CHI distribution for mass bin > 1200 GeV.

Centrality Ratio.

Differential t-channel top-quark production cross sections and normalized differential t-channel top-quark production cross sections as functions of PT(TOPBAR).

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 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.

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

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 $|y(\bar t)|$.

Distribution of Lambda-Phi in the CS frame for Y(1S) production in the |y| range 0.6-1.2.

Distribution of Lambda-Theta-Phi in the CS frame for Y(1S) production in the |y| range 0.0-0.6.

Distribution of Lambda-Theta-Phi in the CS frame for Y(1S) production in the |y| range 0.6-1.2.

Distribution of Lambda-Tilde in the CS frame for Y(1S) production in the |y| range 0.0-0.6.

Distribution of Lambda-Tilde in the CS frame for Y(1S) production in the |y| range 0.6-1.2.

Distribution of Lambda-Theta in the HX frame for Y(1S) production in the |y| range 0.0-0.6.

Distribution of Lambda-Theta in the HX frame for Y(1S) production in the |y| range 0.6-1.2.

Distribution of Lambda-Phi in the HX frame for Y(1S) production in the |y| range 0.0-0.6.

Distribution of Lambda-Phi in the HX frame for Y(1S) production in the |y| range 0.6-1.2.

Distribution of Lambda-Theta-Phi in the HX frame for Y(1S) production in the |y| range 0.0-0.6.

Distribution of Lambda-Theta-Phi in the HX frame for Y(1S) production in the |y| range 0.6-1.2.

Distribution of Lambda-Tilde in the HX frame for Y(1S) production in the |y| range 0.0-0.6.

Distribution of Lambda-Tilde in the HX frame for Y(1S) production in the |y| range 0.6-1.2.

Distribution of Lambda-Theta in the PX frame for Y(1S) production in the |y| range 0.0-0.6.

Distribution of Lambda-Theta in the PX frame for Y(1S) production in the |y| range 0.6-1.2.

Distribution of Lambda-Phi in the PX frame for Y(1S) production in the |y| range 0.0-0.6.

Distribution of Lambda-Phi in the PX frame for Y(1S) production in the |y| range 0.6-1.2.

Distribution of Lambda-Theta-Phi in the PX frame for Y(1S) production in the |y| range 0.0-0.6.

Distribution of Lambda-Theta-Phi in the PX frame for Y(1S) production in the |y| range 0.6-1.2.

Distribution of Lambda-Tilde in the PX frame for Y(1S) production in the |y| range 0.0-0.6.

Distribution of Lambda-Tilde in the PX frame for Y(1S) production in the |y| range 0.6-1.2.

Distribution of Lambda-Theta in the CS frame for Y(2S) production in the |y| range 0.0-0.6.

Distribution of Lambda-Theta in the CS frame for Y(2S) production in the |y| range 0.6-1.2.

Distribution of Lambda-Phi in the CS frame for Y(2S) production in the |y| range 0.0-0.6.

Distribution of Lambda-Phi in the CS frame for Y(2S) production in the |y| range 0.6-1.2.

Distribution of Lambda-Theta-Phi in the CS frame for Y(2S) production in the |y| range 0.0-0.6.

Distribution of Lambda-Theta-Phi in the CS frame for Y(2S) production in the |y| range 0.6-1.2.

Distribution of Lambda-Tilde in the CS frame for Y(2S) production in the |y| range 0.0-0.6.

Distribution of Lambda-Tilde in the CS frame for Y(2S) production in the |y| range 0.6-1.2.

Distribution of Lambda-Theta in the HX frame for Y(2S) production in the |y| range 0.0-0.6.

Distribution of Lambda-Theta in the HX frame for Y(2S) production in the |y| range 0.6-1.2.

Distribution of Lambda-Phi in the HX frame for Y(2S) production in the |y| range 0.0-0.6.

Distribution of Lambda-Phi in the HX frame for Y(2S) production in the |y| range 0.6-1.2.

Distribution of Lambda-Theta-Phi in the HX frame for Y(2S) production in the |y| range 0.0-0.6.

Distribution of Lambda-Theta-Phi in the HX frame for Y(2S) production in the |y| range 0.6-1.2.

Distribution of Lambda-Tilde in the HX frame for Y(2S) production in the |y| range 0.0-0.6.

Distribution of Lambda-Tilde in the HX frame for Y(2S) production in the |y| range 0.6-1.2.

Distribution of Lambda-Theta in the PX frame for Y(2S) production in the |y| range 0.0-0.6.

Distribution of Lambda-Theta in the PX frame for Y(2S) production in the |y| range 0.6-1.2.

Distribution of Lambda-Phi in the PX frame for Y(2S) production in the |y| range 0.0-0.6.

Distribution of Lambda-Phi in the PX frame for Y(2S) production in the |y| range 0.6-1.2.

Distribution of Lambda-Theta-Phi in the PX frame for Y(2S) production in the |y| range 0.0-0.6.

Distribution of Lambda-Theta-Phi in the PX frame for Y(2S) production in the |y| range 0.6-1.2.

Distribution of Lambda-Tilde in the PX frame for Y(2S) production in the |y| range 0.0-0.6.

Distribution of Lambda-Tilde in the PX frame for Y(2S) production in the |y| range 0.6-1.2.

Distribution of Lambda-Theta in the CS frame for Y(3S) production in the |y| range 0.0-0.6.

Distribution of Lambda-Theta in the CS frame for Y(3S) production in the |y| range 0.6-1.2.

Distribution of Lambda-Phi in the CS frame for Y(3S) production in the |y| range 0.0-0.6.

Distribution of Lambda-Phi in the CS frame for Y(3S) production in the |y| range 0.6-1.2.

Distribution of Lambda-Theta-Phi in the CS frame for Y(3S) production in the |y| range 0.0-0.6.

Distribution of Lambda-Theta-Phi in the CS frame for Y(3S) production in the |y| range 0.6-1.2.

Distribution of Lambda-Tilde in the CS frame for Y(3S) production in the |y| range 0.0-0.6.

Distribution of Lambda-Tilde in the CS frame for Y(3S) production in the |y| range 0.6-1.2.

Distribution of Lambda-Theta in the HX frame for Y(3S) production in the |y| range 0.0-0.6.

Distribution of Lambda-Theta in the HX frame for Y(3S) production in the |y| range 0.6-1.2.

Distribution of Lambda-Phi in the HX frame for Y(3S) production in the |y| range 0.0-0.6.

Distribution of Lambda-Phi in the HX frame for Y(3S) production in the |y| range 0.6-1.2.

Distribution of Lambda-Theta-Phi in the HX frame for Y(3S) production in the |y| range 0.0-0.6.

Distribution of Lambda-Theta-Phi in the HX frame for Y(3S) production in the |y| range 0.6-1.2.

Distribution of Lambda-Tilde in the HX frame for Y(3S) production in the |y| range 0.0-0.6.

Distribution of Lambda-Tilde in the HX frame for Y(3S) production in the |y| range 0.6-1.2.

Distribution of Lambda-Theta in the PX frame for Y(3S) production in the |y| range 0.0-0.6.

Distribution of Lambda-Theta in the PX frame for Y(3S) production in the |y| range 0.6-1.2.

Distribution of Lambda-Phi in the PX frame for Y(3S) production in the |y| range 0.0-0.6.

Distribution of Lambda-Phi in the PX frame for Y(3S) production in the |y| range 0.6-1.2.

Distribution of Lambda-Theta-Phi in the PX frame for Y(3S) production in the |y| range 0.0-0.6.

Distribution of Lambda-Theta-Phi in the PX frame for Y(3S) production in the |y| range 0.6-1.2.

Distribution of Lambda-Tilde in the PX frame for Y(3S) production in the |y| range 0.0-0.6.

Distribution of Lambda-Tilde in the PX frame for Y(3S) production in the |y| range 0.6-1.2.

Estimated number of signal events for Y(1S) production.

Estimated number of signal events for Y(2S) production.

Estimated number of signal events for Y(3S) production.

Mean $p_T$, leading in-jet charged particle.

Mean $p_T$, charged particle jets, $p^{ch.jet}_T > 5$ GeV, $|\eta^{ch.jet}| < 1.9$.

Charged jet rate, $p^\text{ch.jet}_T > 5$ GeV, $|\eta^{ch.jet}| < 1.9$.

Charged jet rate, $p^\text{ch.jet}_T > 30$ GeV, $|\eta^{ch.jet}| < 1.9$.

Jet $p_T$ spectrum, $|\eta^{ch.jet}| < 1.9$, $10 < N_\text{ch} \le 30$.

Jet $p_T$ spectrum, $|\eta^{ch.jet}| < 1.9$, $30 < N_\text{ch} \le 50$.

Jet $p_T$ spectrum, $|\eta^{ch.jet}| < 1.9$, $50 < N_\text{ch} \le 80$.

Jet $p_T$ spectrum, $|\eta^{ch.jet}| < 1.9$, $80 < N_\text{ch} \le 110$.

Jet $p_T$ spectrum, $|\eta^{ch.jet}| < 1.9$, $110 < N_\text{ch} \le 140$.

Intrajet ring $p_{T}$ density, $10 < N_\text{ch} \le 30$.

Intrajet ring $p_{T}$ density, $30 < N_\text{ch} \le 50$.

Intrajet ring $p_{T}$ density, $50 < N_\text{ch} \le 80$.

Intrajet ring $p_{T}$ density, $80 < N_\text{ch} \le 110$.

Intrajet ring $p_{T}$ density, $110 < N_\text{ch} \le 140$.

Detector response matrix (PROB) for the acoplanarity variable (ACO) for mu+ mu- channel (empty bins are not reported).

Acoplanarity (ACO) distributions unfolded for detector resolution, and lepton pair trigger, reconstruction and identification efficiencies for e+ e- channel (empty bins are not reported).

Acoplanarity (ACO) distributions unfolded for detector resolution, and lepton pair trigger, reconstruction and identification efficiencies for mu+ mu- channel (empty bins are not reported).

The lepton pair exclusive selection efficiency in the fiducial region for signal MC events as a function of M and Y for e+ e- channel.

The lepton pair exclusive selection efficiency in the fiducial region for signal MC events as a function of M and Y for mu+ mu- channel.

The lepton pair exclusive selection efficiency in the fiducial region for single-dissociative MC events as a function of M and Y for e+ e- channel.

The lepton pair exclusive selection efficiency in the fiducial region for single-dissociative MC events as a function of M and Y for mu+ mu- channel.

Observed and predicted dimuon invariant mass (m_mumu) distribution in the search region. The bin width is constant in log(m_mumu).

Expected and observed 95% CL limits on the cross-section times branching ratio (sigma*B) for Zprime_SSM production and the two E6-motivated Zprime models with lowest and highest sigma*B for the combination of the dielectron and dimuon channels.

Expected sigma*B for Zprime_SSM production and the two E6-motivated Zprime models with lowest and highest sigma*B.

Expected and observed 95% CL limits on sigma*B for Z* boson production for the combination of the dielectron and dimuon channels.

Expected sigma*B for Z* boson production.

Expected and observed 95% CL limits on M_{G*} versus k/Mbar_{Pl} for the combination of dielectron and dimuon channels.

Expected and observed 95% CL limits on M_{TS} versus eta_{TS} for the combination of dielectron and dimuon channels.

Expected and observed 95% CL limits on M_{pi_T} versus M_{rho_T,omega_T} for the combination of dielectron and dimuon channels.

Expected and observed 95% CL limits on M_A versus the coupling strength g-tilde for the combination of dielectron and dimuon channels.

Expected and observed 95% CL limits on g as a function of M_KK, for the combination of dielectron and dimuon channels.

Expected and observed upper limits on gammaprime within the Minimal Zprime Models parameterization, for the combination of dielectron and dimuon channels. The lower boundary corresponds to tan(theta) = 1.43 and the upper boundary to tan(theta) = -1.19. Two representative values of theta are tan(theta) = 0 and tan(theta) = -2 which correspond to the Z_{B-L} and Z_{3R} model at specific values of gammaprime respectively.

Transverse momentum distribution of the sub-leading lepton in the signal region SR1a showing both data points with statistical errors only and the expected standard model background.

Transverse momentum distribution of the 3rd-leading lepton in the signal region SR1a showing both data points with statistical errors only and the expected standard model background.

Missing transverse energy distribution in the signal region SR1a showing both data points with statistical errors only and the expected standard model background.

Mass distribution of Same Flavour Opposite Sign lepton pairs in the signal region SR1a showing both data points with statistical errors only and the expected standard model background.

Jet multiplicity distribution in the signal region SR1a showing both data points with statistical errors only and the expected standard model background.

Transverse mass distribution in the signal region SR1a showing both data points with statistical errors only and the expected standard model background.

Transverse momentum distribution of the leading lepton in the signal region SR2 showing both data points with statistical errors only and the expected standard model background.

Transverse momentum distribution of the sub-leading lepton in the signal region SR2 showing both data points with statistical errors only and the expected standard model background.

Transverse momentum distribution of the 3rd-leading lepton in the signal region SR2 showing both data points with statistical errors only and the expected standard model background.

Missing transverse energy distribution in the signal region SR2 showing both data points with statistical errors only and the expected standard model background.

Jet multiplicity distribution in the signal region SR2 showing both data points with statistical errors only and the expected standard model background.

Transverse mass distribution in the signal region SR2 showing both data points with statistical errors only and the expected standard model background.

Transverse momentum distribution of the leading lepton in the validation region VR1 showing both data points with statistical errors only and the expected standard model background.

Transverse momentum distribution of the sub-leading lepton in the validation region VR1 showing both data points with statistical errors only and the expected standard model background.

Transverse momentum distribution of the 3rd-leading lepton in the validation region VR1 showing both data points with statistical errors only and the expected standard model background.

Transverse momentum distribution of the leading lepton in the validation region VR2 showing both data points with statistical errors only and the expected standard model background.

Transverse momentum distribution of the sub-leading lepton in the validation region VR2 showing both data points with statistical errors only and the expected standard model background.

Transverse momentum distribution of the 3rd-leading lepton in the validation region VR2 showing both data points with statistical errors only and the expected standard model background.

Transverse momentum distribution of the leading lepton in the validation region VR3 showing both data points with statistical errors only and the expected standard model background.

Transverse momentum distribution of the sub-leading lepton in the validation region VR3 showing both data points with statistical errors only and the expected standard model background.

Transverse momentum distribution of the 3rd-leading lepton in the validation region VR3 showing both data points with statistical errors only and the expected standard model background.

The efficiencies in the different signal regions across the MSSM Direct Gaugino grid of the Higgs mass parameter MU and gaugino massess M1 and M2.

The acceptance in the different signal regions across the MSSM Direct Gaugino grid of the Higgs mass parameter MU and gaugino massess M1 and M2.

The total absolute systematic uncertainty (in number of events) in the different signal regions, not including uncertainties from Monte Carlo statistics, across the MSSM Direct Gaugino grid of the Higgs mass parameter MU and gaugino massess M1 and M2.

The observed CL_s values in the different signal regions across the MSSM Direct Gaugino grid of the Higgs mass parameter MU and gaugino massess M1 and M2.

The cross-section across the MSSM Direct Gaugino grid of the Higgs mass parameter MU and gaugino massess M1 and M2.

The number of generated events across the MSSM Direct Gaugino grid of the Higgs mass parameter MU and gaugino massess M1 and M2.

The efficiencies in the different signal regions across the simplified models with and without intermediate sleptons.

The acceptance in the different signal regions across the simplified models with and without intermediate sleptons.

The total absolute systematic uncertainty (in number of events) in the different signal regions, not including uncertainties from Monte Carlo statistics, across the simplified models with and without intermediate sleptons.

The observed CL_s values in the different signal regions across the simplified models with and without intermediate sleptons.

The cross-section across the simplified models with and without intermediate sleptons.

The number of generated events across the simplified models with and without intermediate sleptons.

The transverse momentum distribution of the 4th-leading lepton for events with at least 4 leptons and no Z-boson candidate.

Distribution of missing transverse momentum for events with at least 4 leptons and no Z-boson candidate.

Distribution of effective mass for events with at least 4 leptons and no Z-boson candidate.

Simplified Model (1) Number of generated events (2) Cross-section [pb] (3) CL_{S} [%] for SR1 (4) Acceptance [%] for SR1 (5) Efficiency [%] for SR1 (6) Uncertainty (not including MC statistics) for SR1 (7) CL_{S} [%] for SR2 (8) Acceptance [%] for SR2 (9) Efficiency [%] for SR2 (10) Uncertainty (not including MC statistics) for SR2.

MSUGRA/CMSSM Model (1) Number of generated events (2) Cross-section [pb] (3) CL_{S} [%] for SR1 (4) Acceptance [%] for SR1 (5) Efficiency [%] for SR1 (6) Uncertainty (not including MC statistics) for SR1 (7) CL_{S} [%] for SR2 (8) Acceptance [%] for SR2 (9) Efficiency [%] for SR2 (10) Uncertainty (not including MC statistics) for SR2.