratio of the data to the prediction.
Comparison between data and prediction after the fit to data in the signal region for the subleading-jet $p_{T}$. The last bin includes the overflow. The uncertainty band includes all uncertainties and their correlations. The lower panel of the figure shows the ratio of the data to the prediction.
Comparison between data and prediction after the fit to data in the signal region for the subleading-jet $\eta$. The uncertainty band includes all uncertainties and their correlations. The lower panel of the figure shows the ratio of the data to the prediction.
Comparison between data and prediction after the fit to data in the signal region for the lepton $p_{T}$. The last bin includes the overflow. The uncertainty band includes all uncertainties and their correlations. The lower panel of the figure shows the ratio of the data to the prediction.
Comparison between data and prediction after the fit to data in the signal region for the lepton $\eta$. The uncertainty band includes all uncertainties and their correlations. The lower panel of the figure shows the ratio of the data to the prediction.
Comparison between data and prediction after the fit to data in the signal region for the ${E}_{T}^{miss}$. The last bin includes the overflow. The uncertainty band includes all uncertainties and their correlations. The lower panel of the figure shows the ratio of the data to the prediction.
Comparison between data and prediction after the fit to data in the signal region for the $m_{T}^{W}$. The last bin includes the overflow. The uncertainty band includes all uncertainties and their correlations. The lower panel of the figure shows the ratio of the data to the prediction.
Nuisance parameters ranked according to their post-fit impacts on the best-fit value of the ratio $\mu$ of the measured cross-section to the predicted cross-section. In the figure, only the 20 nuisance parameters with the largest post-fit impacts are shown. The empty (solid) blue rectangles illustrate the pre-fit (post-fit) impact on $\mu$, corresponding to the upper axis. The pre-fit (post-fit) impact of each nuisance parameter, $\Delta\mu$, is calculated as the difference in the fitted value of $\mu$ between the nominal fit and the fit when fixing the corresponding nuisance parameter to $\hat{\theta}\pm\Delta\theta$ ($\hat{\theta}\pm\Delta\hat{\theta}$), where $\hat{\theta}$ is the best-fit value of the nuisance parameter and $\Delta\theta$ ($\Delta\hat{\theta}$) is its pre-fit (post-fit) uncertainty. Several systematic uncertainties are split into different nuisance parameters, which are indicated by NP. JES (JER) indicates jet energy scale (resolution), and $\gamma$ indicates a nuisance parameter associated to the MC statistics in one of the 18 bins numbered from 0 to 17. The black points show the best-fit values of the nuisance parameters, with the error bars representing the post-fit uncertainties. Each nuisance parameter is shown wrt. its nominal value, $\theta_0$, and in units of its pre-fit uncertainty, except the free-floating normalisation factors of the $t\bar{t}$ and $W$+jets backgrounds, and the parameters associated to the MC statistics in each bin, for which the post-fit values and uncertainties are shown.
Correlation matrix of the nuisance parameters and of the ratio $\mu$ of the measured cross-section to the predicted cross-section. The correlations are given after the fit to data. In the figure, only the parameters which have a correlation of at least 0.2 with any other parameter are shown.
Distribution of the MEM discriminant $P(S|X)$ in the SR for MEM discriminant values larger than $2.0\times10^{-4}$, for the collision data used for the measurement, and for 1000 pseudo-data replicas, generated using a bootstrapping technique, in order to assess the statistical correlations between this measurement and others, for the purpose of combinations. The replicas are obtained by reweighting each observed data event by a random integer generated according to Poisson statistics, using the <a href="https://zenodo.org/record/5361038">BootstrapGenerator</a> software package , which implements a technique described in <a href="https://cds.cern.ch/record/2759945/">ATL-PHYS-PUB-2021-011</a>. The ATLAS event number and run number of each event are used as seed to uniquely but reproducibly initialise the random number generator for each event. Each pseudo-data replica is assigned an index, ranging from 0 to 999, corresponding to the random number index used consistently for each observed data event.
Measured values of the signal cross-section and of the $t\bar{t}$ and $W$+jets normalisation factors, obtained by statistical-only fits to the collision data used for the measurement, and to 1000 pseudo-data replicas, generated using a bootstrapping technique, in order to assess the statistical correlations between this measurement and others, for the purpose of combinations. The central values and their statistical uncertainties are obtained by repeating the fit after having fixed all nuisance parameters, except the $t\bar{t}$ and $W$+jets normalisation factors, which are let free-floating (unlike for the statistical uncertainty on the cross-section quoted in the paper). The replicas are obtained by reweighting each observed data event by a random integer generated according to Poisson statistics, using the <a href="https://zenodo.org/record/5361038">BootstrapGenerator</a> software package , which implements a technique described in <a href="https://cds.cern.ch/record/2759945/">ATL-PHYS-PUB-2021-011</a>. The ATLAS event number and run number of each event are used as seed to uniquely but reproducibly initialise the random number generator for each event. Each pseudo-data replica is assigned an index, ranging from 0 to 999, corresponding to the random number index used consistently for each observed data event.
The exclusive production of pion pairs in the process $pp\to pp\pi^+\pi^-$ has been measured at $\sqrt{s}$ = 7 TeV with the ATLAS detector at the LHC, using 80 $\mu$b$^{-1}$ of low-luminosity data. The pion pairs were detected in the ATLAS central detector while outgoing protons were measured in the forward ATLAS ALFA detector system. This represents the first use of proton tagging to measure an exclusive hadronic final state at the LHC. A cross-section measurement is performed in two kinematic regions defined by the proton momenta, the pion rapidities and transverse momenta, and the pion-pion invariant mass. Cross section values of $4.8 \pm 1.0 \text{(stat.)} + {}^{+0.3}_{-0.2} \text{(syst.)}\mu$b and $9 \pm 6 \text{(stat.)} + {}^{+2}_{-2}\text{(syst.)}\mu$b are obtained in the two regions; they are compared with theoretical models and provide a demonstration of the feasibility of measurements of this type.
Measurements of differential cross sections are presented for inclusive isolated-photon production in $pp$ collisions at a centre-of-mass energy of 13 TeV provided by the LHC and using 139 fb$^{-1}$ of data recorded by the ATLAS experiment. The cross sections are measured as functions of the photon transverse energy in different regions of photon pseudorapidity. The photons are required to be isolated by means of a fixed-cone method with two different cone radii. The dependence of the inclusive-photon production on the photon isolation is investigated by measuring the fiducial cross sections as functions of the isolation-cone radius and the ratios of the differential cross sections with different radii in different regions of photon pseudorapidity. The results presented in this paper constitute an improvement with respect to those published by ATLAS earlier: the measurements are provided for different isolation radii and with a more granular segmentation in photon pseudorapidity that can be exploited in improving the determination of the proton parton distribution functions. These improvements provide a more in-depth test of the theoretical predictions. Next-to-leading-order QCD predictions from JETPHOX and SHERPA and next-to-next-to-leading-order QCD predictions from NNLOJET are compared to the measurements, using several parameterisations of the proton parton distribution functions. The measured cross sections are well described by the fixed-order QCD predictions within the experimental and theoretical uncertainties in most of the investigated phase-space region.
Electroweak symmetry breaking explains the origin of the masses of elementary particles through their interactions with the Higgs field. Besides the measurements of the Higgs boson properties, the study of the scattering of massive vector bosons with spin one allows the nature of electroweak symmetry breaking to be probed. Among all processes related to vector-boson scattering, the electroweak production of two jets and a $Z$-boson pair is a rare and important one. Here we report the observation of this process from proton-proton collision data corresponding to an integrated luminosity of 139/fb recorded at a centre-of-mass energy of 13 TeV with the ATLAS detector at the Large Hadron Collider. We consider two different final states originating from the decays of the $Z$-boson pair - one containing four charged leptons and the other containing two charged leptons and two neutrinos. The hypothesis of no electroweak production is rejected with a statistical significance of 5.7 $\sigma$, and the measured cross-section for electroweak production is consistent with the standard model prediction. In addition, we report cross-sections for inclusive production of a $Z$-boson pair and two jets for the two final states.
Measured and predicted fiducial cross-sections in both the lllljj and ll$\nu\nu$jj channels for the inclusive ZZjj processes. Uncertainties due to different sources are presented
Signal strength and significance of EW ZZjj processes
Signal strength and significance of EW ZZjj processes
Measured and predicted fiducial cross-sections in both the lllljj and ll$\nu\nu$jj channels for the inclusive ZZjj processes. Uncertainties due to different sources are presented.
Measured and predicted fiducial cross-sections in both the lllljj and ll$\nu\nu$jj channels for the inclusive ZZjj processes. Uncertainties due to different sources are presented.
Observed and expected multivariate discriminant distribution in the $\ell\ell\ell\ell jj$ QCD CR.
Observed and expected multivariate discriminant distribution in the $\ell\ell\ell\ell jj$ QCD CR.
Observed and expected multivariate discriminant distribution in the $\ell\ell\ell\ell jj$ SR.
Observed and expected multivariate discriminant distribution in the $\ell\ell\ell\ell jj$ SR.
Observed and expected multivariate discriminant distribution in the $\ell\ell\nu\nu jj$ SR.
Observed and expected multivariate discriminant distribution in the $\ell\ell\nu\nu jj$ SR.
Measurements of single-, double-, and triple-differential cross-sections are presented for boosted top-quark pair-production in 13 $\text{TeV}$ proton-proton collisions recorded by the ATLAS detector at the LHC. The top quarks are observed through their hadronic decay and reconstructed as large-radius jets with the leading jet having transverse momentum ($p_{\text{T}}$) greater than 500 GeV. The observed data are unfolded to remove detector effects. The particle-level cross-section, multiplied by the $t\bar{t} \rightarrow W W b \bar{b}$ branching fraction and measured in a fiducial phase space defined by requiring the leading and second-leading jets to have $p_{\text{T}} > 500$ GeV and $p_{\text{T}} > 350$ GeV, respectively, is $331 \pm 3 \text{(stat.)} \pm 39 \text{(syst.)}$ fb. This is approximately 20$\%$ lower than the prediction of $398^{+48}_{-49}$ fb by Powheg+Pythia 8 with next-to-leading-order (NLO) accuracy but consistent within the theoretical uncertainties. Results are also presented at the parton level, where the effects of top-quark decay, parton showering, and hadronization are removed such that they can be compared with fixed-order next-to-next-to-leading-order (NNLO) calculations. The parton-level cross-section, measured in a fiducial phase space similar to that at particle level, is $1.94 \pm 0.02 \text{(stat.)} \pm 0.25 \text{(syst.)}$ pb. This agrees with the NNLO prediction of $1.96^{+0.02}_{-0.17}$ pb. Reasonable agreement with the differential cross-sections is found for most NLO models, while the NNLO calculations are generally in better agreement with the data. The differential cross-sections are interpreted using a Standard Model effective field-theory formalism and limits are set on Wilson coefficients of several four-fermion operators.
Fiducial phase-space cross-section at particle level.
$p_{T}^{t}$ absolute differential cross-section at particle level.
$|y^{t}|$ absolute differential cross-section at particle level.
$p_{T}^{t,1}$ absolute differential cross-section at particle level.
$|{y}^{t,1}|$ absolute differential cross-section at particle level.
$p_{T}^{t,2}$ absolute differential cross-section at particle level.
$|{y}^{t,2}|$ absolute differential cross-section at particle level.
$m^{t\bar{t}}$ absolute differential cross-section at particle level.
$p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level.
$|y^{t\bar{t}}|$ absolute differential cross-section at particle level.
$\chi^{t\bar{t}}$ absolute differential cross-section at particle level.
$|y_{B}^{t\bar{t}}|$ absolute differential cross-section at particle level.
$|p_{out}^{t\bar{t}}|$ absolute differential cross-section at particle level.
$|\Delta \phi(t_{1}, t_{2})|$ absolute differential cross-section at particle level.
$H_{T}^{t\bar{t}}$ absolute differential cross-section at particle level.
$|\cos\theta^{*}|$ absolute differential cross-section at particle level.
$p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level, for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV.
$p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level, for 0.55 TeV < $p_{T}^{t,1}$ < 0.6 TeV.
$p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level, for 0.6 TeV < $p_{T}^{t,1}$ < 0.75 TeV.
$p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level, for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.
$|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at particle level, for 0 < $|{y}^{t,1}|$ < 0.2.
$|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at particle level, for 0.2 < $|{y}^{t,1}|$ < 0.5.
$|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at particle level, for 0.5 < $|{y}^{t,1}|$ < 1.
$|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at particle level, for 1 < $|{y}^{t,1}|$ < 2.
$|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level, for 0 < $|{y}^{t,1}|$ < 0.2.
$|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level, for 0.2 < $|{y}^{t,1}|$ < 0.5.
$|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level, for 0.5 < $|{y}^{t,1}|$ < 1.
$|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level, for 1 < $|{y}^{t,1}|$ < 2.
$|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level, for 0 < $|{y}^{t,2}|$ < 0.2.
$|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level, for 0.2 < $|{y}^{t,2}|$ < 0.5.
$|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level, for 0.5 < $|{y}^{t,2}|$ < 1.
$|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level, for 1 < $|{y}^{t,2}|$ < 2.
$p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level, for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV.
$p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level, for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV.
$p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level, for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV.
$p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level, for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.
$p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level, for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV.
$p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level, for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV.
$p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level, for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV.
$p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level, for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.
$|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level, for 0 < $|{y}^{t\bar{t}}|$ < 0.2.
$|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level, for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.
$|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level, for 0.5 < $|{y}^{t\bar{t}}|$ < 1.
$|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level, for 1 < $|{y}^{t\bar{t}}|$ < 2.
$|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at particle level, for 0 < $|{y}^{t\bar{t}}|$ < 0.2.
$|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at particle level, for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.
$|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at particle level, for 0.5 < $|{y}^{t\bar{t}}|$ < 1.
$|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at particle level, for 1 < $|{y}^{t\bar{t}}|$ < 2.
$|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level, for 0 < $|{y}^{t,1}|$ < 0.2.
$|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level, for 0.2 < $|{y}^{t,1}|$ < 0.5.
$|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level, for 0.5 < $|{y}^{t,1}|$ < 1.
$|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level, for 1 < $|{y}^{t,1}|$ < 2.
$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level, for 0 < $|{y}^{t\bar{t}}|$ < 0.2.
$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level, for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.
$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level, for 0.5 < $|{y}^{t\bar{t}}|$ < 1.
$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level, for 1 < $|{y}^{t\bar{t}}|$ < 2.
$p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level, for 0 TeV < $p_{T}^{t\bar{t}}$ < 0.1 TeV.
$p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level, for 0.1 TeV < $p_{T}^{t\bar{t}}$ < 0.2 TeV.
$p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level, for 0.2 TeV < $p_{T}^{t\bar{t}}$ < 0.35 TeV.
$p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level, for 0.35 TeV < $p_{T}^{t\bar{t}}$ < 1 TeV.
$|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level, for 0 < $|{y}^{t\bar{t}}|$ < 0.2.
$|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level, for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.
$|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level, for 0.5 < $|{y}^{t\bar{t}}|$ < 1.
$|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level, for 1 < $|{y}^{t\bar{t}}|$ < 2.
$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level, for 0 < $|{y}^{t\bar{t}}|$ < 0.3 and 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.
$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level, for 0 < $|{y}^{t\bar{t}}|$ < 0.3 and 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level, for 0 < $|{y}^{t\bar{t}}|$ < 0.3 and 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level, for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9 and 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.
$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level, for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9 and 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level, for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9 and 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level, for 0.9 < $|{y}^{t\bar{t}}|$ < 2 and 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.
$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level, for 0.9 < $|{y}^{t\bar{t}}|$ < 2 and 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level, for 0.9 < $|{y}^{t\bar{t}}|$ < 2 and 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
$p_{T}^{t}$ normalized differential cross-section at particle level.
$|y^{t}|$ normalized differential cross-section at particle level.
$p_{T}^{t,1}$ normalized differential cross-section at particle level.
$|{y}^{t,1}|$ normalized differential cross-section at particle level.
$p_{T}^{t,2}$ normalized differential cross-section at particle level.
$|{y}^{t,2}|$ normalized differential cross-section at particle level.
$m^{t\bar{t}}$ normalized differential cross-section at particle level.
$p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level.
$|y^{t\bar{t}}|$ normalized differential cross-section at particle level.
$\chi^{t\bar{t}}$ normalized differential cross-section at particle level.
$|y_{B}^{t\bar{t}}|$ normalized differential cross-section at particle level.
$|p_{out}^{t\bar{t}}|$ normalized differential cross-section at particle level.
$|\Delta \phi(t_{1}, t_{2})|$ normalized differential cross-section at particle level.
$H_{T}^{t\bar{t}}$ normalized differential cross-section at particle level.
$|\cos\theta^{*}|$ normalized differential cross-section at particle level.
$p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level, for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV.
$p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level, for 0.55 TeV < $p_{T}^{t,1}$ < 0.6 TeV.
$p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level, for 0.6 TeV < $p_{T}^{t,1}$ < 0.75 TeV.
$p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level, for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.
$|{y}^{t,1}|\otimes |{y}^{t,2}|$ normalized differential cross-section at particle level, for 0 < $|{y}^{t,1}|$ < 0.2.
$|{y}^{t,1}|\otimes |{y}^{t,2}|$ normalized differential cross-section at particle level, for 0.2 < $|{y}^{t,1}|$ < 0.5.
$|{y}^{t,1}|\otimes |{y}^{t,2}|$ normalized differential cross-section at particle level, for 0.5 < $|{y}^{t,1}|$ < 1.
$|{y}^{t,1}|\otimes |{y}^{t,2}|$ normalized differential cross-section at particle level, for 1 < $|{y}^{t,1}|$ < 2.
$|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level, for 0 < $|{y}^{t,1}|$ < 0.2.
$|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level, for 0.2 < $|{y}^{t,1}|$ < 0.5.
$|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level, for 0.5 < $|{y}^{t,1}|$ < 1.
$|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level, for 1 < $|{y}^{t,1}|$ < 2.
$|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level, for 0 < $|{y}^{t,2}|$ < 0.2.
$|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level, for 0.2 < $|{y}^{t,2}|$ < 0.5.
$|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level, for 0.5 < $|{y}^{t,2}|$ < 1.
$|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level, for 1 < $|{y}^{t,2}|$ < 2.
$p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level, for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV.
$p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level, for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV.
$p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level, for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV.
$p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level, for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.
$p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level, for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV.
$p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level, for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV.
$p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level, for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV.
$p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level, for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.
$|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level, for 0 < $|{y}^{t\bar{t}}|$ < 0.2.
$|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level, for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.
$|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level, for 0.5 < $|{y}^{t\bar{t}}|$ < 1.
$|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level, for 1 < $|{y}^{t\bar{t}}|$ < 2.
$|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ normalized differential cross-section at particle level, for 0 < $|{y}^{t\bar{t}}|$ < 0.2.
$|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ normalized differential cross-section at particle level, for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.
$|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ normalized differential cross-section at particle level, for 0.5 < $|{y}^{t\bar{t}}|$ < 1.
$|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ normalized differential cross-section at particle level, for 1 < $|{y}^{t\bar{t}}|$ < 2.
$|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level, for 0 < $|{y}^{t,1}|$ < 0.2.
$|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level, for 0.2 < $|{y}^{t,1}|$ < 0.5.
$|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level, for 0.5 < $|{y}^{t,1}|$ < 1.
$|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level, for 1 < $|{y}^{t,1}|$ < 2.
$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level, for 0 < $|{y}^{t\bar{t}}|$ < 0.2.
$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level, for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.
$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level, for 0.5 < $|{y}^{t\bar{t}}|$ < 1.
$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level, for 1 < $|{y}^{t\bar{t}}|$ < 2.
$p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level, for 0 TeV < $p_{T}^{t\bar{t}}$ < 0.1 TeV.
$p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level, for 0.1 TeV < $p_{T}^{t\bar{t}}$ < 0.2 TeV.
$p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level, for 0.2 TeV < $p_{T}^{t\bar{t}}$ < 0.35 TeV.
$p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level, for 0.35 TeV < $p_{T}^{t\bar{t}}$ < 1 TeV.
$|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level, for 0 < $|{y}^{t\bar{t}}|$ < 0.2.
$|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level, for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.
$|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level, for 0.5 < $|{y}^{t\bar{t}}|$ < 1.
$|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level, for 1 < $|{y}^{t\bar{t}}|$ < 2.
$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level, for 0 < $|{y}^{t\bar{t}}|$ < 0.3 and 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.
$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level, for 0 < $|{y}^{t\bar{t}}|$ < 0.3 and 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level, for 0 < $|{y}^{t\bar{t}}|$ < 0.3 and 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level, for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9 and 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.
$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level, for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9 and 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level, for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9 and 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level, for 0.9 < $|{y}^{t\bar{t}}|$ < 2 and 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.
$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level, for 0.9 < $|{y}^{t\bar{t}}|$ < 2 and 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
$|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level, for 0.9 < $|{y}^{t\bar{t}}|$ < 2 and 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Fiducial phase-space cross-section at parton level.
$p_{T}^{t}$ absolute differential cross-section at parton level.
$|y^{t}|$ absolute differential cross-section at parton level.
$p_{T}^{t,1}$ absolute differential cross-section at parton level.
$|y^{t,1}|$ absolute differential cross-section at parton level.
$p_{T}^{t,2}$ absolute differential cross-section at parton level.
$|{y}^{t,2}|$ absolute differential cross-section at parton level.
$m^{t\bar{t}}$ absolute differential cross-section at parton level.
$p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level.
$|{y}^{t\bar{t}}|$ absolute differential cross-section at parton level.
${\chi}^{t\bar{t}}$ absolute differential cross-section at parton level.
$|y_{B}^{t\bar{t}}|$ absolute differential cross-section at parton level.
$|p_{out}^{t\bar{t}}|$ absolute differential cross-section at parton level.
$|\Delta \phi(t_{1}, t_{2})|$ absolute differential cross-section at parton level.
$H_{T}^{t\bar{t}}$ absolute differential cross-section at parton level.
$|\cos\theta^{*}|$ absolute differential cross-section at parton level.
$p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level, for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV.
$p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level, for 0.55 TeV < $p_{T}^{t,1}$ < 0.6 TeV.
$p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level, for 0.6 TeV < $p_{T}^{t,1}$ < 0.75 TeV.
$p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level, for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.
$|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at parton level, for 0 < $|{y}^{t,1}|$ < 0.2.
$|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at parton level, for 0.2 < $|{y}^{t,1}|$ < 0.5.
$|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at parton level, for 0.5 < $|{y}^{t,1}|$ < 1.
$|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at parton level, for 1 < $|{y}^{t,1}|$ < 2.
$|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level, for 0 < $|{y}^{t,1}|$ < 0.2.
$|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level, for 0.2 < $|{y}^{t,1}|$ < 0.5.
$|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level, for 0.5 < $|{y}^{t,1}|$ < 1.
$|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level, for 1 < $|{y}^{t,1}|$ < 2.
$|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level, for 0 < $|{y}^{t,2}|$ < 0.2.
$|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level, for 0.2 < $|{y}^{t,2}|$ < 0.5.
$|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level, for 0.5 < $|{y}^{t,2}|$ < 1.
$|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level, for 1 < $|{y}^{t,2}|$ < 2.
$p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level, for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV.
$p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level, for 0.5 TeV < $p_{T}^{t,1}$ < 0.625 TeV.
$p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level, for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV.
$p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level, for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.
$p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level, for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV.
$p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level, for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV.
$p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level, for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV.
$p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level, for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.
$|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level, for 0 < $|{y}^{t\bar{t}}|$ < 0.2.
$|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level, for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.
$|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level, for 0.5 < $|{y}^{t\bar{t}}|$ < 1.
$|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level, for 1 < $|{y}^{t\bar{t}}|$ < 2.
$p_{T}^{t}$ covariance matrix for the absolute differential cross-section at particle level.
$|{y}^{t}|$ covariance matrix for the absolute differential cross-section at particle level.
$p_{T}^{t,1}$ covariance matrix for the absolute differential cross-section at particle level.
$|{y}^{t,1}|$ covariance matrix for the absolute differential cross-section at particle level.
$p_{T}^{t,2}$ covariance matrix for the absolute differential cross-section at particle level.
$|{y}^{t,2}|$ covariance matrix for the absolute differential cross-section at particle level.
$m^{t\bar{t}}$ covariance matrix for the absolute differential cross-section at particle level.
$p_{T}^{t\bar{t}}$ covariance matrix for the absolute differential cross-section at particle level.
$|y^{t\bar{t}}|$ covariance matrix for the absolute differential cross-section at particle level.
$\chi^{t\bar{t}}$ covariance matrix for the absolute differential cross-section at particle level.
$|y_{B}^{t\bar{t}}|$ covariance matrix for the absolute differential cross-section at particle level.
$|p_{out}^{t\bar{t}}|$ covariance matrix for the absolute differential cross-section at particle level.
$|\Delta \phi(t_{1}, t_{2})|$ covariance matrix for the absolute differential cross-section at particle level.
$H_{T}^{t\bar{t}}$ covariance matrix for the absolute differential cross-section at particle level.
$|\cos\theta^{*}|$ covariance matrix for the absolute differential cross-section at particle level.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level for 0.55 TeV < $p_{T}^{t,1}$ < 0.6 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level for 0.6 TeV < $p_{T}^{t,1}$ < 0.75 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level for 0.55 TeV < $p_{T}^{t,1}$ < 0.6 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level for 0.55 TeV < $p_{T}^{t,1}$ < 0.6 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level for 0.55 TeV < $p_{T}^{t,1}$ < 0.6 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level for 0.6 TeV < $p_{T}^{t,1}$ < 0.75 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level for 0.55 TeV < $p_{T}^{t,1}$ < 0.6 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level for 0.6 TeV < $p_{T}^{t,1}$ < 0.75 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level for 0.6 TeV < $p_{T}^{t,1}$ < 0.75 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level for 0.6 TeV < $p_{T}^{t,1}$ < 0.75 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.
Covariance matrix between the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at particle level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at particle level for 0 < $|{y}^{t,1}|$ < 0.2.
Covariance matrix between the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at particle level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at particle level for 0.2 < $|{y}^{t,1}|$ < 0.5.
Covariance matrix between the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at particle level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at particle level for 0.5 < $|{y}^{t,1}|$ < 1.
Covariance matrix between the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at particle level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at particle level for 1 < $|{y}^{t,1}|$ < 2.
Covariance matrix between the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at particle level for 0.2 < $|{y}^{t,1}|$ < 0.5 and the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at particle level for 0.2 < $|{y}^{t,1}|$ < 0.5.
Covariance matrix between the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at particle level for 0.2 < $|{y}^{t,1}|$ < 0.5 and the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at particle level for 0.5 < $|{y}^{t,1}|$ < 1.
Covariance matrix between the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at particle level for 0.2 < $|{y}^{t,1}|$ < 0.5 and the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at particle level for 1 < $|{y}^{t,1}|$ < 2.
Covariance matrix between the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at particle level for 0.5 < $|{y}^{t,1}|$ < 1 and the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at particle level for 0.5 < $|{y}^{t,1}|$ < 1.
Covariance matrix between the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at particle level for 0.5 < $|{y}^{t,1}|$ < 1 and the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at particle level for 1 < $|{y}^{t,1}|$ < 2.
Covariance matrix between the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at particle level for 1 < $|{y}^{t,1}|$ < 2 and the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at particle level for 1 < $|{y}^{t,1}|$ < 2.
Covariance matrix between the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t,1}|$ < 0.2.
Covariance matrix between the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.2 < $|{y}^{t,1}|$ < 0.5.
Covariance matrix between the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.5 < $|{y}^{t,1}|$ < 1.
Covariance matrix between the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 1 < $|{y}^{t,1}|$ < 2.
Covariance matrix between the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.2 < $|{y}^{t,1}|$ < 0.5 and the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.2 < $|{y}^{t,1}|$ < 0.5.
Covariance matrix between the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.2 < $|{y}^{t,1}|$ < 0.5 and the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.5 < $|{y}^{t,1}|$ < 1.
Covariance matrix between the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.2 < $|{y}^{t,1}|$ < 0.5 and the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 1 < $|{y}^{t,1}|$ < 2.
Covariance matrix between the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.5 < $|{y}^{t,1}|$ < 1 and the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.5 < $|{y}^{t,1}|$ < 1.
Covariance matrix between the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.5 < $|{y}^{t,1}|$ < 1 and the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 1 < $|{y}^{t,1}|$ < 2.
Covariance matrix between the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 1 < $|{y}^{t,1}|$ < 2 and the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 1 < $|{y}^{t,1}|$ < 2.
Covariance matrix between the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level for 0 < $|{y}^{t,2}|$ < 0.2 and the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level for 0 < $|{y}^{t,2}|$ < 0.2.
Covariance matrix between the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level for 0 < $|{y}^{t,2}|$ < 0.2 and the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level for 0.2 < $|{y}^{t,2}|$ < 0.5.
Covariance matrix between the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level for 0 < $|{y}^{t,2}|$ < 0.2 and the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level for 0.5 < $|{y}^{t,2}|$ < 1.
Covariance matrix between the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level for 0 < $|{y}^{t,2}|$ < 0.2 and the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level for 1 < $|{y}^{t,2}|$ < 2.
Covariance matrix between the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level for 0.2 < $|{y}^{t,2}|$ < 0.5 and the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level for 0.2 < $|{y}^{t,2}|$ < 0.5.
Covariance matrix between the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level for 0.2 < $|{y}^{t,2}|$ < 0.5 and the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level for 0.5 < $|{y}^{t,2}|$ < 1.
Covariance matrix between the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level for 0.2 < $|{y}^{t,2}|$ < 0.5 and the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level for 1 < $|{y}^{t,2}|$ < 2.
Covariance matrix between the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level for 0.5 < $|{y}^{t,2}|$ < 1 and the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level for 0.5 < $|{y}^{t,2}|$ < 1.
Covariance matrix between the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level for 0.5 < $|{y}^{t,2}|$ < 1 and the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level for 1 < $|{y}^{t,2}|$ < 2.
Covariance matrix between the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level for 1 < $|{y}^{t,2}|$ < 2 and the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at particle level for 1 < $|{y}^{t,2}|$ < 2.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV and the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV and the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV and the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV and the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV and the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV and the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.5 < $|{y}^{t\bar{t}}|$ < 1.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 1 < $|{y}^{t\bar{t}}|$ < 2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.5 < $|{y}^{t\bar{t}}|$ < 1.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 1 < $|{y}^{t\bar{t}}|$ < 2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.5 < $|{y}^{t\bar{t}}|$ < 1 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.5 < $|{y}^{t\bar{t}}|$ < 1.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.5 < $|{y}^{t\bar{t}}|$ < 1 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 1 < $|{y}^{t\bar{t}}|$ < 2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 1 < $|{y}^{t\bar{t}}|$ < 2 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 1 < $|{y}^{t\bar{t}}|$ < 2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at particle level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at particle level for 0.5 < $|{y}^{t\bar{t}}|$ < 1.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at particle level for 1 < $|{y}^{t\bar{t}}|$ < 2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at particle level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5 and the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at particle level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at particle level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5 and the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at particle level for 0.5 < $|{y}^{t\bar{t}}|$ < 1.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at particle level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5 and the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at particle level for 1 < $|{y}^{t\bar{t}}|$ < 2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at particle level for 0.5 < $|{y}^{t\bar{t}}|$ < 1 and the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at particle level for 0.5 < $|{y}^{t\bar{t}}|$ < 1.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at particle level for 0.5 < $|{y}^{t\bar{t}}|$ < 1 and the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at particle level for 1 < $|{y}^{t\bar{t}}|$ < 2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at particle level for 1 < $|{y}^{t\bar{t}}|$ < 2 and the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at particle level for 1 < $|{y}^{t\bar{t}}|$ < 2.
Covariance matrix between the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0 < $|{y}^{t,1}|$ < 0.2.
Covariance matrix between the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.2 < $|{y}^{t,1}|$ < 0.5.
Covariance matrix between the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.5 < $|{y}^{t,1}|$ < 1.
Covariance matrix between the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 1 < $|{y}^{t,1}|$ < 2.
Covariance matrix between the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.2 < $|{y}^{t,1}|$ < 0.5 and the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.2 < $|{y}^{t,1}|$ < 0.5.
Covariance matrix between the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.2 < $|{y}^{t,1}|$ < 0.5 and the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.5 < $|{y}^{t,1}|$ < 1.
Covariance matrix between the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.2 < $|{y}^{t,1}|$ < 0.5 and the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 1 < $|{y}^{t,1}|$ < 2.
Covariance matrix between the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.5 < $|{y}^{t,1}|$ < 1 and the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.5 < $|{y}^{t,1}|$ < 1.
Covariance matrix between the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.5 < $|{y}^{t,1}|$ < 1 and the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 1 < $|{y}^{t,1}|$ < 2.
Covariance matrix between the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 1 < $|{y}^{t,1}|$ < 2 and the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 1 < $|{y}^{t,1}|$ < 2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.5 < $|{y}^{t\bar{t}}|$ < 1.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 1 < $|{y}^{t\bar{t}}|$ < 2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5 and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5 and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.5 < $|{y}^{t\bar{t}}|$ < 1.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5 and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 1 < $|{y}^{t\bar{t}}|$ < 2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.5 < $|{y}^{t\bar{t}}|$ < 1 and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.5 < $|{y}^{t\bar{t}}|$ < 1.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.5 < $|{y}^{t\bar{t}}|$ < 1 and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 1 < $|{y}^{t\bar{t}}|$ < 2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 1 < $|{y}^{t\bar{t}}|$ < 2 and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 1 < $|{y}^{t\bar{t}}|$ < 2.
Covariance matrix between the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0 TeV < $p_{T}^{t\bar{t}}$ < 0.1 TeV and the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0 TeV < $p_{T}^{t\bar{t}}$ < 0.1 TeV.
Covariance matrix between the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0 TeV < $p_{T}^{t\bar{t}}$ < 0.1 TeV and the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.1 TeV < $p_{T}^{t\bar{t}}$ < 0.2 TeV.
Covariance matrix between the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0 TeV < $p_{T}^{t\bar{t}}$ < 0.1 TeV and the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.2 TeV < $p_{T}^{t\bar{t}}$ < 0.35 TeV.
Covariance matrix between the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0 TeV < $p_{T}^{t\bar{t}}$ < 0.1 TeV and the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.35 TeV < $p_{T}^{t\bar{t}}$ < 1 TeV.
Covariance matrix between the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.1 TeV < $p_{T}^{t\bar{t}}$ < 0.2 TeV and the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.1 TeV < $p_{T}^{t\bar{t}}$ < 0.2 TeV.
Covariance matrix between the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.1 TeV < $p_{T}^{t\bar{t}}$ < 0.2 TeV and the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.2 TeV < $p_{T}^{t\bar{t}}$ < 0.35 TeV.
Covariance matrix between the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.1 TeV < $p_{T}^{t\bar{t}}$ < 0.2 TeV and the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.35 TeV < $p_{T}^{t\bar{t}}$ < 1 TeV.
Covariance matrix between the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.2 TeV < $p_{T}^{t\bar{t}}$ < 0.35 TeV and the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.2 TeV < $p_{T}^{t\bar{t}}$ < 0.35 TeV.
Covariance matrix between the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.2 TeV < $p_{T}^{t\bar{t}}$ < 0.35 TeV and the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.35 TeV < $p_{T}^{t\bar{t}}$ < 1 TeV.
Covariance matrix between the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.35 TeV < $p_{T}^{t\bar{t}}$ < 1 TeV and the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at particle level for 0.35 TeV < $p_{T}^{t\bar{t}}$ < 1 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level for 0.5 < $|{y}^{t\bar{t}}|$ < 1.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level for 1 < $|{y}^{t\bar{t}}|$ < 2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level for 0.5 < $|{y}^{t\bar{t}}|$ < 1.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level for 1 < $|{y}^{t\bar{t}}|$ < 2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level for 0.5 < $|{y}^{t\bar{t}}|$ < 1 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level for 0.5 < $|{y}^{t\bar{t}}|$ < 1.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level for 0.5 < $|{y}^{t\bar{t}}|$ < 1 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level for 1 < $|{y}^{t\bar{t}}|$ < 2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level for 1 < $|{y}^{t\bar{t}}|$ < 2 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at particle level for 1 < $|{y}^{t\bar{t}}|$ < 2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
$p_{T}^{t}$ covariance matrix for the normalized differential cross-section at particle level.
$|y^{t}|$ covariance matrix for the normalized differential cross-section at particle level.
$p_{T}^{t,1}$ covariance matrix for the normalized differential cross-section at particle level.
$|{y}^{t,1}|$ covariance matrix for the normalized differential cross-section at particle level.
$p_{T}^{t,2}$ covariance matrix for the normalized differential cross-section at particle level.
$|{y}^{t,2}|$ covariance matrix for the normalized differential cross-section at particle level.
$m^{t\bar{t}}$ covariance matrix for the normalized differential cross-section at particle level.
$p_{T}^{t\bar{t}}$ covariance matrix for the normalized differential cross-section at particle level.
$|y^{t\bar{t}}|$ covariance matrix for the normalized differential cross-section at particle level.
$\chi^{t\bar{t}}$ covariance matrix for the normalized differential cross-section at particle level.
$|y_{B}^{t\bar{t}}|$ covariance matrix for the normalized differential cross-section at particle level.
$|p_{out}^{t\bar{t}}|$ covariance matrix for the normalized differential cross-section at particle level.
$|\Delta \phi(t_{1}, t_{2})|$ covariance matrix for the normalized differential cross-section at particle level.
$H_{T}^{t\bar{t}}$ covariance matrix for the normalized differential cross-section at particle level.
$|\cos\theta^{*}|$ covariance matrix for the normalized differential cross-section at particle level.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level for 0.55 TeV < $p_{T}^{t,1}$ < 0.6 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level for 0.6 TeV < $p_{T}^{t,1}$ < 0.75 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level for 0.55 TeV < $p_{T}^{t,1}$ < 0.6 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level for 0.55 TeV < $p_{T}^{t,1}$ < 0.6 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level for 0.55 TeV < $p_{T}^{t,1}$ < 0.6 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level for 0.6 TeV < $p_{T}^{t,1}$ < 0.75 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level for 0.55 TeV < $p_{T}^{t,1}$ < 0.6 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level for 0.6 TeV < $p_{T}^{t,1}$ < 0.75 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level for 0.6 TeV < $p_{T}^{t,1}$ < 0.75 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level for 0.6 TeV < $p_{T}^{t,1}$ < 0.75 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.
Covariance matrix between the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ normalized differential cross-section at particle level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ normalized differential cross-section at particle level for 0 < $|{y}^{t,1}|$ < 0.2.
Covariance matrix between the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ normalized differential cross-section at particle level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute normalized cross-section at particle level for 0.2 < $|{y}^{t,1}|$ < 0.5.
Covariance matrix between the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ normalized differential cross-section at particle level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ normalized differential cross-section at particle level for 0.5 < $|{y}^{t,1}|$ < 1.
Covariance matrix between the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ normalized differential cross-section at particle level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ normalized differential cross-section at particle level for 1 < $|{y}^{t,1}|$ < 2.
Covariance matrix between the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ normalized differential cross-section at particle level for 0.2 < $|{y}^{t,1}|$ < 0.5 and the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ normalized differential cross-section at particle level for 0.2 < $|{y}^{t,1}|$ < 0.5.
Covariance matrix between the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ normalized differential cross-section at particle level for 0.2 < $|{y}^{t,1}|$ < 0.5 and the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ normalized differential cross-section at particle level for 0.5 < $|{y}^{t,1}|$ < 1.
Covariance matrix between the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ normalized differential cross-section at particle level for 0.2 < $|{y}^{t,1}|$ < 0.5 and the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ normalized differential cross-section at particle level for 1 < $|{y}^{t,1}|$ < 2.
Covariance matrix between the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ normalized differential cross-section at particle level for 0.5 < $|{y}^{t,1}|$ < 1 and the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ normalized differential cross-section at particle level for 0.5 < $|{y}^{t,1}|$ < 1.
Covariance matrix between the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ normalized differential cross-section at particle level for 0.5 < $|{y}^{t,1}|$ < 1 and the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ normalized differential cross-section at particle level for 1 < $|{y}^{t,1}|$ < 2.
Covariance matrix between the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ normalized differential cross-section at particle level for 1 < $|{y}^{t,1}|$ < 2 and the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ normalized differential cross-section at particle level for 1 < $|{y}^{t,1}|$ < 2.
Covariance matrix between the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0 < $|{y}^{t,1}|$ < 0.2.
Covariance matrix between the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.2 < $|{y}^{t,1}|$ < 0.5.
Covariance matrix between the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.5 < $|{y}^{t,1}|$ < 1.
Covariance matrix between the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 1 < $|{y}^{t,1}|$ < 2.
Covariance matrix between the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.2 < $|{y}^{t,1}|$ < 0.5 and the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.2 < $|{y}^{t,1}|$ < 0.5.
Covariance matrix between the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.2 < $|{y}^{t,1}|$ < 0.5 and the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.5 < $|{y}^{t,1}|$ < 1.
Covariance matrix between the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.2 < $|{y}^{t,1}|$ < 0.5 and the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 1 < $|{y}^{t,1}|$ < 2.
Covariance matrix between the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.5 < $|{y}^{t,1}|$ < 1 and the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.5 < $|{y}^{t,1}|$ < 1.
Covariance matrix between the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.5 < $|{y}^{t,1}|$ < 1 and the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 1 < $|{y}^{t,1}|$ < 2.
Covariance matrix between the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 1 < $|{y}^{t,1}|$ < 2 and the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 1 < $|{y}^{t,1}|$ < 2.
Covariance matrix between the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level for 0 < $|{y}^{t,2}|$ < 0.2 and the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level for 0 < $|{y}^{t,2}|$ < 0.2.
Covariance matrix between the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level for 0 < $|{y}^{t,2}|$ < 0.2 and the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level for 0.2 < $|{y}^{t,2}|$ < 0.5.
Covariance matrix between the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level for 0 < $|{y}^{t,2}|$ < 0.2 and the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level for 0.5 < $|{y}^{t,2}|$ < 1.
Covariance matrix between the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level for 0 < $|{y}^{t,2}|$ < 0.2 and the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level for 1 < $|{y}^{t,2}|$ < 2.
Covariance matrix between the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level for 0.2 < $|{y}^{t,2}|$ < 0.5 and the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level for 0.2 < $|{y}^{t,2}|$ < 0.5.
Covariance matrix between the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level for 0.2 < $|{y}^{t,2}|$ < 0.5 and the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level for 0.5 < $|{y}^{t,2}|$ < 1.
Covariance matrix between the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level for 0.2 < $|{y}^{t,2}|$ < 0.5 and the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level for 1 < $|{y}^{t,2}|$ < 2.
Covariance matrix between the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level for 0.5 < $|{y}^{t,2}|$ < 1 and the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level for 0.5 < $|{y}^{t,2}|$ < 1.
Covariance matrix between the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level for 0.5 < $|{y}^{t,2}|$ < 1 and the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level for 1 < $|{y}^{t,2}|$ < 2.
Covariance matrix between the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level for 1 < $|{y}^{t,2}|$ < 2 and the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at particle level for 1 < $|{y}^{t,2}|$ < 2.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV and the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV and the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV and the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV and the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV and the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.5 < $|{y}^{t\bar{t}}|$ < 1.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 1 < $|{y}^{t\bar{t}}|$ < 2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.5 < $|{y}^{t\bar{t}}|$ < 1.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 1 < $|{y}^{t\bar{t}}|$ < 2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.5 < $|{y}^{t\bar{t}}|$ < 1 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 1 < $|{y}^{t\bar{t}}|$ < 2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 1 < $|{y}^{t\bar{t}}|$ < 2 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 1 < $|{y}^{t\bar{t}}|$ < 2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ normalized differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ normalized differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ normalized differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ normalized differential cross-section at particle level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ normalized differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ normalized differential cross-section at particle level for 0.5 < $|{y}^{t\bar{t}}|$ < 1.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ normalized differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ normalized differential cross-section at particle level for 1 < $|{y}^{t\bar{t}}|$ < 2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ normalized differential cross-section at particle level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5 and the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ normalized differential cross-section at particle level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ normalized differential cross-section at particle level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5 and the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ normalized differential cross-section at particle level for 0.5 < $|{y}^{t\bar{t}}|$ < 1.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ normalized differential cross-section at particle level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5 and the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ normalized differential cross-section at particle level for 1 < $|{y}^{t\bar{t}}|$ < 2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ normalized differential cross-section at particle level for 0.5 < $|{y}^{t\bar{t}}|$ < 1 and the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ normalized differential cross-section at particle level for 0.5 < $|{y}^{t\bar{t}}|$ < 1.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ normalized differential cross-section at particle level for 0.5 < $|{y}^{t\bar{t}}|$ < 1 and the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ normalized differential cross-section at particle level for 1 < $|{y}^{t\bar{t}}|$ < 2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ normalized differential cross-section at particle level for 1 < $|{y}^{t\bar{t}}|$ < 2 and the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ normalized differential cross-section at particle level for 1 < $|{y}^{t\bar{t}}|$ < 2.
Covariance matrix between the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.2 < $|{y}^{t,1}|$ < 0.5.
Covariance matrix between the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.5 < $|{y}^{t,1}|$ < 1.
Covariance matrix between the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 1 < $|{y}^{t,1}|$ < 2.
Covariance matrix between the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.2 < $|{y}^{t,1}|$ < 0.5 and the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.2 < $|{y}^{t,1}|$ < 0.5.
Covariance matrix between the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.2 < $|{y}^{t,1}|$ < 0.5 and the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.5 < $|{y}^{t,1}|$ < 1.
Covariance matrix between the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.2 < $|{y}^{t,1}|$ < 0.5 and the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 1 < $|{y}^{t,1}|$ < 2.
Covariance matrix between the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.5 < $|{y}^{t,1}|$ < 1 and the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.5 < $|{y}^{t,1}|$ < 1.
Covariance matrix between the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.5 < $|{y}^{t,1}|$ < 1 and the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 1 < $|{y}^{t,1}|$ < 2.
Covariance matrix between the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 1 < $|{y}^{t,1}|$ < 2 and the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 1 < $|{y}^{t,1}|$ < 2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.5 < $|{y}^{t\bar{t}}|$ < 1.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 1 < $|{y}^{t\bar{t}}|$ < 2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5 and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5 and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.5 < $|{y}^{t\bar{t}}|$ < 1.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5 and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 1 < $|{y}^{t\bar{t}}|$ < 2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.5 < $|{y}^{t\bar{t}}|$ < 1 and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.5 < $|{y}^{t\bar{t}}|$ < 1.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.5 < $|{y}^{t\bar{t}}|$ < 1 and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 1 < $|{y}^{t\bar{t}}|$ < 2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 1 < $|{y}^{t\bar{t}}|$ < 2 and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 1 < $|{y}^{t\bar{t}}|$ < 2.
Covariance matrix between the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0 TeV < $p_{T}^{t\bar{t}}$ < 0.1 TeV and the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0 TeV < $p_{T}^{t\bar{t}}$ < 0.1 TeV.
Covariance matrix between the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0 TeV < $p_{T}^{t\bar{t}}$ < 0.1 TeV and the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.1 TeV < $p_{T}^{t\bar{t}}$ < 0.2 TeV.
Covariance matrix between the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0 TeV < $p_{T}^{t\bar{t}}$ < 0.1 TeV and the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.2 TeV < $p_{T}^{t\bar{t}}$ < 0.35 TeV.
Covariance matrix between the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0 TeV < $p_{T}^{t\bar{t}}$ < 0.1 TeV and the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.35 TeV < $p_{T}^{t\bar{t}}$ < 1 TeV.
Covariance matrix between the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.1 TeV < $p_{T}^{t\bar{t}}$ < 0.2 TeV and the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.1 TeV < $p_{T}^{t\bar{t}}$ < 0.2 TeV.
Covariance matrix between the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.1 TeV < $p_{T}^{t\bar{t}}$ < 0.2 TeV and the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.2 TeV < $p_{T}^{t\bar{t}}$ < 0.35 TeV.
Covariance matrix between the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.1 TeV < $p_{T}^{t\bar{t}}$ < 0.2 TeV and the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.35 TeV < $p_{T}^{t\bar{t}}$ < 1 TeV.
Covariance matrix between the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.2 TeV < $p_{T}^{t\bar{t}}$ < 0.35 TeV and the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.2 TeV < $p_{T}^{t\bar{t}}$ < 0.35 TeV.
Covariance matrix between the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.2 TeV < $p_{T}^{t\bar{t}}$ < 0.35 TeV and the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.35 TeV < $p_{T}^{t\bar{t}}$ < 1 TeV.
Covariance matrix between the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.35 TeV < $p_{T}^{t\bar{t}}$ < 1 TeV and the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at particle level for 0.35 TeV < $p_{T}^{t\bar{t}}$ < 1 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level for 0.5 < $|{y}^{t\bar{t}}|$ < 1.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level for 1 < $|{y}^{t\bar{t}}|$ < 2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level for 0.5 < $|{y}^{t\bar{t}}|$ < 1.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level for 1 < $|{y}^{t\bar{t}}|$ < 2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level for 0.5 < $|{y}^{t\bar{t}}|$ < 1 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level for 0.5 < $|{y}^{t\bar{t}}|$ < 1.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level for 0.5 < $|{y}^{t\bar{t}}|$ < 1 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level for 1 < $|{y}^{t\bar{t}}|$ < 2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level for 1 < $|{y}^{t\bar{t}}|$ < 2 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at particle level for 1 < $|{y}^{t\bar{t}}|$ < 2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at particle level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
$p_{T}^{t}$ covariance matrix for the absolute differential cross-section at parton level.
$|y^{t}|$ covariance matrix for the absolute differential cross-section at parton level.
$p_{T}^{t,1}$ covariance matrix for the absolute differential cross-section at parton level.
$|y^{t,1}|$ covariance matrix for the absolute differential cross-section at parton level.
$p_{T}^{t,2}$ covariance matrix for the absolute differential cross-section at parton level.
$|{y}^{t,2}|$ covariance matrix for the absolute differential cross-section at parton level.
$m^{t\bar{t}}$ covariance matrix for the absolute differential cross-section at parton level.
$p_{T}^{t\bar{t}}$ covariance matrix for the absolute differential cross-section at parton level.
$|{y}^{t\bar{t}}|$ covariance matrix for the absolute differential cross-section at parton level.
${\chi}^{t\bar{t}}$ covariance matrix for the absolute differential cross-section at parton level.
$|y_{B}^{t\bar{t}}|$ covariance matrix for the absolute differential cross-section at parton level.
$|p_{out}^{t\bar{t}}|$ covariance matrix for the absolute differential cross-section at parton level.
$|\Delta \phi(t_{1}, t_{2})|$ covariance matrix for the absolute differential cross-section at parton level.
$H_{T}^{t\bar{t}}$ covariance matrix for the absolute differential cross-section at parton level.
$|\cos\theta^{*}|$ covariance matrix for the absolute differential cross-section at parton level.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level for 0.55 TeV < $p_{T}^{t,1}$ < 0.6 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level for 0.6 TeV < $p_{T}^{t,1}$ < 0.75 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level for 0.55 TeV < $p_{T}^{t,1}$ < 0.6 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level for 0.55 TeV < $p_{T}^{t,1}$ < 0.6 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level for 0.55 TeV < $p_{T}^{t,1}$ < 0.6 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level for 0.6 TeV < $p_{T}^{t,1}$ < 0.75 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level for 0.55 TeV < $p_{T}^{t,1}$ < 0.6 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level for 0.6 TeV < $p_{T}^{t,1}$ < 0.75 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level for 0.6 TeV < $p_{T}^{t,1}$ < 0.75 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level for 0.6 TeV < $p_{T}^{t,1}$ < 0.75 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.
Covariance matrix between the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at parton level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at parton level for 0 < $|{y}^{t,1}|$ < 0.2.
Covariance matrix between the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at parton level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at parton level for 0.2 < $|{y}^{t,1}|$ < 0.5.
Covariance matrix between the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at parton level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at parton level for 0.5 < $|{y}^{t,1}|$ < 1.
Covariance matrix between the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at parton level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at parton level for 1 < $|{y}^{t,1}|$ < 2.
Covariance matrix between the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at parton level for 0.2 < $|{y}^{t,1}|$ < 0.5 and the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at parton level for 0.2 < $|{y}^{t,1}|$ < 0.5.
Covariance matrix between the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at parton level for 0.2 < $|{y}^{t,1}|$ < 0.5 and the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at parton level for 0.5 < $|{y}^{t,1}|$ < 1.
Covariance matrix between the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at parton level for 0.2 < $|{y}^{t,1}|$ < 0.5 and the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at parton level for 1 < $|{y}^{t,1}|$ < 2.
Covariance matrix between the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at parton level for 0.5 < $|{y}^{t,1}|$ < 1 and the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at parton level for 0.5 < $|{y}^{t,1}|$ < 1.
Covariance matrix between the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at parton level for 0.5 < $|{y}^{t,1}|$ < 1 and the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at parton level for 1 < $|{y}^{t,1}|$ < 2.
Covariance matrix between the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at parton level for 1 < $|{y}^{t,1}|$ < 2 and the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at parton level for 1 < $|{y}^{t,1}|$ < 2.
Covariance matrix between the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t,1}|$ < 0.2.
Covariance matrix between the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.2 < $|{y}^{t,1}|$ < 0.5.
Covariance matrix between the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.5 < $|{y}^{t,1}|$ < 1.
Covariance matrix between the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 1 < $|{y}^{t,1}|$ < 2.
Covariance matrix between the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.2 < $|{y}^{t,1}|$ < 0.5 and the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.5 < $|{y}^{t,1}|$ < 1.
Covariance matrix between the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.5 < $|{y}^{t,1}|$ < 1 and the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.5 < $|{y}^{t,1}|$ < 1.
Covariance matrix between the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.5 < $|{y}^{t,1}|$ < 1 and the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 1 < $|{y}^{t,1}|$ < 2.
Covariance matrix between the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 1 < $|{y}^{t,1}|$ < 2 and the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 1 < $|{y}^{t,1}|$ < 2.
Covariance matrix between the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level for 0 < $|{y}^{t,2}|$ < 0.2 and the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level for 0 < $|{y}^{t,2}|$ < 0.2.
Covariance matrix between the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level for 0 < $|{y}^{t,2}|$ < 0.2 and the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level for 0.2 < $|{y}^{t,2}|$ < 0.5.
Covariance matrix between the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level for 0 < $|{y}^{t,2}|$ < 0.2 and the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level for 0.5 < $|{y}^{t,2}|$ < 1.
Covariance matrix between the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level for 0 < $|{y}^{t,2}|$ < 0.2 and the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level for 1 < $|{y}^{t,2}|$ < 2.
Covariance matrix between the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level for 0.2 < $|{y}^{t,2}|$ < 0.5 and the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level for 0.2 < $|{y}^{t,2}|$ < 0.5.
Covariance matrix between the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level for 0.2 < $|{y}^{t,2}|$ < 0.5 and the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level for 0.5 < $|{y}^{t,2}|$ < 1.
Covariance matrix between the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level for 0.2 < $|{y}^{t,2}|$ < 0.5 and the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level for 1 < $|{y}^{t,2}|$ < 2.
Covariance matrix between the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level for 0.5 < $|{y}^{t,2}|$ < 1 and the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level for 0.5 < $|{y}^{t,2}|$ < 1.
Covariance matrix between the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level for 0.5 < $|{y}^{t,2}|$ < 1 and the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level for 1 < $|{y}^{t,2}|$ < 2.
Covariance matrix between the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level for 1 < $|{y}^{t,2}|$ < 2 and the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ absolute differential cross-section at parton level for 1 < $|{y}^{t,2}|$ < 2.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV and the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV and the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV and the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV and the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV and the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.5 < $|{y}^{t\bar{t}}|$ < 1.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.5 < $|{y}^{t\bar{t}}|$ < 1.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 1 < $|{y}^{t\bar{t}}|$ < 2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.5 < $|{y}^{t\bar{t}}|$ < 1 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.5 < $|{y}^{t\bar{t}}|$ < 1.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.5 < $|{y}^{t\bar{t}}|$ < 1 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 1 < $|{y}^{t\bar{t}}|$ < 2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 1 < $|{y}^{t\bar{t}}|$ < 2 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 1 < $|{y}^{t\bar{t}}|$ < 2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at parton level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at parton level for 0.5 < $|{y}^{t\bar{t}}|$ < 1.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at parton level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5 and the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at parton level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at parton level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5 and the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at parton level for 0.5 < $|{y}^{t\bar{t}}|$ < 1.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at parton level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5 and the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at parton level for 1 < $|{y}^{t\bar{t}}|$ < 2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at parton level for 0.5 < $|{y}^{t\bar{t}}|$ < 1 and the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at parton level for 0.5 < $|{y}^{t\bar{t}}|$ < 1.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at parton level for 0.5 < $|{y}^{t\bar{t}}|$ < 1 and the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at parton level for 1 < $|{y}^{t\bar{t}}|$ < 2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at parton level for 1 < $|{y}^{t\bar{t}}|$ < 2 and the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ absolute differential cross-section at parton level for 1 < $|{y}^{t\bar{t}}|$ < 2.
Covariance matrix between the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0 < $|{y}^{t,1}|$ < 0.2.
Covariance matrix between the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.2 < $|{y}^{t,1}|$ < 0.5.
Covariance matrix between the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.5 < $|{y}^{t,1}|$ < 1.
Covariance matrix between the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 1 < $|{y}^{t,1}|$ < 2.
Covariance matrix between the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.2 < $|{y}^{t,1}|$ < 0.5 and the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.2 < $|{y}^{t,1}|$ < 0.5.
Covariance matrix between the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.2 < $|{y}^{t,1}|$ < 0.5 and the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.5 < $|{y}^{t,1}|$ < 1.
Covariance matrix between the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.2 < $|{y}^{t,1}|$ < 0.5 and the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 1 < $|{y}^{t,1}|$ < 2.
Covariance matrix between the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.5 < $|{y}^{t,1}|$ < 1 and the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.5 < $|{y}^{t,1}|$ < 1.
Covariance matrix between the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.5 < $|{y}^{t,1}|$ < 1 and the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 1 < $|{y}^{t,1}|$ < 2.
Covariance matrix between the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 1 < $|{y}^{t,1}|$ < 2 and the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 1 < $|{y}^{t,1}|$ < 2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.5 < $|{y}^{t\bar{t}}|$ < 1.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 1 < $|{y}^{t\bar{t}}|$ < 2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5 and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5 and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.5 < $|{y}^{t\bar{t}}|$ < 1.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5 and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 1 < $|{y}^{t\bar{t}}|$ < 2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.5 < $|{y}^{t\bar{t}}|$ < 1 and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.5 < $|{y}^{t\bar{t}}|$ < 1.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.5 < $|{y}^{t\bar{t}}|$ < 1 and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 1 < $|{y}^{t\bar{t}}|$ < 2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 1 < $|{y}^{t\bar{t}}|$ < 2 and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 1 < $|{y}^{t\bar{t}}|$ < 2.
Covariance matrix between the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0 TeV < $p_{T}^{t\bar{t}}$ < 0.1 TeV and the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0 TeV < $p_{T}^{t\bar{t}}$ < 0.1 TeV.
Covariance matrix between the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0 TeV < $p_{T}^{t\bar{t}}$ < 0.1 TeV and the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.1 TeV < $p_{T}^{t\bar{t}}$ < 0.2 TeV.
Covariance matrix between the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0 TeV < $p_{T}^{t\bar{t}}$ < 0.1 TeV and the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.2 TeV < $p_{T}^{t\bar{t}}$ < 0.35 TeV.
Covariance matrix between the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0 TeV < $p_{T}^{t\bar{t}}$ < 0.1 TeV and the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.35 TeV < $p_{T}^{t\bar{t}}$ < 1 TeV.
Covariance matrix between the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.1 TeV < $p_{T}^{t\bar{t}}$ < 0.2 TeV and the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.1 TeV < $p_{T}^{t\bar{t}}$ < 0.2 TeV.
Covariance matrix between the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.1 TeV < $p_{T}^{t\bar{t}}$ < 0.2 TeV and the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.2 TeV < $p_{T}^{t\bar{t}}$ < 0.35 TeV.
Covariance matrix between the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.1 TeV < $p_{T}^{t\bar{t}}$ < 0.2 TeV and the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.35 TeV < $p_{T}^{t\bar{t}}$ < 1 TeV.
Covariance matrix between the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.2 TeV < $p_{T}^{t\bar{t}}$ < 0.35 TeV and the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.2 TeV < $p_{T}^{t\bar{t}}$ < 0.35 TeV.
Covariance matrix between the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.2 TeV < $p_{T}^{t\bar{t}}$ < 0.35 TeV and the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.35 TeV < $p_{T}^{t\bar{t}}$ < 1 TeV.
Covariance matrix between the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.35 TeV < $p_{T}^{t\bar{t}}$ < 1 TeV and the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ absolute differential cross-section at parton level for 0.35 TeV < $p_{T}^{t\bar{t}}$ < 1 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level for 0.5 < $|{y}^{t\bar{t}}|$ < 1.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level for 1 < $|{y}^{t\bar{t}}|$ < 2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level for 0.5 < $|{y}^{t\bar{t}}|$ < 1.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level for 1 < $|{y}^{t\bar{t}}|$ < 2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level for 0.5 < $|{y}^{t\bar{t}}|$ < 1 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level for 0.5 < $|{y}^{t\bar{t}}|$ < 1.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level for 0.5 < $|{y}^{t\bar{t}}|$ < 1 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level for 1 < $|{y}^{t\bar{t}}|$ < 2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level for 1 < $|{y}^{t\bar{t}}|$ < 2 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ absolute differential cross-section at parton level for 1 < $|{y}^{t\bar{t}}|$ < 2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ absolute differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
$p_{T}^{t}$ covariance matrix for the normalized differential cross-section at parton level.
$|y^{t}|$ covariance matrix for the normalized differential cross-section at parton level.
$p_{T}^{t,1}$ covariance matrix for the normalized differential cross-section at parton level.
$|y^{t,1}|$ covariance matrix for the normalized differential cross-section at parton level.
$p_{T}^{t,2}$ covariance matrix for the normalized differential cross-section at parton level.
$|{y}^{t,2}|$ covariance matrix for the normalized differential cross-section at parton level.
$m^{t\bar{t}}$ covariance matrix for the normalized differential cross-section at parton level.
$p_{T}^{t\bar{t}}$ covariance matrix for the normalized differential cross-section at parton level.
$|{y}^{t\bar{t}}|$ covariance matrix for the normalized differential cross-section at parton level.
${\chi}^{t\bar{t}}$ covariance matrix for the normalized differential cross-section at parton level.
$|y_{B}^{t\bar{t}}|$ covariance matrix for the normalized differential cross-section at parton level.
$|p_{out}^{t\bar{t}}|$ covariance matrix for the normalized differential cross-section at parton level.
$|\Delta \phi(t_{1}, t_{2})|$ covariance matrix for the normalized differential cross-section at parton level.
$H_{T}^{t\bar{t}}$ covariance matrix for the normalized differential cross-section at parton level.
$|\cos\theta^{*}|$ covariance matrix for the normalized differential cross-section at parton level.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level for 0.55 TeV < $p_{T}^{t,1}$ < 0.6 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level for 0.6 TeV < $p_{T}^{t,1}$ < 0.75 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level for 0.55 TeV < $p_{T}^{t,1}$ < 0.6 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level for 0.55 TeV < $p_{T}^{t,1}$ < 0.6 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level for 0.55 TeV < $p_{T}^{t,1}$ < 0.6 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level for 0.6 TeV < $p_{T}^{t,1}$ < 0.75 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level for 0.55 TeV < $p_{T}^{t,1}$ < 0.6 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level for 0.6 TeV < $p_{T}^{t,1}$ < 0.75 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level for 0.6 TeV < $p_{T}^{t,1}$ < 0.75 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level for 0.6 TeV < $p_{T}^{t,1}$ < 0.75 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.
Covariance matrix between the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ normalized differential cross-section at parton level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ normalized differential cross-section at parton level for 0 < $|{y}^{t,1}|$ < 0.2.
Covariance matrix between the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ normalized differential cross-section at parton level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ normalized differential cross-section at parton level for 0.2 < $|{y}^{t,1}|$ < 0.5.
Covariance matrix between the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ normalized differential cross-section at parton level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ normalized differential cross-section at parton level for 0.5 < $|{y}^{t,1}|$ < 1.
Covariance matrix between the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ normalized differential cross-section at parton level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ normalized differential cross-section at parton level for 1 < $|{y}^{t,1}|$ < 2.
Covariance matrix between the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ normalized differential cross-section at parton level for 0.2 < $|{y}^{t,1}|$ < 0.5 and the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ normalized differential cross-section at parton level for 0.2 < $|{y}^{t,1}|$ < 0.5.
Covariance matrix between the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ normalized differential cross-section at parton level for 0.2 < $|{y}^{t,1}|$ < 0.5 and the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ normalized differential cross-section at parton level for 0.5 < $|{y}^{t,1}|$ < 1.
Covariance matrix between the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ normalized differential cross-section at parton level for 0.2 < $|{y}^{t,1}|$ < 0.5 and the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ normalized differential cross-section at parton level for 1 < $|{y}^{t,1}|$ < 2.
Covariance matrix between the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ normalized differential cross-section at parton level for 0.5 < $|{y}^{t,1}|$ < 1 and the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ normalized differential cross-section at parton level for 0.5 < $|{y}^{t,1}|$ < 1.
Covariance matrix between the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ normalized differential cross-section at parton level for 0.5 < $|{y}^{t,1}|$ < 1 and the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ normalized differential cross-section at parton level for 1 < $|{y}^{t,1}|$ < 2.
Covariance matrix between the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ normalized differential cross-section at parton level for 1 < $|{y}^{t,1}|$ < 2 and the $|{y}^{t,1}|\otimes |{y}^{t,2}|$ normalized differential cross-section at parton level for 1 < $|{y}^{t,1}|$ < 2.
Covariance matrix between the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0 < $|{y}^{t,1}|$ < 0.2.
Covariance matrix between the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.2 < $|{y}^{t,1}|$ < 0.5.
Covariance matrix between the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.5 < $|{y}^{t,1}|$ < 1.
Covariance matrix between the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 1 < $|{y}^{t,1}|$ < 2.
Covariance matrix between the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.2 < $|{y}^{t,1}|$ < 0.5 and the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.2 < $|{y}^{t,1}|$ < 0.5.
Covariance matrix between the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.2 < $|{y}^{t,1}|$ < 0.5 and the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.5 < $|{y}^{t,1}|$ < 1.
Covariance matrix between the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.2 < $|{y}^{t,1}|$ < 0.5 and the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 1 < $|{y}^{t,1}|$ < 2.
Covariance matrix between the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.5 < $|{y}^{t,1}|$ < 1 and the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.5 < $|{y}^{t,1}|$ < 1.
Covariance matrix between the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.5 < $|{y}^{t,1}|$ < 1 and the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 1 < $|{y}^{t,1}|$ < 2.
Covariance matrix between the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 1 < $|{y}^{t,1}|$ < 2 and the $|{y}^{t,1}|\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 1 < $|{y}^{t,1}|$ < 2.
Covariance matrix between the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level for 0 < $|{y}^{t,2}|$ < 0.2 and the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level for 0 < $|{y}^{t,2}|$ < 0.2.
Covariance matrix between the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level for 0 < $|{y}^{t,2}|$ < 0.2 and the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level for 0.2 < $|{y}^{t,2}|$ < 0.5.
Covariance matrix between the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level for 0 < $|{y}^{t,2}|$ < 0.2 and the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level for 0.5 < $|{y}^{t,2}|$ < 1.
Covariance matrix between the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level for 0 < $|{y}^{t,2}|$ < 0.2 and the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level for 1 < $|{y}^{t,2}|$ < 2.
Covariance matrix between the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level for 0.2 < $|{y}^{t,2}|$ < 0.5 and the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level for 0.2 < $|{y}^{t,2}|$ < 0.5.
Covariance matrix between the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level for 0.2 < $|{y}^{t,2}|$ < 0.5 and the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level for 0.5 < $|{y}^{t,2}|$ < 1.
Covariance matrix between the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level for 0.2 < $|{y}^{t,2}|$ < 0.5 and the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level for 1 < $|{y}^{t,2}|$ < 2.
Covariance matrix between the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level for 0.5 < $|{y}^{t,2}|$ < 1 and the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level for 0.5 < $|{y}^{t,2}|$ < 1.
Covariance matrix between the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level for 0.5 < $|{y}^{t,2}|$ < 1 and the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level for 1 < $|{y}^{t,2}|$ < 2.
Covariance matrix between the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level for 1 < $|{y}^{t,2}|$ < 2 and the $|{y}^{t,2}|\otimes p_{T}^{t,2}$ normalized differential cross-section at parton level for 1 < $|{y}^{t,2}|$ < 2.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at parton level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at parton level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at parton level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at parton level for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at parton level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at parton level for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at parton level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at parton level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at parton level for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at parton level for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at parton level for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at parton level for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at parton level for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at parton level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at parton level for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at parton level for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at parton level for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at parton level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at parton level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV and the $p_{T}^{t,1}\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at parton level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0.5 TeV < $p_{T}^{t,1}$ < 0.55 TeV and the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV and the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV and the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0.55 TeV < $p_{T}^{t,1}$ < 0.625 TeV and the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV and the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0.625 TeV < $p_{T}^{t,1}$ < 0.75 TeV and the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.
Covariance matrix between the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV and the $p_{T}^{t,1}\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0.75 TeV < $p_{T}^{t,1}$ < 2 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.5 < $|{y}^{t\bar{t}}|$ < 1.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 1 < $|{y}^{t\bar{t}}|$ < 2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.5 < $|{y}^{t\bar{t}}|$ < 1.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 1 < $|{y}^{t\bar{t}}|$ < 2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.5 < $|{y}^{t\bar{t}}|$ < 1 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.5 < $|{y}^{t\bar{t}}|$ < 1.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.5 < $|{y}^{t\bar{t}}|$ < 1 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 1 < $|{y}^{t\bar{t}}|$ < 2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 1 < $|{y}^{t\bar{t}}|$ < 2 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 1 < $|{y}^{t\bar{t}}|$ < 2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ normalized differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ normalized differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ normalized differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ normalized differential cross-section at parton level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ normalized differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ normalized differential cross-section at parton level for 0.5 < $|{y}^{t\bar{t}}|$ < 1.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ normalized differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ normalized differential cross-section at parton level for 1 < $|{y}^{t\bar{t}}|$ < 2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ normalized differential cross-section at parton level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5 and the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ normalized differential cross-section at parton level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ normalized differential cross-section at parton level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5 and the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ normalized differential cross-section at parton level for 0.5 < $|{y}^{t\bar{t}}|$ < 1.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ normalized differential cross-section at parton level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5 and the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ normalized differential cross-section at parton level for 1 < $|{y}^{t\bar{t}}|$ < 2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ normalized differential cross-section at parton level for 0.5 < $|{y}^{t\bar{t}}|$ < 1 and the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ normalized differential cross-section at parton level for 0.5 < $|{y}^{t\bar{t}}|$ < 1.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ normalized differential cross-section at parton level for 0.5 < $|{y}^{t\bar{t}}|$ < 1 and the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}| $normalized differential cross-section at parton level for 1 < $|{y}^{t\bar{t}}|$ < 2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ normalized differential cross-section at parton level for 1 < $|{y}^{t\bar{t}}|$ < 2 and the $|{y}^{t\bar{t}}|\otimes |{y}^{t,1}|$ normalized differential cross-section at parton level for 1 < $|{y}^{t\bar{t}}|$ < 2.
Covariance matrix between the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0 < $|{y}^{t,1}|$ < 0.2.
Covariance matrix between the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0.2 < $|{y}^{t,1}|$ < 0.5.
Covariance matrix between the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0.5 < $|{y}^{t,1}|$ < 1.
Covariance matrix between the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0 < $|{y}^{t,1}|$ < 0.2 and the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 1 < $|{y}^{t,1}|$ < 2.
Covariance matrix between the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0.2 < $|{y}^{t,1}|$ < 0.5 and the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0.2 < $|{y}^{t,1}|$ < 0.5.
Covariance matrix between the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0.2 < $|{y}^{t,1}|$ < 0.5 and the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0.5 < $|{y}^{t,1}|$ < 1.
Covariance matrix between the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0.2 < $|{y}^{t,1}|$ < 0.5 and the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 1 < $|{y}^{t,1}|$ < 2.
Covariance matrix between the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0.5 < $|{y}^{t,1}|$ < 1 and the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0.5 < $|{y}^{t,1}|$ < 1.
Covariance matrix between the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0.5 < $|{y}^{t,1}|$ < 1 and the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 1 < $|{y}^{t,1}|$ < 2.
Covariance matrix between the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 1 < $|{y}^{t,1}|$ < 2 and the $|{y}^{t,1}|\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 1 < $|{y}^{t,1}|$ < 2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0.5 < $|{y}^{t\bar{t}}|$ < 1.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 1 < $|{y}^{t\bar{t}}|$ < 2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5 and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5 and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0.5 < $|{y}^{t\bar{t}}|$ < 1.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5 and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 1 < $|{y}^{t\bar{t}}|$ < 2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0.5 < $|{y}^{t\bar{t}}|$ < 1 and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0.5 < $|{y}^{t\bar{t}}|$ < 1.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0.5 < $|{y}^{t\bar{t}}|$ < 1 and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 1 < $|{y}^{t\bar{t}}|$ < 2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 1 < $|{y}^{t\bar{t}}|$ < 2 and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 1 < $|{y}^{t\bar{t}}|$ < 2.
Covariance matrix between the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0 TeV < $p_{T}^{t\bar{t}}$ < 0.1 TeV and the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0 TeV < $p_{T}^{t\bar{t}}$ < 0.1 TeV.
Covariance matrix between the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0 TeV < $p_{T}^{t\bar{t}}$ < 0.1 TeV and the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0.1 TeV < $p_{T}^{t\bar{t}}$ < 0.2 TeV.
Covariance matrix between the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0 TeV < $p_{T}^{t\bar{t}}$ < 0.1 TeV and the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0.2 TeV < $p_{T}^{t\bar{t}}$ < 0.35 TeV.
Covariance matrix between the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0 TeV < $p_{T}^{t\bar{t}}$ < 0.1 TeV and the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0.35 TeV < $p_{T}^{t\bar{t}}$ < 1 TeV.
Covariance matrix between the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0.1 TeV < $p_{T}^{t\bar{t}}$ < 0.2 TeV and the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0.1 TeV < $p_{T}^{t\bar{t}}$ < 0.2 TeV.
Covariance matrix between the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0.1 TeV < $p_{T}^{t\bar{t}}$ < 0.2 TeV and the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0.2 TeV < $p_{T}^{t\bar{t}}$ < 0.35 TeV.
Covariance matrix between the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0.1 TeV < $p_{T}^{t\bar{t}}$ < 0.2 TeV and the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0.35 TeV < $p_{T}^{t\bar{t}}$ < 1 TeV.
Covariance matrix between the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0.2 TeV < $p_{T}^{t\bar{t}}$ < 0.35 TeV and the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0.2 TeV < $p_{T}^{t\bar{t}}$ < 0.35 TeV.
Covariance matrix between the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0.2 TeV < $p_{T}^{t\bar{t}}$ < 0.35 TeV and the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0.35 TeV < $p_{T}^{t\bar{t}}$ < 1 TeV.
Covariance matrix between the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0.35 TeV < $p_{T}^{t\bar{t}}$ < 1 TeV and the $p_{T}^{t\bar{t}}\otimes m^{t\bar{t}}$ normalized differential cross-section at parton level for 0.35 TeV < $p_{T}^{t\bar{t}}$ < 1 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at parton level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at parton level for 0.5 < $|{y}^{t\bar{t}}|$ < 1.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.2 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at parton level for 1 < $|{y}^{t\bar{t}}|$ < 2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at parton level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at parton level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at parton level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at parton level for 0.5 < $|{y}^{t\bar{t}}|$ < 1.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at parton level for 0.2 < $|{y}^{t\bar{t}}|$ < 0.5 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at parton level for 1 < $|{y}^{t\bar{t}}|$ < 2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at parton level for 0.5 < $|{y}^{t\bar{t}}|$ < 1 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at parton level for 0.5 < $|{y}^{t\bar{t}}|$ < 1.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at parton level for 0.5 < $|{y}^{t\bar{t}}|$ < 1 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at parton level for 1 < $|{y}^{t\bar{t}}|$ < 2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at parton level for 1 < $|{y}^{t\bar{t}}|$ < 2 and the $|{y}^{t\bar{t}}|\otimes p_{T}^{t\bar{t}}$ normalized differential cross-section at parton level for 1 < $|{y}^{t\bar{t}}|$ < 2.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0 < $|{y}^{t\bar{t}}|$ < 0.3, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.3 < $|{y}^{t\bar{t}}|$ < 0.9, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 0.9 TeV < $m^{t\bar{t}}$ < 1.2 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.2 TeV < $m^{t\bar{t}}$ < 1.5 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Covariance matrix between the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV and the $|{y}^{t\bar{t}}|\otimes m^{t\bar{t}}\otimes p_{T}^{t,1}$ normalized differential cross-section at parton level for 0.9 < $|{y}^{t\bar{t}}|$ < 2, 1.5 TeV < $m^{t\bar{t}}$ < 4 TeV.
Cross-sections for the production of a $Z$ boson in association with two photons are measured in proton$-$proton collisions at a centre-of-mass energy of 13 TeV. The data used correspond to an integrated luminosity of 139 fb$^{-1}$ recorded by the ATLAS experiment during Run 2 of the LHC. The measurements use the electron and muon decay channels of the $Z$ boson, and a fiducial phase-space region where the photons are not radiated from the leptons. The integrated $Z(\rightarrow\ell\ell)\gamma\gamma$ cross-section is measured with a precision of 12% and differential cross-sections are measured as a function of six kinematic variables of the $Z\gamma\gamma$ system. The data are compared with predictions from MC event generators which are accurate to up to next-to-leading order in QCD. The cross-section measurements are used to set limits on the coupling strengths of dimension-8 operators in the framework of an effective field theory.
In a special run of the LHC with $\beta^\star = 2.5~$km, proton-proton elastic-scattering events were recorded at $\sqrt{s} = 13~$TeV with an integrated luminosity of $340~\mu \textrm{b}^{-1}$ using the ALFA subdetector of ATLAS in 2016. The elastic cross section was measured differentially in the Mandelstam $t$ variable in the range from $-t = 2.5 \cdot 10^{-4}~$GeV$^{2}$ to $-t = 0.46~$GeV$^{2}$ using 6.9 million elastic-scattering candidates. This paper presents measurements of the total cross section $\sigma_{\textrm{tot}}$, parameters of the nuclear slope, and the $\rho$-parameter defined as the ratio of the real part to the imaginary part of the elastic-scattering amplitude in the limit $t \rightarrow 0$. These parameters are determined from a fit to the differential elastic cross section using the optical theorem and different parameterizations of the $t$-dependence. The results for $\sigma_{\textrm{tot}}$ and $\rho$ are \begin{equation*} \sigma_{\textrm{tot}}(pp\rightarrow X) = \mbox{104.7} \pm 1.1 \; \mbox{mb} , \; \; \; \rho = \mbox{0.098} \pm 0.011 . \end{equation*} The uncertainty in $\sigma_{\textrm{tot}}$ is dominated by the luminosity measurement, and in $\rho$ by imperfect knowledge of the detector alignment and by modelling of the nuclear amplitude.
The rho-parameter, i.e. the ratio of the real to imaginary part of the elastic scattering amplitude extrapolated to t=0. The systematic uncertainty includes experimental and theoretical uncerainties.
The rho-parameter, i.e. the ratio of the real to imaginary part of the elastic scattering amplitude extrapolated to t=0. The systematic uncertainty includes experimental and theoretical uncerainties.
The total elastic cross section obtained from the fitted parameters, extrapolated to full phase space using only the nuclear amplitude.
The total elastic cross section obtained from the fitted parameters, extrapolated to full phase space using only the nuclear amplitude.
The ratio of elastic to total cross section.
The ratio of elastic to total cross section.
The differential elastic cross section as function of t with statistical and systematic uncertainties. The systematic uncertainties are given as signed relative change for 20 sources of experimental uncertainty associated to nuisance parameters used in the fit for the extraction of physics parameters.
The differential elastic cross section as function of t with statistical and systematic uncertainties. The systematic uncertainties are given as signed relative change for 20 sources of experimental uncertainty associated to nuisance parameters used in the fit for the extraction of physics parameters.
This paper presents studies of Bose-Einstein correlations (BEC) in proton-proton collisions at a centre-of-mass energy of 13 TeV, using data from the ATLAS detector at the CERN Large Hadron Collider. Data were collected in a special low-luminosity configuration with a minimum-bias trigger and a high-multiplicity track trigger, accumulating integrated luminosities of 151 $\mu$b$^{-1}$ and 8.4 nb$^{-1}$ respectively. The BEC are measured for pairs of like-sign charged particles, each with $|\eta|$ < 2.5, for two kinematic ranges: the first with particle $p_T$ > 100 MeV and the second with particle $p_T$ > 500 MeV. The BEC parameters, characterizing the source radius and particle correlation strength, are investigated as functions of charged-particle multiplicity (up to 300) and average transverse momentum of the pair (up to 1.5 GeV). The double-differential dependence on charged-particle multiplicity and average transverse momentum of the pair is also studied. The BEC radius is found to be independent of the charged-particle multiplicity for high charged-particle multiplicity (above 100), confirming a previous observation at lower energy. This saturation occurs independent of the transverse momentum of the pair.
The two-particle double-ratio correlation function, R<sub>2</sub>(Q), for pp collisions for track p<sub>T</sub> >100 MeV at √s=13 TeV in the multiplicity interval 71 ≤ n<sub>ch</sub> < 80 for the minimum-bias (MB) events. The blue dashed and red solid lines show the results of the exponential and Gaussian fits, respectively. The region excluded from the fits is shown. The statistical uncertainty and the systematic uncertainty for imperfections in the data reconstruction procedure are added in quadrature.
Comparison of single-ratio two-particle correlation functions, using the unlike-charge particle (UCP) pair reference sample, for minimum-bias (MB) events, showing C<sub>2</sub><sup>data</sup>(Q) (top panel) at 13 TeV (black circles) and 7 TeV (open blue circles), and the ratio of C<sub>2</sub><sup>7 TeV</sup> (Q) to C<sub>2</sub><sup>13 TeV</sup> (Q) (bottom panel). Comparison of C<sub>2</sub><sup>data</sup> (Q) for representative multiplicity region 3.09 < m<sub>ch</sub> ≤ 3.86. The statistical and systematic uncertainties, combined in quadrature, are presented. The systematic uncertainties include track efficiency, Coulomb correction, non-closure and multiplicity-unfolding uncertainties.
Comparison of single-ratio two-particle correlation functions, using the unlike-charge particle (UCP) pair reference sample, for minimum-bias (MB) events, showing C<sub>2</sub><sup>data</sup>(Q) (top panel) at 13 TeV (black circles) and 7 TeV (open blue circles), and the ratio of C<sub>2</sub><sup>7 TeV</sup> (Q) to C<sub>2</sub><sup>13 TeV</sup> (Q) (bottom panel). Comparison of C<sub>2</sub><sup>data</sup> (Q) for representative k<sub>T</sub> region 400 < k<sub>T</sub> ≤500 MeV. The statistical and systematic uncertainties, combined in quadrature, are presented. The systematic uncertainties include track efficiency, Coulomb correction, non-closure and multiplicity-unfolding uncertainties.
The k<sub>T</sub> dependence of the correlation strength, λ(k<sub>T</sub>), obtained from the exponential fit to the R<sub>2</sub>(Q) correlation functions for events with multiplicity n<sub>ch</sub> ≥ 2 and transfer momentum of tracks with p<sub>T</sub> >100 MeV and p<sub>T</sub> >500 MeV at √s=13 TeV for the minimum-bias (MB) and high-multiplicity track (HMT) events. The uncertainties represent the sum in quadrature of the statistical and systematic contributions. The curves represent the exponential fits to λ(k<sub>T</sub>).
The k<sub>T</sub> dependence of the correlation strength, λ(k<sub>T</sub>), obtained from the exponential fit to the R<sub>2</sub>(Q) correlation functions for events with multiplicity n<sub>ch</sub> ≥ 2 and transfer momentum of tracks with p<sub>T</sub> >100 MeV and p<sub>T</sub> >500 MeV at √s=13 TeV for the minimum-bias (MB) and high-multiplicity track (HMT) events. The uncertainties represent the sum in quadrature of the statistical and systematic contributions. The curves represent the exponential fits to λ(k<sub>T</sub>).
The k<sub>T</sub> dependence of the correlation strength, λ(k<sub>T</sub>), obtained from the exponential fit to the R<sub>2</sub>(Q) correlation functions for events with multiplicity n<sub>ch</sub> ≥ 2 and transfer momentum of tracks with p<sub>T</sub> >100 MeV and p<sub>T</sub> >500 MeV at √s=13 TeV for the minimum-bias (MB) and high-multiplicity track (HMT) events. The uncertainties represent the sum in quadrature of the statistical and systematic contributions. The curves represent the exponential fits to λ(k<sub>T</sub>).
The k<sub>T</sub> dependence of the correlation strength, λ(k<sub>T</sub>), obtained from the exponential fit to the R<sub>2</sub>(Q) correlation functions for events with multiplicity n<sub>ch</sub> ≥ 2 and transfer momentum of tracks with p<sub>T</sub> >100 MeV and p<sub>T</sub> >500 MeV at √s=13 TeV for the minimum-bias (MB) and high-multiplicity track (HMT) events. The uncertainties represent the sum in quadrature of the statistical and systematic contributions. The curves represent the exponential fits to λ(k<sub>T</sub>).
The k<sub>T</sub> dependence of the source radius, R(k<sub>T</sub>), obtained from the exponential fit to the R<sub>2</sub>(Q) correlation functions for events with multiplicity n<sub>ch</sub> ≥ 2 and transfer momentum of tracks with p<sub>T</sub> >100 MeV and p<sub>T</sub> >500 MeV at √s=13 TeV for the minimum-bias (MB) and high-multiplicity track (HMT) events. The uncertainties represent the sum in quadrature of the statistical and systematic contributions. The curves represent the exponential fits to R(k<sub>T</sub>).
The k<sub>T</sub> dependence of the source radius, R(k<sub>T</sub>), obtained from the exponential fit to the R<sub>2</sub>(Q) correlation functions for events with multiplicity n<sub>ch</sub> ≥ 2 and transfer momentum of tracks with p<sub>T</sub> >100 MeV and p<sub>T</sub> >500 MeV at √s=13 TeV for the minimum-bias (MB) and high-multiplicity track (HMT) events. The uncertainties represent the sum in quadrature of the statistical and systematic contributions. The curves represent the exponential fits to R(k<sub>T</sub>).
The k<sub>T</sub> dependence of the source radius, R(k<sub>T</sub>), obtained from the exponential fit to the R<sub>2</sub>(Q) correlation functions for events with multiplicity n<sub>ch</sub> ≥ 2 and transfer momentum of tracks with p<sub>T</sub> >100 MeV and p<sub>T</sub> >500 MeV at √s=13 TeV for the minimum-bias (MB) and high-multiplicity track (HMT) events. The uncertainties represent the sum in quadrature of the statistical and systematic contributions. The curves represent the exponential fits to R(k<sub>T</sub>).
The k<sub>T</sub> dependence of the source radius, R(k<sub>T</sub>), obtained from the exponential fit to the R<sub>2</sub>(Q) correlation functions for events with multiplicity n<sub>ch</sub> ≥ 2 and transfer momentum of tracks with p<sub>T</sub> >100 MeV and p<sub>T</sub> >500 MeV at √s=13 TeV for the minimum-bias (MB) and high-multiplicity track (HMT) events. The uncertainties represent the sum in quadrature of the statistical and systematic contributions. The curves represent the exponential fits to R(k<sub>T</sub>).
The two-dimensional dependence on m<sub>ch</sub> and k<sub>T</sub> for p<sub>T</sub> > 100 MeV for the correlation strength, λ, obtained from the exponential fit to the R<sub>2</sub>(Q) correlation functions using the MB sample for m<sub>ch</sub> ≤ 3.08 and the HMT sample for m<sub>ch</sub> > 3.08.
The two-dimensional dependence on m<sub>ch</sub> and k<sub>T</sub> for p<sub>T</sub> > 100 MeV for the source radius, R, obtained from the exponential fit to the R<sub>2</sub>(Q) correlation functions using the MB sample for m<sub>ch</sub> ≤ 3.08 and the HMT sample for m<sub>ch</sub> > 3.08.
The parameter κ describing the dependence of the source radius, R, on charged-particle scaled multiplicity, m<sub>ch</sub>, for track p<sub>T</sub>>100 MeV and track p<sub>T</sub>>500 MeV in the minimum-bias (MB) and high-multiplicity track (HMT) samples at √s = 13 TeV. The error bars and boxes represent the statistical and systematic contributions, respectively. The black solid and blue dashed curves represent the exponential fit to the parameter κ for tracks with p<sub>T</sub> >100 MeV and for tracks with p<sub>T</sub> >500 MeV, respectively.
The parameter κ describing the dependence of the source radius, R, on charged-particle scaled multiplicity, m<sub>ch</sub>, for track p<sub>T</sub>>100 MeV and track p<sub>T</sub>>500 MeV in the minimum-bias (MB) and high-multiplicity track (HMT) samples at √s = 13 TeV. The error bars and boxes represent the statistical and systematic contributions, respectively. The black solid and blue dashed curves represent the exponential fit to the parameter κ for tracks with p<sub>T</sub> >100 MeV and for tracks with p<sub>T</sub> >500 MeV, respectively.
The parameter κ describing the dependence of the source radius, R, on charged-particle scaled multiplicity, m<sub>ch</sub>, for track p<sub>T</sub>>100 MeV and track p<sub>T</sub>>500 MeV in the minimum-bias (MB) and high-multiplicity track (HMT) samples at √s = 13 TeV. The error bars and boxes represent the statistical and systematic contributions, respectively. The black solid and blue dashed curves represent the exponential fit to the parameter κ for tracks with p<sub>T</sub> >100 MeV and for tracks with p<sub>T</sub> >500 MeV, respectively.
The parameter κ describing the dependence of the source radius, R, on charged-particle scaled multiplicity, m<sub>ch</sub>, for track p<sub>T</sub>>100 MeV and track p<sub>T</sub>>500 MeV in the minimum-bias (MB) and high-multiplicity track (HMT) samples at √s = 13 TeV. The error bars and boxes represent the statistical and systematic contributions, respectively. The black solid and blue dashed curves represent the exponential fit to the parameter κ for tracks with p<sub>T</sub> >100 MeV and for tracks with p<sub>T</sub> >500 MeV, respectively.
The two-dimensional dependence on m<sub>ch</sub> and k<sub>T</sub> for p<sub>T</sub> > 500 MeV for the correlation strength, λ, obtained from the exponential fit to the R<sub>2</sub>(Q) correlation functions using the MB sample for m<sub>ch</sub> ≤ 3.08 and the HMT sample for m<sub>ch</sub> > 3.08.
The two-dimensional dependence on m<sub>ch</sub> and k<sub>T</sub> for p<sub>T</sub> > 500 MeV for the source radius, R, obtained from the exponential fit to the R<sub>2</sub>(Q) correlation functions using the MB sample for m<sub>ch</sub> ≤ 3.08 and the HMT sample for m<sub>ch</sub> > 3.08.
ATLAS and CMS results for the source radius R as a function of n<sub>ch</sub> in pp interactions at 13 TeV. The CMS results (open circles) have been adjusted (by the CMS collaboration) to the ATLAS kinematic region∶ p<sub>T</sub> > 100 MeV and |η|<2.5. The ATLAS uncertainties are the sum in quadrature of the statistical and asymmetric systematic uncertainties. For CMS, only the systematic uncertainties are shown since the statistical uncertainties are smaller than the marker size. The dashed blue (ATLAS) and black (CMS) lines represent the fit to ∛n<sub>ch</sub> at low multiplicity, continued as dotted lines beyond the fit range. The solid green (ATLAS) and broken black (CMS) lines indicate the plateau level at high multiplicity.
ATLAS and CMS results for the source radius R as a function of n<sub>ch</sub> in pp interactions at 13 TeV. The CMS results (open circles) have been adjusted (by the CMS collaboration) to the ATLAS kinematic region∶ p<sub>T</sub> > 100 MeV and |η|<2.5. The ATLAS uncertainties are the sum in quadrature of the statistical and asymmetric systematic uncertainties. For CMS, only the systematic uncertainties are shown since the statistical uncertainties are smaller than the marker size. The dashed blue (ATLAS) and black (CMS) lines represent the fit to ∛n<sub>ch</sub> at low multiplicity, continued as dotted lines beyond the fit range. The solid green (ATLAS) and broken black (CMS) lines indicate the plateau level at high multiplicity.
ATLAS and CMS results for the source radius R as a function of n<sub>ch</sub> in pp interactions at 13 TeV. The CMS results (open circles) have been adjusted (by the CMS collaboration) to the ATLAS kinematic region∶ p<sub>T</sub> > 100 MeV and |η|<2.5. The ATLAS uncertainties are the sum in quadrature of the statistical and asymmetric systematic uncertainties. For CMS, only the systematic uncertainties are shown since the statistical uncertainties are smaller than the marker size. The dashed blue (ATLAS) and black (CMS) lines represent the fit to ∛n<sub>ch</sub> at low multiplicity, continued as dotted lines beyond the fit range. The solid green (ATLAS) and broken black (CMS) lines indicate the plateau level at high multiplicity.
ATLAS and CMS results for the source radius R as a function of ∛n<sub>ch</sub> in pp interactions at 13 TeV. The CMS results (open circles) have been adjusted (by the CMS collaboration) to the ATLAS kinematic region∶ p<sub>T</sub> > 100 MeV and |η|<2.5. The ATLAS uncertainties are the sum in quadrature of the statistical and asymmetric systematic uncertainties. For CMS, only the systematic uncertainties are shown since the statistical uncertainties are smaller than the marker size. The dashed blue (ATLAS) and black (CMS) lines represent the fit to ∛n<sub>ch</sub> at low multiplicity, continued as dotted lines beyond the fit range. The solid green (ATLAS) and broken black (CMS) lines indicate the plateau level at high multiplicity.
ATLAS and CMS results for the source radius R as a function of ∛n<sub>ch</sub> in pp interactions at 13 TeV. The CMS results (open circles) have been adjusted (by the CMS collaboration) to the ATLAS kinematic region∶ p<sub>T</sub> > 100 MeV and |η|<2.5. The ATLAS uncertainties are the sum in quadrature of the statistical and asymmetric systematic uncertainties. For CMS, only the systematic uncertainties are shown since the statistical uncertainties are smaller than the marker size. The dashed blue (ATLAS) and black (CMS) lines represent the fit to ∛n<sub>ch</sub> at low multiplicity, continued as dotted lines beyond the fit range. The solid green (ATLAS) and broken black (CMS) lines indicate the plateau level at high multiplicity.
ATLAS and CMS results for the source radius R as a function of ∛n<sub>ch</sub> in pp interactions at 13 TeV. The CMS results (open circles) have been adjusted (by the CMS collaboration) to the ATLAS kinematic region∶ p<sub>T</sub> > 100 MeV and |η|<2.5. The ATLAS uncertainties are the sum in quadrature of the statistical and asymmetric systematic uncertainties. For CMS, only the systematic uncertainties are shown since the statistical uncertainties are smaller than the marker size. The dashed blue (ATLAS) and black (CMS) lines represent the fit to ∛n<sub>ch</sub> at low multiplicity, continued as dotted lines beyond the fit range. The solid green (ATLAS) and broken black (CMS) lines indicate the plateau level at high multiplicity.
Systematic uncertainties (in percent) in the correlation strength, λ, and source radius, R, for the exponential fit of the two-particle double-ratio correlation functions, R<sub>2</sub>(Q), for p<sub>T</sub> > 100 MeV at √s= 13 TeV for the MB and HMT events. The choice of MC generator gives rise to asymmetric uncertainties, denoted by uparrow and downarrow. This asymmetry propagates through to the cumulative uncertainty. The columns under ‘Uncertainty range’ show the range of systematic uncertainty from the fits in the various n<sub>ch</sub> intervals.
The results of the fits to the dependencies of the correlation strength, λ, and source radius, R, on the average rescaled charged-particle multiplicity, m<sub>ch</sub>, for |η| < 2.5 and both p<sub>T</sub> > 100 MeV and p<sub>T</sub> > 500 MeV at √s = 13 TeV for the minimum-bias (MB) and the high-multiplicity track (HMT) events. The parameters γ and δ resulting from a joint fit to the MB and HMT data are presented. The total uncertainties are shown.
The results of the fits to the dependencies of the correlation strength, λ, and source radius, R, on the pair average transverse momentum, k<sub>T</sub>, for various functional forms and for minimum-bias (MB) and high-multiplicity track (HMT) events for p<sub>T</sub> > 100 MeV and p<sub>T</sub> > 500 MeV at √s = 13 TeV. The total uncertainties are shown.
The single-ratio two-particle correlation functions, C<sub>2</sub><sup>data</sup>(Q), for the minimum-bias (MB) events using the unlike-charge particle (UCP) pairs reference sample for n<sub>ch</sub> - intervals∶ (a) 91 < n<sub>ch</sub> ≤ 100, (b) 101 < n<sub>ch</sub> ≤ 125, (c) 126 < n<sub>ch</sub> ≤ 150, (d) 151 < n<sub>ch</sub> ≤ 200, (e) 201 < n<sub>ch</sub> ≤ 250. The error bars represent the statistical uncertainties. The boxes represent the systematic uncertainties, which are the sum in quadrature of a variation of the Coulomb correction, the track reconstruction efficiency and the unfolding matrix.
The single-ratio two-particle correlation functions, C<sub>2</sub><sup>data</sup>(Q), at 7 TeV for the minimum-bias (MB) events using the unlike-charge particle (UCP) pairs reference sample for n<sub>ch</sub> - intervals∶ (a) 2 < n<sub>ch</sub> ≤ 9, (b) 10 < n<sub>ch</sub> ≤ 18, (c) 19 < n<sub>ch</sub> ≤ 27, (d) 28 < n<sub>ch</sub> ≤ 36, (e) 37 < n<sub>ch</sub> ≤ 45, (f) 46 < n<sub>ch</sub> ≤ 54, (g) 55 < n<sub>ch</sub> ≤ 63, (h) 64 < n<sub>ch</sub> ≤ 72, (i) 73 < n<sub>ch</sub> ≤ 81, (j) 82 < n<sub>ch</sub> ≤ 90, (k) 91 < n<sub>ch</sub> ≤ 113, and (l) 114 < n<sub>ch</sub> ≤ 136. The error bars represent the statistical uncertainties. The boxes represent the systematic uncertainties, which are the sum in quadrature of a variation of the Coulomb correction, the track reconstruction efficiency and the unfolding matrix.
The correlation strength, λ, and source radius, R, of the exponential fits to the two-particle double-ratio correlation functions, R<sub>2</sub>(Q), in dependence on the multiplicity, m<sub>ch</sub>, intervals for the minimum-bias (MB) and the high-multiplicity track (HMT) events for p<sub>T</sub> > 100 MeV at √s = 13 TeV. Statistical uncertainties for √χ<sup>2</sup>/ndf>1 are corrected by the √χ<sup>2</sup>/ndf. The total uncertainties are shown.
The correlation strength, λ, and source radius, R, of the exponential fits to the two-particle double-ratio correlation functions, R<sub>2</sub>(Q), in dependence on the multiplicity, m<sub>ch</sub>, intervals for the minimum-bias (MB) and the high-multiplicity track (HMT) events for p<sub>T</sub> > 500 MeV at √s = 13 TeV. Statistical uncertainties for √χ<sup>2</sup>/ndf>1 are corrected by the √χ<sup>2</sup>/ndf. The total uncertainties are shown.
The correlation strength, λ, and source radius, R, of the exponential fits to the two-particle double-ratio correlation functions, R<sub>2</sub>(Q), in dependence on the pair transverse momentum, k<sub>T</sub>, intervals for the minimum-bias (MB) and the high-multiplicity track (HMT) events for p<sub>T</sub> > 100 MeV at √s = 13 TeV. Statistical uncertainties for √χ<sup>2</sup>/ndf>1 are corrected by the √χ<sup>2</sup>/ndf. The total uncertainties are shown.
The correlation strength, λ, and source radius, R, of the exponential fits to the two-particle double-ratio correlation functions, R<sub>2</sub>(Q), in dependence on the pair transverse momentum, k<sub>T</sub>, intervals for the minimum-bias (MB) and the high-multiplicity track (HMT) events for p<sub>T</sub> > 500 MeV at √s = 13 TeV. Statistical uncertainties for √χ<sup>2</sup>/ndf>1 are corrected by the √χ<sup>2</sup>/ndf. The total uncertainties are shown.
Measurements of Higgs boson production cross-sections are carried out in the diphoton decay channel using 139 fb$^{-1}$ of $pp$ collision data at $\sqrt{s} = 13$ TeV collected by the ATLAS experiment at the LHC. The analysis is based on the definition of 101 distinct signal regions using machine-learning techniques. The inclusive Higgs boson signal strength in the diphoton channel is measured to be $1.04^{+0.10}_{-0.09}$. Cross-sections for gluon-gluon fusion, vector-boson fusion, associated production with a $W$ or $Z$ boson, and top associated production processes are reported. An upper limit of 10 times the Standard Model prediction is set for the associated production process of a Higgs boson with a single top quark, which has a unique sensitivity to the sign of the top quark Yukawa coupling. Higgs boson production is further characterized through measurements of Simplified Template Cross-Sections (STXS). In total, cross-sections of 28 STXS regions are measured. The measured STXS cross-sections are compatible with their Standard Model predictions, with a $p$-value of $93\%$. The measurements are also used to set constraints on Higgs boson coupling strengths, as well as on new interactions beyond the Standard Model in an effective field theory approach. No significant deviations from the Standard Model predictions are observed in these measurements, which provide significant sensitivity improvements compared to the previous ATLAS results.
Cross-sections times H->yy branching ratio for ggF +bbH, VBF, VH, ttH, and tH production, normalized to their SM predictions. The values are obtained from a simultaneous fit to all categories. The theory uncertainties in the predictions include uncertainties due to missing higher-order terms in the perturbative QCD calculations and choices of parton distribution functions and value of alpha_s, as well as the H->yy branching ratio uncertainty.
Correlation matrix for the measurement of production cross-sections of the Higgs boson times the H->yy branching ratio.
Best-fit values and uncertainties for STXS parameters in each of the 28 regions considered, normalized to their SM predictions. The values for the gg->H process also include the contributions from bbH production.
Correlation matrix for the measurement of STXS parameters in each of the 28 regions considered.
Fitted values for kappa_g and kappa_y.
Correlation matrix for the measurement of kappa_g and kappa_y.
Summary of the 68% CL confidence intervals for individual measurements of SMEFT parameters observed in data. In each case, SMEFT parameters other than the one measured are fixed to 0.
Results of the EV parameter measurement in data, in the linear and linear+quadratic parameterizations of the SMEFT. All the EVs parameters are free to vary in the fits. The ranges correspond to 68% CL confidence intervals.
Observed linear correlation coefficients of the EVs parameters in the linear parameterization.
Observed linear correlation coefficients of the EVs parameters in the linear+quadratic parameterization.
Cross-sections times H->yy branching ratio for ggF +bbH, VBF, VH, ttH, and tH production. The values are obtained from a simultaneous fit to all categories. The theory uncertainties in the predictions include uncertainties due to missing higher-order terms in the perturbative QCD calculations and choices of parton distribution functions and value of alpha_s, as well as the H->yy branching ratio uncertainty.
Best-fit values and uncertainties for STXS parameters in each of the 28 regions considered. The values for the gg->H process also include the contributions from bbH production.
Correlation matrix for the measurement of STXS parameters in each of the 33 regions considered.
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