Expected and observed 95% CL upper limits on the production of a heavy, narrow-width, scalar resonance decaying to a pair of Higgs bosons ($X\rightarrow HH$). The final state used in the search consists of a boosted $b\bar{b}$ pair and a boosted hadronically decaying $\tau^{+}\tau^{-}$ pair, and the SM braching ratio of the Higgs boson are assumed. The $\pm 1\sigma$ and $\pm 2\sigma$ variations about the expected limit are indicated by the error bands. Two different requirements are applied on the visible mass of the two boosted Higgs boson candidates for the resonance mass hypotheses of 1.6 TeV and 2.5 TeV, leading to discontinuities in the limits (at 1.6 TeV, the difference between imposing no requirement and $m^{vis}_{HH}>900$ GeV is less than 1% though).

The number of data and fitted simulated events in each bin of the $|d_{0}^{\mu}|$ distribution in the $10<p_{\textrm{T}}^{\mu}<20$ GeV selection in the $\mu-\mu$ channel.

The number of data and fitted simulated events in each bin of the $|d_{0}^{\mu}|$ distribution in the $20<p_{\textrm{T}}^{\mu}<250$ GeV selection in the $e-\mu$ channel.

The number of data and fitted simulated events in each bin of the $|d_{0}^{\mu}|$ distribution in the $20<p_{\textrm{T}}^{\mu}<250$ GeV selection in the $\mu-\mu$ channel.

The measurement of the ratio of the rate of decay of W bosons to τ-leptons and muons, $R(\tau/\mu)=B(W\rightarrow\tau\nu_\tau)/B(W\rightarrow \mu\nu_\mu)$.

Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ = 4 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ = 5 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ = 5 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ = 3 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ = 3 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ = 4 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ = 4 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ = 5 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ = 5 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ = 3 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ = 3 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ = 4 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ = 4 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ = 5 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ = 5 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ $\geq$ 6 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ $\geq$ 6 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ = 3 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ = 3 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ = 4 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ = 4 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ = 5 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ = 5 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ = 3 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ = 3 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ = 4 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ = 4 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ = 5 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ = 5 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ = 3 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ = 3 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ = 4 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ = 4 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ = 5 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ = 5 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ $\geq$ 6 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ $\geq$ 6 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ = 3 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ = 3 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ = 4 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ = 4 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ = 5 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ = 5 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ = 3 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ = 3 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ = 4 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ = 4 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ = 5 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ = 5 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ = 3 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ = 3 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ = 4 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ = 4 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ = 5 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ = 5 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ $\geq$ 6 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ $\geq$ 6 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ = 3 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ = 3 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ = 4 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ = 4 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ = 5 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ = 5 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ = 3 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ = 3 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ = 4 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ = 4 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ = 5 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ = 5 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ = 3 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ = 3 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ = 4 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ = 4 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ = 5 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ = 5 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ $\geq$ 6 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ $\geq$ 6 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ = 3 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ = 3 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ = 4 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ = 4 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ = 5 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ = 5 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ = 3 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ = 3 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ = 4 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ = 4 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ = 5 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ = 5 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ = 3 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ = 3 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ = 4 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ = 4 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ = 5 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ = 5 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ $\geq$ 6 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ $\geq$ 6 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ = 3 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ = 3 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ = 4 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ = 4 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ = 5 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ = 5 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ = 3 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ = 3 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ = 4 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ = 4 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ = 5 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ = 5 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ = 3 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ = 3 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ = 4 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ = 4 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ = 5 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ = 5 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ $\geq$ 6 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ $\geq$ 6 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured total cross section for multijet production as a function of $n^{\textrm{jet}}$ for 1.0 < $H_{\textrm{T2}}$ < 1.5 TeV. The total cross-sections are measured in the same fiducial phase-space region than the measured relative cross-sections as functions of event-shape variables for the corresponding $H_{\textrm{T2}}$ interval. The measurement in the last bin corresponds to $n^{\textrm{jet}}\geq$ 6.

Measured total cross section for multijet production as a function of $n^{\textrm{jet}}$ for 1.0 < $H_{\textrm{T2}}$ < 1.5 TeV. The total cross-sections are measured in the same fiducial phase-space region than the measured relative cross-sections as functions of event-shape variables for the corresponding $H_{\textrm{T2}}$ interval. The measurement in the last bin corresponds to $n^{\textrm{jet}}\geq$ 6.

Measured total cross section for multijet production as a function of $n^{\textrm{jet}}$ for 1.5 < $H_{\textrm{T2}}$ < 2.0 TeV. The total cross-sections are measured in the same fiducial phase-space region than the measured relative cross-sections as functions of event-shape variables for the corresponding $H_{\textrm{T2}}$ interval. The measurement in the last bin corresponds to $n^{\textrm{jet}}\geq$ 6.

Measured total cross section for multijet production as a function of $n^{\textrm{jet}}$ for 1.5 < $H_{\textrm{T2}}$ < 2.0 TeV. The total cross-sections are measured in the same fiducial phase-space region than the measured relative cross-sections as functions of event-shape variables for the corresponding $H_{\textrm{T2}}$ interval. The measurement in the last bin corresponds to $n^{\textrm{jet}}\geq$ 6.

Measured total cross section for multijet production as a function of $n^{\textrm{jet}}$ for $H_{\textrm{T2}}$ > 2.0 TeV. The total cross-sections are measured in the same fiducial phase-space region than the measured relative cross-sections as functions of event-shape variables for the corresponding $H_{\textrm{T2}}$ interval. The measurement in the last bin corresponds to $n^{\textrm{jet}}\geq$ 6.

Measured total cross section for multijet production as a function of $n^{\textrm{jet}}$ for $H_{\textrm{T2}}$ > 2.0 TeV. The total cross-sections are measured in the same fiducial phase-space region than the measured relative cross-sections as functions of event-shape variables for the corresponding $H_{\textrm{T2}}$ interval. The measurement in the last bin corresponds to $n^{\textrm{jet}}\geq$ 6.

Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}\geq$ 3 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}\geq$ 3 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}\geq$4 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}\geq$4 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}\geq$ 5 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}\geq$ 5 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}\geq$ 3 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}\geq$ 3 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}\geq$ 4 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}\geq$ 4 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}\geq$ 5 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}\geq$ 5 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}\geq$ 3 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}\geq$ 3 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}\geq$ 4 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}\geq$ 4 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}\geq$ 5 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}\geq$ 5 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ $\geq$ 6 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ $\geq$ 6 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}\geq$ 3 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}\geq$ 3 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}\geq$ 4 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}\geq$ 4 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}\geq$ 5 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}\geq$ 5 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}\geq$ 3 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}\geq$ 3 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}\geq$ 4 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}\geq$ 4 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}\geq$ 5 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}\geq$ 5 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}\geq$ 3 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}\geq$ 3 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}\geq$ 4 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}\geq$ 4 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}\geq$ 5 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}\geq$ 5 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ $\geq$ 6 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ $\geq$ 6 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}\geq$ 3 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}\geq$ 3 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}\geq$ 4 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}\geq$ 4 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}\geq$ 5 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}\geq$ 5 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}\geq$ 3 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}\geq$ 3 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}\geq$ 4 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}\geq$ 4 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}\geq$ 5 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}\geq$ 5 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}\geq$ 3 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}\geq$ 3 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}\geq$ 4 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}\geq$ 4 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}\geq$ 5 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}\geq$ 5 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ $\geq$ 6 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ $\geq$ 6 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}\geq$ 3 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}\geq$ 3 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}\geq$ 4 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}\geq$ 4 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}\geq$ 5 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}\geq$ 5 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}\geq$ 3 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}\geq$ 3 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}\geq$ 4 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}\geq$ 4 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}\geq$ 5 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}\geq$ 5 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}\geq$ 3 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}\geq$ 3 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}\geq$ 4 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}\geq$ 4 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}\geq$ 5 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}\geq$ 5 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ $\geq$ 6 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ $\geq$ 6 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}\geq$ 3 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}\geq$ 3 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}\geq$ 4 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}\geq$ 4 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}\geq$ 5 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}\geq$ 5 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}\geq$ 3 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}\geq$ 3 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}\geq$ 4 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}\geq$ 4 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}\geq$ 5 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}\geq$ 5 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}\geq$ 3 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}\geq$ 3 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}\geq$ 4 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}\geq$ 4 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}\geq$ 5 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}\geq$ 5 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ $\geq$ 6 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ $\geq$ 6 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}\geq$ 3 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}\geq$ 3 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}\geq$ 4 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}\geq$ 4 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}\geq$ 5 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}\geq$ 5 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}\geq$ 3 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}\geq$ 3 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}\geq$ 4 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}\geq$ 4 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}\geq$ 5 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}\geq$ 5 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.

Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}\geq$ 3 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}\geq$ 3 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}\geq$ 4 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}\geq$ 4 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}\geq$ 5 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}\geq$ 5 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ $\geq$ 6 and $H_{\textrm{T2}}$ > 2.0 TeV.

Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ $\geq$ 6 and $H_{\textrm{T2}}$ > 2.0 TeV.

Signal acceptance times efficiency of HVT ZH(qqbb) events as a function of the resonance mass at different cut stages. Auxiliary table attached for 4 TeV mass point.

The absolute differential cross-section measured in the fiducial phase-space as a function of the minimum $\Delta R$ between the photon and the leptons in the electron-muon channel. The uncertainty is decomposed into four components which are the signal modelling uncertainty, the background modelling uncertainty, the experimental uncertainty, and the data statistical uncertainty.

The absolute differential cross-section measured in the fiducial phase-space as a function of the $\Delta\phi$ between the two leptons in the electron-muon channel. The uncertainty is decomposed into four components which are the signal modelling uncertainty, the background modelling uncertainty, the experimental uncertainty, and the data statistical uncertainty.

The absolute differential cross-section measured in the fiducial phase-space as a function of the $|\Delta\eta|$ between the two leptons in the electron-muon channel. The uncertainty is decomposed into four components which are the signal modelling uncertainty, the background modelling uncertainty, the experimental uncertainty, and the data statistical uncertainty.

The normalised differential cross-section measured in the fiducial phase-space as a function of the photon pT in the electron-muon channel. The uncertainty is decomposed into four components which are the signal modelling uncertainty, the background modelling uncertainty, the experimental uncertainty, and the data statistical uncertainty.

The normalised differential cross-section measured in the fiducial phase-space as a function of the photon $|\eta|$ in the electron-muon channel. The uncertainty is decomposed into four components which are the signal modelling uncertainty, the background modelling uncertainty, the experimental uncertainty, and the data statistical uncertainty.

The normalised differential cross-section measured in the fiducial phase-space as a function of the minimum $\Delta R$ between the photon and the leptons in the electron-muon channel. The uncertainty is decomposed into four components which are the signal modelling uncertainty, the background modelling uncertainty, the experimental uncertainty, and the data statistical uncertainty.

The normalised differential cross-section measured in the fiducial phase-space as a function of the $\Delta\phi$ between the two leptons in the electron-muon channel. The uncertainty is decomposed into four components which are the signal modelling uncertainty, the background modelling uncertainty, the experimental uncertainty, and the data statistical uncertainty.

The normalised differential cross-section measured in the fiducial phase-space as a function of the $|\Delta\eta|$ between the two leptons in the electron-muon channel. The uncertainty is decomposed into four components which are the signal modelling uncertainty, the background modelling uncertainty, the experimental uncertainty, and the data statistical uncertainty.

The total correlation matrix of the absolute differential cross-section measured in the fiducial phase-space as a function of the photon pT in the electron-muon channel. The individual systematic uncertainties are symmetrized before deriving the correlation matrix.

The total correlation matrix of the absolute differential cross-section measured in the fiducial phase-space as a function of the photon $|\eta|$ in the electron-muon channel. The individual systematic uncertainties are symmetrized before deriving the correlation matrix.

The total correlation matrix of the absolute differential cross-section measured in the fiducial phase-space as a function of the minimum $\Delta R$ between the photon and the leptons in the electron-muon channel. The individual systematic uncertainties are symmetrized before deriving the correlation matrix.

The total correlation matrix of the absolute differential cross-section measured in the fiducial phase-space as a function of the $\Delta\phi$ between the two leptons in the electron-muon channel. The individual systematic uncertainties are symmetrized before deriving the correlation matrix.

The total correlation matrix of the absolute differential cross-section measured in the fiducial phase-space as a function of the $|\Delta\eta|$ between the two leptons in the electron-muon channel. The individual systematic uncertainties are symmetrized before deriving the correlation matrix.

The total correlation matrix of the normalised differential cross-section measured in the fiducial phase-space as a function of the photon pT in the electron-muon channel. The individual systematic uncertainties are symmetrized before deriving the correlation matrix.

The total correlation matrix of the normalised differential cross-section measured in the fiducial phase-space as a function of the photon $|\eta|$ in the electron-muon channel. The individual systematic uncertainties are symmetrized before deriving the correlation matrix.

The total correlation matrix of the normalised differential cross-section measured in the fiducial phase-space as a function of the minimum $\Delta R$ between the photon and the leptons in the electron-muon channel. The individual systematic uncertainties are symmetrized before deriving the correlation matrix.

The total correlation matrix of the normalised differential cross-section measured in the fiducial phase-space as a function of the $\Delta\phi$ between the two leptons in the electron-muon channel. The individual systematic uncertainties are symmetrized before deriving the correlation matrix.

The total correlation matrix of the normalised differential cross-section measured in the fiducial phase-space as a function of the $|\Delta\eta|$ between the two leptons in the electron-muon channel. The individual systematic uncertainties are symmetrized before deriving the correlation matrix.

The statistical correlation matrix of all the absolute differential cross-sections measured in the fiducial phase-space in the electron-muon channel.

The statistical correlation matrix of all the normalised differential cross-sections measured in the fiducial phase-space in the electron-muon channel.

Fiducial region definition.

Observed correlations between the measured reduced stage-1.2 simplified template $VH, H \rightarrow b\bar{b}$ cross-sections (STXS), including both the statistical and systematic uncertainties. All leptonic decays of the $V$ bosons (including those to $\tau$ leptons, $\ell = e, \mu, \tau$) are considered.

Linear combination of Wilson coefficients corresponding to SMEFT operators in the Warsaw basis for which this analysis provides orthogonal constraints (eigenvectors). Eigenvalues are shown for each eigenvector, which provides a measure of the experimental sensitivity to that linear combination. The modifications to the $qq\rightarrow ZH$ and $qq\rightarrow WH$ processes due to SMEFT operators are computed at LO, and changes to the $gg\rightarrow ZH$ process are neglected.

Linear combination of Wilson coefficients corresponding to SMEFT operators in the Warsaw basis for which this analysis provides orthogonal constraints (eigenvectors). Eigenvalues are shown for each eigenvector, which provides a measure of the experimental sensitivity to that linear combination. The modifications to the $qq\rightarrow ZH$ and $qq\rightarrow WH$ processes due to SMEFT operators are computed at LO, and changes to the $gg\rightarrow ZH$ process are neglected.

Differential cross-sections for EW $Zjj$ production as a function of $\Delta\phi_{jj}$ with breakdown of associated uncertainties. The statistical uncertainty is correlated across bins according to the statistical cross correlation matrix presented in Table 21.

Differential cross-sections for inclusive $Zjj$ production in the EW $Zjj$ signal region ($N^\mathrm{gap}_\mathrm{jets}=0$, $\xi_Z < 0.5$) as a function of $m_{jj}$ with breakdown of associated uncertainties.

Differential cross-sections for inclusive $Zjj$ production in the EW $Zjj$ signal region ($N^\mathrm{gap}_\mathrm{jets}=0$, $\xi_Z < 0.5$) as a function of $\Delta y_{jj}$ with breakdown of associated uncertainties.

Differential cross-sections for inclusive $Zjj$ production in the EW $Zjj$ signal region ($N^\mathrm{gap}_\mathrm{jets}=0$, $\xi_Z < 0.5$) as a function of $p_{\mathrm{T},\ell\ell}$ with breakdown of associated uncertainties.

Differential cross-sections for inclusive $Zjj$ production in the EW $Zjj$ signal region ($N^\mathrm{gap}_\mathrm{jets}=0$, $\xi_Z < 0.5$) as a function of $\Delta\phi_{jj}$ with breakdown of associated uncertainties.

Differential cross-sections for inclusive $Zjj$ production in control region CRa ($N^\mathrm{gap}_\mathrm{jets} \geq 1$, $\xi_Z < 0.5$) as a function of $m_{jj}$ with breakdown of associated uncertainties.

Differential cross-sections for inclusive $Zjj$ production in control region CRa ($N^\mathrm{gap}_\mathrm{jets} \geq 1$, $\xi_Z < 0.5$) as a function of $\Delta y_{jj}$ with breakdown of associated uncertainties.

Differential cross-sections for inclusive $Zjj$ production in control region CRa ($N^\mathrm{gap}_\mathrm{jets} \geq 1$, $\xi_Z < 0.5$) as a function of $p_{\mathrm{T},\ell\ell}$ with breakdown of associated uncertainties.

Differential cross-sections for inclusive $Zjj$ production in control region CRa ($N^\mathrm{gap}_\mathrm{jets} \geq 1$, $\xi_Z < 0.5$) as a function of $\Delta\phi_{jj}$ with breakdown of associated uncertainties.

Differential cross-sections for inclusive $Zjj$ production in control region CRb ($N^\mathrm{gap}_\mathrm{jets} \geq 1$, $\xi_Z > 0.5$) as a function of $m_{jj}$ with breakdown of associated uncertainties.

Differential cross-sections for inclusive $Zjj$ production in control region CRb ($N^\mathrm{gap}_\mathrm{jets} \geq 1$, $\xi_Z > 0.5$) as a function of $\Delta y_{jj}$ with breakdown of associated uncertainties.

Differential cross-sections for inclusive $Zjj$ production in control region CRb ($N^\mathrm{gap}_\mathrm{jets} \geq 1$, $\xi_Z > 0.5$) as a function of $p_{\mathrm{T},\ell\ell}$ with breakdown of associated uncertainties.

Differential cross-sections for inclusive $Zjj$ production in control region CRb ($N^\mathrm{gap}_\mathrm{jets} \geq 1$, $\xi_Z > 0.5$) as a function of $\Delta\phi_{jj}$ with breakdown of associated uncertainties.

Differential cross-sections for inclusive $Zjj$ production in control region CRc ($N^\mathrm{gap}_\mathrm{jets} = 0$, $\xi_Z > 0.5$) as a function of $m_{jj}$ with breakdown of associated uncertainties.

Differential cross-sections for inclusive $Zjj$ production in control region CRc ($N^\mathrm{gap}_\mathrm{jets} = 0$, $\xi_Z > 0.5$) as a function of $\Delta y_{jj}$ with breakdown of associated uncertainties.

Differential cross-sections for inclusive $Zjj$ production in control region CRc ($N^\mathrm{gap}_\mathrm{jets} = 0$, $\xi_Z > 0.5$) as a function of $p_{\mathrm{T},\ell\ell}$ with breakdown of associated uncertainties.

Differential cross-sections for inclusive $Zjj$ production in control region CRc ($N^\mathrm{gap}_\mathrm{jets} = 0$, $\xi_Z > 0.5$) as a function of $\Delta\phi_{jj}$ with breakdown of associated uncertainties.

Statistical correlation between bins of the differential cross-section measurements of EW $Zjj$ production in the signal region ($N^\mathrm{gap}_\mathrm{jets} = 0$, $\xi_Z < 0.5$). The associated measured central values, statistical uncertainty magnitude and bin ranges are presented in Tables 1-4. The bins are presented in order such that for example mjj_bin_1 spans $m_{jj} \in (1000,1500)$ GeV (see Table 1), while pT_ll_bin7 spans $p_\mathrm{T}^{ll} \in (200,275)$ GeV (see Table 3).

Lower limits at 95$\%$ CL on $\Lambda$ for the dimuon channel for different signal chiralities in the (constructive/destructive interference) SRs of the analysis.

Lower limits at 95$\%$ CL on $\Lambda$ for the dilepton combination for different signal chiralities in the (constructive/destructive interference) SRs of the analysis.

The dielectron data events passing the full selection.

The dimuon data events passing the full selection.

Impact of different categories of systematic uncertainties on the fiducial and inclusive measurements. The quoted values are obtained by repeating the fit, fixing a set of nuisance parameters of the sources corresponding to the considered category, and subtracting in quadrature the resulting uncertainty from the total uncertainty of the nominal fit. The total uncertainty is different from the sum in quadrature of the different components due to correlations between nuisance parameters built by the fit.

Fiducial region definition

Absolute differential cross-section as a function of $\Delta R^{extra1}_{jet1}$ at particle level in the all hadronic 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 $\Delta R^{extra1}_{jet1}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $|y^{t,1}|$ at particle level in the all hadronic 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 $|y^{t,1}|$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $|y^{t,1}|$ at particle level in the all hadronic 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 $|y^{t,1}|$ at particle level in the all hadronic 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 all hadronic 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 all hadronic 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 all hadronic 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 all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $|y^{t,2}|$ at particle level in the all hadronic 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 $|y^{t,2}|$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $|y^{t,2}|$ at particle level in the all hadronic 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 $|y^{t,2}|$ at particle level in the all hadronic 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 all hadronic 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 all hadronic 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 all hadronic 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 all hadronic 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 all hadronic 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 all hadronic 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 all hadronic 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 all hadronic 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 all hadronic 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 all hadronic 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 all hadronic 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 all hadronic 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 all hadronic 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 all hadronic 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 all hadronic 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 all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $N_{jets}$ at particle level in the all hadronic 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 $N_{jets}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $N_{jets}$ at particle level in the all hadronic 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 $N_{jets}$ at particle level in the all hadronic 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 all hadronic 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 all hadronic 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 all hadronic 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 all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $|P_{out}^{t,1}|$ at particle level in the all hadronic 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 $|P_{out}^{t,1}|$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $|P_{out}^{t,1}|$ at particle level in the all hadronic 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 $|P_{out}^{t,1}|$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $|P_{cross}|$ at particle level in the all hadronic 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 $|P_{cross}|$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $|P_{cross}|$ at particle level in the all hadronic 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 $|P_{cross}|$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $Z^{t\bar{t}}$ at particle level in the all hadronic 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 $Z^{t\bar{t}}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $Z^{t\bar{t}}$ at particle level in the all hadronic 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 $Z^{t\bar{t}}$ at particle level in the all hadronic 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 all hadronic 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 all hadronic 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 all hadronic 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 all hadronic 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 all hadronic 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 all hadronic 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 all hadronic 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 all hadronic 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 all hadronic 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 all hadronic 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 all hadronic 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 all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $R_{Wt}^{leading}$ at particle level in the all hadronic 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 $R_{Wt}^{leading}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $R_{Wt}^{leading}$ at particle level in the all hadronic 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 $R_{Wt}^{leading}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $R_{Wt}^{subleading}$ at particle level in the all hadronic 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 $R_{Wt}^{subleading}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $R_{Wt}^{subleading}$ at particle level in the all hadronic 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 $R_{Wt}^{subleading}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $R_{Wb}^{leading}$ at particle level in the all hadronic 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 $R_{Wb}^{leading}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $R_{Wb}^{leading}$ at particle level in the all hadronic 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 $R_{Wb}^{leading}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $R_{Wb}^{subleading}$ at particle level in the all hadronic 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 $R_{Wb}^{subleading}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $R_{Wb}^{subleading}$ at particle level in the all hadronic 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 $R_{Wb}^{subleading}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $\Delta R^{extra1}_{t,close}$ at particle level in the all hadronic 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 $\Delta R^{extra1}_{t,close}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $\Delta R^{extra1}_{t,close}$ at particle level in the all hadronic 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 $\Delta R^{extra1}_{t,close}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $\Delta R^{extra2}_{t,close}$ at particle level in the all hadronic 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 $\Delta R^{extra2}_{t,close}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $\Delta R^{extra2}_{t,close}$ at particle level in the all hadronic 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 $\Delta R^{extra2}_{t,close}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $\Delta R^{extra3}_{t,close}$ at particle level in the all hadronic 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 $\Delta R^{extra3}_{t,close}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $\Delta R^{extra3}_{t,close}$ at particle level in the all hadronic 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 $\Delta R^{extra3}_{t,close}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $R^{pT, extra1}_{t,1}$ at particle level in the all hadronic 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 $R^{pT, extra1}_{t,1}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $R^{pT, extra1}_{t,1}$ at particle level in the all hadronic 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 $R^{pT, extra1}_{t,1}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $R^{pT, extra2}_{t,1}$ at particle level in the all hadronic 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 $R^{pT, extra2}_{t,1}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $R^{pT, extra2}_{t,1}$ at particle level in the all hadronic 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 $R^{pT, extra2}_{t,1}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $R^{pT, extra3}_{t,1}$ at particle level in the all hadronic 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 $R^{pT, extra3}_{t,1}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $R^{pT, extra3}_{t,1}$ at particle level in the all hadronic 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 $R^{pT, extra3}_{t,1}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $R^{pT, t\bar{t}}_{extra1}$ at particle level in the all hadronic 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 $R^{pT, t\bar{t}}_{extra1}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $R^{pT, t\bar{t}}_{extra1}$ at particle level in the all hadronic 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 $R^{pT, t\bar{t}}_{extra1}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $R^{pT, extra1}_{jet1}$ at particle level in the all hadronic 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 $R^{pT, extra1}_{jet1}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $R^{pT, extra1}_{jet1}$ at particle level in the all hadronic 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 $R^{pT, extra1}_{jet1}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $R^{pT, extra2}_{jet1}$ at particle level in the all hadronic 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 $R^{pT, extra2}_{jet1}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $R^{pT, extra2}_{jet1}$ at particle level in the all hadronic 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 $R^{pT, extra2}_{jet1}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $R^{pT, extra3}_{jet1}$ at particle level in the all hadronic 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 $R^{pT, extra3}_{jet1}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $R^{pT, extra3}_{jet1}$ at particle level in the all hadronic 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 $R^{pT, extra3}_{jet1}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $\Delta R^{extra2}_{extra1}$ at particle level in the all hadronic 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 $\Delta R^{extra2}_{extra1}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $\Delta R^{extra2}_{extra1}$ at particle level in the all hadronic 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 $\Delta R^{extra2}_{extra1}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $\Delta R^{extra3}_{extra1}$ at particle level in the all hadronic 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 $\Delta R^{extra3}_{extra1}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $\Delta R^{extra3}_{extra1}$ at particle level in the all hadronic 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 $\Delta R^{extra3}_{extra1}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $R^{pT, extra2}_{extra1}$ at particle level in the all hadronic 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 $R^{pT, extra2}_{extra1}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $R^{pT, extra2}_{extra1}$ at particle level in the all hadronic 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 $R^{pT, extra2}_{extra1}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $R^{pT, extra3}_{extra1}$ at particle level in the all hadronic 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 $R^{pT, extra3}_{extra1}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $R^{pT, extra3}_{extra1}$ at particle level in the all hadronic 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 $R^{pT, extra3}_{extra1}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Total cross-section at particle level in the all hadronic 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 $p_{T}^{t,1}$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 6. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-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 $p_{T}^{t,1}$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 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 $p_{T}^{t,1}$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 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 $p_{T}^{t,1}$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ > 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.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ = 6 and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ = 7 and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ = 7 and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ = 8 and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ = 8 and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ = 8 and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ = 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ > 8 and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ > 8 and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ > 8 and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ = 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ > 8 and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ > 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute double-differential cross-section as a function of $p_{T}^{t,1}$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 6. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-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 $p_{T}^{t,1}$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 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 $p_{T}^{t,1}$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 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 $p_{T}^{t,1}$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ > 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.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ = 6 and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ = 7 and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ = 7 and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ = 8 and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ = 8 and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ = 8 and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ = 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ > 8 and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ > 8 and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ > 8 and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ = 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ > 8 and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $N_{jets}$ in $N_{jets}$ > 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative double-differential cross-section as a function of $p_{T}^{t,2}$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 6. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-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 $p_{T}^{t,2}$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 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 $p_{T}^{t,2}$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 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 $p_{T}^{t,2}$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ > 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.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ = 6 and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ = 7 and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ = 7 and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ = 8 and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ = 8 and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ = 8 and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ = 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ > 8 and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ > 8 and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ > 8 and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ = 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ > 8 and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ > 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute double-differential cross-section as a function of $p_{T}^{t,2}$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 6. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-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 $p_{T}^{t,2}$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 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 $p_{T}^{t,2}$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 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 $p_{T}^{t,2}$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ > 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.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ = 6 and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ = 7 and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ = 7 and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ = 8 and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ = 8 and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ = 8 and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ = 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ > 8 and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ > 8 and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ > 8 and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ = 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ > 8 and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $N_{jets}$ in $N_{jets}$ > 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 6. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-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 all hadronic resolved topology in $N_{jets}$ = 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 $p_{T}^{t\bar{t}}$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 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 $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ > 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.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 6 and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 7 and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 7 and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 8 and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 8 and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 8 and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ > 8 and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ > 8 and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ > 8 and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ > 8 and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ > 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 6. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-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 all hadronic resolved topology in $N_{jets}$ = 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 $p_{T}^{t\bar{t}}$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 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 $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ > 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.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 6 and the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 7 and the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 7 and the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 8 and the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 8 and the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 8 and the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ > 8 and the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ > 8 and the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ > 8 and the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ > 8 and the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ > 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative double-differential cross-section as a function of $|P_{out}^{t,1}|$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 6. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-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 $|P_{out}^{t,1}|$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 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 $|P_{out}^{t,1}|$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 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 $|P_{out}^{t,1}|$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ > 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.

Covariance matrix between the relative double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ = 6 and the relative double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ = 7 and the relative double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ = 7 and the relative double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ = 8 and the relative double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ = 8 and the relative double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ = 8 and the relative double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ = 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ > 8 and the relative double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ > 8 and the relative double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ > 8 and the relative double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ = 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ > 8 and the relative double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ > 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute double-differential cross-section as a function of $|P_{out}^{t,1}|$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 6. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-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 $|P_{out}^{t,1}|$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 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 $|P_{out}^{t,1}|$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 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 $|P_{out}^{t,1}|$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ > 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.

Covariance matrix between the absolute double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ = 6 and the absolute double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ = 7 and the absolute double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ = 7 and the absolute double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ = 8 and the absolute double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ = 8 and the absolute double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ = 8 and the absolute double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ = 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ > 8 and the absolute double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ > 8 and the absolute double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ > 8 and the absolute double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ = 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ > 8 and the absolute double-differential cross-section as function of $|P_{out}^{t,1}|$ vs $N_{jets}$ in $N_{jets}$ > 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative double-differential cross-section as a function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 6. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-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 all hadronic resolved topology in $N_{jets}$ = 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 $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 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 $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ > 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.

Covariance matrix between the relative double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 6 and the relative double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 7 and the relative double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 7 and the relative double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 8 and the relative double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 8 and the relative double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 8 and the relative double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ > 8 and the relative double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ > 8 and the relative double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ > 8 and the relative double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ > 8 and the relative double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ > 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute double-differential cross-section as a function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 6. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-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 all hadronic resolved topology in $N_{jets}$ = 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 $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 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 $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ > 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.

Covariance matrix between the absolute double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 6 and the absolute double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 7 and the absolute double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 7 and the absolute double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 8 and the absolute double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 8 and the absolute double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 8 and the absolute double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ > 8 and the absolute double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ > 8 and the absolute double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ > 8 and the absolute double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ = 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ > 8 and the absolute double-differential cross-section as function of $\Delta\phi^{t\bar{t}}$ vs $N_{jets}$ in $N_{jets}$ > 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative double-differential cross-section as a function of $|P_{cross}|$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 6. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-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 $|P_{cross}|$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 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 $|P_{cross}|$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 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 $|P_{cross}|$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ > 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.

Covariance matrix between the relative double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ = 6 and the relative double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ = 7 and the relative double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ = 7 and the relative double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ = 8 and the relative double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ = 8 and the relative double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ = 8 and the relative double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ = 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ > 8 and the relative double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ > 8 and the relative double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ > 8 and the relative double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ = 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ > 8 and the relative double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ > 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute double-differential cross-section as a function of $|P_{cross}|$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 6. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-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 $|P_{cross}|$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 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 $|P_{cross}|$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ = 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 $|P_{cross}|$ vs $N_{jets}$ at particle level in the all hadronic resolved topology in $N_{jets}$ > 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.

Covariance matrix between the absolute double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ = 6 and the absolute double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ = 7 and the absolute double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ = 7 and the absolute double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ = 8 and the absolute double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ = 8 and the absolute double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ = 8 and the absolute double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ = 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ > 8 and the absolute double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ = 6 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ > 8 and the absolute double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ = 7 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ > 8 and the absolute double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ = 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ > 8 and the absolute double-differential cross-section as function of $|P_{cross}|$ vs $N_{jets}$ in $N_{jets}$ > 8 at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative double-differential cross-section as a function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ at particle level in the all hadronic resolved topology in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 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 $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ at particle level in the all hadronic resolved topology in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 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 $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ at particle level in the all hadronic resolved topology in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 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 $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ at particle level in the all hadronic resolved topology in 1050.0 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 $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute double-differential cross-section as a function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ at particle level in the all hadronic resolved topology in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 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 $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ at particle level in the all hadronic resolved topology in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 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 $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ at particle level in the all hadronic resolved topology in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 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 $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ at particle level in the all hadronic resolved topology in 1050.0 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 $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ at particle level in the all hadronic resolved topology in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 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 all hadronic resolved topology in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 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 all hadronic resolved topology in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 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 all hadronic resolved topology in 1050.0 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 $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ at particle level in the all hadronic resolved topology in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 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 all hadronic resolved topology in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 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 all hadronic resolved topology in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 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 all hadronic resolved topology in 1050.0 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 $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative double-differential cross-section as a function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ at particle level in the all hadronic resolved topology in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 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 $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ at particle level in the all hadronic resolved topology in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 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 $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ at particle level in the all hadronic resolved topology in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 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 $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ at particle level in the all hadronic resolved topology in 1050.0 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 $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV and the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV and the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV and the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV and the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV and the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV and the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute double-differential cross-section as a function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ at particle level in the all hadronic resolved topology in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 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 $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ at particle level in the all hadronic resolved topology in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 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 $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ at particle level in the all hadronic resolved topology in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 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 $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ at particle level in the all hadronic resolved topology in 1050.0 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 $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV and the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV and the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV and the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV and the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV and the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV and the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 620.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 620.0 GeV < $m^{t\bar{t}}$ < 835.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 835.0 GeV < $m^{t\bar{t}}$ < 1050.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 1050.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative double-differential cross-section as a function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ at particle level in the all hadronic resolved topology in 0.0 GeV < $p_{T}^{t,2}$ < 175.0 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 $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ at particle level in the all hadronic resolved topology in 175.0 GeV < $p_{T}^{t,2}$ < 275.0 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 $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ at particle level in the all hadronic resolved topology in 275.0 GeV < $p_{T}^{t,2}$ < 385.0 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 $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ at particle level in the all hadronic resolved topology in 385.0 GeV < $p_{T}^{t,2}$ < 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 $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 0.0 GeV < $p_{T}^{t,2}$ < 175.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 0.0 GeV < $p_{T}^{t,2}$ < 175.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 175.0 GeV < $p_{T}^{t,2}$ < 275.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 0.0 GeV < $p_{T}^{t,2}$ < 175.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 175.0 GeV < $p_{T}^{t,2}$ < 275.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 175.0 GeV < $p_{T}^{t,2}$ < 275.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 275.0 GeV < $p_{T}^{t,2}$ < 385.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 0.0 GeV < $p_{T}^{t,2}$ < 175.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 275.0 GeV < $p_{T}^{t,2}$ < 385.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 175.0 GeV < $p_{T}^{t,2}$ < 275.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 275.0 GeV < $p_{T}^{t,2}$ < 385.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 275.0 GeV < $p_{T}^{t,2}$ < 385.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 385.0 GeV < $p_{T}^{t,2}$ < 1000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 0.0 GeV < $p_{T}^{t,2}$ < 175.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 385.0 GeV < $p_{T}^{t,2}$ < 1000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 175.0 GeV < $p_{T}^{t,2}$ < 275.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 385.0 GeV < $p_{T}^{t,2}$ < 1000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 275.0 GeV < $p_{T}^{t,2}$ < 385.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 385.0 GeV < $p_{T}^{t,2}$ < 1000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 385.0 GeV < $p_{T}^{t,2}$ < 1000.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute double-differential cross-section as a function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ at particle level in the all hadronic resolved topology in 0.0 GeV < $p_{T}^{t,2}$ < 175.0 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 $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ at particle level in the all hadronic resolved topology in 175.0 GeV < $p_{T}^{t,2}$ < 275.0 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 $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ at particle level in the all hadronic resolved topology in 275.0 GeV < $p_{T}^{t,2}$ < 385.0 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 $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ at particle level in the all hadronic resolved topology in 385.0 GeV < $p_{T}^{t,2}$ < 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 $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 0.0 GeV < $p_{T}^{t,2}$ < 175.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 0.0 GeV < $p_{T}^{t,2}$ < 175.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 175.0 GeV < $p_{T}^{t,2}$ < 275.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 0.0 GeV < $p_{T}^{t,2}$ < 175.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 175.0 GeV < $p_{T}^{t,2}$ < 275.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 175.0 GeV < $p_{T}^{t,2}$ < 275.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 275.0 GeV < $p_{T}^{t,2}$ < 385.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 0.0 GeV < $p_{T}^{t,2}$ < 175.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 275.0 GeV < $p_{T}^{t,2}$ < 385.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 175.0 GeV < $p_{T}^{t,2}$ < 275.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 275.0 GeV < $p_{T}^{t,2}$ < 385.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 275.0 GeV < $p_{T}^{t,2}$ < 385.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 385.0 GeV < $p_{T}^{t,2}$ < 1000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 0.0 GeV < $p_{T}^{t,2}$ < 175.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 385.0 GeV < $p_{T}^{t,2}$ < 1000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 175.0 GeV < $p_{T}^{t,2}$ < 275.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 385.0 GeV < $p_{T}^{t,2}$ < 1000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 275.0 GeV < $p_{T}^{t,2}$ < 385.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 385.0 GeV < $p_{T}^{t,2}$ < 1000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 385.0 GeV < $p_{T}^{t,2}$ < 1000.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative double-differential cross-section as a function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ at particle level in the all hadronic resolved topology in 0.0 GeV < $m^{t\bar{t}}$ < 645.0 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 $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ at particle level in the all hadronic resolved topology in 645.0 GeV < $m^{t\bar{t}}$ < 795.0 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 $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ at particle level in the all hadronic resolved topology in 795.0 GeV < $m^{t\bar{t}}$ < 1080.0 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 $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ at particle level in the all hadronic resolved topology in 1080.0 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 $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 645.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 645.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 645.0 GeV < $m^{t\bar{t}}$ < 795.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 645.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 645.0 GeV < $m^{t\bar{t}}$ < 795.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 645.0 GeV < $m^{t\bar{t}}$ < 795.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 795.0 GeV < $m^{t\bar{t}}$ < 1080.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 645.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 795.0 GeV < $m^{t\bar{t}}$ < 1080.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 645.0 GeV < $m^{t\bar{t}}$ < 795.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 795.0 GeV < $m^{t\bar{t}}$ < 1080.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 795.0 GeV < $m^{t\bar{t}}$ < 1080.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 1080.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 645.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 1080.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 645.0 GeV < $m^{t\bar{t}}$ < 795.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 1080.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 795.0 GeV < $m^{t\bar{t}}$ < 1080.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 1080.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 1080.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute double-differential cross-section as a function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ at particle level in the all hadronic resolved topology in 0.0 GeV < $m^{t\bar{t}}$ < 645.0 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 $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ at particle level in the all hadronic resolved topology in 645.0 GeV < $m^{t\bar{t}}$ < 795.0 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 $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ at particle level in the all hadronic resolved topology in 795.0 GeV < $m^{t\bar{t}}$ < 1080.0 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 $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ at particle level in the all hadronic resolved topology in 1080.0 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 $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 645.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 645.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 645.0 GeV < $m^{t\bar{t}}$ < 795.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 645.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 645.0 GeV < $m^{t\bar{t}}$ < 795.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 645.0 GeV < $m^{t\bar{t}}$ < 795.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 795.0 GeV < $m^{t\bar{t}}$ < 1080.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 645.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 795.0 GeV < $m^{t\bar{t}}$ < 1080.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 645.0 GeV < $m^{t\bar{t}}$ < 795.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 795.0 GeV < $m^{t\bar{t}}$ < 1080.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 795.0 GeV < $m^{t\bar{t}}$ < 1080.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 1080.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 645.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 1080.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 645.0 GeV < $m^{t\bar{t}}$ < 795.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 1080.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 795.0 GeV < $m^{t\bar{t}}$ < 1080.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 1080.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ in 1080.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $\chi^{t\bar{t}}$ at parton level in the all hadronic 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 parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $\chi^{t\bar{t}}$ at parton level in the all hadronic 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 parton level in the all hadronic 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 all hadronic 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 all hadronic 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 all hadronic 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 all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $\Delta\phi^{t\bar{t}}$ at parton level in the all hadronic 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 parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $\Delta\phi^{t\bar{t}}$ at parton level in the all hadronic 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 parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $p_{T}^{t,2}$ at parton level in the all hadronic 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 parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $p_{T}^{t,2}$ at parton level in the all hadronic 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 parton level in the all hadronic 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 all hadronic 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 all hadronic 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 all hadronic 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 all hadronic 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 all hadronic 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 all hadronic 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 all hadronic 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 all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $p_{T}^{t,1}$ at parton level in the all hadronic 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 parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $p_{T}^{t,1}$ at parton level in the all hadronic 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 parton level in the all hadronic 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 all hadronic 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 all hadronic 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 all hadronic 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 all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $|y^{t,2}|$ at parton level in the all hadronic 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 $|y^{t,2}|$ at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $|y^{t,2}|$ at parton level in the all hadronic 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 $|y^{t,2}|$ at parton level in the all hadronic 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 all hadronic 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 all hadronic 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 all hadronic 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 all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative differential cross-section as a function of $|y^{t,1}|$ at parton level in the all hadronic 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 $|y^{t,1}|$ at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute differential cross-section as a function of $|y^{t,1}|$ at parton level in the all hadronic 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 $|y^{t,1}|$ at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative double-differential cross-section as a function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 0.0 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 $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 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 $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 970.0 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 $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute double-differential cross-section as a function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 0.0 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 $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 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 $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 970.0 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 $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative double-differential cross-section as a function of $|y^{t,2}|$ vs $|y^{t,1}|$ at parton level in the all hadronic resolved topology in 0.0 < $|y^{t,1}|$ < 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 $|y^{t,2}|$ vs $|y^{t,1}|$ at parton level in the all hadronic resolved topology in 0.5 < $|y^{t,1}|$ < 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 $|y^{t,2}|$ vs $|y^{t,1}|$ at parton level in the all hadronic resolved topology in 1.0 < $|y^{t,1}|$ < 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 $|y^{t,2}|$ vs $|y^{t,1}|$ at parton level in the all hadronic resolved topology in 1.5 < $|y^{t,1}|$ < 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 $|y^{t,2}|$ vs $|y^{t,1}|$ in 0.0 < $|y^{t,1}|$ < 0.5 and the relative double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 0.0 < $|y^{t,1}|$ < 0.5 at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 0.5 < $|y^{t,1}|$ < 1.0 and the relative double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 0.0 < $|y^{t,1}|$ < 0.5 at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 0.5 < $|y^{t,1}|$ < 1.0 and the relative double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 0.5 < $|y^{t,1}|$ < 1.0 at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 1.0 < $|y^{t,1}|$ < 1.5 and the relative double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 0.0 < $|y^{t,1}|$ < 0.5 at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 1.0 < $|y^{t,1}|$ < 1.5 and the relative double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 0.5 < $|y^{t,1}|$ < 1.0 at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 1.0 < $|y^{t,1}|$ < 1.5 and the relative double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 1.0 < $|y^{t,1}|$ < 1.5 at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 1.5 < $|y^{t,1}|$ < 2.5 and the relative double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 0.0 < $|y^{t,1}|$ < 0.5 at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 1.5 < $|y^{t,1}|$ < 2.5 and the relative double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 0.5 < $|y^{t,1}|$ < 1.0 at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 1.5 < $|y^{t,1}|$ < 2.5 and the relative double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 1.0 < $|y^{t,1}|$ < 1.5 at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 1.5 < $|y^{t,1}|$ < 2.5 and the relative double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 1.5 < $|y^{t,1}|$ < 2.5 at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute double-differential cross-section as a function of $|y^{t,2}|$ vs $|y^{t,1}|$ at parton level in the all hadronic resolved topology in 0.0 < $|y^{t,1}|$ < 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 $|y^{t,2}|$ vs $|y^{t,1}|$ at parton level in the all hadronic resolved topology in 0.5 < $|y^{t,1}|$ < 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 $|y^{t,2}|$ vs $|y^{t,1}|$ at parton level in the all hadronic resolved topology in 1.0 < $|y^{t,1}|$ < 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 $|y^{t,2}|$ vs $|y^{t,1}|$ at parton level in the all hadronic resolved topology in 1.5 < $|y^{t,1}|$ < 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 $|y^{t,2}|$ vs $|y^{t,1}|$ in 0.0 < $|y^{t,1}|$ < 0.5 and the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 0.0 < $|y^{t,1}|$ < 0.5 at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 0.5 < $|y^{t,1}|$ < 1.0 and the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 0.0 < $|y^{t,1}|$ < 0.5 at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 0.5 < $|y^{t,1}|$ < 1.0 and the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 0.5 < $|y^{t,1}|$ < 1.0 at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 1.0 < $|y^{t,1}|$ < 1.5 and the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 0.0 < $|y^{t,1}|$ < 0.5 at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 1.0 < $|y^{t,1}|$ < 1.5 and the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 0.5 < $|y^{t,1}|$ < 1.0 at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 1.0 < $|y^{t,1}|$ < 1.5 and the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 1.0 < $|y^{t,1}|$ < 1.5 at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 1.5 < $|y^{t,1}|$ < 2.5 and the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 0.0 < $|y^{t,1}|$ < 0.5 at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 1.5 < $|y^{t,1}|$ < 2.5 and the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 0.5 < $|y^{t,1}|$ < 1.0 at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 1.5 < $|y^{t,1}|$ < 2.5 and the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 1.0 < $|y^{t,1}|$ < 1.5 at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 1.5 < $|y^{t,1}|$ < 2.5 and the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $|y^{t,1}|$ in 1.5 < $|y^{t,1}|$ < 2.5 at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative double-differential cross-section as a function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 0.0 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 $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 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 $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 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 $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 1315.0 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 $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 1315.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 1315.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 1315.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 1315.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 1315.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute double-differential cross-section as a function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 0.0 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 $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 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 $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 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 $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 1315.0 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 $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 1315.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 1315.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 1315.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 1315.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,2}$ vs $m^{t\bar{t}}$ in 1315.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative double-differential cross-section as a function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 0.0 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 $|y^{t,1}|$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 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 $|y^{t,1}|$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 970.0 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 $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the relative double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the relative double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the relative double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute double-differential cross-section as a function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 0.0 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 $|y^{t,1}|$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 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 $|y^{t,1}|$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 970.0 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 $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the absolute double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the absolute double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the absolute double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $|y^{t,1}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative double-differential cross-section as a function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 0.0 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 $|y^{t,2}|$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 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 $|y^{t,2}|$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 970.0 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 $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the relative double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the relative double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the relative double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute double-differential cross-section as a function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 0.0 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 $|y^{t,2}|$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 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 $|y^{t,2}|$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 970.0 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 $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $|y^{t,2}|$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Relative double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Relative double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 1315.0 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 $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1315.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1315.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1315.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1315.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1315.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 1315.0 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 $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 0.0 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 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 0.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 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 < $m^{t\bar{t}}$ < 970.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Covariance matrix between the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1315.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 970.0 GeV < $m^{t\bar{t}}$ < 1315.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute double-differential cross-section as a function of $p_{T}^{t,1}$ vs $m^{t\bar{t}}$ at parton level in the all hadronic resolved topology in 970.0 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 $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 170.0 GeV < $p_{T}^{t,2}$ < 290.0 GeV and the relative double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 170.0 GeV < $p_{T}^{t,2}$ < 290.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

Absolute double-differential cross-section as a function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ at parton level in the all hadronic resolved topology in 290.0 GeV < $p_{T}^{t,2}$ < 450.0 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 $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 450.0 GeV < $p_{T}^{t,2}$ < 1000.0 GeV and the absolute double-differential cross-section as function of $p_{T}^{t,1}$ vs $p_{T}^{t,2}$ in 290.0 GeV < $p_{T}^{t,2}$ < 450.0 GeV at parton level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.