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A search for the production of heavy partners of the top quark with charge 5/3 is performed in events with a pair of same-sign leptons. The data sample corresponds to an integrated luminosity of 19.5 inverse femtobarns and was collected at sqrt(s) = 8 TeV by the CMS experiment. No significant excess is observed in the data above the expected background and the existence of top-quark partners with masses below 800 GeV is excluded at a 95% confidence level, assuming they decay exclusively to tW. This is the first limit on these particles from the LHC, and it is significantly more restrictive than previous limits.
A search is presented for fractionally charged particles with charge below 1$e$, using their small energy loss in the tracking detector as a key variable to observe a signal. The analyzed data set corresponds to an integrated luminosity of 138 fb$^{-1}$ of proton-proton collisions collected at $\sqrt{s}$ = 13 TeV in 2016-2018 at the CERN LHC. This is the first search at the LHC for new particles with charges between $e/$3 and 0.9$e$, including an extension of previous results at a charge of 2$e/$3. Masses up to 640 GeV and charges as low as $e/$3 are excluded at 95% confidence level. These are the most stringent limits to date for the considered Drell-Yan-like production mode.
This paper presents a search for pair production of higgsinos, the supersymmetric partners of the Higgs bosons, in scenarios with gauge-mediated supersymmetry breaking. Each higgsino is assumed to decay into a Higgs boson and a nearly massless gravitino. The search targets events where each Higgs boson decays into $b\bar{b}$, leading to a reconstructed final state with at least three energetic $b$-jets and This paper presents a search for pair production of higgsinos, the supersymmetric partners of the Higgs bosons, in scenarios with gauge-mediated supersymmetry breaking. Each higgsino is assumed to decay into a Higgs boson and a nearly massless gravitino. The search targets events where each Higgs boson decays into $b\bar{b}$, leading to a reconstructed final state with at least three energetic $b$-jets and missing transverse momentum. Two complementary analysis channels are used, with each channel specifically targeting either low or high values of the higgsino mass. The low-mass (high-mass) channel exploits 126 (139) fb$^{-1}$ of $\sqrt{s}=13$ TeV data collected by the ATLAS detector during Run 2 of the Large Hadron Collider. No significant excess above the Standard Model prediction is found. At 95% confidence level, masses between 130 GeV and 940 GeV are excluded for higgsinos decaying exclusively into Higgs bosons and gravitinos. Exclusion limits as a function of the higgsino decay branching ratio to a Higgs boson are also reported.
Higgsinos with masses near the electroweak scale can solve the hierarchy problem and provide a dark matter candidate, while detecting them at the LHC remains challenging if their mass splitting is $\mathcal{O}(1 \text{GeV})$. This Letter presents a novel search for nearly mass-degenerate Higgsinos in events with an energetic jet, missing transverse momentum, and a low-momentum track with a significant transverse impact parameter using 140 fb$^{-1}$ of proton-proton collision data at $\sqrt{s}=13$ TeV collected by the ATLAS experiment. For the first time since LEP, a range of mass splittings between the lightest charged and neutral Higgsinos from $0.3$ GeV to $0.9$ GeV is excluded at 95$\%$ confidence level, with a maximum reach of approximately $170$ GeV in the Higgsino mass.
This paper presents a search for new physics through the process where a new massive particle, X, decays into a Higgs boson and a second particle, Y. The Higgs boson subsequently decays into a bottom quark-antiquark pair, reconstructed as a single large-radius jet. The decay products of Y are also assumed to produce a single large-radius jet. The identification of the Y particle is enhanced by computing the anomaly score of its candidate jet using an autoencoder, which measures deviations from typical QCD multijet jets. This allows a simultaneous search for multiple Y decay scenarios within a single analysis. In the main benchmark process, Y is a scalar particle that decays into W$^+$W$^-$. Two other benchmark processes are also considered, where Y is a scalar particle decaying into a light quark-antiquark pair, or into a top quark-antiquark pair. The last benchmark considers Y as a hadronically decaying top quark, arising from the decay of a vector-like quark into a top quark and a Higgs boson. Data recorded by the CMS experiment at a center-of-mass energy of 13 TeV in 2016$-$2018, and corresponding to an integrated luminosity of 138 fb$^{-1}$, are analyzed. No significant excess is observed, and upper limits on the benchmark signal cross section for various masses of X and Y, at 95% confidence level, are placed.
The expected and observed 95% confidence level upper limits on the cross section $\sigma(\mathrm{pp} \to \mathrm{X} \to (\mathrm{H} \to b\bar{b})(\mathrm{Y} \to WW \to 4q))$ are shown for different values of $M_X$ and $M_Y$. The limits have been evaluated in discrete steps corresponding to the centers of the boxes. The numbers in the boxes are given in fb. In addition to the observed and median expected limits, the expected limits at $\pm1\sigma$ and $\pm2\sigma$ quantiles are also provided. These represent the regions containing 68% and 95%, respectively, of the distribution of limits expected under the background-only hypothesis.
Single- and double-differential cross-section measurements are presented for the production of top-quark pairs, in the lepton + jets channel at particle and parton level. Two topologies, resolved and boosted, are considered and the results are presented as a function of several kinematic variables characterising the top and $t\bar{t}$ system and jet multiplicities. The study was performed using data from $pp$ collisions at centre-of-mass energy of 13 TeV collected in 2015 and 2016 by the ATLAS detector at the CERN Large Hadron Collider (LHC), corresponding to an integrated luminosity of $36~\mathrm{fb}^{-1}$. Due to the large $t\bar{t}$ cross-section at the LHC, such measurements allow a detailed study of the properties of top-quark production and decay, enabling precision tests of several Monte Carlo generators and fixed-order Standard Model predictions. Overall, there is good agreement between the theoretical predictions and the data.
Relative differential cross-section as a function of $p_{T}^{t,had}$ at particle level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Relative differential cross-section as function of $p_{T}^{t,had}$ at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Absolute differential cross-section as a function of $p_{T}^{t,had}$ at particle level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Relative differential cross-section as a function of $|y^{t,had}|$ at particle level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Relative differential cross-section as function of $|y^{t,had}|$ at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Absolute differential cross-section as a function of $|y^{t,had}|$ at particle level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Absolute differential cross-section as function of $|y^{t,had}|$ at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Relative differential cross-section as a function of $p_{T}^{t,1}$ at particle level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Relative differential cross-section as function of $p_{T}^{t,1}$ at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Absolute differential cross-section as a function of $p_{T}^{t,1}$ at particle level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Absolute differential cross-section as function of $p_{T}^{t,1}$ at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Relative differential cross-section as a function of $p_{T}^{t,2}$ at particle level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Relative differential cross-section as function of $p_{T}^{t,2}$ at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Absolute differential cross-section as a function of $p_{T}^{t,2}$ at particle level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Absolute differential cross-section as function of $p_{T}^{t,2}$ at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Relative differential cross-section as a function of $m^{t\bar{t}}$ at particle level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Relative differential cross-section as function of $m^{t\bar{t}}$ at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Absolute differential cross-section as a function of $m^{t\bar{t}}$ at particle level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Absolute differential cross-section as function of $m^{t\bar{t}}$ at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Relative differential cross-section as a function of $p_{T}^{t\bar{t}}$ at particle level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Relative differential cross-section as function of $p_{T}^{t\bar{t}}$ at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Absolute differential cross-section as a function of $p_{T}^{t\bar{t}}$ at particle level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Relative differential cross-section as a function of $|p_{out}^{t,had}|$ at particle level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Relative differential cross-section as function of $|p_{out}^{t,had}|$ at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Absolute differential cross-section as a function of $|p_{out}^{t,had}|$ at particle level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Absolute differential cross-section as function of $|p_{out}^{t,had}|$ at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Relative differential cross-section as a function of $|\Delta\phi(t,\bar{t})|$ at particle level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Relative differential cross-section as function of $|\Delta\phi(t,\bar{t})|$ at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Absolute differential cross-section as a function of $|\Delta\phi(t,\bar{t})|$ at particle level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Absolute differential cross-section as function of $|\Delta\phi(t,\bar{t})|$ at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Relative differential cross-section as a function of $H_{T}^{t\bar{t}}$ at particle level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Relative differential cross-section as function of $H_{T}^{t\bar{t}}$ at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Absolute differential cross-section as a function of $H_{T}^{t\bar{t}}$ at particle level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Relative differential cross-section as a function of $N^{extra jets}$ at particle level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Relative differential cross-section as function of $N^{extra jets}$ at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Absolute differential cross-section as a function of $N^{extra jets}$ at particle level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Absolute differential cross-section as function of $N^{extra jets}$ at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Relative differential cross-section as a function of $|y^{t\bar{t}}|$ at particle level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Relative differential cross-section as function of $|y^{t\bar{t}}|$ at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Absolute differential cross-section as a function of $|y^{t\bar{t}}|$ at particle level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Absolute differential cross-section as function of $|y^{t\bar{t}}|$ at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Relative differential cross-section as a function of $|y_{boost}^{t\bar{t}}|$ at particle level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Relative differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Absolute differential cross-section as a function of $|y_{boost}^{t\bar{t}}|$ at particle level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Relative differential cross-section as a function of $\chi^{t\bar{t}}$ at particle level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Relative differential cross-section as function of $\chi^{t\bar{t}}$ at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Absolute differential cross-section as a function of $\chi^{t\bar{t}}$ at particle level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Absolute differential cross-section as function of $\chi^{t\bar{t}}$ at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Total cross-section at particle level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ at particle level in the resolved topology in 200.0 GeV < $m^{t\bar{t}}$ < 400.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ at particle level in the resolved topology in 400.0 GeV < $m^{t\bar{t}}$ < 550.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ at particle level in the resolved topology in 550.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ at particle level in the resolved topology in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ at particle level in the resolved topology in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 200.0 GeV < $m^{t\bar{t}}$ < 400.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 200.0 GeV < $m^{t\bar{t}}$ < 400.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 400.0 GeV < $m^{t\bar{t}}$ < 550.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 200.0 GeV < $m^{t\bar{t}}$ < 400.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 400.0 GeV < $m^{t\bar{t}}$ < 550.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 400.0 GeV < $m^{t\bar{t}}$ < 550.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 550.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 200.0 GeV < $m^{t\bar{t}}$ < 400.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 550.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 400.0 GeV < $m^{t\bar{t}}$ < 550.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 550.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 550.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 200.0 GeV < $m^{t\bar{t}}$ < 400.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 400.0 GeV < $m^{t\bar{t}}$ < 550.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 550.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 200.0 GeV < $m^{t\bar{t}}$ < 400.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 400.0 GeV < $m^{t\bar{t}}$ < 550.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 550.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Absolute double-differential cross-section as a function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ at particle level in the resolved topology in 200.0 GeV < $m^{t\bar{t}}$ < 400.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ at particle level in the resolved topology in 400.0 GeV < $m^{t\bar{t}}$ < 550.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ at particle level in the resolved topology in 550.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ at particle level in the resolved topology in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ at particle level in the resolved topology in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 200.0 GeV < $m^{t\bar{t}}$ < 400.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 200.0 GeV < $m^{t\bar{t}}$ < 400.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 400.0 GeV < $m^{t\bar{t}}$ < 550.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 200.0 GeV < $m^{t\bar{t}}$ < 400.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 400.0 GeV < $m^{t\bar{t}}$ < 550.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 400.0 GeV < $m^{t\bar{t}}$ < 550.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 550.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 200.0 GeV < $m^{t\bar{t}}$ < 400.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 550.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 400.0 GeV < $m^{t\bar{t}}$ < 550.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 550.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 550.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 200.0 GeV < $m^{t\bar{t}}$ < 400.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 400.0 GeV < $m^{t\bar{t}}$ < 550.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 550.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 200.0 GeV < $m^{t\bar{t}}$ < 400.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 400.0 GeV < $m^{t\bar{t}}$ < 550.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 550.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Relative double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ at particle level in the resolved topology in 200.0 GeV < $m^{t\bar{t}}$ < 400.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ at particle level in the resolved topology in 400.0 GeV < $m^{t\bar{t}}$ < 550.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ at particle level in the resolved topology in 550.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ at particle level in the resolved topology in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ at particle level in the resolved topology in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 200.0 GeV < $m^{t\bar{t}}$ < 400.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 200.0 GeV < $m^{t\bar{t}}$ < 400.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 400.0 GeV < $m^{t\bar{t}}$ < 550.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 200.0 GeV < $m^{t\bar{t}}$ < 400.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 400.0 GeV < $m^{t\bar{t}}$ < 550.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 400.0 GeV < $m^{t\bar{t}}$ < 550.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 550.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 200.0 GeV < $m^{t\bar{t}}$ < 400.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 550.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 400.0 GeV < $m^{t\bar{t}}$ < 550.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 550.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 550.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 200.0 GeV < $m^{t\bar{t}}$ < 400.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 400.0 GeV < $m^{t\bar{t}}$ < 550.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 550.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 200.0 GeV < $m^{t\bar{t}}$ < 400.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 400.0 GeV < $m^{t\bar{t}}$ < 550.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 550.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Absolute double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ at particle level in the resolved topology in 200.0 GeV < $m^{t\bar{t}}$ < 400.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ at particle level in the resolved topology in 400.0 GeV < $m^{t\bar{t}}$ < 550.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ at particle level in the resolved topology in 550.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ at particle level in the resolved topology in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ at particle level in the resolved topology in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 200.0 GeV < $m^{t\bar{t}}$ < 400.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 200.0 GeV < $m^{t\bar{t}}$ < 400.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 400.0 GeV < $m^{t\bar{t}}$ < 550.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 200.0 GeV < $m^{t\bar{t}}$ < 400.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 400.0 GeV < $m^{t\bar{t}}$ < 550.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 400.0 GeV < $m^{t\bar{t}}$ < 550.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 550.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 200.0 GeV < $m^{t\bar{t}}$ < 400.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 550.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 400.0 GeV < $m^{t\bar{t}}$ < 550.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 550.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 550.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 200.0 GeV < $m^{t\bar{t}}$ < 400.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 400.0 GeV < $m^{t\bar{t}}$ < 550.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 550.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 200.0 GeV < $m^{t\bar{t}}$ < 400.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 400.0 GeV < $m^{t\bar{t}}$ < 550.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 550.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Relative double-differential cross-section as a function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ at particle level in the resolved topology in 0.0 GeV < $p_{T}^{t,had}$ < 60.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ at particle level in the resolved topology in 60.0 GeV < $p_{T}^{t,had}$ < 120.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ at particle level in the resolved topology in 120.0 GeV < $p_{T}^{t,had}$ < 200.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ at particle level in the resolved topology in 200.0 GeV < $p_{T}^{t,had}$ < 300.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ at particle level in the resolved topology in 300.0 GeV < $p_{T}^{t,had}$ < 1000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 0.0 GeV < $p_{T}^{t,had}$ < 60.0 GeV and the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 0.0 GeV < $p_{T}^{t,had}$ < 60.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 60.0 GeV < $p_{T}^{t,had}$ < 120.0 GeV and the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 0.0 GeV < $p_{T}^{t,had}$ < 60.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 60.0 GeV < $p_{T}^{t,had}$ < 120.0 GeV and the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 60.0 GeV < $p_{T}^{t,had}$ < 120.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 120.0 GeV < $p_{T}^{t,had}$ < 200.0 GeV and the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 0.0 GeV < $p_{T}^{t,had}$ < 60.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 120.0 GeV < $p_{T}^{t,had}$ < 200.0 GeV and the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 60.0 GeV < $p_{T}^{t,had}$ < 120.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 120.0 GeV < $p_{T}^{t,had}$ < 200.0 GeV and the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 120.0 GeV < $p_{T}^{t,had}$ < 200.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 200.0 GeV < $p_{T}^{t,had}$ < 300.0 GeV and the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 0.0 GeV < $p_{T}^{t,had}$ < 60.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 200.0 GeV < $p_{T}^{t,had}$ < 300.0 GeV and the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 60.0 GeV < $p_{T}^{t,had}$ < 120.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 200.0 GeV < $p_{T}^{t,had}$ < 300.0 GeV and the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 120.0 GeV < $p_{T}^{t,had}$ < 200.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 200.0 GeV < $p_{T}^{t,had}$ < 300.0 GeV and the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 200.0 GeV < $p_{T}^{t,had}$ < 300.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 300.0 GeV < $p_{T}^{t,had}$ < 1000.0 GeV and the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 0.0 GeV < $p_{T}^{t,had}$ < 60.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 300.0 GeV < $p_{T}^{t,had}$ < 1000.0 GeV and the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 60.0 GeV < $p_{T}^{t,had}$ < 120.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 300.0 GeV < $p_{T}^{t,had}$ < 1000.0 GeV and the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 120.0 GeV < $p_{T}^{t,had}$ < 200.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 300.0 GeV < $p_{T}^{t,had}$ < 1000.0 GeV and the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 200.0 GeV < $p_{T}^{t,had}$ < 300.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 300.0 GeV < $p_{T}^{t,had}$ < 1000.0 GeV and the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 300.0 GeV < $p_{T}^{t,had}$ < 1000.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Absolute double-differential cross-section as a function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ at particle level in the resolved topology in 0.0 GeV < $p_{T}^{t,had}$ < 60.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ at particle level in the resolved topology in 60.0 GeV < $p_{T}^{t,had}$ < 120.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ at particle level in the resolved topology in 120.0 GeV < $p_{T}^{t,had}$ < 200.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ at particle level in the resolved topology in 200.0 GeV < $p_{T}^{t,had}$ < 300.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ at particle level in the resolved topology in 300.0 GeV < $p_{T}^{t,had}$ < 1000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 0.0 GeV < $p_{T}^{t,had}$ < 60.0 GeV and the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 0.0 GeV < $p_{T}^{t,had}$ < 60.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 60.0 GeV < $p_{T}^{t,had}$ < 120.0 GeV and the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 0.0 GeV < $p_{T}^{t,had}$ < 60.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 60.0 GeV < $p_{T}^{t,had}$ < 120.0 GeV and the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 60.0 GeV < $p_{T}^{t,had}$ < 120.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 120.0 GeV < $p_{T}^{t,had}$ < 200.0 GeV and the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 0.0 GeV < $p_{T}^{t,had}$ < 60.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 120.0 GeV < $p_{T}^{t,had}$ < 200.0 GeV and the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 60.0 GeV < $p_{T}^{t,had}$ < 120.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 120.0 GeV < $p_{T}^{t,had}$ < 200.0 GeV and the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 120.0 GeV < $p_{T}^{t,had}$ < 200.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 200.0 GeV < $p_{T}^{t,had}$ < 300.0 GeV and the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 0.0 GeV < $p_{T}^{t,had}$ < 60.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 200.0 GeV < $p_{T}^{t,had}$ < 300.0 GeV and the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 60.0 GeV < $p_{T}^{t,had}$ < 120.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 200.0 GeV < $p_{T}^{t,had}$ < 300.0 GeV and the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 120.0 GeV < $p_{T}^{t,had}$ < 200.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 200.0 GeV < $p_{T}^{t,had}$ < 300.0 GeV and the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 200.0 GeV < $p_{T}^{t,had}$ < 300.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 300.0 GeV < $p_{T}^{t,had}$ < 1000.0 GeV and the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 0.0 GeV < $p_{T}^{t,had}$ < 60.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 300.0 GeV < $p_{T}^{t,had}$ < 1000.0 GeV and the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 60.0 GeV < $p_{T}^{t,had}$ < 120.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 300.0 GeV < $p_{T}^{t,had}$ < 1000.0 GeV and the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 120.0 GeV < $p_{T}^{t,had}$ < 200.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 300.0 GeV < $p_{T}^{t,had}$ < 1000.0 GeV and the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 200.0 GeV < $p_{T}^{t,had}$ < 300.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 300.0 GeV < $p_{T}^{t,had}$ < 1000.0 GeV and the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 300.0 GeV < $p_{T}^{t,had}$ < 1000.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Relative double-differential cross-section as a function of $p_{T}^{t,had}$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ = 4.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t,had}$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ = 5.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t,had}$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ = 6.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t,had}$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ $\geq$ 7.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Absolute double-differential cross-section as a function of $p_{T}^{t,had}$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ = 4.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t,had}$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ = 5.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t,had}$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ = 6.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t,had}$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ $\geq$ 7.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Relative double-differential cross-section as a function of $m^{t\bar{t}}$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ = 4.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $m^{t\bar{t}}$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ = 5.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $m^{t\bar{t}}$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ $\geq$ 6.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 6.0 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 6.0 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 6.0 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 6.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Absolute double-differential cross-section as a function of $m^{t\bar{t}}$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ = 4.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $m^{t\bar{t}}$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ = 5.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $m^{t\bar{t}}$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ $\geq$ 6.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 6.0 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 6.0 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 6.0 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 6.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Relative double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ = 4.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ = 5.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ = 6.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ $\geq$ 7.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Absolute double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ = 4.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ = 5.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ = 6.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ $\geq$ 7.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Relative double-differential cross-section as a function of $|p_{out}^{t,had}|$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ = 4.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $|p_{out}^{t,had}|$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ = 5.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $|p_{out}^{t,had}|$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ = 6.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $|p_{out}^{t,had}|$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ $\geq$ 7.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 and the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 5.0 and the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 5.0 and the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 6.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 6.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Absolute double-differential cross-section as a function of $|p_{out}^{t,had}|$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ = 4.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $|p_{out}^{t,had}|$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ = 5.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $|p_{out}^{t,had}|$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ = 6.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $|p_{out}^{t,had}|$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ $\geq$ 7.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 and the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 5.0 and the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 5.0 and the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 6.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 6.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Relative double-differential cross-section as a function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ at particle level in the resolved topology in 3.5 < $N^{jets}$ < 4.5 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ at particle level in the resolved topology in 4.5 < $N^{jets}$ < 5.5 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ at particle level in the resolved topology in 5.5 < $N^{jets}$ < 6.5 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ at particle level in the resolved topology in 6.5 < $N^{jets}$ < 7.5 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Relative double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 3.5 < $N^{jets}$ < 4.5 and the Relative double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 3.5 < $N^{jets}$ < 4.5 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 4.5 < $N^{jets}$ < 5.5 and the Relative double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 3.5 < $N^{jets}$ < 4.5 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 4.5 < $N^{jets}$ < 5.5 and the Relative double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 4.5 < $N^{jets}$ < 5.5 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 5.5 < $N^{jets}$ < 6.5 and the Relative double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 3.5 < $N^{jets}$ < 4.5 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 5.5 < $N^{jets}$ < 6.5 and the Relative double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 4.5 < $N^{jets}$ < 5.5 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 5.5 < $N^{jets}$ < 6.5 and the Relative double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 5.5 < $N^{jets}$ < 6.5 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 6.5 < $N^{jets}$ < 7.5 and the Relative double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 3.5 < $N^{jets}$ < 4.5 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 6.5 < $N^{jets}$ < 7.5 and the Relative double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 4.5 < $N^{jets}$ < 5.5 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 6.5 < $N^{jets}$ < 7.5 and the Relative double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 5.5 < $N^{jets}$ < 6.5 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 6.5 < $N^{jets}$ < 7.5 and the Relative double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 6.5 < $N^{jets}$ < 7.5 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Absolute double-differential cross-section as a function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ at particle level in the resolved topology in 3.5 < $N^{jets}$ < 4.5 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ at particle level in the resolved topology in 4.5 < $N^{jets}$ < 5.5 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ at particle level in the resolved topology in 5.5 < $N^{jets}$ < 6.5 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ at particle level in the resolved topology in 6.5 < $N^{jets}$ < 7.5 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Absolute double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 3.5 < $N^{jets}$ < 4.5 and the Absolute double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 3.5 < $N^{jets}$ < 4.5 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 4.5 < $N^{jets}$ < 5.5 and the Absolute double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 3.5 < $N^{jets}$ < 4.5 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 4.5 < $N^{jets}$ < 5.5 and the Absolute double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 4.5 < $N^{jets}$ < 5.5 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 5.5 < $N^{jets}$ < 6.5 and the Absolute double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 3.5 < $N^{jets}$ < 4.5 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 5.5 < $N^{jets}$ < 6.5 and the Absolute double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 4.5 < $N^{jets}$ < 5.5 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 5.5 < $N^{jets}$ < 6.5 and the Absolute double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 5.5 < $N^{jets}$ < 6.5 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 6.5 < $N^{jets}$ < 7.5 and the Absolute double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 3.5 < $N^{jets}$ < 4.5 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 6.5 < $N^{jets}$ < 7.5 and the Absolute double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 4.5 < $N^{jets}$ < 5.5 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 6.5 < $N^{jets}$ < 7.5 and the Absolute double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 5.5 < $N^{jets}$ < 6.5 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 6.5 < $N^{jets}$ < 7.5 and the Absolute double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 6.5 < $N^{jets}$ < 7.5 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Relative double-differential cross-section as a function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ = 4.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ = 5.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ = 6.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ $\geq$ 7.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Relative double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 and the Relative double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 and the Relative double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 and the Relative double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Relative double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Relative double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Relative double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Relative double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Relative double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Relative double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Relative double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Absolute double-differential cross-section as a function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ = 4.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ = 5.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ = 6.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ $\geq$ 7.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Absolute double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 and the Absolute double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 and the Absolute double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 and the Absolute double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Absolute double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Absolute double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Absolute double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Absolute double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Absolute double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Absolute double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Absolute double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Relative double-differential cross-section as a function of $|y^{t,had}|$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ = 4.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $|y^{t,had}|$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ = 5.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $|y^{t,had}|$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ = 6.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $|y^{t,had}|$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ $\geq$ 7.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Relative double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 and the Relative double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 5.0 and the Relative double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 5.0 and the Relative double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Relative double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Relative double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Relative double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 6.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Relative double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Relative double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Relative double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 6.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Relative double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Absolute double-differential cross-section as a function of $|y^{t,had}|$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ = 4.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $|y^{t,had}|$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ = 5.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $|y^{t,had}|$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ = 6.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $|y^{t,had}|$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ $\geq$ 7.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Absolute double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 and the Absolute double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 5.0 and the Absolute double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 5.0 and the Absolute double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Absolute double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Absolute double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Absolute double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 6.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Absolute double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Absolute double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Absolute double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 6.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Absolute double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Relative double-differential cross-section as a function of $|y^{t\bar{t}}|$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ = 4.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $|y^{t\bar{t}}|$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ = 5.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $|y^{t\bar{t}}|$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ = 6.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $|y^{t\bar{t}}|$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ $\geq$ 7.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 and the Relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ = 5.0 and the Relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ = 5.0 and the Relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ = 6.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ = 6.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Absolute double-differential cross-section as a function of $|y^{t\bar{t}}|$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ = 4.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $|y^{t\bar{t}}|$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ = 5.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $|y^{t\bar{t}}|$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ = 6.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $|y^{t\bar{t}}|$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ $\geq$ 7.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 and the Absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ = 5.0 and the Absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ = 5.0 and the Absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ = 6.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ = 6.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Relative double-differential cross-section as a function of $\chi_{tt}$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ = 4.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $\chi_{tt}$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ = 5.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $\chi_{tt}$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ = 6.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $\chi_{tt}$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ $\geq$ 7.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Relative double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 and the Relative double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 and the Relative double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 and the Relative double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Relative double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Relative double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Relative double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Relative double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Relative double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Relative double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Relative double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Absolute double-differential cross-section as a function of $\chi_{tt}$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ = 4.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $\chi_{tt}$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ = 5.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $\chi_{tt}$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ = 6.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $\chi_{tt}$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ $\geq$ 7.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Absolute double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 and the Absolute double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 and the Absolute double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 and the Absolute double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Absolute double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Absolute double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Absolute double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Absolute double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Absolute double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Absolute double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Absolute double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Relative double-differential cross-section as a function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ at particle level in the resolved topology in 0.0 < $|y^{t,had}|$ < 0.7 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ at particle level in the resolved topology in 0.7 < $|y^{t,had}|$ < 1.4 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ at particle level in the resolved topology in 1.4 < $|y^{t,had}|$ < 2.5 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 0.0 < $|y^{t,had}|$ < 0.7 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 0.0 < $|y^{t,had}|$ < 0.7 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 0.7 < $|y^{t,had}|$ < 1.4 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 0.0 < $|y^{t,had}|$ < 0.7 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 0.7 < $|y^{t,had}|$ < 1.4 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 0.7 < $|y^{t,had}|$ < 1.4 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 1.4 < $|y^{t,had}|$ < 2.5 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 0.0 < $|y^{t,had}|$ < 0.7 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 1.4 < $|y^{t,had}|$ < 2.5 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 0.7 < $|y^{t,had}|$ < 1.4 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 1.4 < $|y^{t,had}|$ < 2.5 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 1.4 < $|y^{t,had}|$ < 2.5 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Absolute double-differential cross-section as a function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ at particle level in the resolved topology in 0.0 < $|y^{t,had}|$ < 0.7 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ at particle level in the resolved topology in 0.7 < $|y^{t,had}|$ < 1.4 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ at particle level in the resolved topology in 1.4 < $|y^{t,had}|$ < 2.5 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 0.0 < $|y^{t,had}|$ < 0.7 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 0.0 < $|y^{t,had}|$ < 0.7 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 0.7 < $|y^{t,had}|$ < 1.4 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 0.0 < $|y^{t,had}|$ < 0.7 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 0.7 < $|y^{t,had}|$ < 1.4 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 0.7 < $|y^{t,had}|$ < 1.4 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 1.4 < $|y^{t,had}|$ < 2.5 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 0.0 < $|y^{t,had}|$ < 0.7 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 1.4 < $|y^{t,had}|$ < 2.5 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 0.7 < $|y^{t,had}|$ < 1.4 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 1.4 < $|y^{t,had}|$ < 2.5 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 1.4 < $|y^{t,had}|$ < 2.5 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Relative double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ at particle level in the resolved topology in 0.0 < $|y^{t\bar{t}}|$ < 0.4 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ at particle level in the resolved topology in 0.4 < $|y^{t\bar{t}}|$ < 0.8 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ at particle level in the resolved topology in 0.8 < $|y^{t\bar{t}}|$ < 1.2 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ at particle level in the resolved topology in 1.2 < $|y^{t\bar{t}}|$ < 2.5 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.4 and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.4 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.4 < $|y^{t\bar{t}}|$ < 0.8 and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.4 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.4 < $|y^{t\bar{t}}|$ < 0.8 and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.4 < $|y^{t\bar{t}}|$ < 0.8 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.8 < $|y^{t\bar{t}}|$ < 1.2 and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.4 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.8 < $|y^{t\bar{t}}|$ < 1.2 and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.4 < $|y^{t\bar{t}}|$ < 0.8 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.8 < $|y^{t\bar{t}}|$ < 1.2 and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.8 < $|y^{t\bar{t}}|$ < 1.2 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.2 < $|y^{t\bar{t}}|$ < 2.5 and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.4 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.2 < $|y^{t\bar{t}}|$ < 2.5 and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.4 < $|y^{t\bar{t}}|$ < 0.8 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.2 < $|y^{t\bar{t}}|$ < 2.5 and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.8 < $|y^{t\bar{t}}|$ < 1.2 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.2 < $|y^{t\bar{t}}|$ < 2.5 and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.2 < $|y^{t\bar{t}}|$ < 2.5 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Absolute double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ at particle level in the resolved topology in 0.0 < $|y^{t\bar{t}}|$ < 0.4 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ at particle level in the resolved topology in 0.4 < $|y^{t\bar{t}}|$ < 0.8 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ at particle level in the resolved topology in 0.8 < $|y^{t\bar{t}}|$ < 1.2 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ at particle level in the resolved topology in 1.2 < $|y^{t\bar{t}}|$ < 2.5 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.4 and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.4 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.4 < $|y^{t\bar{t}}|$ < 0.8 and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.4 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.4 < $|y^{t\bar{t}}|$ < 0.8 and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.4 < $|y^{t\bar{t}}|$ < 0.8 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.8 < $|y^{t\bar{t}}|$ < 1.2 and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.4 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.8 < $|y^{t\bar{t}}|$ < 1.2 and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.4 < $|y^{t\bar{t}}|$ < 0.8 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.8 < $|y^{t\bar{t}}|$ < 1.2 and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.8 < $|y^{t\bar{t}}|$ < 1.2 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.2 < $|y^{t\bar{t}}|$ < 2.5 and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.4 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.2 < $|y^{t\bar{t}}|$ < 2.5 and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.4 < $|y^{t\bar{t}}|$ < 0.8 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.2 < $|y^{t\bar{t}}|$ < 2.5 and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.8 < $|y^{t\bar{t}}|$ < 1.2 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.2 < $|y^{t\bar{t}}|$ < 2.5 and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.2 < $|y^{t\bar{t}}|$ < 2.5 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Relative double-differential cross-section as a function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ at particle level in the resolved topology in 0.0 < $|y^{t\bar{t}}|$ < 0.4 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ at particle level in the resolved topology in 0.4 < $|y^{t\bar{t}}|$ < 0.8 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ at particle level in the resolved topology in 0.8 < $|y^{t\bar{t}}|$ < 1.2 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ at particle level in the resolved topology in 1.2 < $|y^{t\bar{t}}|$ < 2.5 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.4 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.4 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.4 < $|y^{t\bar{t}}|$ < 0.8 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.4 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.4 < $|y^{t\bar{t}}|$ < 0.8 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.4 < $|y^{t\bar{t}}|$ < 0.8 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.8 < $|y^{t\bar{t}}|$ < 1.2 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.4 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.8 < $|y^{t\bar{t}}|$ < 1.2 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.4 < $|y^{t\bar{t}}|$ < 0.8 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.8 < $|y^{t\bar{t}}|$ < 1.2 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.8 < $|y^{t\bar{t}}|$ < 1.2 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.2 < $|y^{t\bar{t}}|$ < 2.5 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.4 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.2 < $|y^{t\bar{t}}|$ < 2.5 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.4 < $|y^{t\bar{t}}|$ < 0.8 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.2 < $|y^{t\bar{t}}|$ < 2.5 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.8 < $|y^{t\bar{t}}|$ < 1.2 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.2 < $|y^{t\bar{t}}|$ < 2.5 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.2 < $|y^{t\bar{t}}|$ < 2.5 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Absolute double-differential cross-section as a function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ at particle level in the resolved topology in 0.0 < $|y^{t\bar{t}}|$ < 0.4 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ at particle level in the resolved topology in 0.4 < $|y^{t\bar{t}}|$ < 0.8 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ at particle level in the resolved topology in 0.8 < $|y^{t\bar{t}}|$ < 1.2 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ at particle level in the resolved topology in 1.2 < $|y^{t\bar{t}}|$ < 2.5 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.4 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.4 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.4 < $|y^{t\bar{t}}|$ < 0.8 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.4 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.4 < $|y^{t\bar{t}}|$ < 0.8 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.4 < $|y^{t\bar{t}}|$ < 0.8 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.8 < $|y^{t\bar{t}}|$ < 1.2 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.4 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.8 < $|y^{t\bar{t}}|$ < 1.2 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.4 < $|y^{t\bar{t}}|$ < 0.8 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.8 < $|y^{t\bar{t}}|$ < 1.2 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.8 < $|y^{t\bar{t}}|$ < 1.2 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.2 < $|y^{t\bar{t}}|$ < 2.5 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.4 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.2 < $|y^{t\bar{t}}|$ < 2.5 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.4 < $|y^{t\bar{t}}|$ < 0.8 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.2 < $|y^{t\bar{t}}|$ < 2.5 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.8 < $|y^{t\bar{t}}|$ < 1.2 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.2 < $|y^{t\bar{t}}|$ < 2.5 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.2 < $|y^{t\bar{t}}|$ < 2.5 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Relative double-differential cross-section as a function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ at particle level in the resolved topology in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 30.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ at particle level in the resolved topology in 30.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ at particle level in the resolved topology in 80.0 GeV < $p_{T}^{t\bar{t}}$ < 190.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ at particle level in the resolved topology in 190.0 GeV < $p_{T}^{t\bar{t}}$ < 800.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 30.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 30.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 30.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 30.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 30.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 30.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 80.0 GeV < $p_{T}^{t\bar{t}}$ < 190.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 30.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 80.0 GeV < $p_{T}^{t\bar{t}}$ < 190.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 30.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 80.0 GeV < $p_{T}^{t\bar{t}}$ < 190.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 80.0 GeV < $p_{T}^{t\bar{t}}$ < 190.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 190.0 GeV < $p_{T}^{t\bar{t}}$ < 800.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 30.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 190.0 GeV < $p_{T}^{t\bar{t}}$ < 800.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 30.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 190.0 GeV < $p_{T}^{t\bar{t}}$ < 800.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 80.0 GeV < $p_{T}^{t\bar{t}}$ < 190.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 190.0 GeV < $p_{T}^{t\bar{t}}$ < 800.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 190.0 GeV < $p_{T}^{t\bar{t}}$ < 800.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Absolute double-differential cross-section as a function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ at particle level in the resolved topology in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 30.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ at particle level in the resolved topology in 30.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ at particle level in the resolved topology in 80.0 GeV < $p_{T}^{t\bar{t}}$ < 190.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ at particle level in the resolved topology in 190.0 GeV < $p_{T}^{t\bar{t}}$ < 800.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 30.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 30.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 30.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 30.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 30.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 30.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 80.0 GeV < $p_{T}^{t\bar{t}}$ < 190.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 30.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 80.0 GeV < $p_{T}^{t\bar{t}}$ < 190.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 30.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 80.0 GeV < $p_{T}^{t\bar{t}}$ < 190.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 80.0 GeV < $p_{T}^{t\bar{t}}$ < 190.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 190.0 GeV < $p_{T}^{t\bar{t}}$ < 800.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 30.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 190.0 GeV < $p_{T}^{t\bar{t}}$ < 800.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 30.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 190.0 GeV < $p_{T}^{t\bar{t}}$ < 800.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 80.0 GeV < $p_{T}^{t\bar{t}}$ < 190.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 190.0 GeV < $p_{T}^{t\bar{t}}$ < 800.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 190.0 GeV < $p_{T}^{t\bar{t}}$ < 800.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t,had}$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t,had}|$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t,had}|$ and the absolute differential cross-section as function of $|y^{t,had}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t,1}$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t,1}$ and the absolute differential cross-section as function of $|y^{t,had}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t,1}$ and the absolute differential cross-section as function of $p_{T}^{t,1}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t,2}$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t,2}$ and the absolute differential cross-section as function of $|y^{t,had}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t,2}$ and the absolute differential cross-section as function of $p_{T}^{t,1}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t,2}$ and the absolute differential cross-section as function of $p_{T}^{t,2}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $m^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $m^{t\bar{t}}$ and the absolute differential cross-section as function of $|y^{t,had}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $m^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,1}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $m^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,2}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $m^{t\bar{t}}$ and the absolute differential cross-section as function of $m^{t\bar{t}}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $|y^{t,had}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,1}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,2}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $m^{t\bar{t}}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|p_{out}^{t,had}|$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|p_{out}^{t,had}|$ and the absolute differential cross-section as function of $|y^{t,had}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|p_{out}^{t,had}|$ and the absolute differential cross-section as function of $p_{T}^{t,1}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|p_{out}^{t,had}|$ and the absolute differential cross-section as function of $p_{T}^{t,2}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|p_{out}^{t,had}|$ and the absolute differential cross-section as function of $m^{t\bar{t}}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|p_{out}^{t,had}|$ and the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|p_{out}^{t,had}|$ and the absolute differential cross-section as function of $|p_{out}^{t,had}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|\Delta\phi(t,\bar{t})|$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|\Delta\phi(t,\bar{t})|$ and the absolute differential cross-section as function of $|y^{t,had}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|\Delta\phi(t,\bar{t})|$ and the absolute differential cross-section as function of $p_{T}^{t,1}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|\Delta\phi(t,\bar{t})|$ and the absolute differential cross-section as function of $p_{T}^{t,2}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|\Delta\phi(t,\bar{t})|$ and the absolute differential cross-section as function of $m^{t\bar{t}}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|\Delta\phi(t,\bar{t})|$ and the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|\Delta\phi(t,\bar{t})|$ and the absolute differential cross-section as function of $|p_{out}^{t,had}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|\Delta\phi(t,\bar{t})|$ and the absolute differential cross-section as function of $|\Delta\phi(t,\bar{t})|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $|y^{t,had}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,1}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,2}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $m^{t\bar{t}}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $|p_{out}^{t,had}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $|\Delta\phi(t,\bar{t})|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{extra jets}$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{extra jets}$ and the absolute differential cross-section as function of $|y^{t,had}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{extra jets}$ and the absolute differential cross-section as function of $p_{T}^{t,1}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{extra jets}$ and the absolute differential cross-section as function of $p_{T}^{t,2}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{extra jets}$ and the absolute differential cross-section as function of $m^{t\bar{t}}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{extra jets}$ and the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{extra jets}$ and the absolute differential cross-section as function of $|p_{out}^{t,had}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{extra jets}$ and the absolute differential cross-section as function of $|\Delta\phi(t,\bar{t})|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{extra jets}$ and the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{extra jets}$ and the absolute differential cross-section as function of $N^{extra jets}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $|y^{t,had}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $p_{T}^{t,1}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $p_{T}^{t,2}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $m^{t\bar{t}}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $|p_{out}^{t,had}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $|\Delta\phi(t,\bar{t})|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $N^{extra jets}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $|y^{t\bar{t}}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ and the absolute differential cross-section as function of $|y^{t,had}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ and the absolute differential cross-section as function of $p_{T}^{t,1}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ and the absolute differential cross-section as function of $p_{T}^{t,2}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ and the absolute differential cross-section as function of $m^{t\bar{t}}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ and the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ and the absolute differential cross-section as function of $|p_{out}^{t,had}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ and the absolute differential cross-section as function of $|\Delta\phi(t,\bar{t})|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ and the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ and the absolute differential cross-section as function of $N^{extra jets}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ and the absolute differential cross-section as function of $|y^{t\bar{t}}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ and the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi^{t\bar{t}}$ and the absolute differential cross-section as function of $|y^{t,had}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,1}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,2}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi^{t\bar{t}}$ and the absolute differential cross-section as function of $m^{t\bar{t}}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi^{t\bar{t}}$ and the absolute differential cross-section as function of $|p_{out}^{t,had}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi^{t\bar{t}}$ and the absolute differential cross-section as function of $|\Delta\phi(t,\bar{t})|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi^{t\bar{t}}$ and the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi^{t\bar{t}}$ and the absolute differential cross-section as function of $N^{extra jets}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi^{t\bar{t}}$ and the absolute differential cross-section as function of $|y^{t\bar{t}}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi^{t\bar{t}}$ and the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi^{t\bar{t}}$ and the absolute differential cross-section as function of $\chi^{t\bar{t}}$ at particle level in the resolved topology.
Relative differential cross-section as a function of $p_{T}^{t}$ at parton level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Relative differential cross-section as function of $p_{T}^{t}$ at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Absolute differential cross-section as a function of $p_{T}^{t}$ at parton level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Absolute differential cross-section as function of $p_{T}^{t}$ at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Relative differential cross-section as a function of $|y^{t}|$ at parton level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Relative differential cross-section as function of $|y^{t}|$ at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Absolute differential cross-section as a function of $|y^{t}|$ at parton level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Absolute differential cross-section as function of $|y^{t}|$ at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Relative differential cross-section as a function of $m^{t\bar{t}}$ at parton level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Relative differential cross-section as function of $m^{t\bar{t}}$ at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Absolute differential cross-section as a function of $m^{t\bar{t}}$ at parton level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Absolute differential cross-section as function of $m^{t\bar{t}}$ at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Relative differential cross-section as a function of $p_{T}^{t\bar{t}}$ at parton level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Relative differential cross-section as function of $p_{T}^{t\bar{t}}$ at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Absolute differential cross-section as a function of $p_{T}^{t\bar{t}}$ at parton level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Relative differential cross-section as a function of $|y^{t\bar{t}}|$ at parton level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Relative differential cross-section as function of $|y^{t\bar{t}}|$ at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Absolute differential cross-section as a function of $|y^{t\bar{t}}|$ at parton level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Absolute differential cross-section as function of $|y^{t\bar{t}}|$ at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Relative differential cross-section as a function of $|y_{boost}^{t\bar{t}}|$ at parton level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Relative differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Absolute differential cross-section as a function of $|y_{boost}^{t\bar{t}}|$ at parton level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Relative differential cross-section as a function of $H_{T}^{t\bar{t}}$ at parton level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Relative differential cross-section as function of $H_{T}^{t\bar{t}}$ at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Absolute differential cross-section as a function of $H_{T}^{t\bar{t}}$ at parton level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Relative differential cross-section as a function of $\chi_{tt}$ at parton level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Relative differential cross-section as function of $\chi_{tt}$ at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Absolute differential cross-section as a function of $\chi_{tt}$ at parton level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Absolute differential cross-section as function of $\chi_{tt}$ at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Relative double-differential cross-section as a function of $p_{T}^{t}$ vs $|y^{t}|$ at parton level in the resolved topology in 0.0 < $|y^{t}|$ < 0.75 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t}$ vs $|y^{t}|$ at parton level in the resolved topology in 0.75 < $|y^{t}|$ < 1.5 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t}$ vs $|y^{t}|$ at parton level in the resolved topology in 1.5 < $|y^{t}|$ < 2.5 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 0.0 < $|y^{t}|$ < 0.75 and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 0.0 < $|y^{t}|$ < 0.75 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 0.75 < $|y^{t}|$ < 1.5 and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 0.0 < $|y^{t}|$ < 0.75 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 0.75 < $|y^{t}|$ < 1.5 and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 0.75 < $|y^{t}|$ < 1.5 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 1.5 < $|y^{t}|$ < 2.5 and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 0.0 < $|y^{t}|$ < 0.75 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 1.5 < $|y^{t}|$ < 2.5 and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 0.75 < $|y^{t}|$ < 1.5 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 1.5 < $|y^{t}|$ < 2.5 and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 1.5 < $|y^{t}|$ < 2.5 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Absolute double-differential cross-section as a function of $p_{T}^{t}$ vs $|y^{t}|$ at parton level in the resolved topology in 0.0 < $|y^{t}|$ < 0.75 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t}$ vs $|y^{t}|$ at parton level in the resolved topology in 0.75 < $|y^{t}|$ < 1.5 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t}$ vs $|y^{t}|$ at parton level in the resolved topology in 1.5 < $|y^{t}|$ < 2.5 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 0.0 < $|y^{t}|$ < 0.75 and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 0.0 < $|y^{t}|$ < 0.75 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 0.75 < $|y^{t}|$ < 1.5 and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 0.0 < $|y^{t}|$ < 0.75 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 0.75 < $|y^{t}|$ < 1.5 and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 0.75 < $|y^{t}|$ < 1.5 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 1.5 < $|y^{t}|$ < 2.5 and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 0.0 < $|y^{t}|$ < 0.75 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 1.5 < $|y^{t}|$ < 2.5 and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 0.75 < $|y^{t}|$ < 1.5 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 1.5 < $|y^{t}|$ < 2.5 and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 1.5 < $|y^{t}|$ < 2.5 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Relative double-differential cross-section as a function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ at parton level in the resolved topology in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ at parton level in the resolved topology in 80.0 GeV < $p_{T}^{t\bar{t}}$ < 180.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ at parton level in the resolved topology in 180.0 GeV < $p_{T}^{t\bar{t}}$ < 330.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ at parton level in the resolved topology in 330.0 GeV < $p_{T}^{t\bar{t}}$ < 800.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 80.0 GeV < $p_{T}^{t\bar{t}}$ < 180.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 80.0 GeV < $p_{T}^{t\bar{t}}$ < 180.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 80.0 GeV < $p_{T}^{t\bar{t}}$ < 180.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 180.0 GeV < $p_{T}^{t\bar{t}}$ < 330.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 180.0 GeV < $p_{T}^{t\bar{t}}$ < 330.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 80.0 GeV < $p_{T}^{t\bar{t}}$ < 180.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 180.0 GeV < $p_{T}^{t\bar{t}}$ < 330.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 180.0 GeV < $p_{T}^{t\bar{t}}$ < 330.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 330.0 GeV < $p_{T}^{t\bar{t}}$ < 800.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 330.0 GeV < $p_{T}^{t\bar{t}}$ < 800.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 80.0 GeV < $p_{T}^{t\bar{t}}$ < 180.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 330.0 GeV < $p_{T}^{t\bar{t}}$ < 800.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 180.0 GeV < $p_{T}^{t\bar{t}}$ < 330.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 330.0 GeV < $p_{T}^{t\bar{t}}$ < 800.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 330.0 GeV < $p_{T}^{t\bar{t}}$ < 800.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Absolute double-differential cross-section as a function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ at parton level in the resolved topology in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ at parton level in the resolved topology in 80.0 GeV < $p_{T}^{t\bar{t}}$ < 180.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ at parton level in the resolved topology in 180.0 GeV < $p_{T}^{t\bar{t}}$ < 330.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ at parton level in the resolved topology in 330.0 GeV < $p_{T}^{t\bar{t}}$ < 800.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 80.0 GeV < $p_{T}^{t\bar{t}}$ < 180.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 80.0 GeV < $p_{T}^{t\bar{t}}$ < 180.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 80.0 GeV < $p_{T}^{t\bar{t}}$ < 180.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 180.0 GeV < $p_{T}^{t\bar{t}}$ < 330.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 180.0 GeV < $p_{T}^{t\bar{t}}$ < 330.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 80.0 GeV < $p_{T}^{t\bar{t}}$ < 180.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 180.0 GeV < $p_{T}^{t\bar{t}}$ < 330.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 180.0 GeV < $p_{T}^{t\bar{t}}$ < 330.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 330.0 GeV < $p_{T}^{t\bar{t}}$ < 800.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 330.0 GeV < $p_{T}^{t\bar{t}}$ < 800.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 80.0 GeV < $p_{T}^{t\bar{t}}$ < 180.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 330.0 GeV < $p_{T}^{t\bar{t}}$ < 800.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 180.0 GeV < $p_{T}^{t\bar{t}}$ < 330.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 330.0 GeV < $p_{T}^{t\bar{t}}$ < 800.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 330.0 GeV < $p_{T}^{t\bar{t}}$ < 800.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Relative double-differential cross-section as a function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ at parton level in the resolved topology in 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ at parton level in the resolved topology in 500.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ at parton level in the resolved topology in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ at parton level in the resolved topology in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 500.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 500.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 500.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 500.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 500.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Absolute double-differential cross-section as a function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ at parton level in the resolved topology in 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ at parton level in the resolved topology in 500.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ at parton level in the resolved topology in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ at parton level in the resolved topology in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 500.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 500.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 500.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 500.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 500.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Relative double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ at parton level in the resolved topology in 0.0 GeV < $|y^{t\bar{t}}|$ < 0.5 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ at parton level in the resolved topology in 0.5 GeV < $|y^{t\bar{t}}|$ < 1.1 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ at parton level in the resolved topology in 1.1 GeV < $|y^{t\bar{t}}|$ < 1.7 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ at parton level in the resolved topology in 1.7 GeV < $|y^{t\bar{t}}|$ < 2.5 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 GeV < $|y^{t\bar{t}}|$ < 0.5 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 GeV < $|y^{t\bar{t}}|$ < 0.5 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.5 GeV < $|y^{t\bar{t}}|$ < 1.1 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 GeV < $|y^{t\bar{t}}|$ < 0.5 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.5 GeV < $|y^{t\bar{t}}|$ < 1.1 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.5 GeV < $|y^{t\bar{t}}|$ < 1.1 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.1 GeV < $|y^{t\bar{t}}|$ < 1.7 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 GeV < $|y^{t\bar{t}}|$ < 0.5 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.1 GeV < $|y^{t\bar{t}}|$ < 1.7 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.5 GeV < $|y^{t\bar{t}}|$ < 1.1 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.1 GeV < $|y^{t\bar{t}}|$ < 1.7 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.1 GeV < $|y^{t\bar{t}}|$ < 1.7 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.7 GeV < $|y^{t\bar{t}}|$ < 2.5 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 GeV < $|y^{t\bar{t}}|$ < 0.5 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.7 GeV < $|y^{t\bar{t}}|$ < 2.5 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.5 GeV < $|y^{t\bar{t}}|$ < 1.1 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.7 GeV < $|y^{t\bar{t}}|$ < 2.5 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.1 GeV < $|y^{t\bar{t}}|$ < 1.7 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.7 GeV < $|y^{t\bar{t}}|$ < 2.5 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.7 GeV < $|y^{t\bar{t}}|$ < 2.5 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Absolute double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ at parton level in the resolved topology in 0.0 GeV < $|y^{t\bar{t}}|$ < 0.5 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ at parton level in the resolved topology in 0.5 GeV < $|y^{t\bar{t}}|$ < 1.1 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ at parton level in the resolved topology in 1.1 GeV < $|y^{t\bar{t}}|$ < 1.7 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ at parton level in the resolved topology in 1.7 GeV < $|y^{t\bar{t}}|$ < 2.5 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 GeV < $|y^{t\bar{t}}|$ < 0.5 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 GeV < $|y^{t\bar{t}}|$ < 0.5 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.5 GeV < $|y^{t\bar{t}}|$ < 1.1 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 GeV < $|y^{t\bar{t}}|$ < 0.5 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.5 GeV < $|y^{t\bar{t}}|$ < 1.1 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.5 GeV < $|y^{t\bar{t}}|$ < 1.1 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.1 GeV < $|y^{t\bar{t}}|$ < 1.7 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 GeV < $|y^{t\bar{t}}|$ < 0.5 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.1 GeV < $|y^{t\bar{t}}|$ < 1.7 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.5 GeV < $|y^{t\bar{t}}|$ < 1.1 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.1 GeV < $|y^{t\bar{t}}|$ < 1.7 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.1 GeV < $|y^{t\bar{t}}|$ < 1.7 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.7 GeV < $|y^{t\bar{t}}|$ < 2.5 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 GeV < $|y^{t\bar{t}}|$ < 0.5 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.7 GeV < $|y^{t\bar{t}}|$ < 2.5 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.5 GeV < $|y^{t\bar{t}}|$ < 1.1 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.7 GeV < $|y^{t\bar{t}}|$ < 2.5 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.1 GeV < $|y^{t\bar{t}}|$ < 1.7 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.7 GeV < $|y^{t\bar{t}}|$ < 2.5 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.7 GeV < $|y^{t\bar{t}}|$ < 2.5 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Relative double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ at parton level in the resolved topology in 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ at parton level in the resolved topology in 500.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ at parton level in the resolved topology in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ at parton level in the resolved topology in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 500.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 500.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 500.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 500.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 500.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Absolute double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ at parton level in the resolved topology in 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ at parton level in the resolved topology in 500.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ at parton level in the resolved topology in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ at parton level in the resolved topology in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 500.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 500.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 500.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 500.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 500.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Relative double-differential cross-section as a function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ at parton level in the resolved topology in 0.0 < $|y^{t\bar{t}}|$ < 0.5 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ at parton level in the resolved topology in 0.5 < $|y^{t\bar{t}}|$ < 1.1 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ at parton level in the resolved topology in 1.1 < $|y^{t\bar{t}}|$ < 1.7 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ at parton level in the resolved topology in 1.7 < $|y^{t\bar{t}}|$ < 2.5 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.5 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.5 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi_{tt}$ and the absolute differential cross-section as function of $p_{T}^{t}$ at parton level in the resolved topology.
Covariance matrix of the Relative differential cross-section as function of $N^{extra jets}$ at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Relative double-differential cross-section as a function of $p_{T}^{t,had}$ vs $|y^{t\bar{t}}|$ at particle level in the boosted topology in 0.0 < $|y^{t\bar{t}}|$ < 1.0 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t,had}$ vs $|y^{t\bar{t}}|$ at particle level in the boosted topology in 1.0 < $|y^{t\bar{t}}|$ < 2.0 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 1.0 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 1.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t\bar{t}}|$ in 1.0 < $|y^{t\bar{t}}|$ < 2.0 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 1.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t\bar{t}}|$ in 1.0 < $|y^{t\bar{t}}|$ < 2.0 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t\bar{t}}|$ in 1.0 < $|y^{t\bar{t}}|$ < 2.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Absolute double-differential cross-section as a function of $p_{T}^{t,had}$ vs $|y^{t\bar{t}}|$ at particle level in the boosted topology in 0.0 < $|y^{t\bar{t}}|$ < 1.0 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t,had}$ vs $|y^{t\bar{t}}|$ at particle level in the boosted topology in 1.0 < $|y^{t\bar{t}}|$ < 2.0 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 1.0 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 1.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t\bar{t}}|$ in 1.0 < $|y^{t\bar{t}}|$ < 2.0 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 1.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t\bar{t}}|$ in 1.0 < $|y^{t\bar{t}}|$ < 2.0 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t\bar{t}}|$ in 1.0 < $|y^{t\bar{t}}|$ < 2.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Relative double-differential cross-section as a function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ at particle level in the boosted topology in 0.0 < $|y^{t,had}|$ < 1.0 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ at particle level in the boosted topology in 1.0 < $|y^{t,had}|$ < 2.0 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 0.0 < $|y^{t,had}|$ < 1.0 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 0.0 < $|y^{t,had}|$ < 1.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 1.0 < $|y^{t,had}|$ < 2.0 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 0.0 < $|y^{t,had}|$ < 1.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 1.0 < $|y^{t,had}|$ < 2.0 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 1.0 < $|y^{t,had}|$ < 2.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Absolute double-differential cross-section as a function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ at particle level in the boosted topology in 0.0 < $|y^{t,had}|$ < 1.0 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ at particle level in the boosted topology in 1.0 < $|y^{t,had}|$ < 2.0 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 0.0 < $|y^{t,had}|$ < 1.0 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 0.0 < $|y^{t,had}|$ < 1.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 1.0 < $|y^{t,had}|$ < 2.0 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 0.0 < $|y^{t,had}|$ < 1.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 1.0 < $|y^{t,had}|$ < 2.0 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 1.0 < $|y^{t,had}|$ < 2.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Relative double-differential cross-section as a function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ at particle level in the boosted topology in 490.0 GeV < $m^{t\bar{t}}$ < 1160.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ at particle level in the boosted topology in 1160.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 490.0 GeV < $m^{t\bar{t}}$ < 1160.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 490.0 GeV < $m^{t\bar{t}}$ < 1160.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 1160.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 490.0 GeV < $m^{t\bar{t}}$ < 1160.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 1160.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 1160.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Absolute double-differential cross-section as a function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ at particle level in the boosted topology in 490.0 GeV < $m^{t\bar{t}}$ < 1160.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ at particle level in the boosted topology in 1160.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 490.0 GeV < $m^{t\bar{t}}$ < 1160.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 490.0 GeV < $m^{t\bar{t}}$ < 1160.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 1160.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 490.0 GeV < $m^{t\bar{t}}$ < 1160.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 1160.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 1160.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Relative double-differential cross-section as a function of $m^{t\bar{t}}$ vs $H_{T}^{t\bar{t}}$ at particle level in the boosted topology in 350.0 GeV < $H_{T}^{t\bar{t}}$ < 780.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $m^{t\bar{t}}$ vs $H_{T}^{t\bar{t}}$ at particle level in the boosted topology in 780.0 GeV < $H_{T}^{t\bar{t}}$ < 2500.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $H_{T}^{t\bar{t}}$ in 350.0 GeV < $H_{T}^{t\bar{t}}$ < 780.0 GeV and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $H_{T}^{t\bar{t}}$ in 350.0 GeV < $H_{T}^{t\bar{t}}$ < 780.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $H_{T}^{t\bar{t}}$ in 780.0 GeV < $H_{T}^{t\bar{t}}$ < 2500.0 GeV and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $H_{T}^{t\bar{t}}$ in 350.0 GeV < $H_{T}^{t\bar{t}}$ < 780.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $H_{T}^{t\bar{t}}$ in 780.0 GeV < $H_{T}^{t\bar{t}}$ < 2500.0 GeV and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $H_{T}^{t\bar{t}}$ in 780.0 GeV < $H_{T}^{t\bar{t}}$ < 2500.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Absolute double-differential cross-section as a function of $m^{t\bar{t}}$ vs $H_{T}^{t\bar{t}}$ at particle level in the boosted topology in 350.0 GeV < $H_{T}^{t\bar{t}}$ < 780.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $m^{t\bar{t}}$ vs $H_{T}^{t\bar{t}}$ at particle level in the boosted topology in 780.0 GeV < $H_{T}^{t\bar{t}}$ < 2500.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $H_{T}^{t\bar{t}}$ in 350.0 GeV < $H_{T}^{t\bar{t}}$ < 780.0 GeV and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $H_{T}^{t\bar{t}}$ in 350.0 GeV < $H_{T}^{t\bar{t}}$ < 780.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $H_{T}^{t\bar{t}}$ in 780.0 GeV < $H_{T}^{t\bar{t}}$ < 2500.0 GeV and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $H_{T}^{t\bar{t}}$ in 350.0 GeV < $H_{T}^{t\bar{t}}$ < 780.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $H_{T}^{t\bar{t}}$ in 780.0 GeV < $H_{T}^{t\bar{t}}$ < 2500.0 GeV and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $H_{T}^{t\bar{t}}$ in 780.0 GeV < $H_{T}^{t\bar{t}}$ < 2500.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Relative double-differential cross-section as a function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ at particle level in the boosted topology in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 40.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ at particle level in the boosted topology in 40.0 GeV < $p_{T}^{t\bar{t}}$ < 150.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ at particle level in the boosted topology in 150.0 GeV < $p_{T}^{t\bar{t}}$ < 1000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 40.0 GeV and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 40.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 40.0 GeV < $p_{T}^{t\bar{t}}$ < 150.0 GeV and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 40.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 40.0 GeV < $p_{T}^{t\bar{t}}$ < 150.0 GeV and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 40.0 GeV < $p_{T}^{t\bar{t}}$ < 150.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 150.0 GeV < $p_{T}^{t\bar{t}}$ < 1000.0 GeV and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 40.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 150.0 GeV < $p_{T}^{t\bar{t}}$ < 1000.0 GeV and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 40.0 GeV < $p_{T}^{t\bar{t}}$ < 150.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 150.0 GeV < $p_{T}^{t\bar{t}}$ < 1000.0 GeV and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 150.0 GeV < $p_{T}^{t\bar{t}}$ < 1000.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Absolute double-differential cross-section as a function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ at particle level in the boosted topology in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 40.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ at particle level in the boosted topology in 40.0 GeV < $p_{T}^{t\bar{t}}$ < 150.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ at particle level in the boosted topology in 150.0 GeV < $p_{T}^{t\bar{t}}$ < 1000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 40.0 GeV and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 40.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 40.0 GeV < $p_{T}^{t\bar{t}}$ < 150.0 GeV and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 40.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 40.0 GeV < $p_{T}^{t\bar{t}}$ < 150.0 GeV and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 40.0 GeV < $p_{T}^{t\bar{t}}$ < 150.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 150.0 GeV < $p_{T}^{t\bar{t}}$ < 1000.0 GeV and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 40.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 150.0 GeV < $p_{T}^{t\bar{t}}$ < 1000.0 GeV and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 40.0 GeV < $p_{T}^{t\bar{t}}$ < 150.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 150.0 GeV < $p_{T}^{t\bar{t}}$ < 1000.0 GeV and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 150.0 GeV < $p_{T}^{t\bar{t}}$ < 1000.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Relative double-differential cross-section as a function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ at particle level in the boosted topology in 0.0 < $|y^{t\bar{t}}|$ < 0.65 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ at particle level in the boosted topology in 0.65 < $|y^{t\bar{t}}|$ < 1.3 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ at particle level in the boosted topology in 1.3 < $|y^{t\bar{t}}|$ < 2.0 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.65 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.65 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.65 < $|y^{t\bar{t}}|$ < 1.3 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.65 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.65 < $|y^{t\bar{t}}|$ < 1.3 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.65 < $|y^{t\bar{t}}|$ < 1.3 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.3 < $|y^{t\bar{t}}|$ < 2.0 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.65 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.3 < $|y^{t\bar{t}}|$ < 2.0 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.65 < $|y^{t\bar{t}}|$ < 1.3 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.3 < $|y^{t\bar{t}}|$ < 2.0 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.3 < $|y^{t\bar{t}}|$ < 2.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Absolute double-differential cross-section as a function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ at particle level in the boosted topology in 0.0 < $|y^{t\bar{t}}|$ < 0.65 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ at particle level in the boosted topology in 0.65 < $|y^{t\bar{t}}|$ < 1.3 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ at particle level in the boosted topology in 1.3 < $|y^{t\bar{t}}|$ < 2.0 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.65 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.65 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.65 < $|y^{t\bar{t}}|$ < 1.3 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.65 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.65 < $|y^{t\bar{t}}|$ < 1.3 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.65 < $|y^{t\bar{t}}|$ < 1.3 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.3 < $|y^{t\bar{t}}|$ < 2.0 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.65 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.3 < $|y^{t\bar{t}}|$ < 2.0 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.65 < $|y^{t\bar{t}}|$ < 1.3 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.3 < $|y^{t\bar{t}}|$ < 2.0 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.3 < $|y^{t\bar{t}}|$ < 2.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Relative double-differential cross-section as a function of $p_{T}^{t,had}$ vs $N^{extra jets}$ at particle level in the boosted topology in $N^{extra jets}$ = 0.5. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t,had}$ vs $N^{extra jets}$ at particle level in the boosted topology in $N^{extra jets}$ = 2.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t,had}$ vs $N^{extra jets}$ at particle level in the boosted topology in $N^{extra jets}$ $\geq$ 3.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 0.5 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 0.5 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 2.0 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 0.5 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 2.0 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 2.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 3.0 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 0.5 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 3.0 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 2.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 3.0 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 3.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Absolute double-differential cross-section as a function of $p_{T}^{t,had}$ vs $N^{extra jets}$ at particle level in the boosted topology in $N^{extra jets}$ = 0.5. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t,had}$ vs $N^{extra jets}$ at particle level in the boosted topology in $N^{extra jets}$ = 2.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t,had}$ vs $N^{extra jets}$ at particle level in the boosted topology in $N^{extra jets}$ $\geq$ 3.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 0.5 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 0.5 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 2.0 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 0.5 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 2.0 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 2.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 3.0 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 0.5 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 3.0 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 2.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 3.0 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 3.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Relative double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $N^{extra jets}$ at particle level in the boosted topology in $N^{extra jets}$ = 0.5. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $N^{extra jets}$ at particle level in the boosted topology in $N^{extra jets}$ $\geq$ 2.5. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 0.5 and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 0.5 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 2.5 and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 0.5 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 2.5 and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 2.5 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Absolute double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $N^{extra jets}$ at particle level in the boosted topology in $N^{extra jets}$ = 0.5. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $N^{extra jets}$ at particle level in the boosted topology in $N^{extra jets}$ $\geq$ 2.5. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 0.5 and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 0.5 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 2.5 and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 0.5 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 2.5 and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 2.5 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Relative double-differential cross-section as a function of $m^{t\bar{t}}$ vs $N^{extra jets}$ at particle level in the boosted topology in $N^{extra jets}$ = 0.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $m^{t\bar{t}}$ vs $N^{extra jets}$ at particle level in the boosted topology in $N^{extra jets}$ = 1.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $m^{t\bar{t}}$ vs $N^{extra jets}$ at particle level in the boosted topology in $N^{extra jets}$ $\geq$ 2.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 0.0 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 0.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 1.0 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 0.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 1.0 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 1.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 2.0 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 0.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 2.0 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 1.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 2.0 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 2.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Absolute double-differential cross-section as a function of $m^{t\bar{t}}$ vs $N^{extra jets}$ at particle level in the boosted topology in $N^{extra jets}$ = 0.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $m^{t\bar{t}}$ vs $N^{extra jets}$ at particle level in the boosted topology in $N^{extra jets}$ = 1.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $m^{t\bar{t}}$ vs $N^{extra jets}$ at particle level in the boosted topology in $N^{extra jets}$ $\geq$ 2.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 0.0 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 0.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 1.0 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 0.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 1.0 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 1.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 2.0 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 0.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 2.0 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 1.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 2.0 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 2.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t,had}$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t,had}|$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t,had}|$ and the absolute differential cross-section as function of $|y^{t,had}|$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t,1}$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t,1}$ and the absolute differential cross-section as function of $|y^{t,had}|$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t,1}$ and the absolute differential cross-section as function of $p_{T}^{t,1}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t,2}$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t,2}$ and the absolute differential cross-section as function of $|y^{t,had}|$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t,2}$ and the absolute differential cross-section as function of $p_{T}^{t,1}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t,2}$ and the absolute differential cross-section as function of $p_{T}^{t,2}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $|y^{t,had}|$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,1}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,2}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $|y^{t,had}|$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $p_{T}^{t,1}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $p_{T}^{t,2}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $|y^{t\bar{t}}|$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $m^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $m^{t\bar{t}}$ and the absolute differential cross-section as function of $|y^{t,had}|$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $m^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,1}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $m^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,2}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $m^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $m^{t\bar{t}}$ and the absolute differential cross-section as function of $|y^{t\bar{t}}|$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $m^{t\bar{t}}$ and the absolute differential cross-section as function of $m^{t\bar{t}}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi^{t\bar{t}}$ and the absolute differential cross-section as function of $|y^{t,had}|$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,1}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,2}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi^{t\bar{t}}$ and the absolute differential cross-section as function of $|y^{t\bar{t}}|$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi^{t\bar{t}}$ and the absolute differential cross-section as function of $m^{t\bar{t}}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi^{t\bar{t}}$ and the absolute differential cross-section as function of $\chi^{t\bar{t}}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|p_{out}^{t,lep}|$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|p_{out}^{t,lep}|$ and the absolute differential cross-section as function of $|y^{t,had}|$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|p_{out}^{t,lep}|$ and the absolute differential cross-section as function of $p_{T}^{t,1}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|p_{out}^{t,lep}|$ and the absolute differential cross-section as function of $p_{T}^{t,2}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|p_{out}^{t,lep}|$ and the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|p_{out}^{t,lep}|$ and the absolute differential cross-section as function of $|y^{t\bar{t}}|$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|p_{out}^{t,lep}|$ and the absolute differential cross-section as function of $m^{t\bar{t}}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|p_{out}^{t,lep}|$ and the absolute differential cross-section as function of $\chi^{t\bar{t}}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|p_{out}^{t,lep}|$ and the absolute differential cross-section as function of $|p_{out}^{t,lep}|$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $|y^{t,had}|$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,1}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,2}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $|y^{t\bar{t}}|$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $m^{t\bar{t}}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $\chi^{t\bar{t}}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $|p_{out}^{t,lep}|$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{extra jets}$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{extra jets}$ and the absolute differential cross-section as function of $|y^{t,had}|$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{extra jets}$ and the absolute differential cross-section as function of $p_{T}^{t,1}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{extra jets}$ and the absolute differential cross-section as function of $p_{T}^{t,2}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{extra jets}$ and the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{extra jets}$ and the absolute differential cross-section as function of $|y^{t\bar{t}}|$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{extra jets}$ and the absolute differential cross-section as function of $m^{t\bar{t}}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{extra jets}$ and the absolute differential cross-section as function of $\chi^{t\bar{t}}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{extra jets}$ and the absolute differential cross-section as function of $|p_{out}^{t,lep}|$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{extra jets}$ and the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{extra jets}$ and the absolute differential cross-section as function of $N^{extra jets}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{subjets}$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{subjets}$ and the absolute differential cross-section as function of $|y^{t,had}|$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{subjets}$ and the absolute differential cross-section as function of $p_{T}^{t,1}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{subjets}$ and the absolute differential cross-section as function of $p_{T}^{t,2}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{subjets}$ and the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{subjets}$ and the absolute differential cross-section as function of $|y^{t\bar{t}}|$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{subjets}$ and the absolute differential cross-section as function of $m^{t\bar{t}}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{subjets}$ and the absolute differential cross-section as function of $\chi^{t\bar{t}}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{subjets}$ and the absolute differential cross-section as function of $|p_{out}^{t,lep}|$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{subjets}$ and the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{subjets}$ and the absolute differential cross-section as function of $N^{extra jets}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{subjets}$ and the absolute differential cross-section as function of $N^{subjets}$ at particle level in the boosted topology.
Relative differential cross-section as a function of $m^{t\bar{t}}$ at parton level in the boosted topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Relative differential cross-section as function of $m^{t\bar{t}}$ at parton level in the boosted topology, accounting for the statistical and systematic uncertainties.
Absolute differential cross-section as a function of $m^{t\bar{t}}$ at parton level in the boosted topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Absolute differential cross-section as function of $m^{t\bar{t}}$ at parton level in the boosted topology, accounting for the statistical and systematic uncertainties.
Relative differential cross-section as a function of $p_{T}^{t}$ at parton level in the boosted topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Relative differential cross-section as function of $p_{T}^{t}$ at parton level in the boosted topology, accounting for the statistical and systematic uncertainties.
Absolute differential cross-section as a function of $p_{T}^{t}$ at parton level in the boosted topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Absolute differential cross-section as function of $p_{T}^{t}$ at parton level in the boosted topology, accounting for the statistical and systematic uncertainties.
Total cross-section at parton level in the boosted topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $m^{t\bar{t}}$ vs $p_{T}^{t}$ at parton level in the boosted topology in 350.0 GeV < $p_{T}^{t}$ < 550.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $m^{t\bar{t}}$ vs $p_{T}^{t}$ at parton level in the boosted topology in 550.0 GeV < $p_{T}^{t}$ < 2000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t}$ in 350.0 GeV < $p_{T}^{t}$ < 550.0 GeV and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t}$ in 350.0 GeV < $p_{T}^{t}$ < 550.0 GeV at parton level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t}$ in 550.0 GeV < $p_{T}^{t}$ < 2000.0 GeV and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t}$ in 350.0 GeV < $p_{T}^{t}$ < 550.0 GeV at parton level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t}$ in 550.0 GeV < $p_{T}^{t}$ < 2000.0 GeV and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t}$ in 550.0 GeV < $p_{T}^{t}$ < 2000.0 GeV at parton level in the boosted topology, accounting for the statistical and systematic uncertainties.
Absolute double-differential cross-section as a function of $m^{t\bar{t}}$ vs $p_{T}^{t}$ at parton level in the boosted topology in 350.0 GeV < $p_{T}^{t}$ < 550.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $m^{t\bar{t}}$ vs $p_{T}^{t}$ at parton level in the boosted topology in 550.0 GeV < $p_{T}^{t}$ < 2000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t}$ in 350.0 GeV < $p_{T}^{t}$ < 550.0 GeV and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t}$ in 350.0 GeV < $p_{T}^{t}$ < 550.0 GeV at parton level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t}$ in 550.0 GeV < $p_{T}^{t}$ < 2000.0 GeV and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t}$ in 350.0 GeV < $p_{T}^{t}$ < 550.0 GeV at parton level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t}$ in 550.0 GeV < $p_{T}^{t}$ < 2000.0 GeV and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t}$ in 550.0 GeV < $p_{T}^{t}$ < 2000.0 GeV at parton level in the boosted topology, accounting for the statistical and systematic uncertainties.
Statistical correlation matrix between the absolute differential cross-section as function of $m^{t\bar{t}}$ and the absolute differential cross-section as function of $m^{t\bar{t}}$ at parton level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t}$ and the absolute differential cross-section as function of $m^{t\bar{t}}$ at parton level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t}$ and the absolute differential cross-section as function of $p_{T}^{t}$ at parton level in the boosted topology.
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.
A search has been performed for the experimental signature of an isolated photon with high transverse momentum, at least one jet identified as originating from a bottom quark, and high missing transverse momentum. Such a final state may originate from supersymmetric models with gauge-mediated supersymmetry breaking in events in which one of a pair of higgsino-like neutralinos decays into a photon and a gravitino while the other decays into a Higgs boson and a gravitino. The search is performed using the full dataset of 7 TeV proton-proton collisions recorded with the ATLAS detector at the LHC in 2011, corresponding to an integrated luminosity of 4.7 fb-1. A total of 7 candidate events are observed while 7.5 pm 2.2 events are expected from the Standard Model background. The results of the search are interpreted in the context of general gauge mediation to exclude certain regions of a benchmark plane for higgsino-like neutralino production.
Measurements of jet substructure describing the composition of quark- and gluon-initiated jets are presented. Proton-proton (pp) collision data at $\sqrt{s}$ =13 TeV collected with the CMS detector are used, corresponding to an integrated luminosity of 35.9 fb$^{-1}$. Generalized angularities are measured that characterize the jet substructure and distinguish quark- and gluon-initiated jets. These observables are sensitive to the distributions of transverse momenta and angular distances within a jet. The analysis is performed using a data sample of dijet events enriched in gluon-initiated jets, and, for the first time, a Z+jet event sample enriched in quark-initiated jets. The observables are measured in bins of jet transverse momentum, and as a function of the jet radius parameter. Each measurement is repeated applying a "soft drop" grooming procedure that removes soft and large angle radiation from the jet. Using these measurements, the ability of various models to describe jet substructure is assessed, showing a clear need for improvements in Monte Carlo generators.
We present an update of a search for supersymmetry in final states containing jets, missing transverse momentum, and one isolated electron or muon, using 1.04 fb^-1 of proton-proton collision data at sqrt{s} = 7 TeV recorded by the ATLAS experiment at the LHC in the first half of 2011. The analysis is carried out in four distinct signal regions with either three or four jets and variations on the (missing) transverse momentum cuts, resulting in optimized limits for various supersymmetry models. No excess above the standard model background expectation is observed. Limits are set on the visible cross-section of new physics within the kinematic requirements of the search. The results are interpreted as limits on the parameters of the minimal supergravity framework, limits on cross-sections of simplified models with specific squark and gluino decay modes, and limits on parameters of a model with bilinear R-parity violation.
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