Fiducial differential cross section of the electroweak $W^\pm W^\pm jj$ production as a function of $N_{\mathrm{gap}\,\mathrm{jets}}$. The correlation of uncertainties of the measured cross section across bins is presented in Table 14.

Fiducial differential cross section of the electroweak $W^\pm W^\pm jj$ production as a function of $\xi_{\mathrm{j}3}$. The correlation of uncertainties of the measured cross section across bins is presented in Table 15.

Fiducial differential cross section of the inclusive $W^\pm W^\pm jj$ production as a function of $m_{\ell\ell}$. The correlation of uncertainties of the measured cross section across bins is presented in Table 16.

Fiducial differential cross section of the inclusive $W^\pm W^\pm jj$ production as a function of $m_{\mathrm{T}}$. The correlation of uncertainties of the measured cross section across bins is presented in Table 17.

Fiducial differential cross section of the inclusive $W^\pm W^\pm jj$ production as a function of $m_{\mathrm{jj}}$. The correlation of uncertainties of the measured cross section across bins is presented in Table 18.

Fiducial differential cross section of the inclusive $W^\pm W^\pm jj$ production as a function of $N_{\mathrm{gap}\,\mathrm{jets}}$. The correlation of uncertainties of the measured cross section across bins is presented in Table 19.

Fiducial differential cross section of the inclusive $W^\pm W^\pm jj$ production as a function of $\xi_{\mathrm{j}3}$. The correlation of uncertainties of the measured cross section across bins is presented in Table 20.

Observed correlations between the bins of the LH-unfolded cross section of the electroweak $W^\pm W^\pm jj$ production as a function of $m_{\ell\ell}$. See Table 1.

Observed correlations between the bins of the LH-unfolded cross section of the electroweak $W^\pm W^\pm jj$ production as a function of $m_{\mathrm{T}}$. See Table 2.

Observed correlations between the bins of the LH-unfolded cross section of the electroweak $W^\pm W^\pm jj$ production as a function of $m_{\mathrm{jj}}$. See Table 3.

Observed correlations between the bins of the LH-unfolded cross section of the electroweak $W^\pm W^\pm jj$ production as a function of $N_{\mathrm{gap}\,\mathrm{jets}}$. See Table 4.

Observed correlations between the bins of the LH-unfolded cross section of the electroweak $W^\pm W^\pm jj$ production as a function of $\xi_{\mathrm{j}3}$. See Table 5.

Observed correlations between the bins of the LH-unfolded cross section of the inclusive $W^\pm W^\pm jj$ production as a function of $m_{\ell\ell}$. See Table 6.

Observed correlations between the bins of the LH-unfolded cross section of the inclusive $W^\pm W^\pm jj$ production as a function of $m_{\mathrm{T}}$. See Table 7.

Observed correlations between the bins of the LH-unfolded cross section of the inclusive $W^\pm W^\pm jj$ production as a function of $m_{\mathrm{jj}}$. See Table 8.

Observed correlations between the bins of the LH-unfolded cross section of the inclusive $W^\pm W^\pm jj$ production as a function of $N_{\mathrm{gap}\,\mathrm{jets}}$. See Table 9.

Observed correlations between the bins of the LH-unfolded cross section of the inclusive $W^\pm W^\pm jj$ production as a function of $\xi_{\mathrm{j}3}$. See Table 10.

Evolution of the one-dimensional expected and observed limits at 95% CL on the parameters corresponding to the quartic operators with label M0 as a function of the cut-off scale. The unitarity bounds as a function of the cut-off scale are defined for one non-zero Wilson coefficient.

Evolution of the one-dimensional expected and observed limits at 95% CL on the parameters corresponding to the quartic operators with label M1 as a function of the cut-off scale. The unitarity bounds as a function of the cut-off scale are defined for one non-zero Wilson coefficient.

Evolution of the one-dimensional expected and observed limits at 95% CL on the parameters corresponding to the quartic operators with label M7 as a function of the cut-off scale. The unitarity bounds as a function of the cut-off scale are defined for one non-zero Wilson coefficient. The limits on M7 were obtained without taking into account the SM-EFT interference for the EW W$^\pm$Zjj final state.

Evolution of the one-dimensional expected and observed limits at 95% CL on the parameters corresponding to the quartic operators with label S02 as a function of the cut-off scale. The unitarity bounds as a function of the cut-off scale are defined for one non-zero Wilson coefficient.

Evolution of the one-dimensional expected and observed limits at 95% CL on the parameters corresponding to the quartic operators with label S1 as a function of the cut-off scale. The unitarity bounds as a function of the cut-off scale are defined for one non-zero Wilson coefficient.

Evolution of the one-dimensional expected and observed limits at 95% CL on the parameters corresponding to the quartic operators with label T0 as a function of the cut-off scale. The unitarity bounds as a function of the cut-off scale are defined for one non-zero Wilson coefficient.

Evolution of the one-dimensional expected and observed limits at 95% CL on the parameters corresponding to the quartic operators with label T1 as a function of the cut-off scale. The unitarity bounds as a function of the cut-off scale are defined for one non-zero Wilson coefficient.

Evolution of the one-dimensional expected and observed limits at 95% CL on the parameters corresponding to the quartic operators with label T2 as a function of the cut-off scale. The unitarity bounds as a function of the cut-off scale are defined for one non-zero Wilson coefficient.

Expected and observed exclusion limits at 95% CL for $\sigma_{\mathrm{VBF}}(\mathrm{H}^{\pm\pm}_5) \times \mathcal{B}(\mathrm{H}^{\pm\pm}_5 \rightarrow W^{\pm}W^{\pm})$ as a function of the doubly-charged Higgs mass.

Expected and observed exclusion limits at 95% CL for $\sin\theta_{\mathrm{H}}$ as a function of the doubly-charged Higgs mass in the Georgi-Machacek model.

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 $|y(\bar t)|$.

Normalised fiducial cross section in bins of the leading lepton PT. Leading Lepton is the lepton in the final state with highest PT.

Correlations in the leading Lepton PT distribution.

Normalised D*+- cross section, corrected to the parton level, as a function of zHem for the D*+- jet sample.

Normalised D*+- cross section, for W < 170 GeV, as a function of zJet for the D*+- jet sample.

Normalised D*+- cross section, for W > 170 GeV, as a function of zJet for the D*+- jet sample.

Normalised D*+- cross section, for W < 170 GeV, as a function of zHem for the D*+- jet sample.

Normalised D*+- cross section, for W > 170 GeV, as a function of zHem for the D*+- jet sample.

Normalised D*+- cross section as a function of zHem for the no D*+- jet sample.

Normalised D*+- cross section, corrected to the parton level, as a function of zHem for the no D*+- jet sample.

Covariance Matrix for the normalised D*+- cross section as a function of zJet for the D*+- jet sample.

Covariance Matrix for the normalised D*+- cross section as a function of zHem for the D*+- jet sample.

Covariance Matrix for the normalised D*+- cross section, corrected to the parton level, as a function of zJet for the D*+- jet sample.

Covariance Matrix for the normalised D*+- cross section, corrected to the parton level, as a function of zHem for the D*+- jet sample.

Covariance Matrix for the normalised D*+- cross section, for W < 170 GeV, as a function of zJet for the D*+- jet sample.

Covariance Matrix for the normalised D*+- cross section, for W > 170 GeV, as a function of zJet for the D*+- jet sample.

Covariance Matrix for the normalised D*+- cross section, for W < 170 GeV, as a function of zHem for the D*+- jet sample.

Covariance Matrix for the normalised D*+- cross section, for W > 170 GeV, as a function of zHem for the D*+- jet sample.

Covariance Matrix for the normalised D*+- cross section as a function of zHem for the no D*+- jet sample.

Covariance Matrix for the normalised D*+- cross section, corrected to the parton level, as a function of zHem for the no D*+- jet sample.

Normalised distribution of (1-THRUST) where THRUST is w.r.t the axis which maximises the sum of the longitudinal momenta in the current hemisphere, for Q = 30.0 to 50.0 GeV and X = 0.04910 .

Normalised distribution of (1-THRUST) where THRUST is w.r.t the axis which maximises the sum of the longitudinal momenta in the current hemisphere, for Q = 50.0 to 70.0 GeV and X = 0.11600 .

Normalised distribution of (1-THRUST) where THRUST is w.r.t the axis which maximises the sum of the longitudinal momenta in the current hemisphere, for Q = 70.0 to 100.0 GeV and X = 0.19900 .

Normalised distribution of (1-THRUST) where THRUST is w.r.t the axis which maximises the sum of the longitudinal momenta in the current hemisphere, for Q = 100.0 to 200.0 GeV and X = 0.32300 .

Normalised distribution of (1-THRUST) where THRUST is w.r.t the vitrual photon axis, for Q = 14.0 to 16.0 GeV and X = 0.00841 .

Normalised distribution of (1-THRUST) where THRUST is w.r.t the vitrual photon axis, for Q = 16.0 to 20.0 GeV and X = 0.01180 .

Normalised distribution of (1-THRUST) where THRUST is w.r.t the vitrual photon axis, for Q = 20.0 to 30.0 GeV and X = 0.02090 .

Normalised distribution of (1-THRUST) where THRUST is w.r.t the vitrual photon axis, for Q = 30.0 to 50.0 GeV and X = 0.04910 .

Normalised distribution of (1-THRUST) where THRUST is w.r.t the vitrual photon axis, for Q = 50.0 to 70.0 GeV and X = 0.11600 .

Normalised distribution of (1-THRUST) where THRUST is w.r.t the vitrual photon axis, for Q = 70.0 to 100.0 GeV and X = 0.19900 .

Normalised distribution of (1-THRUST) where THRUST is w.r.t the vitrual photon axis, for Q = 100.0 to 200.0 GeV and X = 0.32300 .

Normalised distribution of Jet Broadening (B), for Q = 14.0 to 16.0 GeV and X = 0.00841 .

Normalised distribution of Jet Broadening (B), for Q = 16.0 to 20.0 GeV and X = 0.01180 .

Normalised distribution of Jet Broadening (B), for Q = 20.0 to 30.0 GeV and X = 0.02090 .

Normalised distribution of Jet Broadening (B), for Q = 30.0 to 50.0 GeV and X = 0.04910 .

Normalised distribution of Jet Broadening (B), for Q = 50.0 to 70.0 GeV and X = 0.11600 .

Normalised distribution of Jet Broadening (B), for Q = 70.0 to 100.0 GeV and X = 0.19900 .

Normalised distribution of Jet Broadening (B), for Q = 100.0 to 200.0 GeV and X = 0.32300 .

Normalised distribution of the squared Jet Mass (RHO), for Q = 14.0 to 16.0 GeV and X = 0.00841 .

Normalised distribution of the squared Jet Mass (RHO), for Q = 16.0 to 20.0 GeV and X = 0.01180 .

Normalised distribution of the squared Jet Mass (RHO), for Q = 20.0 to 30.0 GeV and X = 0.02090 .

Normalised distribution of the squared Jet Mass (RHO), for Q = 30.0 to 50.0 GeV and X = 0.04910 .

Normalised distribution of the squared Jet Mass (RHO), for Q = 50.0 to 70.0 GeV and X = 0.11600 .

Normalised distribution of the squared Jet Mass (RHO), for Q = 70.0 to 100.0 GeV and X = 0.19900 .

Normalised distribution of the squared Jet Mass (RHO), for Q = 100.0 to 200.0 GeV and X = 0.32300 .

Normalised distribution of the C-Parameter, for Q = 14.0 to 16.0 GeV and X = 0.00841 .

Normalised distribution of the C-Parameter, for Q = 16.0 to 20.0 GeV and X = 0.01180 .

Normalised distribution of the C-Parameter, for Q = 20.0 to 30.0 GeV and X = 0.02090 .

Normalised distribution of the C-Parameter, for Q = 30.0 to 50.0 GeV and X = 0.04910 .

Normalised distribution of the C-Parameter, for Q = 50.0 to 70.0 GeV and X = 0.11600 .

Normalised distribution of the C-Parameter, for Q = 70.0 to 100.0 GeV and X = 0.19900 .

Normalised distribution of the C-Parameter, for Q = 100.0 to 200.0 GeV and X = 0.32300 .

Mean values of the event shape variables.

Covariance matrix for (1-THRUST(C)), for Q = 14.0 to 16.0 GeV and X = 0.00841 .

Covariance matrix for (1-THRUST(C)), for Q = 16.0 to 20.0 GeV and X = 0.01180 .

Covariance matrix for (1-THRUST(C)), for Q = 20.0 to 30.0 GeV and X = 0.02090 .

Covariance matrix for (1-THRUST(C)), for Q = 30.0 to 50.0 GeV and X = 0.04910 .

Covariance matrix for (1-THRUST(C)), for Q = 50.0 to 70.0 GeV and X = 0.11600 .

Covariance matrix for (1-THRUST(C)), for Q = 70.0 to 100.0 GeV and X = 0.19900 .

Covariance matrix for (1-THRUST(C)), for Q = 100.0 to 200.0 GeV and X = 0.32300 .

Covariance matrix for (1-THRUST), for Q = 14.0 to 16.0 GeV and X = 0.00841 .

Covariance matrix for (1-THRUST), for Q = 16.0 to 20.0 GeV and X = 0.01180 .

Covariance matrix for (1-THRUST), for Q = 20.0 to 30.0 GeV and X = 0.02090 .

Covariance matrix for (1-THRUST), for Q = 30.0 to 50.0 GeV and X = 0.04910 .

Covariance matrix for (1-THRUST), for Q = 50.0 to 70.0 GeV and X = 0.11600 .

Covariance matrix for (1-THRUST), for Q = 70.0 to 100.0 GeV and X = 0.19900 .

Covariance matrix for (1-THRUST), for Q = 100.0 to 200.0 GeV and X = 0.32300 .

Covariance matrix for the Jet Broadening (B), for Q = 14.0 to 16.0 GeV and X = 0.00841 .

Covariance matrix for the Jet Broadening (B), for Q = 16.0 to 20.0 GeV and X = 0.01180 .

Covariance matrix for the Jet Broadening (B), for Q = 20.0 to 30.0 GeV and X = 0.02090 .

Covariance matrix for the Jet Broadening (B), for Q = 30.0 to 50.0 GeV and X = 0.04910 .

Covariance matrix for the Jet Broadening (B), for Q = 50.0 to 70.0 GeV and X = 0.11600 .

Covariance matrix for the Jet Broadening (B), for Q = 70.0 to 100.0 GeV and X = 0.19900 .

Covariance matrix for the Jet Broadening (B), for Q = 100.0 to 200.0 GeV and X = 0.32300 .

Covariance matrix for the squared Jet Mass (RHO), for Q = 14.0 to 16.0 GeV and X = 0.00841 .

Covariance matrix for the squared Jet Mass (RHO), for Q = 16.0 to 20.0 GeV and X = 0.01180 .

Covariance matrix for the squared Jet Mass (RHO), for Q = 20.0 to 30.0 GeV and X = 0.02090 .

Covariance matrix for the squared Jet Mass (RHO), for Q = 30.0 to 50.0 GeV and X = 0.04910 .

Covariance matrix for the squared Jet Mass (RHO), for Q = 50.0 to 70.0 GeV and X = 0.11600 .

Covariance matrix for the squared Jet Mass (RHO), for Q = 70.0 to 100.0 GeV and X = 0.19900 .

Covariance matrix for the squared Jet Mass (RHO), for Q = 100.0 to 200.0 GeV and X = 0.32300 .

Covariance matrix for the C-Parameter, for Q = 14.0 to 16.0 GeV and X = 0.00841 .

Covariance matrix for the C-Parameter, for Q = 16.0 to 20.0 GeV and X = 0.01180 .

Covariance matrix for the C-Parameter, for Q = 20.0 to 30.0 GeV and X = 0.02090 .

Covariance matrix for the C-Parameter, for Q = 30.0 to 50.0 GeV and X = 0.04910 .

Covariance matrix for the C-Parameter, for Q = 50.0 to 70.0 GeV and X = 0.11600 .

Covariance matrix for the C-Parameter, for Q = 70.0 to 100.0 GeV and X = 0.19900 .

Covariance matrix for the C-Parameter, for Q = 100.0 to 200.0 GeV and X = 0.32300 .

Correlation matrices obtained with the PYTHIA Monte Carlo in the Q**2 range 11 TO 14 GeV**2.

Correlation matrices obtained with the PYTHIA Monte Carlo in the Q**2 range 14 TO 20 GeV**2.

Correlation matrices obtained with the PYTHIA Monte Carlo in the Q**2 range 20 TO 34 GeV**2.

Correlation matrices obtained with the TWOGAM Monte Carlo in the Q**2 range 11 TO 14 GeV**2.

Correlation matrices obtained with the TWOGAM Monte Carlo in the Q**2 range 14 TO 20 GeV**2.

Correlation matrices obtained with the TWOGAM Monte Carlo in the Q**2 range 20 TO 34 GeV**2.

Measured values of F2/APLHA in the Q**2 range 11 TO 14 GEV**2.

Measured values of F2/APLHA in the Q**2 range 14 TO 20 GEV**2.

Measured values of F2/APLHA in the Q**2 range 20 TO 34 GEV**2.

Measured values of F2/APLHA in the X range 0.01 TO 0.1.

Measured values of F2/APLHA in the X range 0.1 TO 0.2.

Measured values of F2/APLHA in the X range 0.2 TO 0.3.

Measured values of F2/APLHA in the X range 0.3 TO 0.5.

Correlation matrix of negative systematic uncertainties.

The measured value of F2 and DSIG/DX for the SW data sample in the Q**2 range 15 to 30 GeV**2.

The measured value of F2 and DSIG/DX for the FD data sample in the Q**2 range 30 to 50 GeV**2.

The measured value of F2 and DSIG/DX for the FD data sample in the Q**2 range 50 to 150 GeV**2.

The measured value of F2 and DSIG/DX for the EE data sample in the Q**2 range 400 to 2350 GeV**2.

Statistical correlation between the bins for mean Q**2 value 12.1 GeV**2.

Statistical correlation between the bins for mean Q**2 value 19.9 GeV**2.

Statistical correlation between the bins for mean Q**2 value 39.7 GeV**2.

Statistical correlation between the bins for mean Q**2 value 76.4 GeV**2.

Statistical correlation between the bins for mean Q**2 value 780 GeV**2.

F2 and DSIG/DX over the full X range 0.10 to 0.60 as a function of Q**2.

Asymmetry of the Energy Energy Correlation AEEC.

Jet Cone Energy Fraction.

1 - Thrust (1-T).

Oblateness O.

C-Parameter C.

Heavy Jet Mass.

Sum of the Jet Masses.

Difference of the Jet Masses.

Wide Jet Broadening BMAX.

Total Jet Broadening BSUM.

Differential 2-Jet Rate E0 Scheme D2(E0).

Differential 2-Jet Rate P0 Scheme D2(P0).

Differential 2-Jet Rate P Scheme D2(P).

Differential 2-Jet Rate Jade Alogrithm D2(Jad).

Differential 2-Jet Rate Durham Alogrithm D2(Dur).

Differential 2-Jet Rate Geneva Alogrithm D2(Gen).

Differential 2-Jet Rate Cambridge Alogrithm D2(Cam).

Energy Energy Correlation EEC.

Energy Energy Correlation EEC.

Energy Energy Correlation EEC.

Energy Energy Correlation EEC.

Asymmetry of the Energy Energy Correlation AEEC.

Asymmetry of the Energy Energy Correlation AEEC.

Asymmetry of the Energy Energy Correlation AEEC.

Asymmetry of the Energy Energy Correlation AEEC.

Jet Cone Energy Fraction.

Jet Cone Energy Fraction.

Jet Cone Energy Fraction.

Jet Cone Energy Fraction.

1 - Thrust (1-T).