Normalized differential cross section, $(1/\sigma_\text{fid})d\sigma_\text{fid}/d\log(m_{bb}/p_\text{T})$, as a function of $\log(m_{bb}/p_\text{T})$ for $m_{bb}$ the invariant mass of the two b-jets.

Observed 95% CL exclusion contours in the $(m_{N_R}, m_{W_R})$ plane in the muon channel.

Measured fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $p_\text{T}^{\text{lead }\ell}$.

Statistical correlation between bins in data for the measured fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $p_\text{T}^{\text{lead }\ell}$.

Total correlation between bins in data for the measured fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $p_\text{T}^{\text{lead }\ell}$.

Measured fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $m_{e\mu}$.

Statistical correlation between bins in data for the measured fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $m_{e\mu}$.

Total correlation between bins in data for the measured fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $m_{e\mu}$.

Measured fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $p_{T}^{e\mu}$.

Statistical correlation between bins in data for the measured fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $p_{T}^{e\mu}$.

Total correlation between bins in data for the measured fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $p_{T}^{e\mu}$.

Measured fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $|y_{e\mu}|$.

Statistical correlation between bins in data for the measured fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $|y_{e\mu}|$.

Total correlation between bins in data for the measured fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $|y_{e\mu}|$.

Measured fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $\Delta\phi_{e\mu}$.

Statistical correlation between bins in data for the measured fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $\Delta\phi_{e\mu}$.

Total correlation between bins in data for the measured fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $\Delta\phi_{e\mu}$.

Measured fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $|cos(\theta^*)|$.

Statistical correlation between bins in data for the measured fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $|cos(\theta^*)|$.

Total correlation between bins in data for the measured fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $|cos(\theta^*)|$.

Measured normalized fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $p_\text{T}^{\text{lead }\ell}$.

Statistical correlation between bins in data for the measured normalized fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $p_\text{T}^{\text{lead }\ell}$.

Total correlation between bins in data for the measured normalized fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $p_\text{T}^{\text{lead }\ell}$.

Measured normalized fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $m_{e\mu}$.

Statistical correlation between bins in data for the measured normalized fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $m_{e\mu}$.

Total correlation between bins in data for the measured normalized fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $m_{e\mu}$.

Measured normalized fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $p_{T}^{e\mu}$.

Statistical correlation between bins in data for the measured normalized fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $p_{T}^{e\mu}$.

Total correlation between bins in data for the measured normalized fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $p_{T}^{e\mu}$.

Measured normalized fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $|y_{e\mu}|$.

Statistical correlation between bins in data for the measured normalized fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $|y_{e\mu}|$.

Total correlation between bins in data for the measured normalized fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $|y_{e\mu}|$.

Measured normalized fiducial cross section of $WW\rightarrow e\mu$ production for the observable $\Delta\phi_{e\mu}$.

Statistical correlation between bins in data for the measured normalized fiducial cross section of $WW\rightarrow e\mu$ production for the observable $\Delta\phi_{e\mu}$.

Total correlation between bins in data for the measured normalized fiducial cross section of $WW\rightarrow e\mu$ production for the observable $\Delta\phi_{e\mu}$.

Measured normalized fiducial cross section of $WW\rightarrow e\mu$ production for the observable $|cos(\theta^*)|$.

Statistical correlation between bins in data for the measured normalized fiducial cross section of $WW\rightarrow e\mu$ production for the observable $|cos(\theta^*)|$.

Total correlation between bins in data for the measured normalized fiducial cross section of $WW\rightarrow e\mu$ production for the observable $|cos(\theta^*)|$.

List of experimentally considered systematic uncertainties for the WW cross section measurement.

Extrapolated unfolded fiducial cross-section of $WW\rightarrow e\mu$ production as a function of $p_\text{T}^{\text{lead }\ell}$.

Extrapolated unfolded fiducial cross-section of $WW\rightarrow e\mu$ production as a function of $m_{e\mu}$.

Extrapolated unfolded fiducial cross-section of $WW\rightarrow e\mu$ production as a function of $p_{T}^{e\mu}$.

Lower mass requirement for signal regions.

Lower mass requirement for signal regions.

Lower mass requirement for signal regions.

Expected and observed events in the 16 discovery regions along with the according control regions.

Expected and observed events in the 16 discovery regions along with the according control regions.

Expected signal yield and acceptance x efficiency, estimated background and observed number of events in data for the full range of simulated masses in the MS-agnostic R-hadron search.

Expected signal yield and acceptance x efficiency, estimated background and observed number of events in data for the full range of simulated masses in the MS-agnostic R-hadron search.

Expected signal yield and acceptance x efficiency, estimated background and observed number of events in data for the full range of simulated masses in the full-detector R-hadron search.

Expected signal yield and acceptance x efficiency, estimated background and observed number of events in data for the full range of simulated masses in the full-detector R-hadron search.

p0-values and model-independent upper limits on cross-section x acceptance x efficiency for the 16 discovery regions.

p0-values and model-independent upper limits on cross-section x acceptance x efficiency for the 16 discovery regions.

Expected signal yield and acceptance x efficiency, estimated background and observed number of events in data for the full range of simulated masses in the MS-agnostic search for metastable gluino R-hadrons.

Expected signal yield and acceptance x efficiency, estimated background and observed number of events in data for the full range of simulated masses in the MS-agnostic search for metastable gluino R-hadrons.

Expected signal yield and acceptance x efficiency, estimated background and observed number of events in data for the full range of simulated masses in the full-detector direct-stau search.

Expected signal yield and acceptance x efficiency, estimated background and observed number of events in data for the full range of simulated masses in the full-detector direct-stau search.

Expected signal yield and acceptance x efficiency, estimated background and observed number of events in data for the full range of simulated masses in the full-detector chargino search.

Expected signal yield and acceptance x efficiency, estimated background and observed number of events in data for the full range of simulated masses in the full-detector chargino search.

Upper cross-section limit in gluino R-hadron search.

Upper cross-section limit in gluino R-hadron search.

Upper cross-section limit in sbottom R-hadron search.

Upper cross-section limit in sbottom R-hadron search.

Upper cross-section limit in stop R-hadron search.

Upper cross-section limit in stop R-hadron search.

Upper cross-section limit in stau search.

Upper cross-section limit in stau search.

Upper cross-section limit in chargino search.

Upper cross-section limit in chargino search.

Lower mass limit as function of gluino lifetime.

Lower mass limit as function of gluino lifetime.

Acceptance x efficiency, acceptance and efficiency for the full range of simulated masses in the MS-agnostic R-hadron search.

Acceptance x efficiency, acceptance and efficiency for the full range of simulated masses in the MS-agnostic R-hadron search.

Upper cross-section limit in meta-stable gluino R-hadron search.

Upper cross-section limit in meta-stable gluino R-hadron search.

Flavor composition of 800 GeV stop R-hadrons simulated using the generic model as a function of radial distance from the interaction point.

Flavor composition of 800 GeV stop R-hadrons simulated using the generic model as a function of radial distance from the interaction point.

Flavor composition of 800 GeV anti-stop R-hadrons simulated using the generic model as a function of radial distance from the interaction point.

Flavor composition of 800 GeV anti-stop R-hadrons simulated using the generic model as a function of radial distance from the interaction point.

Flavor composition of 800 GeV stop R-hadrons simulated using the Regge model as a function of radial distance from the interaction point.

Flavor composition of 800 GeV stop R-hadrons simulated using the Regge model as a function of radial distance from the interaction point.

Flavor composition of 800 GeV anti-stop R-hadrons simulated using the Regge model as a function of radial distance from the interaction point.

Flavor composition of 800 GeV anti-stop R-hadrons simulated using the Regge model as a function of radial distance from the interaction point.

ETmiss trigger efficiency as function of true ETmiss (EtmissTurnOn).

ETmiss trigger efficiency as function of true ETmiss (EtmissTurnOn).

Single-muon trigger efficiency as function of $|\eta|$ and $\beta$ (SingleMuTurnOn).

Single-muon trigger efficiency as function of $|\eta|$ and $\beta$ (SingleMuTurnOn).

Candidate reconstruction efficiency for ID+Calo selection (IDCaloEff).

Candidate reconstruction efficiency for ID+Calo selection (IDCaloEff).

Candidate reconstruction efficiency for loose selection (LooseEff).

Candidate reconstruction efficiency for loose selection (LooseEff).

Efficiency for a loose candidate to be promoted to a tight candidate (TightPromotionEff).

Efficiency for a loose candidate to be promoted to a tight candidate (TightPromotionEff).

Resolution and average of reconstructed dE/dx mass for a given simulated mass for ID+calo candidates.

Resolution and average of reconstructed dE/dx mass for a given simulated mass for ID+calo candidates.

Resolution and average of reconstructed ToF mass for a given simulated mass for ID+calo candidates.

Resolution and average of reconstructed ToF mass for a given simulated mass for ID+calo candidates.

Resolution and average of reconstructed ToF mass for a given simulated mass for FullDet candidates.

Resolution and average of reconstructed ToF mass for a given simulated mass for FullDet candidates.

Figure 6a, Normalised differential D2 distribution for soft-drop groomed jets, Dijet selection

Figure 7a, Normalised differential ECF2 distribution for soft-drop groomed jets, Dijet selection

Figure 8a, Normalised differential ECF3 distribution for soft-drop groomed jets, Dijet selection

Figure 3b, Normalised differential Nsubjets distribution for soft-drop groomed jets, Top selection

Figure 4b, Normalised differential LHA distribution for soft-drop groomed jets, Top selection

Figure 5b, Normalised differential C2 distribution for soft-drop groomed jets, Top selection

Figure 6b, Normalised differential D2 distribution for soft-drop groomed jets, Top selection

Figure 7b, Normalised differential ECF2 distribution for soft-drop groomed jets, Top selection

Figure 8b, Normalised differential ECF3 distribution for soft-drop groomed jets, Top selection

Figure 9a, Normalised differential Tau21 distribution for soft-drop groomed jets, Top selection

Figure 9b, Normalised differential Tau32 distribution for soft-drop groomed jets, Top selection

Figure 3c, Normalised differential Nsubjets distribution for soft-drop groomed jets, W selection

Figure 4c, Normalised differential LHA distribution for soft-drop groomed jets, W selection

Figure 5c, Normalised differential C2 distribution for soft-drop groomed jets, W selection

Figure 6c, Normalised differential D2 distribution for soft-drop groomed jets, W selection

Figure 7c, Normalised differential ECF2 distribution for soft-drop groomed jets, W selection

Figure 8c, Normalised differential ECF3 distribution for soft-drop groomed jets, W selection

Figure 9c, Normalised differential Tau21 distribution for soft-drop groomed jets, W selection

Figure 9d, Normalised differential Tau32 distribution for soft-drop groomed jets, W selection

Normalised differential Nsubjets distribution for trimmed jets, Dijet selection

Normalised differential LHA distribution for trimmed jets, Dijet selection

Normalised differential C2 distribution for trimmed jets, Dijet selection

Normalised differential D2 distribution for trimmed jets, Dijet selection

Normalised differential ECF2 distribution for trimmed jets, Dijet selection

Normalised differential ECF3 distribution for trimmed jets, Dijet selection

Normalised differential Nsubjets distribution for trimmed jets, Top selection

Normalised differential LHA distribution for trimmed jets, Top selection

Normalised differential C2 distribution for trimmed jets, Top selection

Normalised differential D2 distribution for trimmed jets, Top selection

Normalised differential ECF2 distribution for trimmed jets, Top selection

Normalised differential ECF3 distribution for trimmed jets, Top selection

Normalised differential Tau21 distribution for trimmed jets, Top selection

Normalised differential Tau32 distribution for trimmed jets, Top selection

Normalised differential Nsubjets distribution for trimmed jets, W selection

Normalised differential LHA distribution for trimmed jets, W selection

Normalised differential C2 distribution for trimmed jets, W selection

Normalised differential D2 distribution for trimmed jets, W selection

Normalised differential ECF2 distribution for trimmed jets, W selection

Normalised differential ECF3 distribution for trimmed jets, W selection

Normalised differential Tau21 distribution for trimmed jets, W selection

Normalised differential Tau32 distribution for trimmed jets, W selection

Statistical correlation between bins in data for the normalised differential Nsubjets distribution for soft-drop groomed jets, Dijet selection

Statistical correlation between bins in data for the normalised differential LHA distribution for soft-drop groomed jets, Dijet selection

Statistical correlation between bins in data for the normalised differential C2 distribution for soft-drop groomed jets, Dijet selection

Statistical correlation between bins in data for the normalised differential D2 distribution for soft-drop groomed jets, Dijet selection

Statistical correlation between bins in data for the normalised differential ECF2 distribution for soft-drop groomed jets, Dijet selection

Statistical correlation between bins in data for the normalised differential ECF3 distribution for soft-drop groomed jets, Dijet selection

Statistical correlation between bins in data for the normalised differential Nsubjets distribution for soft-drop groomed jets, Top selection

Statistical correlation between bins in data for the normalised differential LHA distribution for soft-drop groomed jets, Top selection

Statistical correlation between bins in data for the normalised differential C2 distribution for soft-drop groomed jets, Top selection

Statistical correlation between bins in data for the normalised differential D2 distribution for soft-drop groomed jets, Top selection

Statistical correlation between bins in data for the normalised differential ECF2 distribution for soft-drop groomed jets, Top selection

Statistical correlation between bins in data for the normalised differential ECF3 distribution for soft-drop groomed jets, Top selection

Statistical correlation between bins in data for the normalised differential Tau21 distribution for soft-drop groomed jets, Top selection

Statistical correlation between bins in data for the normalised differential Tau32 distribution for soft-drop groomed jets, Top selection

Statistical correlation between bins in data for the normalised differential Nsubjets distribution for soft-drop groomed jets, W selection

Statistical correlation between bins in data for the normalised differential LHA distribution for soft-drop groomed jets, W selection

Statistical correlation between bins in data for the normalised differential C2 distribution for soft-drop groomed jets, W selection

Statistical correlation between bins in data for the normalised differential D2 distribution for soft-drop groomed jets, W selection

Statistical correlation between bins in data for the normalised differential ECF2 distribution for soft-drop groomed jets, W selection

Statistical correlation between bins in data for the normalised differential ECF3 distribution for soft-drop groomed jets, W selection

Statistical correlation between bins in data for the normalised differential Tau21 distribution for soft-drop groomed jets, W selection

Statistical correlation between bins in data for the normalised differential Tau32 distribution for soft-drop groomed jets, W selection

Statistical correlation between bins in data for the normalised differential Nsubjets distribution for trimmed jets, Dijet selection

Statistical correlation between bins in data for the normalised differential LHA distribution for trimmed jets, Dijet selection

Statistical correlation between bins in data for the normalised differential C2 distribution for trimmed jets, Dijet selection

Statistical correlation between bins in data for the normalised differential D2 distribution for trimmed jets, Dijet selection

Statistical correlation between bins in data for the normalised differential ECF2 distribution for trimmed jets, Dijet selection

Statistical correlation between bins in data for the normalised differential ECF3 distribution for trimmed jets, Dijet selection

Statistical correlation between bins in data for the normalised differential Nsubjets distribution for trimmed jets, Top selection

Statistical correlation between bins in data for the normalised differential LHA distribution for trimmed jets, Top selection

Statistical correlation between bins in data for the normalised differential C2 distribution for trimmed jets, Top selection

Statistical correlation between bins in data for the normalised differential D2 distribution for trimmed jets, Top selection

Statistical correlation between bins in data for the normalised differential ECF2 distribution for trimmed jets, Top selection

Statistical correlation between bins in data for the normalised differential ECF3 distribution for trimmed jets, Top selection

Statistical correlation between bins in data for the normalised differential Tau21 distribution for trimmed jets, Top selection

Statistical correlation between bins in data for the normalised differential Tau32 distribution for trimmed jets, Top selection

Statistical correlation between bins in data for the normalised differential Nsubjets distribution for trimmed jets, W selection

Statistical correlation between bins in data for the normalised differential LHA distribution for trimmed jets, W selection

Statistical correlation between bins in data for the normalised differential C2 distribution for trimmed jets, W selection

Statistical correlation between bins in data for the normalised differential D2 distribution for trimmed jets, W selection

Statistical correlation between bins in data for the normalised differential ECF2 distribution for trimmed jets, W selection

Statistical correlation between bins in data for the normalised differential ECF3 distribution for trimmed jets, W selection

Statistical correlation between bins in data for the normalised differential Tau21 distribution for trimmed jets, W selection

Statistical correlation between bins in data for the normalised differential Tau32 distribution for trimmed jets, W selection

The measured normalized differential cross section as a function of the photon $|\eta|$ in the single lepton channel. The uncertainty is decomposed into five components which are the signal modelling uncertainty, the experimental uncertainty, the ttbar modelling uncertainty, the other background estimation uncertainty, and the data statistical uncertainty.

The measured normalized differential cross section as a function of the $\Delta R$ between the photon and the lepton in the single lepton channel. The uncertainty is decomposed into five components which are the signal modelling uncertainty, the experimental uncertainty, the ttbar modelling uncertainty, the other background estimation uncertainty, and the data statistical uncertainty.

The measured normalized differential cross section as a function of the photon pT in the dilepton channel. The uncertainty is decomposed into five components which are the signal modelling uncertainty, the experimental uncertainty, the ttbar modelling uncertainty, the other background estimation uncertainty, and the data statistical uncertainty.

The measured normalized differential cross section as a function of the photon $|\eta|$ in the dilepton channel. The uncertainty is decomposed into five components which are the signal modelling uncertainty, the experimental uncertainty, the ttbar modelling uncertainty, the other background estimation uncertainty, and the data statistical uncertainty.

The measured normalized differential cross section as a function of minimum $\Delta R) between the photon and the leptons in the dilepton channel. The uncertainty is decomposed into five components which are the signal modelling uncertainty, the experimental uncertainty, the ttbar modelling uncertainty, the other background estimation uncertainty, and the data statistical uncertainty.

The measured normalized differential cross section as a function of $|\Delta\eta|$ between the two leptons in the dilepton channel. The uncertainty is decomposed into five components which are the signal modelling uncertainty, the experimental uncertainty, the ttbar modelling uncertainty, the other background estimation uncertainty, and the data statistical uncertainty.

The measured normalized differential cross section as a function of $\Delta\phi$ between the two leptons in the dilepton channel. The uncertainty is decomposed into five components which are the signal modelling uncertainty, the experimental uncertainty, the ttbar modelling uncertainty, the other background estimation uncertainty, and the data statistical uncertainty.

The total correlation matrix of the measured normalized differential cross section as a function of the photon pT in the single lepton channel. The individual systematic uncertainties are symmetrized before deriving the correlation matrix.

The total correlation matrix of the measured normalized differential cross section as a function of the photon $|\eta|$ in the single lepton channel. The individual systematic uncertainties are symmetrized before deriving the correlation matrix.

The total correlation matrix of the measured normalized differential cross section as a function of the $\Delta R$ between the photon and the lepton in the single lepton channel. The individual systematic uncertainties are symmetrized before deriving the correlation matrix.

The total correlation matrix of the measured normalized differential cross section as a function of the photon pT in the dilepton channel. The individual systematic uncertainties are symmetrized before deriving the correlation matrix.

The total correlation matrix of the measured normalized differential cross section as a function of the photon $|\eta|$ in the dilepton channel. The individual systematic uncertainties are symmetrized before deriving the correlation matrix.

The total correlation matrix of the measured normalized differential cross section as a function of the minimum $\Delta R$ between the photon and the leptons in the dilepton channel. The individual systematic uncertainties are symmetrized before deriving the correlation matrix.

The total correlation matrix of the measured normalized differential cross section as a function of the $|\Delta\eta|$ between the two leptons in the dilepton channel. The individual systematic uncertainties are symmetrized before deriving the correlation matrix.

The total correlation matrix of the measured normalized differential cross section as a function of the $\Delta\phi$ between the two leptons in the dilepton channel. The individual systematic uncertainties are symmetrized before deriving the correlation matrix.

The statistical correlation matrix of all the measured normalized differential cross sections in the single lepton channel.

The statistical correlation matrix of all the measured normalized differential cross sections in the dilepton channel.

List of relative uncertainties in the measured cross sections of the $t\bar{t}Z$ and $t\bar{t}W$ processes from the fit, grouped in categories. All uncertainties are symmetrized. The sum in quadrature may not be equal to the total due to correlations between uncertainties introduced by the fit.

The expected and observed 68% and 95% confidence intervals, which include the value 0, for $\mathcal{C}_{i}/\Lambda^{2}$ for the EFT coefficients $\mathcal{C}_{\phi Q}^{(3)}$, $\mathcal{C}_{\phi t}$, $\mathcal{C}_{tB}$ and $\mathcal{C}_{tW}$. The intervals for $\mathcal{C}_{\phi Q}^{(3)}$ are derived setting $\mathcal{C}_{\phi Q}^{(1)}$ to zero; the measurement is sensitive to the difference $\mathcal{C}_{\phi Q}^{(3)}-\mathcal{C}_{\phi Q}^{(1)}$. All results are given in units of 1/TeV$^{2}$. Limits from fits for the EFT coefficients with only the linear term are also shown.

Predicted ratio of cross sections for inclusive isolated-photon production as a function of $E_{\rm T}^{\gamma}$ for $0.6<|\eta^{\gamma}|<1.37$.

Measured ratio of cross sections for inclusive isolated-photon production as a function of $E_{\rm T}^{\gamma}$ for $1.56<|\eta^{\gamma}|<1.81$.

Predicted ratio of cross sections for inclusive isolated-photon production as a function of $E_{\rm T}^{\gamma}$ for $1.56<|\eta^{\gamma}|<1.81$.

Measured ratio of cross sections for inclusive isolated-photon production as a function of $E_{\rm T}^{\gamma}$ for $1.81<|\eta^{\gamma}|<2.37$.

Predicted ratio of cross sections for inclusive isolated-photon production as a function of $E_{\rm T}^{\gamma}$ for $1.81<|\eta^{\gamma}|<2.37$.

Measured double ratio of cross sections for inclusive isolated-photon production and Z-boson production as a function of $E_{\rm T}^{\gamma}$ for $|\eta^{\gamma}|<0.6$.

Predicted double ratio of cross sections for inclusive isolated-photon production and Z-boson production as a function of $E_{\rm T}^{\gamma}$ for $|\eta^{\gamma}|<0.6$.

Measured double ratio of cross sections for inclusive isolated-photon production and Z-boson production as a function of $E_{\rm T}^{\gamma}$ for $0.6<|\eta^{\gamma}|<1.37$.

Predicted double ratio of cross sections for inclusive isolated-photon production and Z-boson production as a function of $E_{\rm T}^{\gamma}$ for $0.6<|\eta^{\gamma}|<1.37$.

Measured double ratio of cross sections for inclusive isolated-photon production and Z-boson production as a function of $E_{\rm T}^{\gamma}$ for $1.56<|\eta^{\gamma}|<1.81$.

Predicted double ratio of cross sections for inclusive isolated-photon production and Z-boson production as a function of $E_{\rm T}^{\gamma}$ for $1.56<|\eta^{\gamma}|<1.81$.

Measured double ratio of cross sections for inclusive isolated-photon production and Z-boson production as a function of $E_{\rm T}^{\gamma}$ for $1.81<|\eta^{\gamma}|<2.37$.

Predicted double ratio of cross sections for inclusive isolated-photon production and Z-boson production as a function of $E_{\rm T}^{\gamma}$ for $1.81<|\eta^{\gamma}|<2.37$.

Observed top-quark mass distribution and expected background in Region A after the fit (Post-Fit) under the background-only hypothesis for the resolved analysis.

Observed top-quark mass distribution and expected background in Region B after the fit (Post-Fit) under the background-only hypothesis for the resolved analysis.

Observed top-quark mass distribution and expected background in Region C after the fit (Post-Fit) under the background-only hypothesis for the resolved analysis.

Observed top-quark mass distribution and expected background in Region D after the fit (Post-Fit) under the background-only hypothesis for the resolved analysis.

Observed top-quark mass distribution and expected background in Region SR1 Medium 1b after the fit (Post-Fit) under the background-only hypothesis for the boosted analysis.

Observed top-quark mass distribution and expected background in Region SR1 Medium 2b after the fit (Post-Fit) under the background-only hypothesis for the boosted analysis.

Observed top-quark mass distribution and expected background in Region SR1 Tight 1b after the fit (Post-Fit) under the background-only hypothesis for the boosted analysis.

Observed top-quark mass distribution and expected background in Region SR1 Tight 2b after the fit (Post-Fit) under the background-only hypothesis for the boosted analysis.

Observed top-quark mass distribution and expected background in Region SR2 Medium 1b after the fit (Post-Fit) under the background-only hypothesis for the boosted analysis.

Observed top-quark mass distribution and expected background in Region SR2 Medium 2b after the fit (Post-Fit) under the background-only hypothesis for the boosted analysis.

Observed top-quark mass distribution and expected background in Region SR2 Tight 1b after the fit (Post-Fit) under the background-only hypothesis for the boosted analysis.

Observed top-quark mass distribution and expected background in Region SR2 Tight 2b after the fit (Post-Fit) under the background-only hypothesis for the boosted analysis.

Expected and observed upper limits on the cross-section times branching fraction of topcolor-assisted-technicolor Z$^{\prime}_{TC2}$ decaying into top-quark pair as a function of the Z$^{\prime}_{TC2}$ mass.

Expected and observed upper limits on the cross-section times branching fraction of A1 axial-vector mediator decaying into top-quark pair as a function of the mediator mass.

Expected and observed upper limits on the cross-section times branching fraction of V1 vector mediator decaying into top-quark pair as a function of the mediator mass.

Expected and observed upper limits on the cross-section times branching fraction of Kaluza-Klein graviton decaying into top-quark pair as a function of the graviton mass.

Expected and observed upper limits on the cross-section times branching fraction of Kaluza-Klein gluon decaying into top-quark pair as a function of the gluon mass.

Expected and observed upper limits on cross-section times branching fraction of Kaluza-Klein gluon decaying into top-quark pair as a function of the width of Kaluza-Klein gluon for masses of 0.5 TeV.

Expected and observed upper limits on cross-section times branching fraction of Kaluza-Klein gluon decaying into top-quark pair as a function of the width of Kaluza-Klein gluon for masses of 1 TeV.

Expected and observed upper limits on cross-section times branching fraction of Kaluza-Klein gluon decaying into top-quark pair as a function of the width of Kaluza-Klein gluon for masses of 1.5 TeV.

Expected upper limits on cross-section times branching fraction of Kaluza-Klein gluon decaying into top-quark pair as a function of the width of Kaluza-Klein gluon for masses of 2 TeV.

Expected upper limits on cross-section times branching fraction of Kaluza-Klein gluon decaying into top-quark pair as a function of the width of Kaluza-Klein gluon for masses of 5 TeV.

Dijet mass distribution for the b-tagged category. Data, estimated background and uncertainties are shown. Events are collected using the combined trigger and contain a $E_T^{\gamma} > 95$ GeV photon and two $p_T^{jet} > 65$ GeV jets.

Upper limits on Gaussian-shape contributions to the dijet mass distributions from the flavour-inclusive category and masses below 450 GeV, for which the single-photon trigger was used.

Upper limits on Gaussian-shape contributions to the dijet mass distributions from the flavour-inclusive category and masses above 450 GeV, for which the combined trigger was used.

Upper limits on Gaussian-shape contributions to the dijet mass distributions from the b-tagged category and masses below 450 GeV, for which the single-photon trigger was used.

Upper limits on Gaussian-shape contributions to the dijet mass distributions from the b-tagged category and masses above 450 GeV, for which the combined trigger was used.

Kinematic acceptance values predicted for the $Z'$ model as a function of mass $m_{Z'}$ for the flavour-inclusive category using the single-photon trigger.

Kinematic acceptance values predicted for the $Z'$ model as a function of mass $m_{Z'}$ for the flavour-inclusive category using the combined trigger.

Kinematic acceptance values predicted for the $Z'$ model as a function of mass $m_{Z'}$ for the b-tagged category using the single-photon trigger.

Kinematic acceptance values predicted for the $Z'$ model as a function of mass $m_{Z'}$ for the b-tagged category using the combined trigger.

Reconstruction efficiency for $Z'$ model, flavour inclusive category, single-photon trigger.

Reconstruction efficiency for $Z'$ model, flavour inclusive category, combined trigger.

Reconstruction efficiency for $Z'$ model, b-tagged category, single-photon trigger.

Reconstruction efficiency for $Z'$ model, b-tagged category, combined trigger.

Sequential impact of each requirement on the number of events passing the selection for the high-$E_T$ analysis.

Sequential impact of each requirement on the number of events passing the selection for the low-$E_T$ analysis.

Application of the modified ABCD method to the final high-$E_T$ and low-$E_T$ selections.

The extrapolated signal efficiencies as a function of proper decay length of the $s$ for several simulated samples in the low-$E_T$ selections.

The extrapolated signal efficiencies as a function of proper decay length of the $s$ for several simulated samples in the high-$E_T$ selections.

The observed limits, expected limits and $\pm 1 \sigma$ and $\pm 2 \sigma$ bands for a model with $m_{\phi} = 125 ~\mathrm{GeV}$ and $m_{s} = 25 ~\mathrm{GeV}$.

The observed limits, expected limits and $\pm 1 \sigma$ and $\pm 2 \sigma$ bands for a model with $m_{\phi} = 600 ~\mathrm{GeV}$ and $m_{s} = 150 ~\mathrm{GeV}$.

Combined limits for the CalRatio and MS analyses, for a model with $m_{\phi} = 125 ~\mathrm{GeV}$ and $m_{s} = 25 ~\mathrm{GeV}$.

Combined limits for the CalRatio and MS analyses, for a model with $m_{\phi} = 600 ~\mathrm{GeV}$ and $m_{s} = 150 ~\mathrm{GeV}$.

The observed limits, expected limits and $\pm 1 \sigma$ and $\pm 2 \sigma$ bands for a model with $m_{\phi} = 125 ~\mathrm{GeV}$ and $m_{s} = 5 ~\mathrm{GeV}$.

The observed limits, expected limits and $\pm 1 \sigma$ and $\pm 2 \sigma$ bands for a model with $m_{\phi} = 125 ~\mathrm{GeV}$ and $m_{s} = 8 ~\mathrm{GeV}$.

The observed limits, expected limits and $\pm 1 \sigma$ and $\pm 2 \sigma$ bands for a model with $m_{\phi} = 125 ~\mathrm{GeV}$ and $m_{s} = 15 ~\mathrm{GeV}$.

The observed limits, expected limits and $\pm 1 \sigma$ and $\pm 2 \sigma$ bands for a model with $m_{\phi} = 125 ~\mathrm{GeV}$ and $m_{s} = 40 ~\mathrm{GeV}$.

The observed limits, expected limits and $\pm 1 \sigma$ and $\pm 2 \sigma$ bands for a model with $m_{\phi} = 125 ~\mathrm{GeV}$ and $m_{s} = 55 ~\mathrm{GeV}$.

The observed limits, expected limits and $\pm 1 \sigma$ and $\pm 2 \sigma$ bands for a model with $m_{\phi} = 200 ~\mathrm{GeV}$ and $m_{s} = 8 ~\mathrm{GeV}$.

The observed limits, expected limits and $\pm 1 \sigma$ and $\pm 2 \sigma$ bands for a model with $m_{\phi} = 200 ~\mathrm{GeV}$ and $m_{s} = 25 ~\mathrm{GeV}$.

The observed limits, expected limits and $\pm 1 \sigma$ and $\pm 2 \sigma$ bands for a model with $m_{\phi} = 200 ~\mathrm{GeV}$ and $m_{s} = 50 ~\mathrm{GeV}$.

The observed limits, expected limits and $\pm 1 \sigma$ and $\pm 2 \sigma$ bands for a model with $m_{\phi} = 400 ~\mathrm{GeV}$ and $m_{s} = 50 ~\mathrm{GeV}$.

The observed limits, expected limits and $\pm 1 \sigma$ and $\pm 2 \sigma$ bands for a model with $m_{\phi} = 400 ~\mathrm{GeV}$ and $m_{s} = 100 ~\mathrm{GeV}$.

The observed limits, expected limits and $\pm 1 \sigma$ and $\pm 2 \sigma$ bands for a model with $m_{\phi} = 600 ~\mathrm{GeV}$ and $m_{s} = 50 ~\mathrm{GeV}$.

The observed limits, expected limits and $\pm 1 \sigma$ and $\pm 2 \sigma$ bands for a model with $m_{\phi} = 1000 ~\mathrm{GeV}$ and $m_{s} = 50 ~\mathrm{GeV}$.

The observed limits, expected limits and $\pm 1 \sigma$ and $\pm 2 \sigma$ bands for a model with $m_{\phi} = 1000 ~\mathrm{GeV}$ and $m_{s} = 150 ~\mathrm{GeV}$.

The observed limits, expected limits and $\pm 1 \sigma$ and $\pm 2 \sigma$ bands for a model with $m_{\phi} = 1000 ~\mathrm{GeV}$ and $m_{s} = 400 ~\mathrm{GeV}$.

Combined limits for the CalRatio and MS analyses, for a model with $m_{\phi} = 125 ~\mathrm{GeV}$ and $m_{s} = 5 ~\mathrm{GeV}$.

Combined limits for the CalRatio and MS analyses, for a model with $m_{\phi} = 125 ~\mathrm{GeV}$ and $m_{s} = 8 ~\mathrm{GeV}$.

Combined limits for the CalRatio and MS analyses, for a model with $m_{\phi} = 125 ~\mathrm{GeV}$ and $m_{s} = 15 ~\mathrm{GeV}$.

Combined limits for the CalRatio and MS analyses, for a model with $m_{\phi} = 125 ~\mathrm{GeV}$ and $m_{s} = 40 ~\mathrm{GeV}$.

Combined limits for the CalRatio and MS analyses, for a model with $m_{\phi} = 200 ~\mathrm{GeV}$ and $m_{s} = 8 ~\mathrm{GeV}$.

Combined limits for the CalRatio and MS analyses, for a model with $m_{\phi} = 200 ~\mathrm{GeV}$ and $m_{s} = 25 ~\mathrm{GeV}$.

Combined limits for the CalRatio and MS analyses, for a model with $m_{\phi} = 200 ~\mathrm{GeV}$ and $m_{s} = 50 ~\mathrm{GeV}$.

Combined limits for the CalRatio and MS analyses, for a model with $m_{\phi} = 400 ~\mathrm{GeV}$ and $m_{s} = 50 ~\mathrm{GeV}$.

Combined limits for the CalRatio and MS analyses, for a model with $m_{\phi} = 400 ~\mathrm{GeV}$ and $m_{s} = 100 ~\mathrm{GeV}$.

Combined limits for the CalRatio and MS analyses, for a model with $m_{\phi} = 600 ~\mathrm{GeV}$ and $m_{s} = 50 ~\mathrm{GeV}$.

Combined limits for the CalRatio and MS analyses, for a model with $m_{\phi} = 1000 ~\mathrm{GeV}$ and $m_{s} = 50 ~\mathrm{GeV}$.

Combined limits for the CalRatio and MS analyses, for a model with $m_{\phi} = 1000 ~\mathrm{GeV}$ and $m_{s} = 150 ~\mathrm{GeV}$.

Combined limits for the CalRatio and MS analyses, for a model with $m_{\phi} = 1000 ~\mathrm{GeV}$ and $m_{s} = 400 ~\mathrm{GeV}$.

Upper limits on $\sigma\times B$ as a function of $m_{e^*}$ in the $e\nu J$ channel. The $\pm 1(2)\sigma$ uncertainty bands around the expected limit represent all sources of systematic and statistical uncertainties.

Lower limits on $\Lambda$ as a function of $m_{e^*}$ for the $eejj$ channel. The $\pm\ 1(2)\sigma$ uncertainty bands around the expected limit represent all sources of systematic and statistical uncertainties. The limits for $m_{e^*}\gt4$ TeV are the result of extrapolation.

Lower limits on $\Lambda$ as a function of $m_{e^*}$ for the $e\nu J$ channel. The $\pm\ 1(2)\sigma$ uncertainty bands around the expected limit represent all sources of systematic and statistical uncertainties.

Lower limits on $\Lambda$ as a function of $m_{e^*}$ combined for the $eejj$ and the $e\nu J$ channels. The $\pm\ 1(2)\sigma$ uncertainty bands around the expected limit represent all sources of systematic and statistical uncertainties. The limits for $m_{e^*}\gt4$ TeV are the result of extrapolation.

Observed 95% confidence-level upper limits on the cross section for Drell-Yan spin-1/2 HECO production as a function of mass for various values of electric charge in the range $20\le|z|\le100$.

Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for $g=1g_\textrm{D}$ monopoles of mass 200 GeV.

Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for $g=1g_\textrm{D}$ monopoles of mass 500 GeV.

Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for $g=1g_\textrm{D}$ monopoles of mass 1000 GeV.

Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for $g=1g_\textrm{D}$ monopoles of mass 1500 GeV.

Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for $g=1g_\textrm{D}$ monopoles of mass 2000 GeV.

Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for $g=1g_\textrm{D}$ monopoles of mass 2500 GeV.

Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for $g=1g_\textrm{D}$ monopoles of mass 3000 GeV.

Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for $g=1g_\textrm{D}$ monopoles of mass 4000 GeV.

Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for $g=2g_\textrm{D}$ monopoles of mass 200 GeV.

Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for $g=2g_\textrm{D}$ monopoles of mass 500 GeV.

Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for $g=2g_\textrm{D}$ monopoles of mass 1000 GeV.

Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for $g=2g_\textrm{D}$ monopoles of mass 1500 GeV.

Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for $g=2g_\textrm{D}$ monopoles of mass 2000 GeV.

Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for $g=2g_\textrm{D}$ monopoles of mass 2500 GeV.

Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for $g=2g_\textrm{D}$ monopoles of mass 3000 GeV.

Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for $g=2g_\textrm{D}$ monopoles of mass 4000 GeV.

Total selection efficiency (i.e., the fraction of MC HECOs surviving the trigger and offline selection criteria) as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=20$ of mass 200 GeV.

Total selection efficiency (i.e., the fraction of MC HECOs surviving the trigger and offline selection criteria) as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=20$ of mass 500 GeV.

Total selection efficiency (i.e., the fraction of MC HECOs surviving the trigger and offline selection criteria) as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=20$ of mass 1000 GeV.

Total selection efficiency (i.e., the fraction of MC HECOs surviving the trigger and offline selection criteria) as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=20$ of mass 1500 GeV.

Total selection efficiency (i.e., the fraction of MC HECOs surviving the trigger and offline selection criteria) as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=20$ of mass 2000 GeV.

Total selection efficiency (i.e., the fraction of MC HECOs surviving the trigger and offline selection criteria) as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=20$ of mass 2500 GeV.

Total selection efficiency (i.e., the fraction of MC HECOs surviving the trigger and offline selection criteria) as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=20$ of mass 3000 GeV.

Total selection efficiency (i.e., the fraction of MC HECOs surviving the trigger and offline selection criteria) as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=20$ of mass 4000 GeV.

Total selection efficiency (i.e., the fraction of MC HECOs surviving the trigger and offline selection criteria) as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=40$ of mass 200 GeV.

Total selection efficiency (i.e., the fraction of MC HECOs surviving the trigger and offline selection criteria) as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=40$ of mass 500 GeV.

Total selection efficiency (i.e., the fraction of MC HECOs surviving the trigger and offline selection criteria) as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=40$ of mass 1000 GeV.

Total selection efficiency (i.e., the fraction of MC HECOs surviving the trigger and offline selection criteria) as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=40$ of mass 1500 GeV.

Total selection efficiency (i.e., the fraction of MC HECOs surviving the trigger and offline selection criteria) as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=40$ of mass 2000 GeV.

Total selection efficiency (i.e., the fraction of MC HECOs surviving the trigger and offline selection criteria) as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=40$ of mass 2500 GeV.

Total selection efficiency (i.e., the fraction of MC HECOs surviving the trigger and offline selection criteria) as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=40$ of mass 3000 GeV.

Total selection efficiency (i.e., the fraction of MC HECOs surviving the trigger and offline selection criteria) as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=40$ of mass 4000 GeV.

Total selection efficiency (i.e., the fraction of MC HECOs surviving the trigger and offline selection criteria) as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=60$ of mass 200 GeV.

Total selection efficiency (i.e., the fraction of MC HECOs surviving the trigger and offline selection criteria) as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=60$ of mass 500 GeV.

Total selection efficiency (i.e., the fraction of MC HECOs surviving the trigger and offline selection criteria) as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=60$ of mass 1000 GeV.

Total selection efficiency (i.e., the fraction of MC HECOs surviving the trigger and offline selection criteria) as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=60$ of mass 1500 GeV.

Total selection efficiency (i.e., the fraction of MC HECOs surviving the trigger and offline selection criteria) as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=60$ of mass 2000 GeV.

Total selection efficiency (i.e., the fraction of MC HECOs surviving the trigger and offline selection criteria) as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=60$ of mass 2500 GeV.

Total selection efficiency (i.e., the fraction of MC HECOs surviving the trigger and offline selection criteria) as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=60$ of mass 3000 GeV.

Total selection efficiency (i.e., the fraction of MC HECOs surviving the trigger and offline selection criteria) as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=60$ of mass 4000 GeV.

Total selection efficiency (i.e., the fraction of MC HECOs surviving the trigger and offline selection criteria) as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=80$ of mass 200 GeV.

Total selection efficiency (i.e., the fraction of MC HECOs surviving the trigger and offline selection criteria) as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=80$ of mass 500 GeV.

Total selection efficiency (i.e., the fraction of MC HECOs surviving the trigger and offline selection criteria) as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=80$ of mass 1000 GeV.

Total selection efficiency (i.e., the fraction of MC HECOs surviving the trigger and offline selection criteria) as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=80$ of mass 1500 GeV.

Total selection efficiency (i.e., the fraction of MC HECOs surviving the trigger and offline selection criteria) as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=80$ of mass 2000 GeV.

Total selection efficiency (i.e., the fraction of MC HECOs surviving the trigger and offline selection criteria) as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=80$ of mass 2500 GeV.

Total selection efficiency (i.e., the fraction of MC HECOs surviving the trigger and offline selection criteria) as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=80$ of mass 3000 GeV.

Total selection efficiency (i.e., the fraction of MC HECOs surviving the trigger and offline selection criteria) as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=80$ of mass 4000 GeV.

Total selection efficiency (i.e., the fraction of MC HECOs surviving the trigger and offline selection criteria) as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=100$ of mass 200 GeV.

Total selection efficiency (i.e., the fraction of MC HECOs surviving the trigger and offline selection criteria) as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=100$ of mass 500 GeV.

Total selection efficiency (i.e., the fraction of MC HECOs surviving the trigger and offline selection criteria) as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=100$ of mass 1000 GeV.

Total selection efficiency (i.e., the fraction of MC HECOs surviving the trigger and offline selection criteria) as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=100$ of mass 1500 GeV.

Total selection efficiency (i.e., the fraction of MC HECOs surviving the trigger and offline selection criteria) as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=100$ of mass 2000 GeV.

Total selection efficiency (i.e., the fraction of MC HECOs surviving the trigger and offline selection criteria) as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=100$ of mass 2500 GeV.

Total selection efficiency (i.e., the fraction of MC HECOs surviving the trigger and offline selection criteria) as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=100$ of mass 3000 GeV.

Total selection efficiency (i.e., the fraction of MC HECOs surviving the trigger and offline selection criteria) as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=100$ of mass 4000 GeV.

transmax region : Mean sum of transverse momenta ($\langle \Sigma p_{T} \rangle \pm stat. \pm syst.det. \pm syst.gen.[GeV]$)

away region : Mean sum of transverse momenta ($\langle \Sigma p_{T} \rangle \pm stat. \pm syst.det. \pm syst.gen.[GeV]$)

Figure 09b, mean nTracks toward, toward region: Mean charged particle multiplicity ($\langle N_{ch} \rangle \pm stat. \pm syst.det. \pm syst.gen.$)

transverse region: Mean charged particle multiplicity ($\langle N_{ch} \rangle \pm stat. \pm syst.det. \pm syst.gen.$)

Figure 09a, mean nTracks transmin, transmin region: Mean charged particle multiplicity ($\langle N_{ch} \rangle \pm stat. \pm syst.det. \pm syst.gen.$)

transmax region: Mean charged particle multiplicity ($\langle N_{ch} \rangle \pm stat. \pm syst.det. \pm syst.gen.$)

away region: Mean charged particle multiplicity ($\langle N_{ch} \rangle \pm stat. \pm syst.det. \pm syst.gen.$)

Figure 10b, mean meanPt toward, toward region : Mean of arithmetic mean of transverse momenta ($\langle mean p_{T} \rangle \pm stat. \pm syst.det.\pm syst.gen.[GeV]$)

transverse region : Mean of arithmetic mean of transverse momenta ($\langle mean p_{T} \rangle \pm stat. \pm syst.det.\pm syst.gen.[GeV]$)

Figure 10a, mean meanPt transmin, transmin region : Mean of arithmetic mean of transverse momenta ($\langle mean p_{T} \rangle \pm stat. \pm syst.det.\pm syst.gen.[GeV]$)

transmax region : Mean of arithmetic mean of transverse momenta ($\langle mean p_{T} \rangle \pm stat. \pm syst.det.\pm syst.gen.[GeV]$)

away region : Mean of arithmetic mean of transverse momenta ($\langle mean p_{T} \rangle \pm stat. \pm syst.det.\pm syst.gen.[GeV]$)

Figure 04c from auxiliary figures, mean sumPt toward low thrust, toward region : low thrust ($T<0.75$) Mean sum of transverse momenta ($\langle \Sigma p_{T} \rangle \pm stat. \pm syst.det. \pm syst.gen.[GeV]$)

transverse region : low thrust ($T<0.75$) Mean sum of transverse momenta ($\langle \Sigma p_{T} \rangle \pm stat. \pm syst.det. \pm syst.gen.[GeV]$)

Figure 11c, mean sumPt transmin low thrust, transmin region : low thrust ($T<0.75$) Mean sum of transverse momenta ($\langle \Sigma p_{T} \rangle \pm stat. \pm syst.det. \pm syst.gen.[GeV]$)

transmax region : low thrust ($T<0.75$) Mean sum of transverse momenta ($\langle \Sigma p_{T} \rangle \pm stat. \pm syst.det. \pm syst.gen.[GeV]$)

away region : low thrust ($T<0.75$) Mean sum of transverse momenta ($\langle \Sigma p_{T} \rangle \pm stat. \pm syst.det. \pm syst.gen.[GeV]$)

Figure 04a from auxiliary figures, mean nTracks toward low thrust, toward region : low thrust ($T<0.75$) Mean charged particle multiplicity ($\langle N_{ch} \rangle \pm stat. \pm syst.det. \pm syst.gen.$)

transverse region : low thrust ($T<0.75$) Mean charged particle multiplicity ($\langle N_{ch} \rangle \pm stat. \pm syst.det. \pm syst.gen.$)

Figure 11a, mean nTracks transmin low thrust, transmin region : low thrust ($T<0.75$) Mean charged particle multiplicity ($\langle N_{ch} \rangle \pm stat. \pm syst.det. \pm syst.gen.$)

transmax region : low thrust ($T<0.75$) Mean charged particle multiplicity ($\langle N_{ch} \rangle \pm stat. \pm syst.det. \pm syst.gen.$)

away region : low thrust ($T<0.75$) Mean charged particle multiplicity ($\langle N_{ch} \rangle \pm stat. \pm syst.det. \pm syst.gen.$)

Figure 06a from auxiliary figures, mean meanPt toward low thrust, toward region : low thrust ($T<0.75$) Mean of arithmetic mean of transverse momenta ($\langle mean p_{T} \rangle \pm stat. \pm syst.det.\pm syst.gen.[GeV]$)

transverse region : low thrust ($T<0.75$) Mean of arithmetic mean of transverse momenta ($\langle mean p_{T} \rangle \pm stat. \pm syst.det.\pm syst.gen.[GeV]$)

Figure 12a, mean meanPt transmin low thrust, transmin region : low thrust ($T<0.75$) Mean of arithmetic mean of transverse momenta ($\langle mean p_{T} \rangle \pm stat. \pm syst.det.\pm syst.gen.[GeV]$)

transmax region : low thrust ($T<0.75$) Mean of arithmetic mean of transverse momenta ($\langle mean p_{T} \rangle \pm stat. \pm syst.det.\pm syst.gen.[GeV]$)

away region : low thrust ($T<0.75$) Mean of arithmetic mean of transverse momenta ($\langle mean p_{T} \rangle \pm stat. \pm syst.det.\pm syst.gen.[GeV]$)

Figure 04d from auxiliary figures, mean sumPt toward high thrust, toward region : hight thrust ($0.75\leq T$) Mean sum of transverse momenta ($\langle \Sigma p_{T} \rangle \pm stat. \pm syst.det. \pm syst.gen.[GeV]$)

transverse region : hight thrust ($0.75\leq T$) Mean sum of transverse momenta ($\langle \Sigma p_{T} \rangle \pm stat. \pm syst.det. \pm syst.gen.[GeV]$)

Figure 11d, mean sumPt transmin high thrust, transmin region : hight thrust ($0.75\leq T$) Mean sum of transverse momenta ($\langle \Sigma p_{T} \rangle \pm stat. \pm syst.det. \pm syst.gen.[GeV]$)

transmax region : hight thrust ($0.75\leq T$) Mean sum of transverse momenta ($\langle \Sigma p_{T} \rangle \pm stat. \pm syst.det. \pm syst.gen.[GeV]$)

away region : hight thrust ($0.75\leq T$) Mean sum of transverse momenta ($\langle \Sigma p_{T} \rangle \pm stat. \pm syst.det. \pm syst.gen.[GeV]$)

Figure 04b from auxiliary figures, mean nTracks toward high thrust, toward region : hight thrust ($0.75\leq T$) Mean charged particle multiplicity ($\langle N_{ch} \rangle \pm stat. \pm syst.det. \pm syst.gen.$)

transverse region : hight thrust ($0.75\leq T$) Mean charged particle multiplicity ($\langle N_{ch} \rangle \pm stat. \pm syst.det. \pm syst.gen.$)

Figure 11b, mean nTracks transmin high thrust, transmin region : hight thrust ($0.75\leq T$) Mean charged particle multiplicity ($\langle N_{ch} \rangle \pm stat. \pm syst.det. \pm syst.gen.$)

transmax region : hight thrust ($0.75\leq T$) Mean charged particle multiplicity ($\langle N_{ch} \rangle \pm stat. \pm syst.det. \pm syst.gen.$)

away region : hight thrust ($0.75\leq T$) Mean charged particle multiplicity ($\langle N_{ch} \rangle \pm stat. \pm syst.det. \pm syst.gen.$)

Figure 06b from auxiliary figures, mean meanPt toward high thrust, toward region : hight thrust ($0.75\leq T$) Mean of arithmetic mean of transverse momenta ($\langle mean p_{T} \rangle \pm stat. \pm syst.det.\pm syst.gen.[GeV]$)

transverse region : hight thrust ($0.75\leq T$) Mean of arithmetic mean of transverse momenta ($\langle mean p_{T} \rangle \pm stat. \pm syst.det.\pm syst.gen.[GeV]$)

Figure 12b, mean meanPt transmin high thrust, transmin region : hight thrust ($0.75\leq T$) Mean of arithmetic mean of transverse momenta ($\langle mean p_{T} \rangle \pm stat. \pm syst.det.\pm syst.gen.[GeV]$)

transmax region : hight thrust ($0.75\leq T$) Mean of arithmetic mean of transverse momenta ($\langle mean p_{T} \rangle \pm stat. \pm syst.det.\pm syst.gen.[GeV]$)

away region : hight thrust ($0.75\leq T$) Mean of arithmetic mean of transverse momenta ($\langle mean p_{T} \rangle \pm stat. \pm syst.det.\pm syst.gen.[GeV]$)

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,toward region,$0GeV<p_{T}^{Z}<10GeV$

Figure 01a from auxiliary figures, ptSpec toward_zptregion2, $\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,toward region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,toward region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,toward region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,toward region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,toward region,$80GeV<p_{T}^{Z}<120GeV$

Figure 02a from auxiliary figures, ptSpec toward_zptregion7, $\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,toward region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,toward region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transverse region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transverse region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transverse region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transverse region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transverse region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transverse region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transverse region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transverse region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmin region,$0GeV<p_{T}^{Z}<10GeV$

Figure 04a, ptSpec transmin_zptregion2, $\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmin region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmin region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmin region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmin region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmin region,$80GeV<p_{T}^{Z}<120GeV$

Figure 05a, ptSpec transmin_zptregion7, $\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmin region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmin region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmax region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmax region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmax region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmax region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmax region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmax region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmax region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmax region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,away region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,away region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,away region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,away region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,away region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,away region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,away region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,away region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,toward region,$0GeV<p_{T}^{Z}<10GeV$

Figure 01b from auxiliary figures, nTracks toward_zptregion2, $\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,toward region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,toward region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,toward region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,toward region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,toward region,$80GeV<p_{T}^{Z}<120GeV$

Figure 02b from auxiliary figures, nTracks toward_zptregion7, $\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,toward region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,toward region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,transverse region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,transverse region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,transverse region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,transverse region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,transverse region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,transverse region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,transverse region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,transverse region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,transmin region,$0GeV<p_{T}^{Z}<10GeV$

Figure 04b, nTracks transmin_zptregion2, $\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,transmin region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,transmin region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,transmin region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,transmin region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,transmin region,$80GeV<p_{T}^{Z}<120GeV$

Figure 05b, nTracks transmin_zptregion7, $\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,transmin region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,transmin region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,transmax region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,transmax region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,transmax region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,transmax region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,transmax region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,transmax region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,transmax region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,transmax region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,away region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,away region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,away region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,away region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,away region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,away region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,away region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,away region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,toward region,$0GeV<p_{T}^{Z}<10GeV$

Figure 01c from auxiliary figures, sumPt toward_zptregion2, $\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,toward region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,toward region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,toward region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,toward region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,toward region,$80GeV<p_{T}^{Z}<120GeV$

Figure 02c from auxiliary figures, sumPt toward_zptregion7, $\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,toward region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,toward region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transverse region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transverse region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transverse region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transverse region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transverse region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transverse region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transverse region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transverse region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmin region,$0GeV<p_{T}^{Z}<10GeV$

Figure 04c, sumPt transmin_zptregion2, $\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmin region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmin region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmin region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmin region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmin region,$80GeV<p_{T}^{Z}<120GeV$

Figure 05c, sumPt transmin_zptregion7, $\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmin region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmin region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmax region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmax region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmax region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmax region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmax region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmax region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmax region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmax region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,away region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,away region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,away region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,away region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,away region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,away region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,away region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,away region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,toward region,$0GeV<p_{T}^{Z}<10GeV$

Figure 01d from auxiliary figures, meanPt toward_zptregion2, $\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,toward region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,toward region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,toward region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,toward region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,toward region,$80GeV<p_{T}^{Z}<120GeV$

Figure 02d from auxiliary figures, meanPt toward_zptregion7, $\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,toward region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,toward region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transverse region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transverse region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transverse region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transverse region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transverse region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transverse region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transverse region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transverse region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmin region,$0GeV<p_{T}^{Z}<10GeV$

Figure 04d, meanPt transmin_zptregion2, $\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmin region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmin region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmin region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmin region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmin region,$80GeV<p_{T}^{Z}<120GeV$

Figure 05d, meanPt transmin_zptregion7, $\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmin region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmin region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmax region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmax region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmax region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmax region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmax region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmax region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmax region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,transmax region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,away region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,away region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,away region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,away region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,away region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,away region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,away region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,away region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),toward region,$0GeV<p_{T}^{Z}<10GeV$

Figure 03a from auxiliary figures, ptSpec toward_zptregion2 low thrust, $\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),toward region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),toward region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),toward region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),toward region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),toward region,$80GeV<p_{T}^{Z}<120GeV$

Figure 03c from auxiliary figures, ptSpec toward_zptregion7 low thrust, $\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),toward region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),toward region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transverse region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transverse region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transverse region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transverse region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transverse region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transverse region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transverse region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transverse region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transmin region,$0GeV<p_{T}^{Z}<10GeV$

Figure 06a, ptSpec transmin_zptregion2 low thrust, $\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transmin region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transmin region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transmin region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transmin region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transmin region,$80GeV<p_{T}^{Z}<120GeV$

Figure 06c, ptSpec transmin_zptregion7 low thrust, $\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transmin region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transmin region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transmax region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transmax region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transmax region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transmax region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transmax region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transmax region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transmax region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transmax region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),away region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),away region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),away region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),away region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),away region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),away region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),away region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{t}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),away region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),toward region,$0GeV<p_{T}^{Z}<10GeV$

Figure 05a from auxiliary figures, nTracks toward_zptregion2 low thrust, $\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),toward region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),toward region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),toward region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),toward region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),toward region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),toward region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),toward region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),transverse region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),transverse region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),transverse region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),transverse region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),transverse region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),transverse region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),transverse region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),transverse region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),transmin region,$0GeV<p_{T}^{Z}<10GeV$

Figure 07a, nTracks transmin_zptregion2 low thrust, $\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),transmin region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),transmin region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),transmin region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),transmin region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),transmin region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),transmin region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),transmin region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),transmax region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),transmax region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),transmax region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),transmax region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),transmax region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),transmax region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),transmax region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),transmax region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),away region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),away region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),away region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),away region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),away region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),away region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),away region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,low thrust(T<0.75),away region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),toward region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),toward region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),toward region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),toward region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),toward region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),toward region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),toward region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),toward region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transverse region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transverse region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transverse region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transverse region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transverse region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transverse region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transverse region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transverse region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transmin region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transmin region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transmin region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transmin region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transmin region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transmin region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transmin region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transmin region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transmax region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transmax region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transmax region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transmax region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transmax region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transmax region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transmax region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),transmax region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),away region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),away region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),away region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),away region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),away region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),away region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),away region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,low thrust(T<0.75),away region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),toward region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),toward region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),toward region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),toward region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),toward region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),toward region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),toward region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),toward region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),transverse region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),transverse region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),transverse region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),transverse region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),transverse region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),transverse region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),transverse region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),transverse region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),transmin region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),transmin region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),transmin region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),transmin region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),transmin region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),transmin region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),transmin region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),transmin region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),transmax region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),transmax region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),transmax region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),transmax region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),transmax region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),transmax region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),transmax region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),transmax region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),away region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),away region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),away region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),away region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),away region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),away region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),away region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{N_{ev}}{d(mean p_{t})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust(T<0.75),away region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),toward region,$0GeV<p_{T}^{Z}<10GeV$

Figure 03b from auxiliary figures, ptSpec toward_zptregion2 high thrust, $\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),toward region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),toward region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),toward region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),toward region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),toward region,$80GeV<p_{T}^{Z}<120GeV$

Figure 03d from auxiliary figures, ptSpec toward_zptregion7 high thrust, $\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),toward region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),toward region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transverse region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transverse region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transverse region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transverse region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transverse region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transverse region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transverse region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transverse region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transmin region,$0GeV<p_{T}^{Z}<10GeV$

Figure 06b, ptSpec transmin_zptregion2 high thrust, $\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transmin region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transmin region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transmin region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transmin region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transmin region,$80GeV<p_{T}^{Z}<120GeV$

Figure 06d, ptSpec transmin_zptregion7 high thrust, $\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transmin region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transmin region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transmax region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transmax region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transmax region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transmax region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transmax region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transmax region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transmax region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transmax region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),away region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),away region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),away region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),away region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),away region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),away region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),away region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ch}} \frac{dN_{ch}}{dp_{T}}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),away region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,high thrust (0.75<=T$),toward region,$0GeV<p_{T}^{Z}<10GeV$

Figure 05b from auxiliary figures, nTracks toward_zptregion2 high thrust, $\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,high thrust (0.75<=T$),toward region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,high thrust (0.75<=T$),toward region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,high thrust (0.75<=T$),toward region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,high thrust (0.75<=T$),toward region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,high thrust (0.75<=T$),toward region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,high thrust (0.75<=T$),toward region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,high thrust (0.75<=T$),toward region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,high thrust (0.75<=T$),transverse region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,high thrust (0.75<=T$),transverse region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,high thrust (0.75<=T$),transverse region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,high thrust (0.75<=T$),transverse region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,high thrust (0.75<=T$),transverse region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,high thrust (0.75<=T$),transverse region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,high thrust (0.75<=T$),transverse region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,high thrust (0.75<=T$),transverse region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,high thrust (0.75<=T$),transmin region,$0GeV<p_{T}^{Z}<10GeV$

Figure 07b, nTracks transmin_zptregion2 high thrust, $\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,high thrust (0.75<=T$),transmin region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,high thrust (0.75<=T$),transmin region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,high thrust (0.75<=T$),transmin region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,high thrust (0.75<=T$),transmin region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,high thrust (0.75<=T$),transmin region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,high thrust (0.75<=T$),transmin region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,high thrust (0.75<=T$),transmin region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,high thrust (0.75<=T$),transmax region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,high thrust (0.75<=T$),transmax region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,high thrust (0.75<=T$),transmax region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,high thrust (0.75<=T$),transmax region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,high thrust (0.75<=T$),transmax region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,high thrust (0.75<=T$),transmax region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,high thrust (0.75<=T$),transmax region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,high thrust (0.75<=T$),transmax region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,high thrust (0.75<=T$),away region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,high thrust (0.75<=T$),away region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,high thrust (0.75<=T$),away region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,high thrust (0.75<=T$),away region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,high thrust (0.75<=T$),away region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,high thrust (0.75<=T$),away region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,high thrust (0.75<=T$),away region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{dN_{ch}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.$,high thrust (0.75<=T$),away region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),toward region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),toward region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),toward region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),toward region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),toward region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),toward region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),toward region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),toward region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transverse region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transverse region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transverse region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transverse region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transverse region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transverse region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transverse region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transverse region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transmin region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transmin region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transmin region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transmin region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transmin region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transmin region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transmin region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transmin region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transmax region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transmax region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transmax region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transmax region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transmax region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transmax region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transmax region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),transmax region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),away region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),away region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),away region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),away region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),away region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),away region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),away region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d\Sigma p_{t}/\delta\eta\delta\phi}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75=<T),away region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d(mean p_{T})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75<=T),toward region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d(mean p_{T})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75<=T),toward region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d(mean p_{T})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75<=T),toward region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d(mean p_{T})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75<=T),toward region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d(mean p_{T})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75<=T),toward region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d(mean p_{T})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75<=T),toward region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d(mean p_{T})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75<=T),toward region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d(mean p_{T})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75<=T),toward region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d(mean p_{T})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75<=T),transverse region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d(mean p_{T})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75<=T),transverse region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d(mean p_{T})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75<=T),transverse region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d(mean p_{T})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75<=T),transverse region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d(mean p_{T})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75<=T),transverse region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d(mean p_{T})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75<=T),transverse region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d(mean p_{T})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75<=T),transverse region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d(mean p_{T})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75<=T),transverse region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d(mean p_{T})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75<=T),transmin region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d(mean p_{T})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75<=T),transmin region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d(mean p_{T})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75<=T),transmin region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d(mean p_{T})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75<=T),transmin region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d(mean p_{T})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75<=T),transmin region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d(mean p_{T})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75<=T),transmin region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d(mean p_{T})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75<=T),transmin region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d(mean p_{T})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75<=T),transmin region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d(mean p_{T})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75<=T),transmax region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d(mean p_{T})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75<=T),transmax region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d(mean p_{T})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75<=T),transmax region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d(mean p_{T})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75<=T),transmax region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d(mean p_{T})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75<=T),transmax region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d(mean p_{T})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75<=T),transmax region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d(mean p_{T})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75<=T),transmax region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d(mean p_{T})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75<=T),transmax region,$200GeV<p_{T}^{Z}<500GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d(mean p_{T})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75<=T),away region,$0GeV<p_{T}^{Z}<10GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d(mean p_{T})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75<=T),away region,$10GeV<p_{T}^{Z}<20GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d(mean p_{T})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75<=T),away region,$20GeV<p_{T}^{Z}<40GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d(mean p_{T})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75<=T),away region,$40GeV<p_{T}^{Z}<60GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d(mean p_{T})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75<=T),away region,$60GeV<p_{T}^{Z}<80GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d(mean p_{T})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75<=T),away region,$80GeV<p_{T}^{Z}<120GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d(mean p_{T})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75<=T),away region,$120GeV<p_{T}^{Z}<200GeV$

$\frac{1}{N_{ev}} \frac{dN_{ev}}{d(mean p_{T})}\pm stat.\pm syst.gen.\pm syst.det.[GeV^{-1}]$,high thrust (0.75<=T),away region,$200GeV<p_{T}^{Z}<500GeV$

Measured cross sections for inclusive isolated-photon production as a function of $E_{\rm T}^{\gamma}$ for $1.81<|\eta^{\gamma}|<2.37$.

Predicted cross sections for inclusive isolated-photon production as a function of $E_{\rm T}^{\gamma}$ for $|\eta^{\gamma}|<0.6$.

Predicted cross sections for inclusive isolated-photon production as a function of $E_{\rm T}^{\gamma}$ for $0.6<|\eta^{\gamma}|<1.37$.

Predicted cross sections for inclusive isolated-photon production as a function of $E_{\rm T}^{\gamma}$ for $1.56<|\eta^{\gamma}|<1.81$.

Predicted cross sections for inclusive isolated-photon production as a function of $E_{\rm T}^{\gamma}$ for $1.81<|\eta^{\gamma}|<2.37$.

Upper limits at the 95% CL on the cross section for SSM $W^\prime$ production and decay to the muon+neutrino channel as a function of the $W^\prime$ pole mass.

Combined (electron and muon channels) upper limits at the 95% CL on the cross section for SSM $W^\prime$ production and decay to a single lepton generation as a function of the $W^\prime$ pole mass.

Observed upper limits at the 95% CL on the cross section for generic $W^\prime$ production and decay to the electron+neutrino channel as a function of the $W^\prime$ pole mass.

Observed upper limits at the 95% CL on the cross section for generic $W^\prime$ production and decay to the muon+neutrino channel as a function of the $W^\prime$ pole mass.

Combined (electron and muon channels) observed upper limits at the 95% CL on the cross section for generic $W^\prime$ production and decay to a single lepton generation as a function of the $W^\prime$ pole mass.

Observed upper limits at the 95% CL on the visible cross section in the electron+neutrino channel as a function of the transverse mass threshold.

Observed upper limits at the 95% CL on the visible cross section in the muon+neutrino channel as a function of the transverse mass threshold.

Product of acceptance and efficiency for the electron and muon selections as a function of the $W^\prime$ pole mass.

Expected upper limits at the 95% CL on the cross section for generic $W^\prime$ production and decay to the electron+neutrino channel as a function of the $W^\prime$ pole mass.

Expected upper limits at the 95% CL on the cross section for generic $W^\prime$ production and decay to the muon+neutrino channel as a function of the $W^\prime$ pole mass.

Combined (electron and muon channels) expected upper limits at the 95% CL on the cross section for generic $W^\prime$ production and decay to a single lepton generation as a function of the $W^\prime$ pole mass.

Upper limits at 95% CL on the cross-section of the resonant Higgs boson pair production for a spin-0 heavy scalar

Upper limits at 95% CL on the cross-section of the resonant Higgs boson pair production for a spin-0 heavy scalar

Upper limits at 95% CL on the cross-section of the resonant Higgs boson pair production for a spin-0 heavy scalar

Upper limits at 95% CL on the cross-section of the resonant Higgs boson pair production for a spin-0 heavy scalar

Upper limits at 95% CL on the cross-section of the resonant Higgs boson pair production for a spin-0 heavy scalar

Upper limits at 95% CL on the cross-section of the resonant Higgs boson pair production for a spin-0 heavy scalar

Upper limits at 95% CL on the cross-section of the resonant Higgs boson pair production for a spin-0 heavy scalar

Upper limits at 95% CL on the cross-section of the resonant Higgs boson pair production for a spin-0 heavy scalar

Upper limits at 95% CL on the cross-section of the resonant Higgs boson pair production for a spin-2 KK graviton with k/M&#772;_Pl = 1

Upper limits at 95% CL on the cross-section of the resonant Higgs boson pair production for a spin-2 KK graviton with k/M&#772;_Pl = 1

Upper limits at 95% CL on the cross-section of the resonant Higgs boson pair production for a spin-2 KK graviton with k/M&#772;_Pl = 1

Upper limits at 95% CL on the cross-section of the resonant Higgs boson pair production for a spin-2 KK graviton with k/M&#772;_Pl = 1

Upper limits at 95% CL on the cross-section of the resonant Higgs boson pair production for a spin-2 KK graviton with k/M&#772;_Pl = 1

Upper limits at 95% CL on the cross-section of the resonant Higgs boson pair production for a spin-2 KK graviton with k/M&#772;_Pl = 1

Upper limits at 95% CL on the cross-section of the resonant Higgs boson pair production for a spin-2 KK graviton with k/M&#772;_Pl = 2

Upper limits at 95% CL on the cross-section of the resonant Higgs boson pair production for a spin-2 KK graviton with k/M&#772;_Pl = 2

Upper limits at 95% CL on the cross-section of the resonant Higgs boson pair production for a spin-2 KK graviton with k/M&#772;_Pl = 2

Upper limits at 95% CL on the cross-section of the resonant Higgs boson pair production for a spin-2 KK graviton with k/M&#772;_Pl = 2

Upper limits at 95% CL on the cross-section of the resonant Higgs boson pair production for a spin-2 KK graviton with k/M&#772;_Pl = 2

Upper limits at 95% CL on the cross-section of the resonant Higgs boson pair production for a spin-2 KK graviton with k/M&#772;_Pl = 2

Expected exclusion regions for the EWK-singlet model for tan &beta; = 1. The theoretical contour points with width over mass of the resonance equal to 10% are included in the table to identify the experimental-invalid regions.

Observed exclusion regions for the EWK-singlet model for tan &beta; = 1. The theoretical contour points with width over mass of the resonance equal to 10% are included in the table to identify the experimental-invalid regions.

Expected exclusion regions for the EWK-singlet model for tan &beta; = 2. The theoretical contour points with width over mass of the resonance equal to 10% are included in the table to identify the experimental-invalid regions.

Observed exclusion regions for the EWK-singlet model for tan &beta; = 2. The theoretical contour points with width over mass of the resonance equal to 10% are included in the table to identify the experimental-invalid regions.

Expected exclusion regions in the EWK-singlet model for m_S= 260 GeV. The theoretical contour points with width over mass of the resonance equal to 10% are included in the table to identify the experimental-invalid regions.

Observed exclusion regions in the EWK-singlet model for m_S= 260 GeV. The theoretical contour points with width over mass of the resonance equal to 10% are included in the table to identify the experimental-invalid regions.

Expected exclusion regions in the hMSSM model

Expected exclusion regions (-1 sigma band) in the hMSSM model

Expected exclusion regions (+1 sigma band) in the hMSSM model

Observed exclusion regions in the hMSSM model

Upper limits at 95% CL on the signal cross-section of the ggF non-resonant Higgs boson pair production as a function of &kappa;_&lambda; with statistical uncertainties only. The limits are shown in dashed lines. The combined limit including all systematic uncertainties is also shown with a solid line.

Expected exclusion regions for the EWK-singlet model with tan &beta; = 5.0. The theoretical contour points with width over mass of the resonance equal to 10% are included in the table to identify the experimental-invalid regions.

Observed exclusion regions for the EWK-singlet model with tan &beta; = 5.0. The theoretical contour points with width over mass of the resonance equal to 10% are included in the table to identify the experimental-invalid regions.

Expected exclusion regions for the EWK-singlet model with m_S = 300 GeV. The theoretical contour points with width over mass of the resonance equal to 10% are included in the table to identify the experimental-invalid regions.

Observed exclusion regions for the EWK-singlet model with m_S = 300 GeV. The theoretical contour points with width over mass of the resonance equal to 10% are included in the table to identify the experimental-invalid regions.

Expected exclusion regions for the EWK-singlet model with m_S = 400 GeV. The theoretical contour points with width over mass of the resonance equal to 10% are included in the table to identify the experimental-invalid regions.

Observed exclusion regions for the EWK-singlet model with m_S = 400 GeV. The theoretical contour points with width over mass of the resonance equal to 10% are included in the table to identify the experimental-invalid regions.

Expected exclusion regions for the EWK-singlet model with m_S = 500 GeV. The theoretical contour points with width over mass of the resonance equal to 10% are included in the table to identify the experimental-invalid regions.

Observed exclusion regions for the EWK-singlet model with m_S = 500 GeV. The theoretical contour points with width over mass of the resonance equal to 10% are included in the table to identify the experimental-invalid regions.

Dependence of the overall signal efficiency on the pT of the long-lived Z' for Z' -> ee. The error bars indicate the total uncertainties.

Dependence of the overall signal efficiency on the transverse decay radius Rxy of the long-lived Z' for Z' -> emu. The error bars indicate the total uncertainties.

Dependence of the overall signal efficiency on the pT of the long-lived Z' for Z' -> emu. The error bars indicate the total uncertainties.

Dependence of the overall signal efficiency on the transverse decay radius Rxy of the long-lived Z' for Z' -> mumu. The error bars indicate the total uncertainties.

Dependence of the overall signal efficiency on the pT of the long-lived Z' for Z' -> mumu. The error bars indicate the total uncertainties.

Overall signal efficiency as a function of the mean proper lifetime (ctau) of the neutralino for the lambda121 scenario of the RPV SUSY model. The error bars indicate the total uncertainties.

Overall signal efficiency as a function of the mean proper lifetime (ctau) of the neutralino for the lambda122 scenario of the RPV SUSY model. The error bars indicate the total uncertainties.

95% CL upper limits on the squark-antisquark production cross-section as a function of the mean proper lifetime (ctau) of the neutralino for the lambda121 scenario of the RPV SUSY model and a 700 GeV squark. The uncertainties of the expected limit indicate the +-1sigma variations.

95% CL upper limits on the squark-antisquark production cross-section as a function of the mean proper lifetime (ctau) of the neutralino for the lambda122 scenario of the RPV SUSY model and a 700 GeV squark. The uncertainties of the expected limit indicate the +-1sigma variations.

95% CL upper limits on the squark-antisquark production cross-section as a function of the mean proper lifetime (ctau) of the neutralino for the lambda121 scenario of the RPV SUSY model and a 1600 GeV squark. The uncertainties of the expected limit indicate the +-1sigma variations.

95% CL upper limits on the squark-antisquark production cross-section as a function of the mean proper lifetime (ctau) of the neutralino for the lambda122 scenario of the RPV SUSY model and a 1600 GeV squark. The uncertainties of the expected limit indicate the +-1sigma variations.

Fraction of detector volume covered by the material veto as a function of z and Rxy of the displaced dilepton vertex.

Fraction of detector volume covered by the disabled pixel modules veto veto as a function of z and Rxy of the displaced dilepton vertex.

Observed Rxy distribution of vertices composed of two non-leptonic tracks in a control sample in the data and the predicted distribution obtained from the event mixing. The error bars indicate the statistical uncertainties.

Rxy distributions of Kshort vertices from the large radius tracking in the data and background MC samples. Data has been normalised such that the total number of Kshort from the standard tracking in the data agrees with the total number of Kshort from the standard tracking in the MC. The error bars indicate the statistical uncertainties.

Acceptance per decay as a function of the mean proper lifetime (ctau) of the neutralino for neutralino -> eenu. The error bars indicate the statistical uncertainties.

Acceptance per decay as a function of the mean proper lifetime (ctau) of the neutralino for neutralino -> emunu. The error bars indicate the statistical uncertainties.

Acceptance per decay as a function of the mean proper lifetime (ctau) of the neutralino for neutralino -> mumunu. The error bars indicate the statistical uncertainties.

Detection efficiency per decay as a function of the mean proper lifetime (ctau) of the neutralino for neutralino -> eenu. The error bars indicate the total uncertainties.

Detection efficiency per decay as a function of the mean proper lifetime (ctau) of the neutralino for neutralino -> emunu. The error bars indicate the total uncertainties.

Detection efficiency per decay as a function of the mean proper lifetime (ctau) of the neutralino for neutralino -> mumunu. The error bars indicate the total uncertainties.

Overall signal efficiency (acceptance times efficiency) per decay as a function of the mean proper lifetime (ctau) of the neutralino for neutralino -> eenu. The error bars indicate the total uncertainties.

Overall signal efficiency (acceptance times efficiency) per decay as a function of the mean proper lifetime (ctau) of the neutralino for neutralino -> emunu. The error bars indicate the total uncertainties.

Overall signal efficiency (acceptance times efficiency) per decay as a function of the mean proper lifetime (ctau) of the neutralino for neutralino -> mumunu. The error bars indicate the total uncertainties.

Detection efficiency per decay for Rxy < 22 mm as a function of the invariant mass and pT of the electron pair in LLP -> eeX.

Detection efficiency per decay for 22 <= Rxy < 38 mm as a function of the invariant mass and pT of the electron pair in LLP -> eeX.

Detection efficiency per decay for 38 <= Rxy < 73 mm as a function of the invariant mass and pT of the electron pair in LLP -> eeX.

Detection efficiency per decay for 73 <= Rxy < 111 mm as a function of the invariant mass and pT of the electron pair in LLP -> eeX.

Detection efficiency per decay for 111 <= Rxy < 145 mm as a function of the invariant mass and pT of the electron pair in LLP -> eeX.

Detection efficiency per decay for 145 <= Rxy < 300 mm as a function of the invariant mass and pT of the electron pair in LLP -> eeX.

Detection efficiency per decay for Rxy < 22 mm as a function of the invariant mass and pT of the electron and muon pair in LLP -> emuX.

Detection efficiency per decay for 22 <= Rxy < 38 mm as a function of the invariant mass and pT of the electron and muon pair in LLP -> emuX.

Detection efficiency per decay for 38 <= Rxy < 73 mm as a function of the invariant mass and pT of the electron and muon pair in LLP -> emuX.

Detection efficiency per decay for 73 <= Rxy < 111 mm as a function of the invariant mass and pT of the electron and muon pair in LLP -> emuX.

Detection efficiency per decay for 111 <= Rxy < 145 mm as a function of the invariant mass and pT of the electron and muon pair in LLP -> emuX.

Detection efficiency per decay for 145 <= Rxy < 300 mm as a function of the invariant mass and pT of the electron and muon pair in LLP -> emuX.