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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.
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 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.
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.
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 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 $p_{T}^{t\bar{t}}$ 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 1.7 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 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.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t}$ and the absolute differential cross-section as function of $p_{T}^{t}$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t}|$ and the absolute differential cross-section as function of $p_{T}^{t}$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t}|$ and the absolute differential cross-section as function of $|y^{t}|$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $m^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t}$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $m^{t\bar{t}}$ and the absolute differential cross-section as function of $|y^{t}|$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $m^{t\bar{t}}$ and the absolute differential cross-section as function of $m^{t\bar{t}}$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t}$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $|y^{t}|$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $m^{t\bar{t}}$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $p_{T}^{t}$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $|y^{t}|$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $m^{t\bar{t}}$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $|y^{t\bar{t}}|$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ and the absolute differential cross-section as function of $p_{T}^{t}$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ and the absolute differential cross-section as function of $|y^{t}|$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ and the absolute differential cross-section as function of $m^{t\bar{t}}$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ and the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ and the absolute differential cross-section as function of $|y^{t\bar{t}}|$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ and the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t}$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $|y^{t}|$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $m^{t\bar{t}}$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $|y^{t\bar{t}}|$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi_{tt}$ and the absolute differential cross-section as function of $p_{T}^{t}$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi_{tt}$ and the absolute differential cross-section as function of $|y^{t}|$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi_{tt}$ and the absolute differential cross-section as function of $m^{t\bar{t}}$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi_{tt}$ and the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi_{tt}$ and the absolute differential cross-section as function of $|y^{t\bar{t}}|$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi_{tt}$ and the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi_{tt}$ and the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi_{tt}$ and the absolute differential cross-section as function of $\chi_{tt}$ at parton level in the resolved topology.
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.
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.
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.
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.
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.
Relative differential cross-section as a function of $p_{T}^{t,had}$ at particle 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 $p_{T}^{t,had}$ at particle level in the boosted 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 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 $p_{T}^{t,had}$ at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Relative differential cross-section as a function of $|y^{t,had}|$ at particle 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 $|y^{t,had}|$ at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Absolute differential cross-section as a function of $|y^{t,had}|$ at particle 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 $|y^{t,had}|$ at particle level in the boosted 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 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 $p_{T}^{t,1}$ at particle level in the boosted 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 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 $p_{T}^{t,1}$ at particle level in the boosted 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 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 $p_{T}^{t,2}$ at particle level in the boosted 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 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 $p_{T}^{t,2}$ at particle level in the boosted 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 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 $p_{T}^{t\bar{t}}$ at particle level in the boosted 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 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 $p_{T}^{t\bar{t}}$ at particle level in the boosted 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 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 $|y^{t\bar{t}}|$ at particle level in the boosted 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 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 $|y^{t\bar{t}}|$ at particle level in the boosted 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 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 particle 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 particle 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 particle level in the boosted 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 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 $\chi^{t\bar{t}}$ at particle level in the boosted 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 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 $\chi^{t\bar{t}}$ at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Relative differential cross-section as a function of $|p_{out}^{t,lep}|$ at particle 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 $|p_{out}^{t,lep}|$ at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Absolute differential cross-section as a function of $|p_{out}^{t,lep}|$ at particle 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 $|p_{out}^{t,lep}|$ at particle level in the boosted 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 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 $H_{T}^{t\bar{t}}$ at particle level in the boosted 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 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 $H_{T}^{t\bar{t}}$ at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Relative differential cross-section as a function of $N^{extra jets}$ at particle 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 $N^{extra jets}$ at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Absolute differential cross-section as a function of $N^{extra jets}$ at particle 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 $N^{extra jets}$ at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Relative differential cross-section as a function of $N^{subjets}$ at particle 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 $N^{subjets}$ at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Absolute differential cross-section as a function of $N^{subjets}$ at particle 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 $N^{subjets}$ at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Total cross-section at particle 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 $p_{T}^{t,had}$ 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 $p_{T}^{t,had}$ 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 $p_{T}^{t,had}$ 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 $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 40.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 40.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 40.0 GeV < $p_{T}^{t\bar{t}}$ < 150.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 40.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 40.0 GeV < $p_{T}^{t\bar{t}}$ < 150.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 40.0 GeV < $p_{T}^{t\bar{t}}$ < 150.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 150.0 GeV < $p_{T}^{t\bar{t}}$ < 1000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 40.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 150.0 GeV < $p_{T}^{t\bar{t}}$ < 1000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 40.0 GeV < $p_{T}^{t\bar{t}}$ < 150.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 150.0 GeV < $p_{T}^{t\bar{t}}$ < 1000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 150.0 GeV < $p_{T}^{t\bar{t}}$ < 1000.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Absolute double-differential cross-section as a function of $p_{T}^{t,had}$ 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 $p_{T}^{t,had}$ 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 $p_{T}^{t,had}$ 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 $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 40.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 40.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 40.0 GeV < $p_{T}^{t\bar{t}}$ < 150.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 40.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 40.0 GeV < $p_{T}^{t\bar{t}}$ < 150.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 40.0 GeV < $p_{T}^{t\bar{t}}$ < 150.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 150.0 GeV < $p_{T}^{t\bar{t}}$ < 1000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 40.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 150.0 GeV < $p_{T}^{t\bar{t}}$ < 1000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 40.0 GeV < $p_{T}^{t\bar{t}}$ < 150.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 150.0 GeV < $p_{T}^{t\bar{t}}$ < 1000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 150.0 GeV < $p_{T}^{t\bar{t}}$ < 1000.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
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 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.
Results are presented from a search for new decaying massive particles whose presence is inferred from an imbalance in transverse momentum and which are produced in association with a single top quark that decays into a bottom quark and two light quarks. The measurement is performed using 19.7 inverse femtobarns of data from proton-proton collisions at a center-of-mass energy of 8 TeV, collected with the CMS detector at the CERN LHC. No deviations from the standard model predictions are observed and lower limits are set on the masses of new invisible bosons. In particular, scalar and vector particles, with masses below 330 and 650 GeV, respectively, are excluded at 95% confidence level, thus substantially extending a previous limit published by the CDF Collaboration.
The ratio between the prompt psi(2S) and J/psi yields, reconstructed via their decays into muon pairs, is measured in PbPb and pp collisions at sqrt(s[NN]) = 2.76 TeV. The analysis is based on PbPb and pp data samples collected by CMS at the LHC, corresponding to integrated luminosities of 150 inverse microbarns and 5.4 inverse picobarns, respectively. The double ratio of measured yields, (N[psi(2S)]/N[J/psi])[PbPb] / (N[psi(2S)]/ N[J/psi])[pp], is computed in three PbPb collision centrality bins and two kinematic ranges: one at midrapidity, abs(y) < 1.6, covering the transverse momentum range 6.5 < pt < 30 GeV/c, and the other at forward rapidity, 1.6 < abs(y) < 2.4, extending to lower pt values, 3 < pt < 30 GeV/c. The centrality-integrated double ratio changes from 0.45 +/- 0.13 (stat) +/- 0.07 (syst) in the first range to 1.67 +/- 0.34 (stat) +/- 0.27 (syst) in the second. This difference is most pronounced in the most central collisions.
The first study of W boson production in pPb collisions is presented, for bosons decaying to a muon or electron, and a neutrino. The measurements are based on a data sample corresponding to an integrated luminosity of 34.6 inverse nanobarns at a nucleon-nucleon centre-of-mass energy of sqrt(s[NN]) = 5.02 TeV, collected by the CMS experiment. The W boson differential cross sections, lepton charge asymmetry, and forward-backward asymmetries are measured for leptons of transverse momentum exceeding 25 GeV, and as a function of the lepton pseudorapidity in the abs(eta[lab]) < 2.4 range. Deviations from the expectations based on currently available parton distribution functions are observed, showing the need for including W boson data in nuclear parton distribution global fits.
Measurements of transverse energy-energy correlations and their associated asymmetries in multi-jet events using the ATLAS detector at the LHC are presented. The data used correspond to $\sqrt{s} = 8$ TeV proton-proton collisions with an integrated luminosity of 20.2 fb$^{-1}$. The results are presented in bins of the scalar sum of the transverse momenta of the two leading jets, unfolded to the particle level and compared to the predictions from Monte Carlo simulations. A comparison with next-to-leading-order perturbative QCD is also performed, showing excellent agreement within the uncertainties. From this comparison, the value of the strong coupling constant is extracted for different energy regimes, thus testing the running of $\alpha_s(\mu)$ predicted in QCD up to scales over 1 TeV. A global fit to the transverse energy-energy correlation distributions yields $\alpha_s(m_Z) = 0.1162 \pm 0.0011 \mbox{ (exp.)}^{+0.0084}_{-0.0070} \mbox{ (theo.)}$, while a global fit to the asymmetry distributions yields a value of $\alpha_s(m_Z) = 0.1196 \pm 0.0013 \mbox{ (exp.)}^{+0.0075}_{-0.0045} \mbox{ (theo.)}$.
The cross-section for the production of two jets in association with a leptonically decaying Z boson ($Zjj$) is measured in proton-proton collisions at a centre-of-mass energy of 13 TeV, using data recorded with the ATLAS detector at the Large Hadron Collider, corresponding to an integrated luminosity of 3.2 fb$^{-1}$. The electroweak $Zjj$ cross-section is extracted in a fiducial region chosen to enhance the electroweak contribution relative to the dominant Drell-Yan $Zjj$ process, which is constrained using a data-driven approach. The measured fiducial electroweak cross-section is $\sigma^{Zjj}_{EW}= 119\pm 16 (\mathrm{stat.}) \pm 20 (\mathrm{syst.})\pm 2 (\mathrm{lumi.})$ for dijet invariant mass greater than 250 GeV, and $34.2\pm 5.8 (\mathrm{stat.})\pm 5.5 (\mathrm{syst.})\pm 0.7 (\mathrm{lumi.})$ for dijet invariant mass greater than 1 TeV. Standard Model predictions are in agreement with the measurements. The inclusive $Zjj$ cross-section is also measured in six different fiducial regions with varying contributions from electroweak and Drell-Yan $Zjj$ production.
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