Detailed list of the contribution of each source of uncertainty to the total uncertainty on the measured values of $\sigma(tq)$, $\sigma(\bar{t}q)$, $R_t$, and $\sigma(tq+\bar{t}q)$. The evaluation of the systematic uncertainties has a statistical uncertainty of $0.3\,\%$. Uncertainties contributing less than $1.0\,\%$ are marked with "$<1$" in the paper. To provide numerical values for this table in HEPdata, these uncertainties are approximated with $\pm 0.5\,\%$. This approximation is applied to all measurements for the following uncertainties$:$ JES statistical, JES physics modeling, JES mixed detector and modeling, JES close-by-jets, JES pileup, $b$-JES, jet vertex fraction, mistag efficiency and $W+\;$jets shape variation. For the measurement of $\sigma(tq)$ the approximation is applied in addition to the following uncertainties$:$ JES flavor response, $c$-tagging efficiency, $t\bar{t}$ generator + parton shower and $t\bar{t}$ ISR/FSR. For the measurement of $\sigma(\bar{t}q)$ the approximation is applied in addition to these uncertainties$:$ JES flavor response, $b/\bar{b}$ acceptance, and $t\bar{t}$ ISR/FSR. For the measurement of $R_t$ the approximation is applied in addition to these uncertainties$:$ JES detector, $b$-tagging efficiency, $c$-tagging efficiency, $b/\bar{b}$ acceptance and $tq$ scale variations. For the measurement of $\sigma(tq+\bar{t}q)$ the approximation is applied in addition to these uncertainties$:$ JES flavor response, $c$-tagging efficiency, $b/\bar{b}$ acceptance, $t\bar{t}$ generator + parton shower and $t\bar{t}$ ISR/FSR.

Differential t-channel top-quark production cross sections and normalized differential t-channel top-quark production cross sections as functions of ABS(YRAP(T)).

The cross sections for top-quark and top-antiquark production in the t-channel, together with the cross-section ratio.

Differential t-channel top-quark production cross sections and normalized differential t-channel top-quark production cross sections as functions of ABS(YRAP(TBAR)).

Parametrization factors for the $m_{t}$ dependence [see Eq. (4) in the paper] of $\sigma(tq)$, $\sigma(\bar tq)$, and $\sigma(t q+\bar t q)$.

The cross sections for top-quark and top-antiquark production in the t-channel, together with the cross-section ratio.

The value of $|V_{tb}|^{2}$ is extracted by dividing the measured value of $\sigma(t q+\bar t q)$ by the prediction of the approximate NNLO calculation. The experimental and theoretical uncertainties are added in quadrature.

Event yields for the 2-jet-$\ell^{+}$ and 2-jet-$\ell^{-}$ HPR channels. The expectation for the signal and background yields correspond to the result of the binned maximum-likelihood fit described in Sec. $\mathrm{VI~D}$ in the paper. The uncertainty of the expectations is the normalization uncertainty of each process after the fit, as described in Sec. $\mathrm{VII~F}$ in the paper.

Migration matrix relating the parton level $p_{\mathrm{T}}(t)$ shown on the $y$ axis and the reconstruction level $p_{\mathrm{T}}(\ell \nu b)$ shown on the $x$ axis for the top-quark $p_{\mathrm{T}}$ distribution.

Migration matrix relating the parton level $p_{\mathrm{T}}(\bar t)$ shown on the $y$ axis and the reconstruction level $p_{\mathrm{T}}(\ell \nu b)$ shown on the $x$ axis for the top-antiquark $p_{\mathrm{T}}$ distribution.

Migration matrix relating the parton level $|y(t)|$ shown on the $y$ axis and the reconstruction level $|y(\ell \nu b)|$ shown on the $x$ axis for the top-quark $|y|$ distribution.

Migration matrix relating the parton level $|y(\bar t)|$ shown on the $y$ axis and the reconstruction level $|y(\ell \nu b)|$ shown on the $x$ axis for the top-antiquark $|y|$ distribution.

Differential t-channel top-quark production cross section as a function of $p_{\mathrm{T}}(t)$ with the uncertainties for each bin given in percent.

Differential t-channel top-quark production cross section as a function of $p_{\mathrm{T}}(\bar t)$ with the uncertainties for each bin given in percent.

Differential t-channel top-quark production cross section as a function of $|y(t)|$ with the uncertainties for each bin given in percent.

Differential t-channel top-quark production cross section as a function of $|y(\bar t)|$ with the uncertainties for each bin given in percent.

Normalized differential t-channel top-quark production cross section as a function of $p_{\mathrm{T}}(t)$ with the uncertainties for each bin given in percent.

Normalized differential t-channel top-quark production cross section as a function of $p_{\mathrm{T}}(\bar t)$ with the uncertainties for each bin given in percent.

Normalized differential t-channel top-quark production cross section as a function of $|y(t)|$ with the uncertainties for each bin given in percent.

Normalized differential t-channel top-quark production cross section as a function of $|y(\bar t)|$ with the uncertainties for each bin given in percent.

Comparison between the measured differential cross sections and the predictions from the NLO calculation using the MSTW2008 PDF set. For each variable and prediction a $\chi^{2}$ value is calculated with HERAfitter using the covariance matrix of each measured spectrum. The theory uncertainties of the predictions are treated as uncorrelated. The number of degrees of freedom (NDF) is equal to the number of bins in the measured spectrum.

Detailed list of the contribution of each source of uncertainty to the total relative uncertainty on the measured $\dfrac{\mathrm{d}\sigma}{\mathrm{d}p_{\mathrm{T}}(t)}$ distribution given in percent for each bin. The list includes only those uncertainties that contribute with more than $1\%$. The following uncertainties contribute to the total uncertainty with less than $1\%$ to each bin content$:$ JES detector, JES statistical, JES physics modeling, JES mixed detector and modeling, JES close-by jets, JES pileup, JES flavor composition, JES flavor response, jet-vertex fraction, $b/\bar{b}$ acceptance, $E_{\mathrm{T}}^{\mathrm{miss}}$ modeling, $W+$ jets shape variation, and $t \bar{t}$ generator. In cases when the uncertainty is report to be "$<1\%$" in the table of the paper the uncertainty is approximated by a value of $0.5\%$.

Detailed list of the contribution of each source of uncertainty to the total relative uncertainty on the measured $\dfrac{\mathrm{d}\sigma}{\mathrm{d}p_{\mathrm{T}}(\bar t)}$ distribution given in percent for each bin. The list includes only those uncertainties that contribute with more than $1\%$. The following uncertainties contribute to the total uncertainty with less than $1\%$ to each bin content$:$ JES detector, JES statistical, JES physics modeling, JES mixed detector and modeling, JES close-by jets, JES pileup, JES flavor composition, JES flavor response, $b-$JES, jet-vertex fraction, mistag efficiency, $b/\bar{b}$ acceptance, $E_{\mathrm{T}}^{\mathrm{miss}}$ modeling, $W+$ jets shape variation, and $t \bar{t}$ generator. In cases when the uncertainty is report to be "$<1\%$" in the table of the paper the uncertainty is approximated by a value of $0.5\%$.

Detailed list of the contribution of each source of uncertainty to the total relative uncertainty on the measured $\dfrac{\mathrm{d}\sigma}{\mathrm{d}|y(t)|}$ distribution given in percent for each bin. The list includes only those uncertainties that contribute with more than $1\%$. The following uncertainties contribute to the total uncertainty with less than $1\%$ to each bin content$:$ JES detector, JES statistical, JES physics modeling, JES mixed detector and modeling, JES close-by jets, JES pileup, JES flavor composition, JES flavor response, jet-vertex fraction, $b/\bar{b}$ acceptance, $E_{\mathrm{T}}^{\mathrm{miss}}$ modeling, $W+$ jets shape variation, $t \bar{t}$ generator, $t \bar{t}$ ISR/FSR, and unfolding. In cases when the uncertainty is report to be "$<1\%$" in the table of the paper the uncertainty is approximated by a value of $0.5\%$.

Detailed list of the contribution of each source of uncertainty to the total relative uncertainty on the measured $\dfrac{\mathrm{d}\sigma}{\mathrm{d}|y(\bar t)|}$ distribution given in percent for each bin. The list includes only those uncertainties that contribute with more than $1\%$. The following uncertainties contribute to the total uncertainty with less than $1\%$ to each bin content$:$ JES detector, JES statistical, JES physics modeling, JES mixed detector and modeling, JES close-by jets, JES pileup, JES flavor composition, JES flavor response, $b-$JES, jet-vertex fraction, $b/\bar{b}$ acceptance, mistag efficiency, $E_{\mathrm{T}}^{\mathrm{miss}}$ modeling, $W+$ jets shape variation, $t \bar{t}$ generator, $t \bar{t}$ ISR/FSR, and unfolding. In cases when the uncertainty is report to be "$<1\%$" in the table of the paper the uncertainty is approximated by a value of $0.5\%$.

Detailed list of the contribution of each source of uncertainty to the total relative uncertainty on the measured $\dfrac{1}{\sigma}\dfrac{\mathrm{d}\sigma}{\mathrm{d}p_{\mathrm{T}}(t)}$ distribution given in percent for each bin. The list includes only those uncertainties that contribute with more than $1\%$. The JES $\eta$ intercalibration uncertainty has a sign switch from the first to the second bin. For the $tq$ generator $+$ parton shower uncertainty a sign switch is denoted with $\mp$. The following uncertainties contribute to the total uncertainty with less than $1\%$ to each bin content$:$ JES detector, JES statistical, JES physics modeling, JES mixed detector and modeling, JES close-by jets, JES pileup, JES flavor composition, JES flavor response, $b-$JES, jet-vertex fraction, $b/\bar{b}$ acceptance, $c-$tagging efficiency, $E_{\mathrm{T}}^{\mathrm{miss}}$ modeling, lepton uncertainties, $W+$ jets shape variation, and $t \bar{t}$ generator. In cases when the uncertainty is report to be "$<1\%$" in the table of the paper the uncertainty is approximated by a value of $0.5\%$.

Detailed list of the contribution of each source of uncertainty to the total relative uncertainty on the measured $\dfrac{1}{\sigma}\dfrac{\mathrm{d}\sigma}{\mathrm{d}p_{\mathrm{T}}(\bar t)}$ distribution given in percent for each bin. The list includes only those uncertainties that contribute with more than $1\%$. Sign switches within one uncertainty are denoted with $\mp$ and $\pm$. The following uncertainties contribute to the total uncertainty with less than $1\%$ to each bin content$:$ JES detector, JES statistical, JES physics modeling, JES mixed detector and modeling, JES close-by jets, JES pileup, JES flavor composition, JES flavor response, $b-$JES, jet-vertex fraction, $b/\bar{b}$ acceptance, mistag efficiency, $E_{\mathrm{T}}^{\mathrm{miss}}$ modeling, lepton uncertainties, $W+$ jets shape variation, and $t \bar{t}$ generator. In cases when the uncertainty is report to be "$<1\%$" in the table of the paper the uncertainty is approximated by a value of $0.5\%$.

Detailed list of the contribution of each source of uncertainty to the total relative uncertainty on the measured $\dfrac{1}{\sigma}\dfrac{\mathrm{d}\sigma}{\mathrm{d}|y(t)|}$ distribution given in percent for each bin. The list includes only those uncertainties that contribute with more than $1\%$. Sign switches within one uncertainty are denoted with $\mp$ and $\pm$. The following uncertainties contribute to the total uncertainty with less than $1\%$ to each bin content$:$ JES detector, JES statistical, JES physics modeling, JES mixed detector and modeling, JES close-by jets, JES pileup, JES flavor composition, JES flavor response, b-JES, jet-vertex fraction, $b/\bar{b}$ acceptance, $b-$tagging efficiency, $c-$tagging efficiency, mistag efficiency, $E_{\mathrm{T}}^{\mathrm{miss}}$ modeling, lepton uncertainties, $W+$jets shape variation, $t \bar{t}$ generator, $t \bar{t}$ISR/FSR, and unfolding. In cases when the uncertainty is report to be "$<1\%$" in the table of the paper the uncertainty is approximated by a value of $0.5\%$.

Detailed list of the contribution of each source of uncertainty to the total relative uncertainty on the measured $\dfrac{1}{\sigma}\dfrac{\mathrm{d}\sigma}{\mathrm{d}|y(\bar t)|}$ distribution given in percent for each bin. The list includes only those uncertainties that contribute with more than $1\%$. Sign switches within one uncertainty are denoted with $\mp$ and $\pm$. The following uncertainties contribute to the total uncertainty with less than $1\%$ to each bin content $:$ JES detector, JES statistical, JES physics modeling, JES mixed detector and modeling, JES close-by jets, JES pileup, JES flavor composition, JES flavor response, b-JES, jet energy resolution, jet-vertex fraction, $b/\bar{b}$ acceptance, $b-$tagging efficiency, $c-$ tagging efficiency, mistag efficiency, $E_{\mathrm{T}}^{\mathrm{miss}}$ modeling, lepton uncertainties, $W+$ jets shape variation, $t \bar{t}$ generator, $t \bar{t}$ ISR/FSR, and unfolding. In cases when the uncertainty is report to be "$<1\%$" in the table of the paper the uncertainty is approximated by a value of $0.5\%$.

Statistical correlation matrices for the differential cross section as a function of $p_{\mathrm{T}}(t)$.

Statistical correlation matrices for the differential cross section as a function of $p_{\mathrm{T}}(\bar t)$.

Statistical correlation matrices for the differential cross section as a function of $|y(t)|$.

Statistical correlation matrices for the differential cross section as a function of $|y(\bar t)|$.

Statistical correlation matrices for the normalized differential cross section as a function of $p_{\mathrm{T}}(t)$.

Statistical correlation matrices for the normalized differential cross section as a function of $p_{\mathrm{T}}(\bar t)$.

Statistical correlation matrices for the normalized differential cross section as a function of $|y(t)|$.

Statistical correlation matrices for the normalized differential cross section as a function of $|y(\bar t)|$.

Fiducial phase-space relative differential cross-sections after combining the e+jets and $\mu$+jets channels for the $t\bar{t}$ system transverse momentum $p_{T}^{t\bar{t}}$. All uncertainties are quoted as a percentage with respect to the cross-section values in each bin.

Fiducial phase-space absolute differential cross-sections after combining the e+jets and $\mu$+jets channels for the $t\bar{t$}$ system absolute rapidity $|y^{t\bar{t}}|$. All uncertainties are quoted as a percentage with respect to the cross-section values in each bin.

Fiducial phase-space relative differential cross-sections after combining the e+jets and $\mu$+jets channels for the $t\bar{t$}$ system absolute rapidity $|y^{t\bar{t}}|$. All uncertainties are quoted as a percentage with respect to the cross-section values in each bin.

Fiducial phase-space absolute differential cross-sections after combining the e+jets and $\mu$+jets channels for the hadronic top-quark transverse momentum $p_{T}^{t}$. All uncertainties are quoted as a percentage with respect to the cross-section values in each bin.

Fiducial phase-space relative differential cross-sections after combining the e+jets and $\mu$+jets channels for the hadronic top-quark transverse momentum $p_{T}^{t}$. All uncertainties are quoted as a percentage with respect to the cross-section values in each bin.

Fiducial phase-space absolute differential cross-sections after combining the e+jets and $\mu$+jets channels for the hadronic top-quark absolute rapidity $|y^{t}|$. All uncertainties are quoted as a percentage with respect to the cross-section values in each bin.

Fiducial phase-space relative differential cross-sections after combining the e+jets and $\mu$+jets channels for the hadronic top-quark absolute rapidity $|y^{t}|$. All uncertainties are quoted as a percentage with respect to the cross-section values in each bin.

Fiducial phase-space absolute differential cross-sections after combining the e+jets and $\mu$+jets channels for the $t\bar{t}$ system absolute out-of-plane momentum $|p_{out}^{t\bar{t}}|$. All uncertainties are quoted as a percentage with respect to the cross-section values in each bin.

Fiducial phase-space relative differential cross-sections after combining the e+jets and $\mu$+jets channels for the $t\bar{t}$ system absolute out-of-plane momentum $|p_{out}^{t\bar{t}}|$. All uncertainties are quoted as a percentage with respect to the cross-section values in each bin.

Fiducial phase-space absolute differential cross-sections after combining the e+jets and $\mu$+jets channels for the $t\bar{t}$ system azimuthal angle $\Delta \phi^{t\bar{t}}$. All uncertainties are quoted as a percentage with respect to the cross-section values in each bin.

Fiducial phase-space relative differential cross-sections after combining the e+jets and $\mu$+jets channels for the $t\bar{t}$ system azimuthal angle $\Delta \phi^{t\bar{t}}$. All uncertainties are quoted as a percentage with respect to the cross-section values in each bin.

Fiducial phase-space absolute differential cross-sections after combining the e+jets and $\mu$+jets channels for the scalar sum of the hadronic and leptonic top-quark transverse momenta $H_{T}^{t\bar{t}}$. All uncertainties are quoted as a percentage with respect to the cross-section values in each bin.

Fiducial phase-space relative differential cross-sections after combining the e+jets and $\mu$+jets channels for the scalar sum of the hadronic and leptonic top-quark transverse momenta $H_{T}^{t\bar{t}}$. All uncertainties are quoted as a percentage with respect to the cross-section values in each bin.

Fiducial phase-space absolute differential cross-sections after combining the e+jets and $\mu$+jets channels for $y_{boost}^{t\bar{t}}$. All uncertainties are quoted as a percentage with respect to the cross-section values in each bin.

Fiducial phase-space relative differential cross-sections after combining the e+jets and $\mu$+jets channels for $y_{boost}^{t\bar{t}}$. All uncertainties are quoted as a percentage with respect to the cross-section values in each bin.

Fiducial phase-space absolute differential cross-sections after combining the e+jets and $\mu$+jets channels for $\chi^{t\bar{t}}$. All uncertainties are quoted as a percentage with respect to the cross-section values in each bin.

Fiducial phase-space relative differential cross-sections after combining the e+jets and $\mu$+jets channels for $\chi^{t\bar{t}}$. All uncertainties are quoted as a percentage with respect to the cross-section values in each bin.

Fiducial phase-space absolute differential cross-sections after combining the e+jets and $\mu$+jets channels for $R_{Wt}$. All uncertainties are quoted as a percentage with respect to the cross-section values in each bin.

Fiducial phase-space relative differential cross-sections after combining the e+jets and $\mu$+jets channels for $R_{Wt}$. All uncertainties are quoted as a percentage with respect to the cross-section values in each bin.

Full phase-space absolute differential cross-sections after combining the e+jets and $\mu$+jets channels for the $t\bar{t}$ system invariant mass $m^{t\bar{t}}$. All uncertainties are quoted as a percentage with respect to the cross-section values in each bin.

Full phase-space relative differential cross-sections after combining the e+jets and $\mu$+jets channels for the $t\bar{t}$ system invariant mass $m^{t\bar{t}}$. All uncertainties are quoted as a percentage with respect to the cross-section values in each bin.

Full phase-space absolute differential cross-sections after combining the e+jets and $\mu$+jets channels for the $t\bar{t}$ system transverse momentum $p_{T}^{t\bar{t}}$. All uncertainties are quoted as a percentage with respect to the cross-section values in each bin.

Full phase-space relative differential cross-sections after combining the e+jets and $\mu$+jets channels for the $t\bar{t}$ system transverse momentum $p_{T}^{t\bar{t}}$. All uncertainties are quoted as a percentage with respect to the cross-section values in each bin.

Full phase-space absolute differential cross-sections after combining the e+jets and $\mu$+jets channels for the $t\bar{t}$ system absolute rapidity $|y^{t\bar{t}}|$. All uncertainties are quoted as a percentage with respect to the cross-section values in each bin.

Full phase-space relative differential cross-sections after combining the e+jets and $\mu$+jets channels for the $t\bar{t}$ system absolute rapidity $|y^{t\bar{t}}|$. All uncertainties are quoted as a percentage with respect to the cross-section values in each bin.

Full phase-space absolute differential cross-sections after combining the e+jets and $\mu$+jets channels for the top-quark transverse momentum $p_{T}^{t}$. All uncertainties are quoted as a percentage with respect to the cross-section values in each bin.

Full phase-space relative differential cross-sections after combining the e+jets and $\mu$+jets channels for the top-quark transverse momentum $p_{T}^{t}$. All uncertainties are quoted as a percentage with respect to the cross-section values in each bin.

Full phase-space absolute differential cross-sections after combining the e+jets and $\mu$+jets channels for the top-quark absolute rapidity $|y^{t}|$. All uncertainties are quoted as a percentage with respect to the cross-section values in each bin.

Full phase-space relative differential cross-sections after combining the e+jets and $\mu$+jets channels for the top-quark absolute rapidity $|y^{t}|$. All uncertainties are quoted as a percentage with respect to the cross-section values in each bin.

Full phase-space absolute differential cross-sections after combining the e+jets and $\mu$+jets channels for the $t\bar{t}$ system absolute out-of-plane momentum $|p_{out}^{t\bar{t}}|$. All uncertainties are quoted as a percentage with respect to the cross-section values in each bin.

Full phase-space relative differential cross-sections after combining the e+jets and $\mu$+jets channels for the $t\bar{t}$ system absolute out-of-plane momentum $|p_{out}^{t\bar{t}}|$. All uncertainties are quoted as a percentage with respect to the cross-section values in each bin.

Full phase-space absolute differential cross-sections after combining the e+jets and $\mu$+jets channels for the $t\bar{t}$ system azimuthal angle $\Delta \phi^{t\bar{t}}$. All uncertainties are quoted as a percentage with respect to the cross-section values in each bin.

Full phase-space relative differential cross-sections after combining the e+jets and $\mu$+jets channels for the $t\bar{t}$ system azimuthal angle $\Delta \phi^{t\bar{t}}$. All uncertainties are quoted as a percentage with respect to the cross-section values in each bin.

Full phase-space absolute differential cross-sections after combining the e+jets and $\mu$+jets channels for the scalar sum of the hadronic and leptonic top-quark transverse momenta $H_{T}^{t\bar{t}}$. All uncertainties are quoted as a percentage with respect to the cross-section values in each bin.

Full phase-space relative differential cross-sections after combining the e+jets and $\mu$+jets channels for the scalar sum of the hadronic and leptonic top-quark transverse momenta $H_{T}^{t\bar{t}}$. All uncertainties are quoted as a percentage with respect to the cross-section values in each bin.

Full phase-space absolute differential cross-sections after combining the e+jets and $\mu$+jets channels for $y_{boost}^{t\bar{t}}$. All uncertainties are quoted as a percentage with respect to the cross-section values in each bin.

Full phase-space relative differential cross-sections after combining the e+jets and $\mu$+jets channels for $y_{boost}^{t\bar{t}}$. All uncertainties are quoted as a percentage with respect to the cross-section values in each bin.

Full phase-space absolute differential cross-sections after combining the e+jets and $\mu$+jets channels for $\chi^{t\bar{t}}$. All uncertainties are quoted as a percentage with respect to the cross-section values in each bin.

Full phase-space relative differential cross-sections after combining the e+jets and $\mu$+jets channels for $\chi^{t\bar{t}}$. All uncertainties are quoted as a percentage with respect to the cross-section values in each bin.

Absolute statistics-only correlation matrix of the fiducial phase-space differential cross-section as a function of the the $t\bar{t}$ system invariant mass $m^{t\bar{t}}$.

Relative statistics-only correlation matrix of the fiducial phase-space differential cross-section as a function of the the $t\bar{t}$ system invariant mass $m^{t\bar{t}}$.

Absolute systematics-only correlation matrix of the fiducial phase-space differential cross-section as a function of the the $t\bar{t}$ system invariant mass $m^{t\bar{t}}$.

Relative systematics-only correlation matrix of the fiducial phase-space differential cross-section as a function of the the $t\bar{t}$ system invariant mass $m^{t\bar{t}}$.

Absolute statistics-only correlation matrix of the fiducial phase-space differential cross-section as a function of the the $t\bar{t}$ system transverse momentum $p_{T}^{t\bar{t}}$.

Relative statistics-only correlation matrix of the fiducial phase-space differential cross-section as a function of the the $t\bar{t}$ system transverse momentum $p_{T}^{t\bar{t}}$.

Absolute systematics-only correlation matrix of the fiducial phase-space differential cross-section as a function of the the $t\bar{t}$ system transverse momentum $p_{T}^{t\bar{t}}$.

Relative systematics-only correlation matrix of the fiducial phase-space differential cross-section as a function of the the $t\bar{t}$ system transverse momentum $p_{T}^{t\bar{t}}$.

Absolute statistics-only correlation matrix of the fiducial phase-space differential cross-section as a function of the the $t\bar{t$}$ system absolute rapidity $|y^{t\bar{t}}|$.

Relative statistics-only correlation matrix of the fiducial phase-space differential cross-section as a function of the the $t\bar{t$}$ system absolute rapidity $|y^{t\bar{t}}|$.

Absolute systematics-only correlation matrix of the fiducial phase-space differential cross-section as a function of the the $t\bar{t$}$ system absolute rapidity $|y^{t\bar{t}}|$.

Relative systematics-only correlation matrix of the fiducial phase-space differential cross-section as a function of the the $t\bar{t$}$ system absolute rapidity $|y^{t\bar{t}}|$.

Absolute statistics-only correlation matrix of the fiducial phase-space differential cross-section as a function of the the hadronic top-quark transverse momentum $p_{T}^{t}$.

Relative statistics-only correlation matrix of the fiducial phase-space differential cross-section as a function of the the hadronic top-quark transverse momentum $p_{T}^{t}$.

Absolute systematics-only correlation matrix of the fiducial phase-space differential cross-section as a function of the the hadronic top-quark transverse momentum $p_{T}^{t}$.

Relative systematics-only correlation matrix of the fiducial phase-space differential cross-section as a function of the the hadronic top-quark transverse momentum $p_{T}^{t}$.

Absolute statistics-only correlation matrix of the fiducial phase-space differential cross-section as a function of the the hadronic top-quark absolute rapidity $|y^{t}|$.

Relative statistics-only correlation matrix of the fiducial phase-space differential cross-section as a function of the the hadronic top-quark absolute rapidity $|y^{t}|$.

Absolute systematics-only correlation matrix of the fiducial phase-space differential cross-section as a function of the the hadronic top-quark absolute rapidity $|y^{t}|$.

Relative systematics-only correlation matrix of the fiducial phase-space differential cross-section as a function of the the hadronic top-quark absolute rapidity $|y^{t}|$.

Absolute statistics-only correlation matrix of the fiducial phase-space differential cross-section as a function of the the $t\bar{t}$ system out-of-plane momentum $|p_{out}^{t\bar{t}}|$.

Relative statistics-only correlation matrix of the fiducial phase-space differential cross-section as a function of the the $t\bar{t}$ system out-of-plane momentum $|p_{out}^{t\bar{t}}|$.

Absolute systematics-only correlation matrix of the fiducial phase-space differential cross-section as a function of the the $t\bar{t}$ system out-of-plane momentum $|p_{out}^{t\bar{t}}|$.

Relative systematics-only correlation matrix of the fiducial phase-space differential cross-section as a function of the the $t\bar{t}$ system out-of-plane momentum $|p_{out}^{t\bar{t}}|$.

Absolute statistics-only correlation matrix of the fiducial phase-space differential cross-section as a function of the the $t\bar{t}$ system azimuthal angle $\Delta \phi^{t\bar{t}}$.

Relative statistics-only correlation matrix of the fiducial phase-space differential cross-section as a function of the the $t\bar{t}$ system azimuthal angle $\Delta \phi^{t\bar{t}}$.

Absolute systematics-only correlation matrix of the fiducial phase-space differential cross-section as a function of the the $t\bar{t}$ system azimuthal angle $\Delta \phi^{t\bar{t}}$.

Relative systematics-only correlation matrix of the fiducial phase-space differential cross-section as a function of the the $t\bar{t}$ system azimuthal angle $\Delta \phi^{t\bar{t}}$.

Absolute statistics-only correlation matrix of the fiducial phase-space differential cross-section as a function of the the scalar sum of the hadronic and leptonic top-quark transverse momenta $H_{T}^{t\bar{t}}$.

Relative statistics-only correlation matrix of the fiducial phase-space differential cross-section as a function of the the scalar sum of the hadronic and leptonic top-quark transverse momenta $H_{T}^{t\bar{t}}$.

Absolute systematics-only correlation matrix of the fiducial phase-space differential cross-section as a function of the the scalar sum of the hadronic and leptonic top-quark transverse momenta $H_{T}^{t\bar{t}}$.

Relative systematics-only correlation matrix of the fiducial phase-space differential cross-section as a function of the the scalar sum of the hadronic and leptonic top-quark transverse momenta $H_{T}^{t\bar{t}}$.

Absolute statistics-only correlation matrix of the fiducial phase-space differential cross-section as a function of the longitudinal boost $y_{boost}^{t\bar{t}}$.

Relative statistics-only correlation matrix of the fiducial phase-space differential cross-section as a function of the longitudinal boost $y_{boost}^{t\bar{t}}$.

Absolute systematics-only correlation matrix of the fiducial phase-space differential cross-section as a function of the longitudinal boost $y_{boost}^{t\bar{t}}$.

Relative systematics-only correlation matrix of the fiducial phase-space differential cross-section as a function of the longitudinal boost $y_{boost}^{t\bar{t}}$.

Absolute statistics-only correlation matrix of the fiducial phase-space differential cross-section as a function of the production angle $\chi^{t\bar{t}}$.

Relative statistics-only correlation matrix of the fiducial phase-space differential cross-section as a function of the production angle $\chi^{t\bar{t}}$.

Absolute systematics-only correlation matrix of the fiducial phase-space differential cross-section as a function of the production angle $\chi^{t\bar{t}}$.

Relative systematics-only correlation matrix of the fiducial phase-space differential cross-section as a function of the production angle $\chi^{t\bar{t}}$.

Absolute statistics-only correlation matrix of the fiducial phase-space differential cross-section as a function of the ratio of the hadronic W and the hadronic top transverse momenta $R_{Wt}$.

Relative statistics-only correlation matrix of the fiducial phase-space differential cross-section as a function of the ratio of the hadronic W and the hadronic top transverse momenta $R_{Wt}$.

Absolute systematics-only correlation matrix of the fiducial phase-space differential cross-section as a function of the ratio of the hadronic W and the hadronic top transverse momenta $R_{Wt}$.

Relative systematics-only correlation matrix of the fiducial phase-space differential cross-section as a function of the ratio of the hadronic W and the hadronic top transverse momenta $R_{Wt}$.

Absolute statistics-only correlation matrix of the full phase-space differential cross-section as a function of the the $t\bar{t}$ system invariant mass $m^{t\bar{t}}$.

Relative statistics-only correlation matrix of the full phase-space differential cross-section as a function of the the $t\bar{t}$ system invariant mass $m^{t\bar{t}}$.

Absolute systematics-only correlation matrix of the full phase-space differential cross-section as a function of the the $t\bar{t}$ system invariant mass $m^{t\bar{t}}$.

Relative systematics-only correlation matrix of the full phase-space differential cross-section as a function of the the $t\bar{t}$ system invariant mass $m^{t\bar{t}}$.

Absolute statistics-only correlation matrix of the full phase-space differential cross-section as a function of the the $t\bar{t}$ system transverse momentum $p_{T}^{t\bar{t}}$.

Relative statistics-only correlation matrix of the full phase-space differential cross-section as a function of the the $t\bar{t}$ system transverse momentum $p_{T}^{t\bar{t}}$.

Absolute systematics-only correlation matrix of the full phase-space differential cross-section as a function of the the $t\bar{t}$ system transverse momentum $p_{T}^{t\bar{t}}$.

Relative systematics-only correlation matrix of the full phase-space differential cross-section as a function of the the $t\bar{t}$ system transverse momentum $p_{T}^{t\bar{t}}$.

Absolute statistics-only correlation matrix of the full phase-space differential cross-section as a function of the the $t\bar{t$}$ system absolute rapidity $|y^{t\bar{t}}|$.

Relative statistics-only correlation matrix of the full phase-space differential cross-section as a function of the the $t\bar{t$}$ system absolute rapidity $|y^{t\bar{t}}|$.

Absolute systematics-only correlation matrix of the full phase-space differential cross-section as a function of the the $t\bar{t$}$ system absolute rapidity $|y^{t\bar{t}}|$.

Relative systematics-only correlation matrix of the full phase-space differential cross-section as a function of the the $t\bar{t$}$ system absolute rapidity $|y^{t\bar{t}}|$.

Absolute statistics-only correlation matrix of the full phase-space differential cross-section as a function of the the hadronic top-quark transverse momentum $p_{T}^{t}$.

Relative statistics-only correlation matrix of the full phase-space differential cross-section as a function of the the hadronic top-quark transverse momentum $p_{T}^{t}$.

Absolute systematics-only correlation matrix of the full phase-space differential cross-section as a function of the the hadronic top-quark transverse momentum $p_{T}^{t}$.

Relative systematics-only correlation matrix of the full phase-space differential cross-section as a function of the the hadronic top-quark transverse momentum $p_{T}^{t}$.

Absolute statistics-only correlation matrix of the full phase-space differential cross-section as a function of the the hadronic top-quark absolute rapidity $|y^{t}|$.

Relative statistics-only correlation matrix of the full phase-space differential cross-section as a function of the the hadronic top-quark absolute rapidity $|y^{t}|$.

Absolute systematics-only correlation matrix of the full phase-space differential cross-section as a function of the the hadronic top-quark absolute rapidity $|y^{t}|$.

Relative systematics-only correlation matrix of the full phase-space differential cross-section as a function of the the hadronic top-quark absolute rapidity $|y^{t}|$.

Absolute statistics-only correlation matrix of the full phase-space differential cross-section as a function of the the $t\bar{t}$ system out-of-plane momentum $|p_{out}^{t\bar{t}}|$.

Relative statistics-only correlation matrix of the full phase-space differential cross-section as a function of the the $t\bar{t}$ system out-of-plane momentum $|p_{out}^{t\bar{t}}|$.

Absolute systematics-only correlation matrix of the full phase-space differential cross-section as a function of the the $t\bar{t}$ system out-of-plane momentum $|p_{out}^{t\bar{t}}|$.

Relative systematics-only correlation matrix of the full phase-space differential cross-section as a function of the the $t\bar{t}$ system out-of-plane momentum $|p_{out}^{t\bar{t}}|$.

Absolute statistics-only correlation matrix of the full phase-space differential cross-section as a function of the the $t\bar{t}$ system azimuthal angle $\Delta \phi^{t\bar{t}}$.

Relative statistics-only correlation matrix of the full phase-space differential cross-section as a function of the the $t\bar{t}$ system azimuthal angle $\Delta \phi^{t\bar{t}}$.

Absolute systematics-only correlation matrix of the full phase-space differential cross-section as a function of the the $t\bar{t}$ system azimuthal angle $\Delta \phi^{t\bar{t}}$.

Relative systematics-only correlation matrix of the full phase-space differential cross-section as a function of the the $t\bar{t}$ system azimuthal angle $\Delta \phi^{t\bar{t}}$.

Absolute statistics-only correlation matrix of the full phase-space differential cross-section as a function of the the scalar sum of the hadronic and leptonic top-quark transverse momenta $H_{T}^{t\bar{t}}$.

Relative statistics-only correlation matrix of the full phase-space differential cross-section as a function of the the scalar sum of the hadronic and leptonic top-quark transverse momenta $H_{T}^{t\bar{t}}$.

Absolute systematics-only correlation matrix of the full phase-space differential cross-section as a function of the the scalar sum of the hadronic and leptonic top-quark transverse momenta $H_{T}^{t\bar{t}}$.

Relative systematics-only correlation matrix of the full phase-space differential cross-section as a function of the the scalar sum of the hadronic and leptonic top-quark transverse momenta $H_{T}^{t\bar{t}}$.

Absolute statistics-only correlation matrix of the full phase-space differential cross-section as a function of the longitudinal boost $y_{boost}^{t\bar{t}}$.

Relative statistics-only correlation matrix of the full phase-space differential cross-section as a function of the longitudinal boost $y_{boost}^{t\bar{t}}$.

Absolute systematics-only correlation matrix of the full phase-space differential cross-section as a function of the longitudinal boost $y_{boost}^{t\bar{t}}$.

Relative systematics-only correlation matrix of the full phase-space differential cross-section as a function of the longitudinal boost $y_{boost}^{t\bar{t}}$.

Absolute statistics-only correlation matrix of the full phase-space differential cross-section as a function of the production angle $\chi^{t\bar{t}}$.

Relative statistics-only correlation matrix of the full phase-space differential cross-section as a function of the production angle $\chi^{t\bar{t}}$.

Absolute systematics-only correlation matrix of the full phase-space differential cross-section as a function of the production angle $\chi^{t\bar{t}}$.

Relative systematics-only correlation matrix of the full phase-space differential cross-section as a function of the production angle $\chi^{t\bar{t}}$.

Statistical correlation matrix between |$p_{out}^{t\bar{t}}$| (rows) in the 4-jet inclusive configuration and |$p_{out}^{t\bar{t}}$| (columns) in the 4-jet inclusive configuration, obtained at parton level from absolute spectra through the Bootstrap Method. The binning is the following: Rows: [0-40, 40-80, 80-120, 120-170, 170-230, 230-600] GeV Columns: [0-40, 40-80, 80-120, 120-170, 170-230, 230-600] GeV

Statistical correlation matrix between |$p_{out}^{t\bar{t}}$| (rows) in the 4-jet inclusive configuration and $\chi^{t\bar{t}}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from absolute spectra through the Bootstrap Method. The binning is the following: Rows: [0-40, 40-80, 80-120, 120-170, 170-230, 230-600] GeV Columns: [1-1.4, 1.4-1.9, 1.9-2.5, 2.5-3.2, 3.2-4.2, 4.2-5.5, 5.5-7.2, 7.2-9.3, 9.3-12, 12-20] GeV

Statistical correlation matrix between |$p_{out}^{t\bar{t}}$| (rows) in the 4-jet inclusive configuration and $\Delta\phi^{t\bar{t}}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from absolute spectra through the Bootstrap Method. The binning is the following: Rows: [0-40, 40-80, 80-120, 120-170, 170-230, 230-600] GeV Columns: [0.0-2.0, 2.0-2.75, 2.75-3.0, 3.0-3.15]

Statistical correlation matrix between |$p_{out}^{t\bar{t}}$| (rows) in the 4-jet inclusive configuration and $H_T^{t\bar{t}}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from absolute spectra through the Bootstrap Method. The binning is the following: Rows: [0-40, 40-80, 80-120, 120-170, 170-230, 230-600] GeV Columns: [0-90, 90-140, 140-195, 195-255, 255-320, 320-385, 385-455, 455-530, 530-610, 610-695, 695-780, 780-865, 865-950, 950-1041, 1041-1500] GeV

Statistical correlation matrix between |$p_{out}^{t\bar{t}}$| (rows) in the 4-jet inclusive configuration and $y_{boost}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from absolute spectra through the Bootstrap Method. The binning is the following: Rows: [0-40, 40-80, 80-120, 120-170, 170-230, 230-600] GeV Columns: [0-0.1, 0.1-0.2, 0.2-0.3, 0.3-0.4, 0.4-0.5, 0.5-0.6, 0.6-0.7, 0.7-0.8, 0.8-0.9, 0.9-1, 1-1.1, 1.1-1.2, 1.2-1.3, 1.3-1.4, 1.4-1.5, 1.5-2] GeV

Statistical correlation matrix between |$p_{out}^{t\bar{t}}$| (rows) in the 4-jet inclusive configuration and $|y^{t,had}|$ (columns) in the 4-jet inclusive configuration, obtained at parton level from absolute spectra through the Bootstrap Method. The binning is the following: Rows: [0-40, 40-80, 80-120, 120-170, 170-230, 230-600] GeV Columns: [0-0.4, 0.4-0.8, 0.8-1.2, 1.2-1.6, 1.6-2.5]

Statistical correlation matrix between |$p_{out}^{t\bar{t}}$| (rows) in the 4-jet inclusive configuration and $p_{T}^{t,had}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from absolute spectra through the Bootstrap Method. The binning is the following: Rows: [0-40, 40-80, 80-120, 120-170, 170-230, 230-600] GeV Columns: [0-60, 60-100, 100-150, 150-200, 200-260, 260-320, 320-400, 400-500] GeV

Statistical correlation matrix between |$p_{out}^{t\bar{t}}$| (rows) in the 4-jet inclusive configuration and $|y^{t\bar{t}}|$ (columns) in the 4-jet inclusive configuration, obtained at parton level from absolute spectra through the Bootstrap Method. The binning is the following: Rows: [0-40, 40-80, 80-120, 120-170, 170-230, 230-600] GeV Columns: [0-0.3, 0.3-0.6, 0.6-0.9, 0.9-1.3, 1.3-2.5]

Statistical correlation matrix between |$p_{out}^{t\bar{t}}$| (rows) in the 4-jet inclusive configuration and $m^{t\bar{t}}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from absolute spectra through the Bootstrap Method. The binning is the following: Rows: [0-40, 40-80, 80-120, 120-170, 170-230, 230-600] GeV Columns: [345-400, 400-470, 470-550, 550-650, 650-800, 800-1100, 1100-1600] GeV

Statistical correlation matrix between |$p_{out}^{t\bar{t}}$| (rows) in the 4-jet inclusive configuration and $p_{T}^{t\bar{t}}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from absolute spectra through the Bootstrap Method. The binning is the following: Rows: [0-40, 40-80, 80-120, 120-170, 170-230, 230-600] GeV Columns: [0-20, 20-45, 45-75, 75-120, 120-190, 190-300] GeV

Statistical correlation matrix between $\chi^{t\bar{t}}$ (rows) in the 4-jet inclusive configuration and $\chi^{t\bar{t}}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from absolute spectra through the Bootstrap Method. The binning is the following: Rows: [1-1.4, 1.4-1.9, 1.9-2.5, 2.5-3.2, 3.2-4.2, 4.2-5.5, 5.5-7.2, 7.2-9.3, 9.3-12, 12-20] GeV Columns: [1-1.4, 1.4-1.9, 1.9-2.5, 2.5-3.2, 3.2-4.2, 4.2-5.5, 5.5-7.2, 7.2-9.3, 9.3-12, 12-20] GeV

Statistical correlation matrix between $\chi^{t\bar{t}}$ (rows) in the 4-jet inclusive configuration and $\Delta\phi^{t\bar{t}}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from absolute spectra through the Bootstrap Method. The binning is the following: Rows: [1-1.4, 1.4-1.9, 1.9-2.5, 2.5-3.2, 3.2-4.2, 4.2-5.5, 5.5-7.2, 7.2-9.3, 9.3-12, 12-20] GeV Columns: [0.0-2.0, 2.0-2.75, 2.75-3.0, 3.0-3.15]

Statistical correlation matrix between $\chi^{t\bar{t}}$ (rows) in the 4-jet inclusive configuration and $H_T^{t\bar{t}}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from absolute spectra through the Bootstrap Method. The binning is the following: Rows: [1-1.4, 1.4-1.9, 1.9-2.5, 2.5-3.2, 3.2-4.2, 4.2-5.5, 5.5-7.2, 7.2-9.3, 9.3-12, 12-20] GeV Columns: [0-90, 90-140, 140-195, 195-255, 255-320, 320-385, 385-455, 455-530, 530-610, 610-695, 695-780, 780-865, 865-950, 950-1041, 1041-1500] GeV

Statistical correlation matrix between $\chi^{t\bar{t}}$ (rows) in the 4-jet inclusive configuration and $y_{boost}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from absolute spectra through the Bootstrap Method. The binning is the following: Rows: [1-1.4, 1.4-1.9, 1.9-2.5, 2.5-3.2, 3.2-4.2, 4.2-5.5, 5.5-7.2, 7.2-9.3, 9.3-12, 12-20] GeV Columns: [0-0.1, 0.1-0.2, 0.2-0.3, 0.3-0.4, 0.4-0.5, 0.5-0.6, 0.6-0.7, 0.7-0.8, 0.8-0.9, 0.9-1, 1-1.1, 1.1-1.2, 1.2-1.3, 1.3-1.4, 1.4-1.5, 1.5-2] GeV

Statistical correlation matrix between $\chi^{t\bar{t}}$ (rows) in the 4-jet inclusive configuration and $|y^{t,had}|$ (columns) in the 4-jet inclusive configuration, obtained at parton level from absolute spectra through the Bootstrap Method. The binning is the following: Rows: [1-1.4, 1.4-1.9, 1.9-2.5, 2.5-3.2, 3.2-4.2, 4.2-5.5, 5.5-7.2, 7.2-9.3, 9.3-12, 12-20] GeV Columns: [0-0.4, 0.4-0.8, 0.8-1.2, 1.2-1.6, 1.6-2.5]

Statistical correlation matrix between $\chi^{t\bar{t}}$ (rows) in the 4-jet inclusive configuration and $p_{T}^{t,had}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from absolute spectra through the Bootstrap Method. The binning is the following: Rows: [1-1.4, 1.4-1.9, 1.9-2.5, 2.5-3.2, 3.2-4.2, 4.2-5.5, 5.5-7.2, 7.2-9.3, 9.3-12, 12-20] GeV Columns: [0-60, 60-100, 100-150, 150-200, 200-260, 260-320, 320-400, 400-500] GeV

Statistical correlation matrix between $\chi^{t\bar{t}}$ (rows) in the 4-jet inclusive configuration and $|y^{t\bar{t}}|$ (columns) in the 4-jet inclusive configuration, obtained at parton level from absolute spectra through the Bootstrap Method. The binning is the following: Rows: [1-1.4, 1.4-1.9, 1.9-2.5, 2.5-3.2, 3.2-4.2, 4.2-5.5, 5.5-7.2, 7.2-9.3, 9.3-12, 12-20] GeV Columns: [0-0.3, 0.3-0.6, 0.6-0.9, 0.9-1.3, 1.3-2.5]

Statistical correlation matrix between $\chi^{t\bar{t}}$ (rows) in the 4-jet inclusive configuration and $m^{t\bar{t}}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from absolute spectra through the Bootstrap Method. The binning is the following: Rows: [1-1.4, 1.4-1.9, 1.9-2.5, 2.5-3.2, 3.2-4.2, 4.2-5.5, 5.5-7.2, 7.2-9.3, 9.3-12, 12-20] GeV Columns: [345-400, 400-470, 470-550, 550-650, 650-800, 800-1100, 1100-1600] GeV

Statistical correlation matrix between $\chi^{t\bar{t}}$ (rows) in the 4-jet inclusive configuration and $p_{T}^{t\bar{t}}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from absolute spectra through the Bootstrap Method. The binning is the following: Rows: [1-1.4, 1.4-1.9, 1.9-2.5, 2.5-3.2, 3.2-4.2, 4.2-5.5, 5.5-7.2, 7.2-9.3, 9.3-12, 12-20] GeV Columns: [0-20, 20-45, 45-75, 75-120, 120-190, 190-300] GeV

Statistical correlation matrix between $\Delta\phi^{t\bar{t}}$ (rows) in the 4-jet inclusive configuration and $\Delta\phi^{t\bar{t}}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from absolute spectra through the Bootstrap Method. The binning is the following: Rows: [0.0-2.0, 2.0-2.75, 2.75-3.0, 3.0-3.15] Columns: [0.0-2.0, 2.0-2.75, 2.75-3.0, 3.0-3.15]

Statistical correlation matrix between $\Delta\phi^{t\bar{t}}$ (rows) in the 4-jet inclusive configuration and $H_T^{t\bar{t}}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from absolute spectra through the Bootstrap Method. The binning is the following: Rows: [0.0-2.0, 2.0-2.75, 2.75-3.0, 3.0-3.15] Columns: [0-90, 90-140, 140-195, 195-255, 255-320, 320-385, 385-455, 455-530, 530-610, 610-695, 695-780, 780-865, 865-950, 950-1041, 1041-1500] GeV

Statistical correlation matrix between $\Delta\phi^{t\bar{t}}$ (rows) in the 4-jet inclusive configuration and $y_{boost}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from absolute spectra through the Bootstrap Method. The binning is the following: Rows: [0.0-2.0, 2.0-2.75, 2.75-3.0, 3.0-3.15] Columns: [0-0.1, 0.1-0.2, 0.2-0.3, 0.3-0.4, 0.4-0.5, 0.5-0.6, 0.6-0.7, 0.7-0.8, 0.8-0.9, 0.9-1, 1-1.1, 1.1-1.2, 1.2-1.3, 1.3-1.4, 1.4-1.5, 1.5-2] GeV

Statistical correlation matrix between $\Delta\phi^{t\bar{t}}$ (rows) in the 4-jet inclusive configuration and $|y^{t,had}|$ (columns) in the 4-jet inclusive configuration, obtained at parton level from absolute spectra through the Bootstrap Method. The binning is the following: Rows: [0.0-2.0, 2.0-2.75, 2.75-3.0, 3.0-3.15] Columns: [0-0.4, 0.4-0.8, 0.8-1.2, 1.2-1.6, 1.6-2.5]

Statistical correlation matrix between $\Delta\phi^{t\bar{t}}$ (rows) in the 4-jet inclusive configuration and $p_{T}^{t,had}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from absolute spectra through the Bootstrap Method. The binning is the following: Rows: [0.0-2.0, 2.0-2.75, 2.75-3.0, 3.0-3.15] Columns: [0-60, 60-100, 100-150, 150-200, 200-260, 260-320, 320-400, 400-500] GeV

Statistical correlation matrix between $\Delta\phi^{t\bar{t}}$ (rows) in the 4-jet inclusive configuration and $|y^{t\bar{t}}|$ (columns) in the 4-jet inclusive configuration, obtained at parton level from absolute spectra through the Bootstrap Method. The binning is the following: Rows: [0.0-2.0, 2.0-2.75, 2.75-3.0, 3.0-3.15] Columns: [0-0.3, 0.3-0.6, 0.6-0.9, 0.9-1.3, 1.3-2.5]

Statistical correlation matrix between $\Delta\phi^{t\bar{t}}$ (rows) in the 4-jet inclusive configuration and $m^{t\bar{t}}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from absolute spectra through the Bootstrap Method. The binning is the following: Rows: [0.0-2.0, 2.0-2.75, 2.75-3.0, 3.0-3.15] Columns: [345-400, 400-470, 470-550, 550-650, 650-800, 800-1100, 1100-1600] GeV

Statistical correlation matrix between $\Delta\phi^{t\bar{t}}$ (rows) in the 4-jet inclusive configuration and $p_{T}^{t\bar{t}}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from absolute spectra through the Bootstrap Method. The binning is the following: Rows: [0.0-2.0, 2.0-2.75, 2.75-3.0, 3.0-3.15] Columns: [0-20, 20-45, 45-75, 75-120, 120-190, 190-300] GeV

Statistical correlation matrix between $H_T^{t\bar{t}}$ (rows) in the 4-jet inclusive configuration and $H_T^{t\bar{t}}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from absolute spectra through the Bootstrap Method. The binning is the following: Rows: [0-90, 90-140, 140-195, 195-255, 255-320, 320-385, 385-455, 455-530, 530-610, 610-695, 695-780, 780-865, 865-950, 950-1041, 1041-1500] GeV Columns: [0-90, 90-140, 140-195, 195-255, 255-320, 320-385, 385-455, 455-530, 530-610, 610-695, 695-780, 780-865, 865-950, 950-1041, 1041-1500] GeV

Statistical correlation matrix between $H_T^{t\bar{t}}$ (rows) in the 4-jet inclusive configuration and $y_{boost}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from absolute spectra through the Bootstrap Method. The binning is the following: Rows: [0-90, 90-140, 140-195, 195-255, 255-320, 320-385, 385-455, 455-530, 530-610, 610-695, 695-780, 780-865, 865-950, 950-1041, 1041-1500] GeV Columns: [0-0.1, 0.1-0.2, 0.2-0.3, 0.3-0.4, 0.4-0.5, 0.5-0.6, 0.6-0.7, 0.7-0.8, 0.8-0.9, 0.9-1, 1-1.1, 1.1-1.2, 1.2-1.3, 1.3-1.4, 1.4-1.5, 1.5-2] GeV

Statistical correlation matrix between $H_T^{t\bar{t}}$ (rows) in the 4-jet inclusive configuration and $|y^{t,had}|$ (columns) in the 4-jet inclusive configuration, obtained at parton level from absolute spectra through the Bootstrap Method. The binning is the following: Rows: [0-90, 90-140, 140-195, 195-255, 255-320, 320-385, 385-455, 455-530, 530-610, 610-695, 695-780, 780-865, 865-950, 950-1041, 1041-1500] GeV Columns: [0-0.4, 0.4-0.8, 0.8-1.2, 1.2-1.6, 1.6-2.5]

Statistical correlation matrix between $H_T^{t\bar{t}}$ (rows) in the 4-jet inclusive configuration and $p_{T}^{t,had}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from absolute spectra through the Bootstrap Method. The binning is the following: Rows: [0-90, 90-140, 140-195, 195-255, 255-320, 320-385, 385-455, 455-530, 530-610, 610-695, 695-780, 780-865, 865-950, 950-1041, 1041-1500] GeV Columns: [0-60, 60-100, 100-150, 150-200, 200-260, 260-320, 320-400, 400-500] GeV

Statistical correlation matrix between $H_T^{t\bar{t}}$ (rows) in the 4-jet inclusive configuration and $|y^{t\bar{t}}|$ (columns) in the 4-jet inclusive configuration, obtained at parton level from absolute spectra through the Bootstrap Method. The binning is the following: Rows: [0-90, 90-140, 140-195, 195-255, 255-320, 320-385, 385-455, 455-530, 530-610, 610-695, 695-780, 780-865, 865-950, 950-1041, 1041-1500] GeV Columns: [0-0.3, 0.3-0.6, 0.6-0.9, 0.9-1.3, 1.3-2.5]

Statistical correlation matrix between $H_T^{t\bar{t}}$ (rows) in the 4-jet inclusive configuration and $m^{t\bar{t}}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from absolute spectra through the Bootstrap Method. The binning is the following: Rows: [0-90, 90-140, 140-195, 195-255, 255-320, 320-385, 385-455, 455-530, 530-610, 610-695, 695-780, 780-865, 865-950, 950-1041, 1041-1500] GeV Columns: [345-400, 400-470, 470-550, 550-650, 650-800, 800-1100, 1100-1600] GeV

Statistical correlation matrix between $H_T^{t\bar{t}}$ (rows) in the 4-jet inclusive configuration and $p_{T}^{t\bar{t}}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from absolute spectra through the Bootstrap Method. The binning is the following: Rows: [0-90, 90-140, 140-195, 195-255, 255-320, 320-385, 385-455, 455-530, 530-610, 610-695, 695-780, 780-865, 865-950, 950-1041, 1041-1500] GeV Columns: [0-20, 20-45, 45-75, 75-120, 120-190, 190-300] GeV

Statistical correlation matrix between $y_{boost}$ (rows) in the 4-jet inclusive configuration and $y_{boost}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from absolute spectra through the Bootstrap Method. The binning is the following: Rows: [0-0.1, 0.1-0.2, 0.2-0.3, 0.3-0.4, 0.4-0.5, 0.5-0.6, 0.6-0.7, 0.7-0.8, 0.8-0.9, 0.9-1, 1-1.1, 1.1-1.2, 1.2-1.3, 1.3-1.4, 1.4-1.5, 1.5-2] GeV Columns: [0-0.1, 0.1-0.2, 0.2-0.3, 0.3-0.4, 0.4-0.5, 0.5-0.6, 0.6-0.7, 0.7-0.8, 0.8-0.9, 0.9-1, 1-1.1, 1.1-1.2, 1.2-1.3, 1.3-1.4, 1.4-1.5, 1.5-2] GeV

Statistical correlation matrix between $y_{boost}$ (rows) in the 4-jet inclusive configuration and $|y^{t,had}|$ (columns) in the 4-jet inclusive configuration, obtained at parton level from absolute spectra through the Bootstrap Method. The binning is the following: Rows: [0-0.1, 0.1-0.2, 0.2-0.3, 0.3-0.4, 0.4-0.5, 0.5-0.6, 0.6-0.7, 0.7-0.8, 0.8-0.9, 0.9-1, 1-1.1, 1.1-1.2, 1.2-1.3, 1.3-1.4, 1.4-1.5, 1.5-2] GeV Columns: [0-0.4, 0.4-0.8, 0.8-1.2, 1.2-1.6, 1.6-2.5]

Statistical correlation matrix between $y_{boost}$ (rows) in the 4-jet inclusive configuration and $p_{T}^{t,had}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from absolute spectra through the Bootstrap Method. The binning is the following: Rows: [0-0.1, 0.1-0.2, 0.2-0.3, 0.3-0.4, 0.4-0.5, 0.5-0.6, 0.6-0.7, 0.7-0.8, 0.8-0.9, 0.9-1, 1-1.1, 1.1-1.2, 1.2-1.3, 1.3-1.4, 1.4-1.5, 1.5-2] GeV Columns: [0-60, 60-100, 100-150, 150-200, 200-260, 260-320, 320-400, 400-500] GeV

Statistical correlation matrix between $y_{boost}$ (rows) in the 4-jet inclusive configuration and $|y^{t\bar{t}}|$ (columns) in the 4-jet inclusive configuration, obtained at parton level from absolute spectra through the Bootstrap Method. The binning is the following: Rows: [0-0.1, 0.1-0.2, 0.2-0.3, 0.3-0.4, 0.4-0.5, 0.5-0.6, 0.6-0.7, 0.7-0.8, 0.8-0.9, 0.9-1, 1-1.1, 1.1-1.2, 1.2-1.3, 1.3-1.4, 1.4-1.5, 1.5-2] GeV Columns: [0-0.3, 0.3-0.6, 0.6-0.9, 0.9-1.3, 1.3-2.5]

Statistical correlation matrix between $y_{boost}$ (rows) in the 4-jet inclusive configuration and $m^{t\bar{t}}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from absolute spectra through the Bootstrap Method. The binning is the following: Rows: [0-0.1, 0.1-0.2, 0.2-0.3, 0.3-0.4, 0.4-0.5, 0.5-0.6, 0.6-0.7, 0.7-0.8, 0.8-0.9, 0.9-1, 1-1.1, 1.1-1.2, 1.2-1.3, 1.3-1.4, 1.4-1.5, 1.5-2] GeV Columns: [345-400, 400-470, 470-550, 550-650, 650-800, 800-1100, 1100-1600] GeV

Statistical correlation matrix between $y_{boost}$ (rows) in the 4-jet inclusive configuration and $p_{T}^{t\bar{t}}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from absolute spectra through the Bootstrap Method. The binning is the following: Rows: [0-0.1, 0.1-0.2, 0.2-0.3, 0.3-0.4, 0.4-0.5, 0.5-0.6, 0.6-0.7, 0.7-0.8, 0.8-0.9, 0.9-1, 1-1.1, 1.1-1.2, 1.2-1.3, 1.3-1.4, 1.4-1.5, 1.5-2] GeV Columns: [0-20, 20-45, 45-75, 75-120, 120-190, 190-300] GeV

Statistical correlation matrix between $|y^{t,had}|$ (rows) in the 4-jet inclusive configuration and $|y^{t,had}|$ (columns) in the 4-jet inclusive configuration, obtained at parton level from absolute spectra through the Bootstrap Method. The binning is the following: Rows: [0-0.4, 0.4-0.8, 0.8-1.2, 1.2-1.6, 1.6-2.5] Columns: [0-0.4, 0.4-0.8, 0.8-1.2, 1.2-1.6, 1.6-2.5]

Statistical correlation matrix between $|y^{t,had}|$ (rows) in the 4-jet inclusive configuration and $p_{T}^{t,had}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from absolute spectra through the Bootstrap Method. The binning is the following: Rows: [0-0.4, 0.4-0.8, 0.8-1.2, 1.2-1.6, 1.6-2.5] Columns: [0-60, 60-100, 100-150, 150-200, 200-260, 260-320, 320-400, 400-500] GeV

Statistical correlation matrix between $|y^{t,had}|$ (rows) in the 4-jet inclusive configuration and $|y^{t\bar{t}}|$ (columns) in the 4-jet inclusive configuration, obtained at parton level from absolute spectra through the Bootstrap Method. The binning is the following: Rows: [0-0.4, 0.4-0.8, 0.8-1.2, 1.2-1.6, 1.6-2.5] Columns: [0-0.3, 0.3-0.6, 0.6-0.9, 0.9-1.3, 1.3-2.5]

Statistical correlation matrix between $|y^{t,had}|$ (rows) in the 4-jet inclusive configuration and $m^{t\bar{t}}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from absolute spectra through the Bootstrap Method. The binning is the following: Rows: [0-0.4, 0.4-0.8, 0.8-1.2, 1.2-1.6, 1.6-2.5] Columns: [345-400, 400-470, 470-550, 550-650, 650-800, 800-1100, 1100-1600] GeV

Statistical correlation matrix between $|y^{t,had}|$ (rows) in the 4-jet inclusive configuration and $p_{T}^{t\bar{t}}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from absolute spectra through the Bootstrap Method. The binning is the following: Rows: [0-0.4, 0.4-0.8, 0.8-1.2, 1.2-1.6, 1.6-2.5] Columns: [0-20, 20-45, 45-75, 75-120, 120-190, 190-300] GeV

Statistical correlation matrix between $p_{T}^{t,had}$ (rows) in the 4-jet inclusive configuration and $p_{T}^{t,had}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from absolute spectra through the Bootstrap Method. The binning is the following: Rows: [0-60, 60-100, 100-150, 150-200, 200-260, 260-320, 320-400, 400-500] GeV Columns: [0-60, 60-100, 100-150, 150-200, 200-260, 260-320, 320-400, 400-500] GeV

Statistical correlation matrix between $p_{T}^{t,had}$ (rows) in the 4-jet inclusive configuration and $|y^{t\bar{t}}|$ (columns) in the 4-jet inclusive configuration, obtained at parton level from absolute spectra through the Bootstrap Method. The binning is the following: Rows: [0-60, 60-100, 100-150, 150-200, 200-260, 260-320, 320-400, 400-500] GeV Columns: [0-0.3, 0.3-0.6, 0.6-0.9, 0.9-1.3, 1.3-2.5]

Statistical correlation matrix between $p_{T}^{t,had}$ (rows) in the 4-jet inclusive configuration and $m^{t\bar{t}}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from absolute spectra through the Bootstrap Method. The binning is the following: Rows: [0-60, 60-100, 100-150, 150-200, 200-260, 260-320, 320-400, 400-500] GeV Columns: [345-400, 400-470, 470-550, 550-650, 650-800, 800-1100, 1100-1600] GeV

Statistical correlation matrix between $p_{T}^{t,had}$ (rows) in the 4-jet inclusive configuration and $p_{T}^{t\bar{t}}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from absolute spectra through the Bootstrap Method. The binning is the following: Rows: [0-60, 60-100, 100-150, 150-200, 200-260, 260-320, 320-400, 400-500] GeV Columns: [0-20, 20-45, 45-75, 75-120, 120-190, 190-300] GeV

Statistical correlation matrix between $|y^{t\bar{t}}|$ (rows) in the 4-jet inclusive configuration and $|y^{t\bar{t}}|$ (columns) in the 4-jet inclusive configuration, obtained at parton level from absolute spectra through the Bootstrap Method. The binning is the following: Rows: [0-0.3, 0.3-0.6, 0.6-0.9, 0.9-1.3, 1.3-2.5] Columns: [0-0.3, 0.3-0.6, 0.6-0.9, 0.9-1.3, 1.3-2.5]

Statistical correlation matrix between $|y^{t\bar{t}}|$ (rows) in the 4-jet inclusive configuration and $m^{t\bar{t}}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from absolute spectra through the Bootstrap Method. The binning is the following: Rows: [0-0.3, 0.3-0.6, 0.6-0.9, 0.9-1.3, 1.3-2.5] Columns: [345-400, 400-470, 470-550, 550-650, 650-800, 800-1100, 1100-1600] GeV

Statistical correlation matrix between $|y^{t\bar{t}}|$ (rows) in the 4-jet inclusive configuration and $p_{T}^{t\bar{t}}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from absolute spectra through the Bootstrap Method. The binning is the following: Rows: [0-0.3, 0.3-0.6, 0.6-0.9, 0.9-1.3, 1.3-2.5] Columns: [0-20, 20-45, 45-75, 75-120, 120-190, 190-300] GeV

Statistical correlation matrix between $m^{t\bar{t}}$ (rows) in the 4-jet inclusive configuration and $m^{t\bar{t}}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from absolute spectra through the Bootstrap Method. The binning is the following: Rows: [345-400, 400-470, 470-550, 550-650, 650-800, 800-1100, 1100-1600] GeV Columns: [345-400, 400-470, 470-550, 550-650, 650-800, 800-1100, 1100-1600] GeV

Statistical correlation matrix between $m^{t\bar{t}}$ (rows) in the 4-jet inclusive configuration and $p_{T}^{t\bar{t}}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from absolute spectra through the Bootstrap Method. The binning is the following: Rows: [345-400, 400-470, 470-550, 550-650, 650-800, 800-1100, 1100-1600] GeV Columns: [0-20, 20-45, 45-75, 75-120, 120-190, 190-300] GeV

Statistical correlation matrix between $p_{T}^{t\bar{t}}$ (rows) in the 4-jet inclusive configuration and $p_{T}^{t\bar{t}}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from absolute spectra through the Bootstrap Method. The binning is the following: Rows: [0-20, 20-45, 45-75, 75-120, 120-190, 190-300] GeV Columns: [0-20, 20-45, 45-75, 75-120, 120-190, 190-300] GeV

Statistical correlation matrix between |$p_{out}^{t\bar{t}}$| (rows) in the 4-jet inclusive configuration and |$p_{out}^{t\bar{t}}$| (columns) in the 4-jet inclusive configuration, obtained at parton level from relative spectra through the Bootstrap Method. The binning is the following: Rows: [0-40, 40-80, 80-120, 120-170, 170-230, 230-600] GeV Columns: [0-40, 40-80, 80-120, 120-170, 170-230, 230-600] GeV

Statistical correlation matrix between |$p_{out}^{t\bar{t}}$| (rows) in the 4-jet inclusive configuration and $\chi^{t\bar{t}}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from relative spectra through the Bootstrap Method. The binning is the following: Rows: [0-40, 40-80, 80-120, 120-170, 170-230, 230-600] GeV Columns: [1-1.4, 1.4-1.9, 1.9-2.5, 2.5-3.2, 3.2-4.2, 4.2-5.5, 5.5-7.2, 7.2-9.3, 9.3-12, 12-20] GeV

Statistical correlation matrix between |$p_{out}^{t\bar{t}}$| (rows) in the 4-jet inclusive configuration and $\Delta\phi^{t\bar{t}}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from relative spectra through the Bootstrap Method. The binning is the following: Rows: [0-40, 40-80, 80-120, 120-170, 170-230, 230-600] GeV Columns: [0.0-2.0, 2.0-2.75, 2.75-3.0, 3.0-3.15]

Statistical correlation matrix between |$p_{out}^{t\bar{t}}$| (rows) in the 4-jet inclusive configuration and $H_T^{t\bar{t}}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from relative spectra through the Bootstrap Method. The binning is the following: Rows: [0-40, 40-80, 80-120, 120-170, 170-230, 230-600] GeV Columns: [0-90, 90-140, 140-195, 195-255, 255-320, 320-385, 385-455, 455-530, 530-610, 610-695, 695-780, 780-865, 865-950, 950-1041, 1041-1500] GeV

Statistical correlation matrix between |$p_{out}^{t\bar{t}}$| (rows) in the 4-jet inclusive configuration and $y_{boost}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from relative spectra through the Bootstrap Method. The binning is the following: Rows: [0-40, 40-80, 80-120, 120-170, 170-230, 230-600] GeV Columns: [0-0.1, 0.1-0.2, 0.2-0.3, 0.3-0.4, 0.4-0.5, 0.5-0.6, 0.6-0.7, 0.7-0.8, 0.8-0.9, 0.9-1, 1-1.1, 1.1-1.2, 1.2-1.3, 1.3-1.4, 1.4-1.5, 1.5-2] GeV

Statistical correlation matrix between |$p_{out}^{t\bar{t}}$| (rows) in the 4-jet inclusive configuration and $|y^{t,had}|$ (columns) in the 4-jet inclusive configuration, obtained at parton level from relative spectra through the Bootstrap Method. The binning is the following: Rows: [0-40, 40-80, 80-120, 120-170, 170-230, 230-600] GeV Columns: [0-0.4, 0.4-0.8, 0.8-1.2, 1.2-1.6, 1.6-2.5]

Statistical correlation matrix between |$p_{out}^{t\bar{t}}$| (rows) in the 4-jet inclusive configuration and $p_{T}^{t,had}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from relative spectra through the Bootstrap Method. The binning is the following: Rows: [0-40, 40-80, 80-120, 120-170, 170-230, 230-600] GeV Columns: [0-60, 60-100, 100-150, 150-200, 200-260, 260-320, 320-400, 400-500] GeV

Statistical correlation matrix between |$p_{out}^{t\bar{t}}$| (rows) in the 4-jet inclusive configuration and $|y^{t\bar{t}}|$ (columns) in the 4-jet inclusive configuration, obtained at parton level from relative spectra through the Bootstrap Method. The binning is the following: Rows: [0-40, 40-80, 80-120, 120-170, 170-230, 230-600] GeV Columns: [0-0.3, 0.3-0.6, 0.6-0.9, 0.9-1.3, 1.3-2.5]

Statistical correlation matrix between |$p_{out}^{t\bar{t}}$| (rows) in the 4-jet inclusive configuration and $m^{t\bar{t}}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from relative spectra through the Bootstrap Method. The binning is the following: Rows: [0-40, 40-80, 80-120, 120-170, 170-230, 230-600] GeV Columns: [345-400, 400-470, 470-550, 550-650, 650-800, 800-1100, 1100-1600] GeV

Statistical correlation matrix between |$p_{out}^{t\bar{t}}$| (rows) in the 4-jet inclusive configuration and $p_{T}^{t\bar{t}}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from relative spectra through the Bootstrap Method. The binning is the following: Rows: [0-40, 40-80, 80-120, 120-170, 170-230, 230-600] GeV Columns: [0-20, 20-45, 45-75, 75-120, 120-190, 190-300] GeV

Statistical correlation matrix between $\chi^{t\bar{t}}$ (rows) in the 4-jet inclusive configuration and $\chi^{t\bar{t}}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from relative spectra through the Bootstrap Method. The binning is the following: Rows: [1-1.4, 1.4-1.9, 1.9-2.5, 2.5-3.2, 3.2-4.2, 4.2-5.5, 5.5-7.2, 7.2-9.3, 9.3-12, 12-20] GeV Columns: [1-1.4, 1.4-1.9, 1.9-2.5, 2.5-3.2, 3.2-4.2, 4.2-5.5, 5.5-7.2, 7.2-9.3, 9.3-12, 12-20] GeV

Statistical correlation matrix between $\chi^{t\bar{t}}$ (rows) in the 4-jet inclusive configuration and $\Delta\phi^{t\bar{t}}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from relative spectra through the Bootstrap Method. The binning is the following: Rows: [1-1.4, 1.4-1.9, 1.9-2.5, 2.5-3.2, 3.2-4.2, 4.2-5.5, 5.5-7.2, 7.2-9.3, 9.3-12, 12-20] GeV Columns: [0.0-2.0, 2.0-2.75, 2.75-3.0, 3.0-3.15]

Statistical correlation matrix between $\chi^{t\bar{t}}$ (rows) in the 4-jet inclusive configuration and $H_T^{t\bar{t}}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from relative spectra through the Bootstrap Method. The binning is the following: Rows: [1-1.4, 1.4-1.9, 1.9-2.5, 2.5-3.2, 3.2-4.2, 4.2-5.5, 5.5-7.2, 7.2-9.3, 9.3-12, 12-20] GeV Columns: [0-90, 90-140, 140-195, 195-255, 255-320, 320-385, 385-455, 455-530, 530-610, 610-695, 695-780, 780-865, 865-950, 950-1041, 1041-1500] GeV

Statistical correlation matrix between $\chi^{t\bar{t}}$ (rows) in the 4-jet inclusive configuration and $y_{boost}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from relative spectra through the Bootstrap Method. The binning is the following: Rows: [1-1.4, 1.4-1.9, 1.9-2.5, 2.5-3.2, 3.2-4.2, 4.2-5.5, 5.5-7.2, 7.2-9.3, 9.3-12, 12-20] GeV Columns: [0-0.1, 0.1-0.2, 0.2-0.3, 0.3-0.4, 0.4-0.5, 0.5-0.6, 0.6-0.7, 0.7-0.8, 0.8-0.9, 0.9-1, 1-1.1, 1.1-1.2, 1.2-1.3, 1.3-1.4, 1.4-1.5, 1.5-2] GeV

Statistical correlation matrix between $\chi^{t\bar{t}}$ (rows) in the 4-jet inclusive configuration and $|y^{t,had}|$ (columns) in the 4-jet inclusive configuration, obtained at parton level from relative spectra through the Bootstrap Method. The binning is the following: Rows: [1-1.4, 1.4-1.9, 1.9-2.5, 2.5-3.2, 3.2-4.2, 4.2-5.5, 5.5-7.2, 7.2-9.3, 9.3-12, 12-20] GeV Columns: [0-0.4, 0.4-0.8, 0.8-1.2, 1.2-1.6, 1.6-2.5]

Statistical correlation matrix between $\chi^{t\bar{t}}$ (rows) in the 4-jet inclusive configuration and $p_{T}^{t,had}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from relative spectra through the Bootstrap Method. The binning is the following: Rows: [1-1.4, 1.4-1.9, 1.9-2.5, 2.5-3.2, 3.2-4.2, 4.2-5.5, 5.5-7.2, 7.2-9.3, 9.3-12, 12-20] GeV Columns: [0-60, 60-100, 100-150, 150-200, 200-260, 260-320, 320-400, 400-500] GeV

Statistical correlation matrix between $\chi^{t\bar{t}}$ (rows) in the 4-jet inclusive configuration and $|y^{t\bar{t}}|$ (columns) in the 4-jet inclusive configuration, obtained at parton level from relative spectra through the Bootstrap Method. The binning is the following: Rows: [1-1.4, 1.4-1.9, 1.9-2.5, 2.5-3.2, 3.2-4.2, 4.2-5.5, 5.5-7.2, 7.2-9.3, 9.3-12, 12-20] GeV Columns: [0-0.3, 0.3-0.6, 0.6-0.9, 0.9-1.3, 1.3-2.5]

Statistical correlation matrix between $\chi^{t\bar{t}}$ (rows) in the 4-jet inclusive configuration and $m^{t\bar{t}}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from relative spectra through the Bootstrap Method. The binning is the following: Rows: [1-1.4, 1.4-1.9, 1.9-2.5, 2.5-3.2, 3.2-4.2, 4.2-5.5, 5.5-7.2, 7.2-9.3, 9.3-12, 12-20] GeV Columns: [345-400, 400-470, 470-550, 550-650, 650-800, 800-1100, 1100-1600] GeV

Statistical correlation matrix between $\chi^{t\bar{t}}$ (rows) in the 4-jet inclusive configuration and $p_{T}^{t\bar{t}}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from relative spectra through the Bootstrap Method. The binning is the following: Rows: [1-1.4, 1.4-1.9, 1.9-2.5, 2.5-3.2, 3.2-4.2, 4.2-5.5, 5.5-7.2, 7.2-9.3, 9.3-12, 12-20] GeV Columns: [0-20, 20-45, 45-75, 75-120, 120-190, 190-300] GeV

Statistical correlation matrix between $\Delta\phi^{t\bar{t}}$ (rows) in the 4-jet inclusive configuration and $\Delta\phi^{t\bar{t}}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from relative spectra through the Bootstrap Method. The binning is the following: Rows: [0.0-2.0, 2.0-2.75, 2.75-3.0, 3.0-3.15] Columns: [0.0-2.0, 2.0-2.75, 2.75-3.0, 3.0-3.15]

Statistical correlation matrix between $\Delta\phi^{t\bar{t}}$ (rows) in the 4-jet inclusive configuration and $H_T^{t\bar{t}}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from relative spectra through the Bootstrap Method. The binning is the following: Rows: [0.0-2.0, 2.0-2.75, 2.75-3.0, 3.0-3.15] Columns: [0-90, 90-140, 140-195, 195-255, 255-320, 320-385, 385-455, 455-530, 530-610, 610-695, 695-780, 780-865, 865-950, 950-1041, 1041-1500] GeV

Statistical correlation matrix between $\Delta\phi^{t\bar{t}}$ (rows) in the 4-jet inclusive configuration and $y_{boost}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from relative spectra through the Bootstrap Method. The binning is the following: Rows: [0.0-2.0, 2.0-2.75, 2.75-3.0, 3.0-3.15] Columns: [0-0.1, 0.1-0.2, 0.2-0.3, 0.3-0.4, 0.4-0.5, 0.5-0.6, 0.6-0.7, 0.7-0.8, 0.8-0.9, 0.9-1, 1-1.1, 1.1-1.2, 1.2-1.3, 1.3-1.4, 1.4-1.5, 1.5-2] GeV

Statistical correlation matrix between $\Delta\phi^{t\bar{t}}$ (rows) in the 4-jet inclusive configuration and $|y^{t,had}|$ (columns) in the 4-jet inclusive configuration, obtained at parton level from relative spectra through the Bootstrap Method. The binning is the following: Rows: [0.0-2.0, 2.0-2.75, 2.75-3.0, 3.0-3.15] Columns: [0-0.4, 0.4-0.8, 0.8-1.2, 1.2-1.6, 1.6-2.5]

Statistical correlation matrix between $\Delta\phi^{t\bar{t}}$ (rows) in the 4-jet inclusive configuration and $p_{T}^{t,had}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from relative spectra through the Bootstrap Method. The binning is the following: Rows: [0.0-2.0, 2.0-2.75, 2.75-3.0, 3.0-3.15] Columns: [0-60, 60-100, 100-150, 150-200, 200-260, 260-320, 320-400, 400-500] GeV

Statistical correlation matrix between $\Delta\phi^{t\bar{t}}$ (rows) in the 4-jet inclusive configuration and $|y^{t\bar{t}}|$ (columns) in the 4-jet inclusive configuration, obtained at parton level from relative spectra through the Bootstrap Method. The binning is the following: Rows: [0.0-2.0, 2.0-2.75, 2.75-3.0, 3.0-3.15] Columns: [0-0.3, 0.3-0.6, 0.6-0.9, 0.9-1.3, 1.3-2.5]

Statistical correlation matrix between $\Delta\phi^{t\bar{t}}$ (rows) in the 4-jet inclusive configuration and $m^{t\bar{t}}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from relative spectra through the Bootstrap Method. The binning is the following: Rows: [0.0-2.0, 2.0-2.75, 2.75-3.0, 3.0-3.15] Columns: [345-400, 400-470, 470-550, 550-650, 650-800, 800-1100, 1100-1600] GeV

Statistical correlation matrix between $\Delta\phi^{t\bar{t}}$ (rows) in the 4-jet inclusive configuration and $p_{T}^{t\bar{t}}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from relative spectra through the Bootstrap Method. The binning is the following: Rows: [0.0-2.0, 2.0-2.75, 2.75-3.0, 3.0-3.15] Columns: [0-20, 20-45, 45-75, 75-120, 120-190, 190-300] GeV

Statistical correlation matrix between $H_T^{t\bar{t}}$ (rows) in the 4-jet inclusive configuration and $H_T^{t\bar{t}}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from relative spectra through the Bootstrap Method. The binning is the following: Rows: [0-90, 90-140, 140-195, 195-255, 255-320, 320-385, 385-455, 455-530, 530-610, 610-695, 695-780, 780-865, 865-950, 950-1041, 1041-1500] GeV Columns: [0-90, 90-140, 140-195, 195-255, 255-320, 320-385, 385-455, 455-530, 530-610, 610-695, 695-780, 780-865, 865-950, 950-1041, 1041-1500] GeV

Statistical correlation matrix between $H_T^{t\bar{t}}$ (rows) in the 4-jet inclusive configuration and $y_{boost}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from relative spectra through the Bootstrap Method. The binning is the following: Rows: [0-90, 90-140, 140-195, 195-255, 255-320, 320-385, 385-455, 455-530, 530-610, 610-695, 695-780, 780-865, 865-950, 950-1041, 1041-1500] GeV Columns: [0-0.1, 0.1-0.2, 0.2-0.3, 0.3-0.4, 0.4-0.5, 0.5-0.6, 0.6-0.7, 0.7-0.8, 0.8-0.9, 0.9-1, 1-1.1, 1.1-1.2, 1.2-1.3, 1.3-1.4, 1.4-1.5, 1.5-2] GeV

Statistical correlation matrix between $H_T^{t\bar{t}}$ (rows) in the 4-jet inclusive configuration and $|y^{t,had}|$ (columns) in the 4-jet inclusive configuration, obtained at parton level from relative spectra through the Bootstrap Method. The binning is the following: Rows: [0-90, 90-140, 140-195, 195-255, 255-320, 320-385, 385-455, 455-530, 530-610, 610-695, 695-780, 780-865, 865-950, 950-1041, 1041-1500] GeV Columns: [0-0.4, 0.4-0.8, 0.8-1.2, 1.2-1.6, 1.6-2.5]

Statistical correlation matrix between $H_T^{t\bar{t}}$ (rows) in the 4-jet inclusive configuration and $p_{T}^{t,had}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from relative spectra through the Bootstrap Method. The binning is the following: Rows: [0-90, 90-140, 140-195, 195-255, 255-320, 320-385, 385-455, 455-530, 530-610, 610-695, 695-780, 780-865, 865-950, 950-1041, 1041-1500] GeV Columns: [0-60, 60-100, 100-150, 150-200, 200-260, 260-320, 320-400, 400-500] GeV

Statistical correlation matrix between $H_T^{t\bar{t}}$ (rows) in the 4-jet inclusive configuration and $|y^{t\bar{t}}|$ (columns) in the 4-jet inclusive configuration, obtained at parton level from relative spectra through the Bootstrap Method. The binning is the following: Rows: [0-90, 90-140, 140-195, 195-255, 255-320, 320-385, 385-455, 455-530, 530-610, 610-695, 695-780, 780-865, 865-950, 950-1041, 1041-1500] GeV Columns: [0-0.3, 0.3-0.6, 0.6-0.9, 0.9-1.3, 1.3-2.5]

Statistical correlation matrix between $H_T^{t\bar{t}}$ (rows) in the 4-jet inclusive configuration and $m^{t\bar{t}}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from relative spectra through the Bootstrap Method. The binning is the following: Rows: [0-90, 90-140, 140-195, 195-255, 255-320, 320-385, 385-455, 455-530, 530-610, 610-695, 695-780, 780-865, 865-950, 950-1041, 1041-1500] GeV Columns: [345-400, 400-470, 470-550, 550-650, 650-800, 800-1100, 1100-1600] GeV

Statistical correlation matrix between $H_T^{t\bar{t}}$ (rows) in the 4-jet inclusive configuration and $p_{T}^{t\bar{t}}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from relative spectra through the Bootstrap Method. The binning is the following: Rows: [0-90, 90-140, 140-195, 195-255, 255-320, 320-385, 385-455, 455-530, 530-610, 610-695, 695-780, 780-865, 865-950, 950-1041, 1041-1500] GeV Columns: [0-20, 20-45, 45-75, 75-120, 120-190, 190-300] GeV

Statistical correlation matrix between $y_{boost}$ (rows) in the 4-jet inclusive configuration and $y_{boost}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from relative spectra through the Bootstrap Method. The binning is the following: Rows: [0-0.1, 0.1-0.2, 0.2-0.3, 0.3-0.4, 0.4-0.5, 0.5-0.6, 0.6-0.7, 0.7-0.8, 0.8-0.9, 0.9-1, 1-1.1, 1.1-1.2, 1.2-1.3, 1.3-1.4, 1.4-1.5, 1.5-2] GeV Columns: [0-0.1, 0.1-0.2, 0.2-0.3, 0.3-0.4, 0.4-0.5, 0.5-0.6, 0.6-0.7, 0.7-0.8, 0.8-0.9, 0.9-1, 1-1.1, 1.1-1.2, 1.2-1.3, 1.3-1.4, 1.4-1.5, 1.5-2] GeV

Statistical correlation matrix between $y_{boost}$ (rows) in the 4-jet inclusive configuration and $|y^{t,had}|$ (columns) in the 4-jet inclusive configuration, obtained at parton level from relative spectra through the Bootstrap Method. The binning is the following: Rows: [0-0.1, 0.1-0.2, 0.2-0.3, 0.3-0.4, 0.4-0.5, 0.5-0.6, 0.6-0.7, 0.7-0.8, 0.8-0.9, 0.9-1, 1-1.1, 1.1-1.2, 1.2-1.3, 1.3-1.4, 1.4-1.5, 1.5-2] GeV Columns: [0-0.4, 0.4-0.8, 0.8-1.2, 1.2-1.6, 1.6-2.5]

Statistical correlation matrix between $y_{boost}$ (rows) in the 4-jet inclusive configuration and $p_{T}^{t,had}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from relative spectra through the Bootstrap Method. The binning is the following: Rows: [0-0.1, 0.1-0.2, 0.2-0.3, 0.3-0.4, 0.4-0.5, 0.5-0.6, 0.6-0.7, 0.7-0.8, 0.8-0.9, 0.9-1, 1-1.1, 1.1-1.2, 1.2-1.3, 1.3-1.4, 1.4-1.5, 1.5-2] GeV Columns: [0-60, 60-100, 100-150, 150-200, 200-260, 260-320, 320-400, 400-500] GeV

Statistical correlation matrix between $y_{boost}$ (rows) in the 4-jet inclusive configuration and $|y^{t\bar{t}}|$ (columns) in the 4-jet inclusive configuration, obtained at parton level from relative spectra through the Bootstrap Method. The binning is the following: Rows: [0-0.1, 0.1-0.2, 0.2-0.3, 0.3-0.4, 0.4-0.5, 0.5-0.6, 0.6-0.7, 0.7-0.8, 0.8-0.9, 0.9-1, 1-1.1, 1.1-1.2, 1.2-1.3, 1.3-1.4, 1.4-1.5, 1.5-2] GeV Columns: [0-0.3, 0.3-0.6, 0.6-0.9, 0.9-1.3, 1.3-2.5]

Statistical correlation matrix between $y_{boost}$ (rows) in the 4-jet inclusive configuration and $m^{t\bar{t}}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from relative spectra through the Bootstrap Method. The binning is the following: Rows: [0-0.1, 0.1-0.2, 0.2-0.3, 0.3-0.4, 0.4-0.5, 0.5-0.6, 0.6-0.7, 0.7-0.8, 0.8-0.9, 0.9-1, 1-1.1, 1.1-1.2, 1.2-1.3, 1.3-1.4, 1.4-1.5, 1.5-2] GeV Columns: [345-400, 400-470, 470-550, 550-650, 650-800, 800-1100, 1100-1600] GeV

Statistical correlation matrix between $y_{boost}$ (rows) in the 4-jet inclusive configuration and $p_{T}^{t\bar{t}}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from relative spectra through the Bootstrap Method. The binning is the following: Rows: [0-0.1, 0.1-0.2, 0.2-0.3, 0.3-0.4, 0.4-0.5, 0.5-0.6, 0.6-0.7, 0.7-0.8, 0.8-0.9, 0.9-1, 1-1.1, 1.1-1.2, 1.2-1.3, 1.3-1.4, 1.4-1.5, 1.5-2] GeV Columns: [0-20, 20-45, 45-75, 75-120, 120-190, 190-300] GeV

Statistical correlation matrix between $|y^{t,had}|$ (rows) in the 4-jet inclusive configuration and $|y^{t,had}|$ (columns) in the 4-jet inclusive configuration, obtained at parton level from relative spectra through the Bootstrap Method. The binning is the following: Rows: [0-0.4, 0.4-0.8, 0.8-1.2, 1.2-1.6, 1.6-2.5] Columns: [0-0.4, 0.4-0.8, 0.8-1.2, 1.2-1.6, 1.6-2.5]

Statistical correlation matrix between $|y^{t,had}|$ (rows) in the 4-jet inclusive configuration and $p_{T}^{t,had}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from relative spectra through the Bootstrap Method. The binning is the following: Rows: [0-0.4, 0.4-0.8, 0.8-1.2, 1.2-1.6, 1.6-2.5] Columns: [0-60, 60-100, 100-150, 150-200, 200-260, 260-320, 320-400, 400-500] GeV

Statistical correlation matrix between $|y^{t,had}|$ (rows) in the 4-jet inclusive configuration and $|y^{t\bar{t}}|$ (columns) in the 4-jet inclusive configuration, obtained at parton level from relative spectra through the Bootstrap Method. The binning is the following: Rows: [0-0.4, 0.4-0.8, 0.8-1.2, 1.2-1.6, 1.6-2.5] Columns: [0-0.3, 0.3-0.6, 0.6-0.9, 0.9-1.3, 1.3-2.5]

Statistical correlation matrix between $|y^{t,had}|$ (rows) in the 4-jet inclusive configuration and $m^{t\bar{t}}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from relative spectra through the Bootstrap Method. The binning is the following: Rows: [0-0.4, 0.4-0.8, 0.8-1.2, 1.2-1.6, 1.6-2.5] Columns: [345-400, 400-470, 470-550, 550-650, 650-800, 800-1100, 1100-1600] GeV

Statistical correlation matrix between $|y^{t,had}|$ (rows) in the 4-jet inclusive configuration and $p_{T}^{t\bar{t}}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from relative spectra through the Bootstrap Method. The binning is the following: Rows: [0-0.4, 0.4-0.8, 0.8-1.2, 1.2-1.6, 1.6-2.5] Columns: [0-20, 20-45, 45-75, 75-120, 120-190, 190-300] GeV

Statistical correlation matrix between $p_{T}^{t,had}$ (rows) in the 4-jet inclusive configuration and $p_{T}^{t,had}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from relative spectra through the Bootstrap Method. The binning is the following: Rows: [0-60, 60-100, 100-150, 150-200, 200-260, 260-320, 320-400, 400-500] GeV Columns: [0-60, 60-100, 100-150, 150-200, 200-260, 260-320, 320-400, 400-500] GeV

Statistical correlation matrix between $p_{T}^{t,had}$ (rows) in the 4-jet inclusive configuration and $|y^{t\bar{t}}|$ (columns) in the 4-jet inclusive configuration, obtained at parton level from relative spectra through the Bootstrap Method. The binning is the following: Rows: [0-60, 60-100, 100-150, 150-200, 200-260, 260-320, 320-400, 400-500] GeV Columns: [0-0.3, 0.3-0.6, 0.6-0.9, 0.9-1.3, 1.3-2.5]

Statistical correlation matrix between $p_{T}^{t,had}$ (rows) in the 4-jet inclusive configuration and $m^{t\bar{t}}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from relative spectra through the Bootstrap Method. The binning is the following: Rows: [0-60, 60-100, 100-150, 150-200, 200-260, 260-320, 320-400, 400-500] GeV Columns: [345-400, 400-470, 470-550, 550-650, 650-800, 800-1100, 1100-1600] GeV

Statistical correlation matrix between $p_{T}^{t,had}$ (rows) in the 4-jet inclusive configuration and $p_{T}^{t\bar{t}}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from relative spectra through the Bootstrap Method. The binning is the following: Rows: [0-60, 60-100, 100-150, 150-200, 200-260, 260-320, 320-400, 400-500] GeV Columns: [0-20, 20-45, 45-75, 75-120, 120-190, 190-300] GeV

Statistical correlation matrix between $|y^{t\bar{t}}|$ (rows) in the 4-jet inclusive configuration and $|y^{t\bar{t}}|$ (columns) in the 4-jet inclusive configuration, obtained at parton level from relative spectra through the Bootstrap Method. The binning is the following: Rows: [0-0.3, 0.3-0.6, 0.6-0.9, 0.9-1.3, 1.3-2.5] Columns: [0-0.3, 0.3-0.6, 0.6-0.9, 0.9-1.3, 1.3-2.5]

Statistical correlation matrix between $|y^{t\bar{t}}|$ (rows) in the 4-jet inclusive configuration and $m^{t\bar{t}}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from relative spectra through the Bootstrap Method. The binning is the following: Rows: [0-0.3, 0.3-0.6, 0.6-0.9, 0.9-1.3, 1.3-2.5] Columns: [345-400, 400-470, 470-550, 550-650, 650-800, 800-1100, 1100-1600] GeV

Statistical correlation matrix between $|y^{t\bar{t}}|$ (rows) in the 4-jet inclusive configuration and $p_{T}^{t\bar{t}}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from relative spectra through the Bootstrap Method. The binning is the following: Rows: [0-0.3, 0.3-0.6, 0.6-0.9, 0.9-1.3, 1.3-2.5] Columns: [0-20, 20-45, 45-75, 75-120, 120-190, 190-300] GeV

Statistical correlation matrix between $m^{t\bar{t}}$ (rows) in the 4-jet inclusive configuration and $m^{t\bar{t}}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from relative spectra through the Bootstrap Method. The binning is the following: Rows: [345-400, 400-470, 470-550, 550-650, 650-800, 800-1100, 1100-1600] GeV Columns: [345-400, 400-470, 470-550, 550-650, 650-800, 800-1100, 1100-1600] GeV

Statistical correlation matrix between $m^{t\bar{t}}$ (rows) in the 4-jet inclusive configuration and $p_{T}^{t\bar{t}}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from relative spectra through the Bootstrap Method. The binning is the following: Rows: [345-400, 400-470, 470-550, 550-650, 650-800, 800-1100, 1100-1600] GeV Columns: [0-20, 20-45, 45-75, 75-120, 120-190, 190-300] GeV

Statistical correlation matrix between $p_{T}^{t\bar{t}}$ (rows) in the 4-jet inclusive configuration and $p_{T}^{t\bar{t}}$ (columns) in the 4-jet inclusive configuration, obtained at parton level from relative spectra through the Bootstrap Method. The binning is the following: Rows: [0-20, 20-45, 45-75, 75-120, 120-190, 190-300] GeV Columns: [0-20, 20-45, 45-75, 75-120, 120-190, 190-300] GeV

Covariance matrix of the relative cross-section as function of the top quark pT, accounting for the statistical and systematic uncertainties in the resolved topology.

Covariance matrix for the absolute cross-section as function of the hadronic top-quark top quark pT, accounting for the statistic and systematic uncertainties in the boosted topology.

Covariance matrix for the absolute cross-section as function of the hadronic top-quark top quark pT, accounting for the statistic and systematic uncertainties in the boosted topology.

Covariance matrix for the relative cross-section as function of the hadronic top-quark top quark pT, accounting for the statistic and systematic uncertainties in the boosted topology.

Covariance matrix for the relative cross-section as function of the hadronic top-quark top quark pT, accounting for the statistic and systematic uncertainties in the boosted topology.

Covariance matrix of the absolute cross-section as function of the absolute value of the rapidity of the top quark, accounting for the statistical and systematic uncertainties in the resolved topology.

Covariance matrix of the absolute cross-section as function of the absolute value of the rapidity of the top quark, accounting for the statistical and systematic uncertainties in the resolved topology.

Covariance matrix of the relative cross-section as function of the absolute value of the rapidity of the top quark, accounting for the statistical and systematic uncertainties in the resolved topology.

Covariance matrix of the relative cross-section as function of the absolute value of the rapidity of the top quark, accounting for the statistical and systematic uncertainties in the resolved topology.

Covariance matrix for the absolute cross-section as function of the absolute value of the rapidity of the top quark, accounting for the statistic and systematic uncertainties in the boosted topology.

Covariance matrix for the absolute cross-section as function of the absolute value of the rapidity of the top quark, accounting for the statistic and systematic uncertainties in the boosted topology.

Covariance matrix for the relative cross-section as function of the absolute value of the rapidity of the top quark, accounting for the statistic and systematic uncertainties in the boosted topology.

Covariance matrix for the relative cross-section as function of the absolute value of the rapidity of the top quark, accounting for the statistic and systematic uncertainties in the boosted topology.

Covariance matrix of the absolute cross-section as function of the mass of the tt̄ system, accounting for the statistical and systematic uncertainties in the resolved topology.

Covariance matrix of the absolute cross-section as function of the mass of the tt̄ system, accounting for the statistical and systematic uncertainties in the resolved topology.

Covariance matrix of the relative cross-section as function of the mass of the tt̄ system, accounting for the statistical and systematic uncertainties in the resolved topology.

Covariance matrix of the relative cross-section as function of the mass of the tt̄ system, accounting for the statistical and systematic uncertainties in the resolved topology.

Covariance matrix of the absolute cross-section as function of the tt̄ system pT, accounting for the statistical and systematic uncertainties in the resolved topology.

Covariance matrix of the absolute cross-section as function of the tt̄ system pT, accounting for the statistical and systematic uncertainties in the resolved topology.

Covariance matrix of the relative cross-section as function of the tt̄ system pT, accounting for the statistical and systematic uncertainties in the resolved topology.

Covariance matrix of the relative cross-section as function of the tt̄ system pT, accounting for the statistical and systematic uncertainties in the resolved topology.

Covariance matrix of the absolute cross-section as function of the absolute value of the rapidity of the tt̄ system, accounting for the statistical and systematic uncertainties in the resolved topology.

Covariance matrix of the absolute cross-section as function of the absolute value of the rapidity of the tt̄ system, accounting for the statistical and systematic uncertainties in the resolved topology.

Covariance matrix of the absolute cross-section as function of the absolute value of the rapidity of the tt̄ system, accounting for the statistical and systematic uncertainties in the resolved topology.

Covariance matrix of the absolute cross-section as function of the absolute value of the rapidity of the tt̄ system, accounting for the statistical and systematic uncertainties in the resolved topology.

Table of systematic uncertainties for the absolute differential cross-section at particle level for the top quark transverse momentum in the resolved regime. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text.

Table of systematic uncertainties for the absolute differential cross-section at particle level for the top quark transverse momentum in the resolved regime. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text.

Table of systematic uncertainties for the relative differential cross-section at particle level for the top quark transverse momentum in the resolved regime. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text.

Table of systematic uncertainties for the relative differential cross-section at particle level for the top quark transverse momentum in the resolved regime. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text.

Table of systematic uncertainties for the absolute differential cross-section at particle level for the absolute value of the top quark rapidity in the resolved regime. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text.

Table of systematic uncertainties for the absolute differential cross-section at particle level for the absolute value of the top quark rapidity in the resolved regime. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text.

Table of systematic uncertainties for the relative differential cross-section at particle level for the absolute value of the top quark rapidity in the resolved regime. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text.

Table of systematic uncertainties for the relative differential cross-section at particle level for the absolute value of the top quark rapidity in the resolved regime. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text.

Table of systematic uncertainties for the absolute differential cross-section at particle level for the tt̄ system transverse momentum in the resolved regime. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text.

Table of systematic uncertainties for the absolute differential cross-section at particle level for the tt̄ system transverse momentum in the resolved regime. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text.

Table of systematic uncertainties for the relative differential cross-section at particle level for the tt̄ system transverse momentum in the resolved regime. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text.

Table of systematic uncertainties for the relative differential cross-section at particle level for the tt̄ system transverse momentum in the resolved regime. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text.

Table of systematic uncertainties for the absolute differential cross-section at particle level for the absolute value of the tt̄ system rapidity in the resolved regime. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text.

Table of systematic uncertainties for the absolute differential cross-section at particle level for the absolute value of the tt̄ system rapidity in the resolved regime. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text.

Table of systematic uncertainties for the relative differential cross-section at particle level for the absolute value of the tt̄ system rapidity in the resolved regime. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text.

Table of systematic uncertainties for the relative differential cross-section at particle level for the absolute value of the tt̄ system rapidity in the resolved regime. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text.

Table of systematic uncertainties for the absolute differential cross-section at particle level for the mass of the tt̄ system in the resolved regime. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text.

Table of systematic uncertainties for the absolute differential cross-section at particle level for the mass of the tt̄ system in the resolved regime. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text.

Table of systematic uncertainties for the relative differential cross-section at particle level for the mass of the tt̄ system in the resolved regime. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text.

Table of systematic uncertainties for the relative differential cross-section at particle level for the mass of the tt̄ system in the resolved regime. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text.

Table of systematic uncertainties for the absolute differential cross-section at particle level for the top quark transverse momentum in the boosted regime. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text.

Table of systematic uncertainties for the absolute differential cross-section at particle level for the top quark transverse momentum in the boosted regime. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text.

Table of systematic uncertainties for the relative differential cross-section at particle level for the top quark transverse momentum in the boosted regime. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text.

Table of systematic uncertainties for the relative differential cross-section at particle level for the top quark transverse momentum in the boosted regime. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text.

Table of systematic uncertainties for the absolute differential cross-section at particle level for the absolute value of the top quark rapidity in the boosted regime. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text.

Table of systematic uncertainties for the absolute differential cross-section at particle level for the absolute value of the top quark rapidity in the boosted regime. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text.

Table of systematic uncertainties for the relative differential cross-section at particle level for the absolute value of the top quark rapidity in the boosted regime. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text.

Table of systematic uncertainties for the relative differential cross-section at particle level for the absolute value of the top quark rapidity in the boosted regime. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text.

Measured $t\bar{t}$ differential cross-section and relative uncertainty as a function of the hadronic pseudo-top-quark $|y(\hat{t}_{\mathrm{h}})|$ in the electron channel. The results shown in this table are one of the inputs for the combined results.

Measured $t\bar{t}$ differential cross-section and relative uncertainty as a function of the leptonic pseudo-top-quark $p_{\mathrm{T}}(\hat{t}_{\mathrm{l}})$ in the muon channel. The results shown in this table are one of the inputs for the combined results.

Measured $t\bar{t}$ differential cross-section and relative uncertainty as a function of the leptonic pseudo-top-quark $p_{\mathrm{T}}(\hat{t}_{\mathrm{l}})$ in the electron channel. The results shown in this table are one of the inputs for the combined results.

Measured $t\bar{t}$ differential cross-section and relative uncertainty as a function of the leptonic pseudo-top-quark $|y(\hat{t}_{\mathrm{l}})|$ in the muon channel. The results shown in this table are one of the inputs for the combined results.

Measured $t\bar{t}$ differential cross-section and relative uncertainty as a function of the leptonic pseudo-top-quark $|y(\hat{t}_{\mathrm{l}})|$ in the electron channel. The results shown in this table are one of the inputs for the combined results.

Measured $t\bar{t}$ differential cross-section and relative uncertainty as a function of the pseudo-top-quark-pair $p_{\mathrm{T}}(\hat{t}_{\mathrm{l}}\hat{t}_{\mathrm{h}})$ in the muon channel.The results shown in this table are one of the inputs for the combined results.

Measured $t\bar{t}$ differential cross-section and relative uncertainty as a function of the pseudo-top-quark-pair $p_{\mathrm{T}}(\hat{t}_{\mathrm{l}}\hat{t}_{\mathrm{h}})$ in the electron channel. The results shown in this table are one of the inputs for the combined results.

Measured $t\bar{t}$ differential cross-section and relative uncertainty as a function of the pseudo-top-quark-pair $|y(\hat{t}_{\mathrm{l}}\hat{t}_{\mathrm{h}})|$ in the muon channel. The results shown in this table are one of the inputs for the combined results.

Measured $t\bar{t}$ differential cross-section and relative uncertainty as a function of the pseudo-top-quark-pair $|y(\hat{t}_{\mathrm{l}}\hat{t}_{\mathrm{h}})|$ in the electron channel. The results shown in this table are one of the inputs for the combined results.

Measured $t\bar{t}$ differential cross-section and relative uncertainty as a function of the pseudo-top-quark-pair $m(\hat{t}_{\mathrm{l}}\hat{t}_{\mathrm{h}})$ in the muon channel. The results shown in this table are one of the inputs for the combined results.

Measured $t\bar{t}$ differential cross-section and relative uncertainty as a function of the pseudo-top-quark-pair $m(\hat{t}_{\mathrm{l}}\hat{t}_{\mathrm{h}})$ in the electron channel. The results shown in this table are one of the inputs for the combined results.

Measured $t\bar{t}$ differential cross-section and relative uncertainty as a function of the hadronic pseudo-top-quark $p_{\mathrm{T}}(\hat{t}_{\mathrm{h}})$ after the electron and muon channel combination. The results shown in this table correspond to the results presented in figure 11(a).

Measured $t\bar{t}$ differential cross-section and relative uncertainty as a function of the hadronic pseudo-top-quark $|y(\hat{t}_{\mathrm{h}})|$ after the electron and muon channel combination. The results shown in this table correspond to the results presentedin figure 12(a).

Measured $t\bar{t}$ differential cross-section and relative uncertainty as a function of theleptonic pseudo-top-quark $p_{\mathrm{T}}(\hat{t}_{\mathrm{l}})$ after the electron and muon channel combination.The results shown in this table correspond to the results presented in figure 11(b).

Measured $t\bar{t}$ differential cross-section and relative uncertaintyas a function of the leptonic pseudo-top-quark $|y(\hat{t}_{\mathrm{l}})|$ after the electron and muon channel combination.The results shown in this table correspond to the results presented in figure 12(b).

Measured $t\bar{t}$ differential cross-section and relative uncertainty as a function ofthe pseudo-top-quark-pair $p_{\mathrm{T}}(\hat{t}_{\mathrm{l}}\hat{t}_{\mathrm{h}})$ after the electron and muon channel combination.The results shown in this table correspond to the results presented in figure 13(a).

Measured $t\bar{t}$ differential cross-section and relative uncertainty as a function of the pseudo-top-quark-pair $|y(\hat{t}_{\mathrm{l}}\hat{t}_{\mathrm{h}})|$ after the electron and muon channel combination.The results shown in this table correspond to the results presented in figure 13(b).

Measured $t\bar{t}$ differential cross-section and relative uncertainty as a function of the pseudo-top-quark-pair $m(\hat{t}_{\mathrm{l}}\hat{t}_{\mathrm{h}})$after the electron and muon channel combination. The results shown in this table correspond to the results presented in figure 13(c).

The leptonic asymmetry dependence on the invariant mass of top-antitop system ($m_{t\bar{t}}$) in the fiducial volume.

The leptonic asymmetry dependence on the longitudinal boost of the top-antitop system ($\beta_z^{t\bar{t}}$) in the fiducial volume.

The leptonic asymmetry dependence on the transverse momentum of the top-antitop system ($p_T^{t\bar{t}}$) in the fiducial volume.

The top-antitop inclusive asymmetry in the fiducial volume.

The top-antitop asymmetry dependence on the invariant mass of top-antitop system ($m_{t\bar{t}}$) in the fiducial volume.

The top-antitop asymmetry dependence on the longitudinal boost of the top-antitop system ($\beta_z^{t\bar{t}}$) in the fiducial volume.

The top-antitop asymmetry dependence on the transverse momentum of the top-antitop system ($p_T^{t\bar{t}}$) in the fiducial volume.

Measured charge asymmetry, $A_c$, values for the electron and muon channels combined after unfolding as a function of the $t\bar{t}$ transverse momentum, $p_{{\rm T}, t\bar{t}}$. The quoted uncertainties include statistical and systematic components after the marginalisation.

Correlation coefficients $\rho_{i,j}$ for the statistical and systematic uncertainties between the $i$-th and $j$-th bin of the differential $A_c$ measurement as a function of the $t\bar{t}$ invariant mass, $m_{t\bar{t}}$.

Correlation coefficients $\rho_{i,j}$ for the statistical and systematic uncertainties between the $i$-th and $j$-th bin of the differential $A_c$ measurement as a function of the $t\bar{t}$ velocity along the z-axis, $\beta_{z,t\bar{t}}$.

Correlation coefficients $\rho_{i,j}$ for the statistical and systematic uncertainties between the $i$-th and $j$-th bin of the differential $A_c$ measurement as a function of the transverse momentum, $p_{{\rm T}, t\bar{t}}$.

Parton-level normalized $t\bar t$ differential cross-sections for $t\bar t$ system mass $m_{t\bar t}$ at $\sqrt{s}$ = 8 TeV. The uncertainties quoted in the second column represent the statistical and systematic uncertainties added in quadrature.

Parton-level normalized $t\bar t$ differential cross-sections for the $t\bar t$ system transverse momentum $p_{T, t\bar t}$ at $\sqrt{s}$ = 8 TeV. The uncertainties quoted in the second column represent the statistical and systematic uncertainties added in quadrature.

Parton-level normalized $t\bar t$ differential cross-sections for the $t\bar t$ system absolute rapidity $|y_{t\bar t}|$ at $\sqrt{s}$ = 8 TeV. The uncertainties quoted in the second column represent the statistical and systematic uncertainties added in quadrature.

Parton-level absolute $t\bar t$ differential cross-sections for $t\bar t$ system mass $m_{t\bar t}$ at $\sqrt{s}$ = 7 TeV. The cross-sections in the last bins include events (if any) beyond of the bin edges. The uncertainties quoted in the second column represent the statistical and systematic uncertainties added in quadrature.

Parton-level absolute $t\bar t$ differential cross-sections for the $t\bar t$ system transverse momentum $p_{T, t\bar t}$ at $\sqrt{s}$ = 7 TeV. The cross-sections in the last bins include events (if any) beyond of the bin edges. The uncertainties quoted in the second column represent the statistical and systematic uncertainties added in quadrature.

Parton-level absolute $t\bar t$ differential cross-sections for the $t\bar t$ system absolute rapidity $|y_{t\bar t}|$ at $\sqrt{s}$ = 7 TeV. The cross-sections in the last bins include events (if any) beyond of the bin edges. The uncertainties quoted in the second column represent the statistical and systematic uncertainties added in quadrature.

Parton-level absolute $t\bar t$ differential cross-sections for $t\bar t$ system mass $m_{t\bar t}$ at $\sqrt{s}$ = 8 TeV. The uncertainties quoted in the second column represent the statistical and systematic uncertainties added in quadrature.

Parton-level absolute $t\bar t$ differential cross-sections for the $t\bar t$ system transverse momentum $p_{T, t\bar t}$ at $\sqrt{s}$ = 8 TeV. The uncertainties quoted in the second column represent the statistical and systematic uncertainties added in quadrature.

Parton-level absolute $t\bar t$ differential cross-sections for the $t\bar t$ system absolute rapidity $|y_{t\bar t}|$ at $\sqrt{s}$ = 8 TeV. The uncertainties quoted in the second column represent the statistical and systematic uncertainties added in quadrature.

Full covariance matrix of the normalized $t\bar t$ differential cross-sections for $t\bar t$ system mass $m_{t\bar t}$ at $\sqrt{s}$ = 7 TeV. The elements of the covariance matrix are in units of 10$^{-6}$ GeV$^{-2}$.

Full covariance matrix of the normalized $t\bar t$ differential cross-sections for $t\bar t$ system transverse momentum $p_{T, t\bar t}$ at $\sqrt{s}$ = 7 TeV. The elements of the covariance matrix are in units of 10$^{-6}$ GeV$^{-2}$.

Full covariance matrix of the normalized $t\bar t$ differential cross-sections for $t\bar t$ system absolute rapidity $|y_{t\bar t}|$ at $\sqrt{s}$ = 7 TeV. The elements of the covariance matrix are unit-less.

Full covariance matrix of the normalized $t\bar t$ differential cross-sections for $t\bar t$ system mass $m_{t\bar t}$ at $\sqrt{s}$ = 8 TeV. The elements of the covariance matrix are in units of 10$^{-6}$ GeV$^{-2}$.

Full covariance matrix of the normalized $t\bar t$ differential cross-sections for $t\bar t$ system transverse momentum $p_{T, t\bar t}$ at $\sqrt{s}$ = 8 TeV. The elements of the covariance matrix are in units of 10$^{-6}$ GeV$^{-2}$.

Full covariance matrix of the normalized $t\bar t$ differential cross-sections for $t\bar t$ system absolute rapidity $|y_{t\bar t}|$ at $\sqrt{s}$ = 8 TeV. The elements of the covariance matrix are unit-less.

Full covariance matrix of the absolute $t\bar t$ differential cross-sections for $t\bar t$ system mass $m_{t\bar t}$ at $\sqrt{s}$ = 7 TeV. The elements of the covariance matrix are in units of pb$^2$ GeV$^{-2}$.

Full covariance matrix of the absolute $t\bar t$ differential cross-sections for $t\bar t$ system transverse momentum $p_{T, t\bar t}$ at $\sqrt{s}$ = 7 TeV. The elements of the covariance matrix are in units of pb$^2$ GeV$^{-2}$.

Full covariance matrix of the normalized $t\bar t$ differential cross-sections for $t\bar t$ system absolute rapidity $|y_{t\bar t}|$ at $\sqrt{s}$ = 7 TeV. The elements of the covariance matrix are pb$^2$.

Full covariance matrix of the absolute $t\bar t$ differential cross-sections for $t\bar t$ system mass $m_{t\bar t}$ at $\sqrt{s}$ = 8 TeV. The elements of the covariance matrix are in units of pb$^2$ GeV$^{-2}$.

Full covariance matrix of the absolute $t\bar t$ differential cross-sections for $t\bar t$ system transverse momentum $p_{T, t\bar t}$ at $\sqrt{s}$ = 8 TeV. The elements of the covariance matrix are in units of pb$^2$ GeV$^{-2}$.

Full covariance matrix of the normalized $t\bar t$ differential cross-sections for $t\bar t$ system absolute rapidity $|y_{t\bar t}|$ at $\sqrt{s}$ = 8 TeV. The elements of the covariance matrix are pb$^2$.

Statistical bin-to-bin correlations in the normalized $t\bar t$ differential cross-sections for $t\bar t$ system mass $m_{t\bar t}$ at $\sqrt{s}$ = 7 TeV. The off-diagonal correlations mainly due to bin migrations in unfolding and the normalization condition.

Statistical bin-to-bin correlations in the normalized $t\bar t$ differential cross-sections for $t\bar t$ system transverse momentum $p_{T, t\bar t}$ at $\sqrt{s}$ = 7 TeV. The off-diagonal correlations mainly due to bin migrations in unfolding and the normalization condition.

Statistical bin-to-bin correlations in the normalized $t\bar t$ differential cross-sections for $t\bar t$ system absolute rapidity $|y_{t\bar t}|$ at $\sqrt{s}$ = 7 TeV. The off-diagonal correlations mainly due to bin migrations in unfolding and the normalization condition.

Statistical bin-to-bin correlations in the normalized $t\bar t$ differential cross-sections for $t\bar t$ system mass $m_{t\bar t}$ at $\sqrt{s}$ = 8 TeV. The off-diagonal correlations mainly due to bin migrations in unfolding and the normalization condition.

Statistical bin-to-bin correlations in the normalized $t\bar t$ differential cross-sections for $t\bar t$ system transverse momentum $p_{T, t\bar t}$ at $\sqrt{s}$ = 8 TeV. The off-diagonal correlations mainly due to bin migrations in unfolding and the normalization condition.

Statistical bin-to-bin correlations in the normalized $t\bar t$ differential cross-sections for $t\bar t$ system absolute rapidity $|y_{t\bar t}|$ at $\sqrt{s}$ = 8 TeV. The off-diagonal correlations mainly due to bin migrations in unfolding and the normalization condition.

Statistical bin-to-bin correlations in the absolute $t\bar t$ differential cross-sections for $t\bar t$ system mass $m_{t\bar t}$ at $\sqrt{s}$ = 7 TeV. The off-diagonal correlations mainly due to bin migrations in unfolding and the normalization condition.

Statistical bin-to-bin correlations in the absolute $t\bar t$ differential cross-sections for $t\bar t$ system transverse momentum $p_{T, t\bar t}$ at $\sqrt{s}$ = 7 TeV. The off-diagonal correlations mainly due to bin migrations in unfolding and the normalization condition.

Statistical bin-to-bin correlations in the absolute $t\bar t$ differential cross-sections for $t\bar t$ system absolute rapidity $|y_{t\bar t}|$ at $\sqrt{s}$ = 7 TeV. The off-diagonal correlations mainly due to bin migrations in unfolding and the normalization condition.

Statistical bin-to-bin correlations in the absolute $t\bar t$ differential cross-sections for $t\bar t$ system mass $m_{t\bar t}$ at $\sqrt{s}$ = 8 TeV. The off-diagonal correlations mainly due to bin migrations in unfolding and the normalization condition.

Statistical bin-to-bin correlations in the absolute $t\bar t$ differential cross-sections for $t\bar t$ system transverse momentum $p_{T, t\bar t}$ at $\sqrt{s}$ = 8 TeV. The off-diagonal correlations mainly due to bin migrations in unfolding and the normalization condition.

Statistical bin-to-bin correlations in the absolute $t\bar t$ differential cross-sections for $t\bar t$ system absolute rapidity $|y_{t\bar t}|$ at $\sqrt{s}$ = 8 TeV. The off-diagonal correlations mainly due to bin migrations in unfolding and the normalization condition.

Comparison of data with estimated backgrounds in the $\tilde{E}_\text{T}^\text{miss}$ distribution with the TZCR1 event selection except for the requirement on $\tilde{E}_\text{T}^\text{miss}$. The variables $\tilde{E}_\text{T}^\text{miss}$ and $\tilde{m}_\text{T}$ are constructed in the same way as $E_\text{T}^\text{miss}$ and $m_\text{T}$ but treating the leading photon transverse momentum as invisible. The predicted backgrounds are scaled with normalization factors. The uncertainty band includes statistical and all experimental systematic uncertainties. The last bin includes overflow.

Comparison of data with estimated backgrounds in the $\tilde{m}_\text{T}$ distribution with the TZCR1 event selection except for the requirement on $\tilde{m}_\text{T}$. The variables $\tilde{E}_\text{T}^\text{miss}$ and $\tilde{m}_\text{T}$ are constructed in the same way as $E_\text{T}^\text{miss}$ and $m_\text{T}$ but treating the leading photon transverse momentum as invisible. The predicted backgrounds are scaled with normalization factors. The uncertainty band includes statistical and all experimental systematic uncertainties. The last bin includes overflow.

Comparison of the observed data ($n_\text{obs}$) with the predicted background ($n_\text{exp}$) in the validation and signal regions. The background predictions are obtained using the background-only fit configuration. The bottom panel shows the significance of the difference between data and predicted background, where the significance is based on the total uncertainty ($\sigma_\text{tot}$).

Jet multiplicity distributions for events where exactly two signal leptons are selected. No correction factors are included in the background normalizations. The uncertainty band includes statistical and all experimental systematic uncertainties. The last bin includes overflow.

Jet multiplicity distributions for events where exactly one lepton plus one $\tau$ candidate are selected. No correction factors are included in the background normalizations. The uncertainty band includes statistical and all experimental systematic uncertainties. The last bin includes overflow.

The $E_\text{T}^\text{miss}$ distribution in SR1. In the plot, the full event selection in the corresponding signal region is applied, except for the requirement on $E_\text{T}^\text{miss}$. The predicted backgrounds are scaled with normalization factors. The uncertainty band includes statistical and all experimental systematic uncertainties. The last bin contains the overflow. Benchmark signal models are overlaid for comparison. The benchmark models are specified by the gluino and stop masses, given in TeV in the table.

The $m_\text{T}$ distribution in SR1. In the plot, the full event selection in the corresponding signal region is applied, except for the requirement on $m_\text{T}$. The predicted backgrounds are scaled with normalization factors. The uncertainty band includes statistical and all experimental systematic uncertainties. The last bin contains the overflow. Benchmark signal models are overlaid for comparison. The benchmark models are specified by the gluino and stop masses, given in TeV in the table.

Expected (black dashed) 95% excluded regions in the plane of $m_{\tilde{g}}$ versus $m_{\tilde{t}_1}$ for gluino-mediated stop production.

Observed (red solid) 95% excluded regions in the plane of $m_{\tilde{g}}$ versus $m_{\tilde{t}_1}$ for gluino-mediated stop production.

Expected (black dashed) 95% excluded regions in the plane of $m_{\tilde{t}_1}$ versus $m_{\tilde{\chi}_1^0}$ for direct stop production.

Observed (red solid) 95% excluded regions in the plane of $m_{\tilde{t}_1}$ versus $m_{\tilde{\chi}_1^0}$ for direct stop production.

The expected upper limits on $T$ quark pair production times the squared branching ratio for $T \rightarrow tZ$ as a function of the $T$ quark mass.

The observed upper limits on $T$ quark pair production times the squared branching ratio for $T \rightarrow tZ$ as a function of the $T$ quark mass.

The expected limits on $T$ quarks as a function of the branching ratios $B\left(T \rightarrow bW\right)$ and $B\left(T \rightarrow tH\right)$ for a $T$ quark with a mass of 800 GeV. The $T$ is assumed to decay in three possible ways: $T \to tZ$, $T \to tH$, and $T \to bW$.

The observed limits on $T$ quarks as a function of the branching ratios $B\left(T \rightarrow bW\right)$ and $B\left(T \rightarrow tH\right)$ for a $T$ quark with a mass of 800 GeV. The $T$ is assumed to decay in three possible ways: $T \to tZ$, $T \to tH$, and $T \to bW$.

The $m_\text{T}$ distribution in the WVR2-tail validation region which has the same preselection and jet $p_\text{T}$ requirements as SR2.

The $am_\text{T2}$ distribution in the WVR2-tail validation region which has the same preselection and jet $p_\text{T}$ requirements as SR2.

Large-radius jet mass ($R=1.2$), decomposed into the number of small-radius jet constituents. The lower panel shows the ratio of the total data to the total prediction (summed over all jet multiplicities). Events are required to have one lepton, four jets with $p_\text{T}>80,50,40,40$ GeV, at least one $b$-tagged jet, $E_\text{T}^\text{miss}>200$ GeV, and $m_\text{T}>30$ GeV.

Distribution of $m_\text{T2}^\tau$ in data for a selection enriched in $t\bar{t}$ events with one hadronically decaying $\tau$. Events that have no hadronic $\tau$ candidate (that passes the Loose identification criteria, as well as other requirements) are not shown in the plot.

Upper limits on the model cross-section in units of pb for the gluino-mediated stop models.

Upper limits on the model cross-section in units of pb for the models with direct stop pair production.

Illustration of the best expected signal region per signal grid point for the gluino-mediated stop models. This mapping is used for the final combined exclusion limits.

Illustration of the best expected signal region per signal grid point for models with direct stop pair production. This mapping is used for the final combined exclusion limits.

Expected $CL_s$ values for the gluino-mediated stop models.

Observed $CL_s$ values for the gluino-mediated stop models.

Expected $CL_s$ values for the direct stop pair production models.

Observed $CL_s$ values for the direct stop pair production models.

Expected limit using SR1 for models with direct stop pair production and an unpolarized stop (and bino LSP).

Expected limit using SR1 for models with direct stop pair production with $\tilde{t}_1=\tilde{t}_L$ (and bino LSP).

Expected limit using SR1 for models with direct stop pair production with $\tilde{t}_1\sim\tilde{t}_R$ (and bino LSP).

Observed limit using SR1 for models with direct stop pair production and an unpolarized stop (and bino LSP).

Observed limit using SR1 for models with direct stop pair production with $\tilde{t}_1=\tilde{t}_L$ (and bino LSP).

Observed limit using SR1 for models with direct stop pair production with $\tilde{t}_1\sim\tilde{t}_R$ (and bino LSP).

Expected limit using SR2 for models with direct stop pair production and an unpolarized stop (and bino LSP).

Expected limit using SR2 for models with direct stop pair production with $\tilde{t}_1=\tilde{t}_L$ (and bino LSP).

Expected limit using SR2 for models with direct stop pair production with $\tilde{t}_1\sim\tilde{t}_R$ (and bino LSP).

Observed limit using SR2 for models with direct stop pair production and an unpolarized stop (and bino LSP).

Observed limit using SR2 for models with direct stop pair production with $\tilde{t}_1=\tilde{t}_L$ (and bino LSP).

Observed limit using SR2 for models with direct stop pair production with $\tilde{t}_1\sim\tilde{t}_R$ (and bino LSP).

Expected limit using SR1+SR2 (best expected) for models with direct stop pair production and an unpolarized stop (and bino LSP).

Expected limit using SR1+SR2 (best expected) for models with direct stop pair production with $\tilde{t}_1=\tilde{t}_L$ (and bino LSP).

Expected limit using SR1+SR2 (best expected) for models with direct stop pair production with $\tilde{t}_1\sim\tilde{t}_R$ (and bino LSP).

Observed limit using SR1+SR2 (best expected) for models with direct stop pair production and an unpolarized stop (and bino LSP).

Observed limit using SR1+SR2 (best expected) for models with direct stop pair production with $\tilde{t}_1=\tilde{t}_L$ (and bino LSP).

Observed limit using SR1+SR2 (best expected) for models with direct stop pair production with $\tilde{t}_1\sim\tilde{t}_R$ (and bino LSP).

Acceptance for SR1 in the gluino-mediated stop models. The acceptance is defined as the fraction of signal events that pass the analysis selection performed on generator-level objects, therefore emulating an ideal detector with perfect particle identification and no measurement resolution effects.

Acceptance for SR1 in the direct stop pair production. The acceptance is defined as the fraction of signal events that pass the analysis selection performed on generator-level objects, therefore emulating an ideal detector with perfect particle identification and no measurement resolution effects.

Acceptance for SR2 in the gluino-mediated stop models. The acceptance is defined as the fraction of signal events that pass the analysis selection performed on generator-level objects, therefore emulating an ideal detector with perfect particle identification and no measurement resolution effects.

Acceptance for SR2 in the direct stop pair production. The acceptance is defined as the fraction of signal events that pass the analysis selection performed on generator-level objects, therefore emulating an ideal detector with perfect particle identification and no measurement resolution effects.

Acceptance for SR3 in the gluino-mediated stop models. The acceptance is defined as the fraction of signal events that pass the analysis selection performed on generator-level objects, therefore emulating an ideal detector with perfect particle identification and no measurement resolution effects.

Acceptance for SR3 in the direct stop pair production. The acceptance is defined as the fraction of signal events that pass the analysis selection performed on generator-level objects, therefore emulating an ideal detector with perfect particle identification and no measurement resolution effects.

Efficiency for SR1 in the gluino-mediated stop models. The efficiency is the ratio between the expected signal rate calculated with simulated data passing all the reconstruction level cuts applied to reconstructed objects, and the signal rate for an ideal detector (with perfect particle identification and no measurement resolution effects).

Efficiency for SR1 in the direct stop pair production. The efficiency is the ratio between the expected signal rate calculated with simulated data passing all the reconstruction level cuts applied to reconstructed objects, and the signal rate for an ideal detector (with perfect particle identification and no measurement resolution effects).

Efficiency for SR2 in the gluino-mediated stop models. The efficiency is the ratio between the expected signal rate calculated with simulated data passing all the reconstruction level cuts applied to reconstructed objects, and the signal rate for an ideal detector (with perfect particle identification and no measurement resolution effects).

Efficiency for SR2 in the direct stop pair production. The efficiency is the ratio between the expected signal rate calculated with simulated data passing all the reconstruction level cuts applied to reconstructed objects, and the signal rate for an ideal detector (with perfect particle identification and no measurement resolution effects).

Efficiency for SR3 in the gluino-mediated stop models. The efficiency is the ratio between the expected signal rate calculated with simulated data passing all the reconstruction level cuts applied to reconstructed objects, and the signal rate for an ideal detector (with perfect particle identification and no measurement resolution effects).

Efficiency for SR3 in the direct stop pair production. The efficiency is the ratio between the expected signal rate calculated with simulated data passing all the reconstruction level cuts applied to reconstructed objects, and the signal rate for an ideal detector (with perfect particle identification and no measurement resolution effects).