The unfolded differential charge asymmetry as a function of the transverse momentum of the top pair system. The measured values are given with statistical and systematic uncertainties. The SM theory predictions calculated at NNLO in QCD and NLO in EW theory are listed. The scale uncertainty is obtained by varying renormalisation and factorisation scales independently by a factor of 2 or 0.5 around $\mu_0$ to calculate the maximum and minimum value of the asymmetry, respectively. The nominal value $\mu_0$ is chosen as $H_T/4$. The variations in which one scale is multiplied by 2 while the other scale is divided by 2 are excluded. Finally, the scale and MC integration uncertainties are added in quadrature.

The unfolded differential charge asymmetry as a function of the longitudinal boost of the top pair system. The measured values are given with statistical and systematic uncertainties. The SM theory predictions calculated at NNLO in QCD and NLO in EW theory are listed. The scale uncertainty is obtained by varying renormalisation and factorisation scales independently by a factor of 2 or 0.5 around $\mu_0$ to calculate the maximum and minimum value of the asymmetry, respectively. The nominal value $\mu_0$ is chosen as $H_T/4$. The variations in which one scale is multiplied by 2 while the other scale is divided by 2 are excluded. Finally, the scale and MC integration uncertainties are added in quadrature.

The unfolded inclusive leptonic asymmetry. The unfolded $A_C^{\ell\bar{\ell}}$ is obtained in the reduced phase-space defined by the requirement $|\Delta |\eta_{\ell\bar{\ell}}||<2.5$. The measured values are given with statistical and systematic uncertainties. The SM theory predictions calculated at NLO in QCD and NLO in EW theory are listed. The theory uncertainty is obtained by varying both scales by a factor of 0.5 or 2.0 to calculate the minimum and maximum value of the asymmetry, respectively.

The unfolded differential leptonic asymmetry as a function of the invariant mass of the di-lepton pair. The unfolded $A_C^{\ell\bar{\ell}}$ is obtained in the reduced phase-space defined by the requirement $|\Delta |\eta_{\ell\bar{\ell}}||<2.5$. The measured values are given with statistical and systematic uncertainties. The SM theory predictions calculated at NLO in QCD and NLO in EW theory are listed. The theory uncertainty is obtained by varying both scales by a factor of 0.5 or 2.0 to calculate the minimum and maximum value of the asymmetry, respectively.

The unfolded differential leptonic asymmetry as a function of the transverse momentum of the di-lepton pair. The unfolded $A_C^{\ell\bar{\ell}}$ is obtained in the reduced phase-space defined by the requirement $|\Delta |\eta_{\ell\bar{\ell}}||<2.5$. The measured values are given with statistical and systematic uncertainties. The SM theory predictions calculated at NLO in QCD and NLO in EW theory are listed. The theory uncertainty is obtained by varying both scales by a factor of 0.5 or 2.0 to calculate the minimum and maximum value of the asymmetry, respectively.

The unfolded differential leptonic asymmetry as a function of the longitudinal boost of the di-lepton pair. The unfolded $A_C^{\ell\bar{\ell}}$ is obtained in the reduced phase-space defined by the requirement $|\Delta |\eta_{\ell\bar{\ell}}||<2.5$. The measured values are given with statistical and systematic uncertainties. The SM theory predictions calculated at NLO in QCD and NLO in EW theory are listed. The theory uncertainty is obtained by varying both scales by a factor of 0.5 or 2.0 to calculate the minimum and maximum value of the asymmetry, respectively.

Individual 68% and 95% CL bounds on the relevant Wilson coefficients of the SM Effective Field Theory in units of $\text{TeV}^{-2}$. The bounds are derived from the $A_C^{t\bar{t}}$ inclusive measurement. The experimental uncertainties are accounted for, in the form of the complete covariance matrix that keeps track of correlations between bins for the differential measurement. The theory uncertainty from the NNLO QCD + NLO EW calculation is included by explicitly varying the renormalization and factorization scales, or the parton density functions, in the calculation and registering the variations in the intervals.

Individual 68% and 95% CL bounds on the relevant Wilson coefficients of the SM Effective Field Theory in units of $\text{TeV}^{-2}$. The bounds are derived from the $A_C^{t\bar{t}}$ vs $m_{t\bar{t}}$ measurement. The experimental uncertainties are accounted for, in the form of the complete covariance matrix that keeps track of correlations between bins for the differential measurement. The theory uncertainty from the NNLO QCD + NLO EW calculation is included by explicitly varying the renormalization and factorization scales, or the parton density functions, in the calculation and registering the variations in the intervals.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\bar{t}}$ inclusive measurement. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\bar{t}}$ vs $\beta_{z,t\bar{t}}$ measurement for $\beta_{z,t\bar{t}}$ $\in$ [0,0.3]. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\bar{t}}$ vs $\beta_{z,t\bar{t}}$ measurement for $\beta_{z,t\bar{t}}$ $\in$ [0.3,0.6]. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\bar{t}}$ vs $\beta_{z,t\bar{t}}$ measurement for $\beta_{z,t\bar{t}}$ $\in$ [0.6,0.8]. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\bar{t}}$ vs $\beta_{z,t\bar{t}}$ measurement for $\beta_{z,t\bar{t}}$ $\in$ [0.8,1]. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\bar{t}}$ vs $m_{t\bar{t}}$ measurement for $m_{t\bar{t}}$ < 500 GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\bar{t}}$ vs $m_{t\bar{t}}$ measurement for $m_{t\bar{t}}$ $\in$ [500,750] GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\bar{t}}$ vs $m_{t\bar{t}}$ measurement for $m_{t\bar{t}}$ $\in$ [750,1000] GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\bar{t}}$ vs $m_{t\bar{t}}$ measurement for $m_{t\bar{t}}$ $\in$ [1000,1500] GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\bar{t}}$ vs $m_{t\bar{t}}$ measurement for $m_{t\bar{t}}$ > 1500 GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\bar{t}}$ vs $p_{T,t\bar{t}}$ measurement for $p_{T,t\bar{t}}$ < 30 GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\bar{t}}$ vs $p_{T,t\bar{t}}$ measurement for $p_{T,t\bar{t}}$ $\in$ [30,120] GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\bar{t}}$ vs $p_{T,t\bar{t}}$ measurement for $p_{T,t\bar{t}}$ > 120 GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{\ell\ell}$ inclusive measurement. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{\ell\ell}$ vs $\beta_{z,\ell\bar{\ell}}$ measurement for $\beta_{z,\ell\bar{\ell}}$ $\in$[0,0.3]. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{\ell\ell}$ vs $\beta_{z,\ell\bar{\ell}}$ measurement for $\beta_{z,\ell\bar{\ell}}$ $\in$[0.3,0.6]. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{\ell\ell}$ vs $\beta_{z,\ell\bar{\ell}}$ measurement for $\beta_{z,\ell\bar{\ell}}$ $\in$[0.6,0.8]. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{\ell\ell}$ vs $\beta_{z,\ell\bar{\ell}}$ measurement for $\beta_{z,\ell\bar{\ell}}$ $\in$[0.8,1]. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{\ell\ell}$ vs $m_{\ell\bar{\ell}}$ measurement for $m_{\ell\bar{\ell}}$ < 200 GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{\ell\ell}$ vs $m_{\ell\bar{\ell}}$ measurement for $m_{\ell\bar{\ell}}$ $\in$ [200,300] GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{\ell\ell}$ vs $m_{\ell\bar{\ell}}$ measurement for $m_{\ell\bar{\ell}}$ $\in$ [300,400] GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{\ell\ell}$ vs $m_{\ell\bar{\ell}}$ measurement for $m_{\ell\bar{\ell}}$ > 400 GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{\ell\ell}$ vs $p_{T,\ell\bar{\ell}}$ measurement for $p_{T,\ell\bar{\ell}}$ < 20 GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{\ell\ell}$ vs $p_{T,\ell\bar{\ell}}$ measurement for $p_{T,\ell\bar{\ell}}$ $\in$ [20, 70] GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{\ell\ell}$ vs $p_{T,\ell\bar{\ell}}$ measurement for $p_{T,\ell\bar{\ell}}$ > 70 GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Post-marginalisation correlation coefficients $\rho_{ij}$ of nuisance parameters for the $A_C^{t\bar{t}}$ inclusive measurement. Only $|\rho_{ij}| > 0.05$ values are included.

Post-marginalisation correlation coefficients $\rho_{ij}$ of nuisance parameters for the $A_C^{t\bar{t}}$ vs $m_{t\bar{t}}$ measurement. Only $|\rho_{ij}| > 0.05$ values are included.

Post-marginalisation correlation coefficients $\rho_{ij}$ of nuisance parameters for the $A_C^{t\bar{t}}$ vs $p_{T,t\bar{t}}$ measurement. Only $|\rho_{ij}| > 0.05$ values are included.

Post-marginalisation correlation coefficients $\rho_{ij}$ of nuisance parameters for the $A_C^{t\bar{t}}$ vs $\beta_{z,t\bar{t}}$ measurement. Only $|\rho_{ij}| > 0.05$ values are included.

Post-marginalisation correlation coefficients $\rho_{ij}$ of nuisance parameters for the $A_C^{\ell\ell}$ inclusive measurement. Only $|\rho_{ij}| > 0.05$ values are included.

Post-marginalisation correlation coefficients $\rho_{ij}$ of nuisance parameters for the $A_C^{\ell\ell}$ vs $m_{\ell\bar{\ell}}$ measurement. Only $|\rho_{ij}| > 0.05$ values are included.

Post-marginalisation correlation coefficients $\rho_{ij}$ of nuisance parameters for the $A_C^{\ell\ell}$ vs $p_{T,\ell\bar{\ell}}$ measurement. Only $|\rho_{ij}| > 0.05$ values are included.

Post-marginalisation correlation coefficients $\rho_{ij}$ of nuisance parameters for the $A_C^{\ell\ell}$ vs $\beta_{z,\ell\bar{\ell}}$ measurement. Only $|\rho_{ij}| > 0.05$ values are included.

Covariance matrix for the $A_C^{t\bar{t}}$ vs $m_{t\bar{t}}$ measurement. The total (stat. + syst.) uncertainties are considered.

Covariance matrix for the $A_C^{t\bar{t}}$ vs $p_{T,t\bar{t}}$ measurement. The total (stat. + syst.) uncertainties are considered.

Covariance matrix for the $A_C^{t\bar{t}}$ vs $\beta_{z,t\bar{t}}$ measurement. The total (stat. + syst.) uncertainties are considered.

Covariance matrix for the $A_C^{\ell\ell}$ vs $m_{\ell\bar{\ell}}$ measurement. The total (stat. + syst.) uncertainties are considered.

Covariance matrix for the $A_C^{\ell\ell}$ vs $p_{T,\ell\bar{\ell}}$ measurement. The total (stat. + syst.) uncertainties are considered.

Covariance matrix for the $A_C^{\ell\ell}$ vs $\beta_{z,\ell\bar{\ell}}$ measurement. The total (stat. + syst.) uncertainties are considered.

Correlated Systematic Uncertainties for W- production.

Cross sections for W+ production from the combined electron and muon data sets in the defined fiducial regions. The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.

Correlated Systematic Uncertainties for W+ production.

Combined lepton charge asymmetry from W boson decays.

Fiducial cross sections of Z0 versus W+ from fitting the combined electron and muon decay data sets. The table shows the fitted ellipse centre in Z0 W+ space plus the ellipse radii and angle using the total uncertainties and only the experimental uncertainties.

Fiducial cross sections of Z0 versus W- from fitting the combined electron and muon decay data sets. The table shows the fitted ellipse centre in Z0 W- space plus the ellipse radii and angle using the total uncertainties and only the experimental uncertainties.

Fiducial cross sections of Z0 versus W+- from fitting the combined electron and muon decay data sets. The table shows the fitted ellipse centre in Z0 W+- space plus the ellipse radii and angle using the total uncertainties and only the experimental uncertainties.

Fiducial cross sections of W- versus W+ from fitting the combined electron and muon decay data sets. The table shows the fitted ellipse centre in W- W+ space plus the ellipse radii and angle using the total uncertainties and only the experimental uncertainties.

Total cross sections of Z0 versus W+ from fitting the combined electron and muon decay data sets. The table shows the fitted ellipse centre in Z0 W+ space plus the ellipse radii and angle using the total uncertainties and only the experimental uncertainties.

Total cross sections of Z0 versus W- from fitting the combined electron and muon decay data sets. The table shows the fitted ellipse centre in Z0 W- space plus the ellipse radii and angle using the total uncertainties and only the experimental uncertainties.

Total cross sections of Z0 versus W+- from fitting the combined electron and muon decay data sets. The table shows the fitted ellipse centre in Z0 W+- space plus the ellipse radii and angle using the total uncertainties and only the experimental uncertainties.

Total cross sections of W- versus W+ from fitting the combined electron and muon decay data sets. The table shows the fitted ellipse centre in W- W+ space plus the ellipse radii and angle using the total uncertainties and only the experimental uncertainties.

Factors to correct the measured cross-sections for different treatments of photon final-state radiation (QED FSR) to: - dressed leptons, recombined with FSR photons in a cone of DeltaR < 0.1 and - bare leptons, defined after FSR. These correction factors are found to be (pseudo)-rapidity independent.

Theory prediction from FEWZ program at NNLO QCD for fiducial Z0 production cross section times leptonic branching using different PDF sets. The first error (stat) is the numerical statistical uncertainty of the calculation, while second and third give the asymmetric uncertainty from the PDF set.

Theory prediction from FEWZ program at NNLO QCD for total Z0 production cross section times leptonic branching using different PDF sets. The first error (stat) is the numerical statistical uncertainty of the calculation, while second and third give the asymmetric uncertainty from the PDF set.

Theory prediction from FEWZ program at NNLO QCD for fiducial W+ + W- production cross section times leptonic branching using different PDF sets. The first error (stat) is the numerical statistical uncertainty of the calculation, while second and third give the asymmetric uncertainty from the PDF set.

Theory prediction from FEWZ program at NNLO QCD for total W+ + W- production cross section times leptonic branching using different PDF sets. The first error (stat) is the numerical statistical uncertainty of the calculation, while second and third give the asymmetric uncertainty from the PDF set.

dDeltaPhi distribution in 7 TeV P-P collisions.

The Collins and Sivers asymmetry as a function of X for 'ALL' negative pions from the 2003-2004 data.. Errors are statistical only.

The Collins and Sivers asymmetry as a function of PT for 'ALL' negative pions from the 2003-2004 data.. Errors are statistical only.

The Collins and Sivers asymmetry as a function of Z for 'ALL' negative pions from the 2003-2004 data.. Errors are statistical only.

The Collins and Sivers asymmetry as a function of X for 'ALL' positive kaons from the 2003-2004 data.. Errors are statistical only.

The Collins and Sivers asymmetry as a function of PT for 'ALL' positive kaons from the 2003-2004 data.. Errors are statistical only.

The Collins and Sivers asymmetry as a function of Z for 'ALL' positive kaons from the 2003-2004 data.. Errors are statistical only.

The Collins and Sivers asymmetry as a function of X for 'ALL' negative kaons from the 2003-2004 data.. Errors are statistical only.

The Collins and Sivers asymmetry as a function of PT for 'ALL' negative kaons from the 2003-2004 data.. Errors are statistical only.

The Collins and Sivers asymmetry as a function of Z for 'ALL' negative kaons from the 2003-2004 data.. Errors are statistical only.

The Collins and Sivers asymmetry as a function of X for 'ALL' neutral kaons from the 2002-2004 data.. Errors are statistical only.

The Collins and Sivers asymmetry as a function of PT for 'ALL' neutral kaons from the 2002-2004 data.. Errors are statistical only.

The Collins and Sivers asymmetry as a function of Z for 'ALL' neutral kaons from the 2002-2004 data.. Errors are statistical only.

The Collins and Sivers asymmetry as a function of X for 'LEADING' positive pions from the 2003-2004 data.. Errors are statistical only.

The Collins and Sivers asymmetry as a function of PT for 'LEADING' positivepions from the 2003-2004 data.. Errors are statistical only.

The Collins and Sivers asymmetry as a function of Z for 'LEADING' positive pions from the 2003-2004 data.. Errors are statistical only.

The Collins and Sivers asymmetry as a function of X for 'LEADING' negative pions from the 2003-2004 data.. Errors are statistical only.

The Collins and Sivers asymmetry as a function of PT for 'LEADING' negativepions from the 2003-2004 data.. Errors are statistical only.

The Collins and Sivers asymmetry as a function of Z for 'LEADING' negative pions from the 2003-2004 data.. Errors are statistical only.

The Collins and Sivers asymmetry as a function of X for 'LEADING' positive kaons from the 2003-2004 data.. Errors are statistical only.

The Collins and Sivers asymmetry as a function of PT for 'LEADING' positivekaons from the 2003-2004 data.. Errors are statistical only.

The Collins and Sivers asymmetry as a function of Z for 'LEADING' positive kaons from the 2003-2004 data.. Errors are statistical only.

The Collins and Sivers asymmetry as a function of X for 'LEADING' negative kaons from the 2003-2004 data.. Errors are statistical only.

The Collins and Sivers asymmetry as a function of PT for 'LEADING' negativekaons from the 2003-2004 data.. Errors are statistical only.

The Collins and Sivers asymmetry as a function of Z for 'LEADING' negative kaons from the 2003-2004 data.. Errors are statistical only.

The Collins and Sivers asymmetry as a function of X for 'LEADING' neutral kaons from the 2002-2004 data.. Errors are statistical only.

The Collins and Sivers asymmetry as a function of PT for 'LEADING' neutral kaons from the 2002-2004 data.. Errors are statistical only.

The Collins and Sivers asymmetry as a function of Z for 'LEADING' neutral kaons from the 2002-2004 data.. Errors are statistical only.

Collins asymmetry against PT for leading negative hadrons.

Collins asymmetry against Bjorken X for leading negative hadrons.

Collins asymmetry against Z for leading negative hadrons.

Collins asymmetry against PT for all positive hadrons.

Collins asymmetry against Bjorken X for all positive hadrons.

Collins asymmetry against Z for all positive hadrons.

Collins asymmetry against PT for leading positive hadrons.

Collins asymmetry against Bjorken X for leading positive hadrons.

Collins asymmetry against Z for leading positive hadrons.

Sivers asymmetry against PT for all negative hadrons.

Sivers asymmetry against Bjorken X for all negative hadrons.

Sivers asymmetry against Z for all negative hadrons.

Sivers asymmetry against PT for leading negative hadrons.

Sivers asymmetry against Bjorken X for leading negative hadrons.

Sivers asymmetry against Z for leading negative hadrons.

Sivers asymmetry against PT for all positive hadrons.

Sivers asymmetry against Bjorken X for all positive hadrons.

Sivers asymmetry against Z for all positive hadrons.

Sivers asymmetry against PT for leading positive hadrons.

Sivers asymmetry against Bjorken X for leading positive hadrons.

Sivers asymmetry against Z for leading positive hadrons.

Differential cross sections for non-radiative E+ E- --> E+ E- events at centre of mass energy 196 GeV.

Differential cross sections for non-radiative E+ E- --> E+ E- events at centre of mass energy 200 GeV.

Differential cross sections for non-radiative E+ E- --> E+ E- events at centre of mass energy 202 GeV.

Differential cross sections for non-radiative E+ E- --> E+ E- events at centre of mass energy 205 GeV.

Differential cross sections for non-radiative E+ E- --> E+ E- events at centre of mass energy 207 GeV.

Measured cross sections and forward-backward asymmetries for inclusive E+ E- --> MU+ MU- events.

Measured cross sections and forward-backward asymmetries for non-radiative E+ E- --> MU+ MU- events.

Differential cross sections for non-radiative E+ E- --> MU+ MU- events at centre of mass energy 183 GeV.

Differential cross sections for non-radiative E+ E- --> MU+ MU- events at centre of mass energy 189 GeV.

Differential cross sections for non-radiative E+ E- --> MU+ MU- events at centre of mass energy 192 GeV.

Differential cross sections for non-radiative E+ E- --> MU+ MU- events at centre of mass energy 196 GeV.

Differential cross sections for non-radiative E+ E- --> MU+ MU- events at centre of mass energy 200 GeV.

Differential cross sections for non-radiative E+ E- --> MU+ MU- events at centre of mass energy 202 GeV.

Differential cross sections for non-radiative E+ E- --> MU+ MU- events at centre of mass energy 205 GeV.

Differential cross sections for non-radiative E+ E- --> MU+ MU- events at centre of mass energy 207 GeV.

Measured cross sections and forward-backward asymmetries for inclusive E+ E- --> TAU+ TAU- events.

Measured cross sections and forward-backward asymmetries for non-radiative E+ E- --> TAU+ TAU- events.

Differential cross sections for non-radiative E+ E- --> TAU+ TAU- events atcentre of mass energy 183 GeV.

Differential cross sections for non-radiative E+ E- --> TAU+ TAU- events atcentre of mass energy 189 GeV.

Differential cross sections for non-radiative E+ E- --> TAU+ TAU- events atcentre of mass energy 192 GeV.

Differential cross sections for non-radiative E+ E- --> TAU+ TAU- events atcentre of mass energy 196 GeV.

Differential cross sections for non-radiative E+ E- --> TAU+ TAU- events atcentre of mass energy 200 GeV.

Differential cross sections for non-radiative E+ E- --> TAU+ TAU- events atcentre of mass energy 202 GeV.

Differential cross sections for non-radiative E+ E- --> TAU+ TAU- events atcentre of mass energy 205 GeV.

Differential cross sections for non-radiative E+ E- --> TAU+ TAU- events atcentre of mass energy 207 GeV.

Measured values of the inclusive and non radiative cross sections for the process E+ E- --> Q QBAR.

Asymmetries as a function of X for ALL hadrons.

Asymmetries as a function of Z for ALL hadrons.

Asymmetries as a function of PT for ALL hadrons.

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