Measured cross sections for isolated-photon plus 1jet production as a function of $|\cos\theta^{\star}|$.

Measured cross sections for isolated-photon plus 1jet production as a function of $|\cos\theta^{\star}|$ for the range $467 < m^{\gamma-\rm jet1} < 510$ GeV.

Measured cross sections for isolated-photon plus 1jet production as a function of $|\cos\theta^{\star}|$ for the range $510 < m^{\gamma-\rm jet1} < 590$ GeV.

Measured cross sections for isolated-photon plus 1jet production as a function of $|\cos\theta^{\star}|$ for the range $590 < m^{\gamma-\rm jet1} < 670$ GeV.

Measured cross sections for isolated-photon plus 1jet production as a function of $|\cos\theta^{\star}|$ for the range $670 < m^{\gamma-\rm jet1} < 760$ GeV.

Measured cross sections for isolated-photon plus 1jet production as a function of $|\cos\theta^{\star}|$ for the range $760 < m^{\gamma-\rm jet1} < 850$ GeV.

Measured cross sections for isolated-photon plus 1jet production as a function of $|\cos\theta^{\star}|$ for the range $850 < m^{\gamma-\rm jet1} < 950$ GeV.

Measured cross sections for isolated-photon plus 1jet production as a function of $|\cos\theta^{\star}|$ for the range $0.95 < m^{\gamma-\rm jet1} < 1.05$ TeV.

Measured cross sections for isolated-photon plus 1jet production as a function of $|\cos\theta^{\star}|$ for the range $1.05 < m^{\gamma-\rm jet1} < 1.25$ TeV.

Measured cross sections for isolated-photon plus 1jet production as a function of $|\cos\theta^{\star}|$ for the range $1.25 < m^{\gamma-\rm jet1} < 2.45$ TeV.

Measured cross sections for isolated-photon plus 2jet production as a function of $E_{\rm T}^{\gamma}$.

Measured cross sections for isolated-photon plus 2jet production as a function of $p_{\rm T}^{\rm jet2}$.

Measured cross sections for isolated-photon plus 2jet production as a function of $\Delta\phi^{\rm \gamma-jet2}$.

Measured cross sections for isolated-photon plus 2jet production as a function of $\Delta\phi^{\rm jet1-jet2}$.

Measured cross sections for isolated-photon plus 2jet production as a function of $\Delta\phi^{\rm \gamma-jet2}$ for the range $130< E_{\rm T}^{\gamma} <300$ GeV.

Measured cross sections for isolated-photon plus 2jet production as a function of $\Delta\phi^{\rm \gamma-jet2}$ for the range $E_{\rm T}^{\gamma} >300$ GeV.

Measured cross sections for isolated-photon plus 2jet production as a function of $\Delta\phi^{\rm jet1-jet2}$ for the range $130< E_{\rm T}^{\gamma} <300$ GeV.

Measured cross sections for isolated-photon plus 2jet production as a function of $\Delta\phi^{\rm jet1-jet2}$ for the range $E_{\rm T}^{\gamma} >300$ GeV.

Measured cross sections for isolated-photon plus 2jet production as a function of $\beta^{\rm jet1}$.

Measured cross sections for isolated-photon plus 2jet production as a function of $\beta^{\gamma}$.

Ratio of measured cross sections for isolated-photon plus 2jet production as a function of $\beta$.

Measured cross sections for isolated-photon plus 3jet production as a function of $E_{\rm T}^{\gamma}$.

Measured cross sections for isolated-photon plus 3jet production as a function of $p_{\rm T}^{\rm jet3}$.

Measured cross sections for isolated-photon plus 3jet production as a function of $\Delta\phi^{\rm \gamma-jet3}$.

Measured cross sections for isolated-photon plus 3jet production as a function of $\Delta\phi^{\rm jet1-jet3}$.

Measured cross sections for isolated-photon plus 3jet production as a function of $\Delta\phi^{\rm jet2-jet3}$.

Measured cross sections for isolated-photon plus 3jet production as a function of $\Delta\phi^{\rm \gamma-jet3}$ for the range $130< E_{\rm T}^{\gamma} <300$ GeV.

Measured cross sections for isolated-photon plus 3jet production as a function of $\Delta\phi^{\rm \gamma-jet3}$ for the range $E_{\rm T}^{\gamma} >300$ GeV.

Measured cross sections for isolated-photon plus 3jet production as a function of $\Delta\phi^{\rm jet1-jet3}$ for the range $130< E_{\rm T}^{\gamma} <300$ GeV.

Measured cross sections for isolated-photon plus 3jet production as a function of $\Delta\phi^{\rm jet1-jet3}$ for the range $E_{\rm T}^{\gamma} >300$ GeV.

Measured cross sections for isolated-photon plus 3jet production as a function of $\Delta\phi^{\rm jet2-jet3}$ for the range $130< E_{\rm T}^{\gamma} <300$ GeV.

Measured cross sections for isolated-photon plus 3jet production as a function of $\Delta\phi^{\rm jet2-jet3}$ for the range $E_{\rm T}^{\gamma} >300$ GeV.

Unfolded $\nu_\mu$ CC1$\pi^+$ differential cross section as a function of $p_\mu$ in the reduced phase-space of $p_{\pi^+} > 200$ MeV/$c$, $p_\mu > 200$ MeV/c, $\cos(\theta_{\pi^+}) > 0.3$ and $\cos(\theta_\mu) > 0.3$.

Unfolded $\nu_\mu$ CC1$\pi^+$ differential cross section as a function of $\cos\theta_\mu$ in the reduced phase-space of $p_{\pi^+} > 200$ MeV/$c$, $p_\mu > 200$ MeV/c, $\cos(\theta_{\pi^+}) > 0.3$ and $\cos(\theta_\mu) > 0.3$.

Unfolded $\nu_\mu$ CC1$\pi^+$ differential cross section as a function of $\cos\theta_{\mu,\pi}$ in the reduced phase-space of $p_{\pi^+} > 200$ MeV/$c$, $p_\mu > 200$ MeV/c, $\cos(\theta_{\pi^+}) > 0.3$ and $\cos(\theta_\mu) > 0.3$.

Unfolded $\nu_\mu$ CC1$\pi^+$ differential cross section as a function of $E_\nu^{\rm rec}$ ($\Delta$) in the reduced phase-space of $p_{\pi^+} > 200$ MeV/$c$, $p_\mu > 200$ MeV/c, $\cos(\theta_{\pi^+}) > 0.3$ and $\cos(\theta_\mu) > 0.3$.

Unfolded $\nu_\mu$ CC1$\pi^+$ differential cross section as a function of $E_\nu^{\rm rec}$ ($\mu$, $\pi$) in the reduced phase-space of $p_{\pi^+} > 200$ MeV/$c$, $p_\mu > 200$ MeV/c, $\cos(\theta_{\pi^+}) > 0.3$ and $\cos(\theta_\mu) > 0.3$.

Experimental cross-section values per bin in PB for COS(THETA*(2GAMMA)).

The luminosity weighted average polarized differential cross sections. The data are averaged over the eight centre of mass energies and over the COS(THETA(W)) bin width.

The luminosity weighted average CP-odd and CPThat-odd observables. For definition of SIG(C=+-) etc. see the text of the paper.

The luminosity weighted average CP-odd and CPThat-odd observables. For definition of SIG(C=+0) etc. see the text of the paper.

The luminosity weighted average CP-odd and CPThat-odd observables. For definition of SIG(C=-0) etc. see the text of the paper.

Measured cross section for TAU+ TAU- production. The data are corrected to no interference between initial and final state radiation.

Measured cross section for E+ E- production.

Measured cross section for E+ E- production.

Measured cross section for E+ E- production.

Measured forward backward asymmetries for MU+ MU- production. The data are corrected to no interference between initial and final state radiation.

Measured forward backward asymmetries for TAU+ TAU- production. The data are corrected to no interference between initial and final state radiation.

Measured forward backward asymmetries for E+ E- production.

Differential cross section (angular distribution) for QUARK QUARKBAR (HADRON) production. The data are corrected to no interference between initial and final state radiation. The systematic (DSYS) errors quoted here do not include the errors on the luminosity given above.

Differential cross section (angular distribution) for QUARK QUARKBAR (HADRON) production. The data are corrected to no interference between initial and final state radiation. The systematic (DSYS) errors quoted here do not include the errors on the luminosity given above.

Differential cross section (angular distribution) for MU+ MU- production. The data are corrected to no interference between initial and final state radiation. The systematic (DSYS) errors quoted here do not include the errors on the luminosity given above.

Differential cross section (angular distribution) for MU+ MU- production. The data are corrected to no interference between initial and final state radiation. The systematic (DSYS) errors quoted here do not include the errors on the luminosity given above.

Differential cross section (angular distribution) for TAU+ TAU- production.The data are corrected to no interference between initial and final state radia tion. The systematic (DSYS) errors quoted here do not include the errors on the luminosity given above.

Differential cross section (angular distribution) for TAU+ TAU- production.The data are corrected to no interference between initial and final state radia tion. The systematic (DSYS) errors quoted here do not include the errors on the luminosity given above.

Differential cross sections(angulardistribution) for E+ E- production.

Differential cross sections(angulardistribution) for E+ E- production.

The di-jet cross section as a function of the mean transverse energy of thedi-jet system for the region where either X(C=GAMMA+) or X(C=GAMMA-) are < 0.75 .

The di-jet cross section as a function of the mean transverse energy of thedi-jet system for the region where both X(C=GAMMA+) and X(C=GAMMA-) are < 0.75.

The di-jet cross section as a function of X(C=GAMMA) for transverse energy from 5 TO 7 GeV for the full X(C=GAMMA+) and X(C=GAMMA-) region.

The di-jet cross section as a function of X(C=GAMMA) for mean transverse energy 7 TO 11 GeV for the full X(C=GAMMA+)-X(C=GAMMA-) region.

The di-jet cross section as a function of X(C=GAMMA) for mean transverse energy 11 TO 25 for the full X(C=GAMMA+)-X(C=GAMMA-) region.

The di-jet cross section as a function of X(C=GAMMA) for mean transverse energy 5 TO 7 GeV in the region where either X(C=GAMMA+) or X(C=GAMMA-) are < 0.75.

The di-jet cross section as a function of X(C=GAMMA) for mean transverse energy 7 TO 11 GeV in the region where either X(C=GAMMA+) or X(C=GAMMA-) are < 0.75.

The di-jet cross section as a function of X(C=GAMMA) for mean transverse energy 5 TO 7 GeV in the region where both X(C=GAMMA+) and X(C=GAMMA-) are < 0.75.

The di-jet cross section as a function of X(C=GAMMA) for mean transverse energy 7 TO 11 GeV in the region where both X(C=GAMMA+) and X(C=GAMMA-) are < 0.75.

The di-jet cross section as a function of LOG10(X(C =GAMMA)) for mean transverse energy 5 TO 7 GeV for the full X(C=GAMMA+)-X(C=GAMMA-) region.

The di-jet cross section as a function of LOG10(X(C =GAMMA)) for mean transverse energy 5 TO 7 for the region where either X(C=GAMMA+) or X(C=GAMMA-) are <0.75.

The di-jet cross section as a function of LOG10(X(C =GAMMA)) for mean transverse energy 5 to 7 GeV for the region where both X(C=GAMMA+) and X(C=GAMMA-) are < 0.75.

The di-jet cross section as a function of the absolute pseudorapidity difference of the two leading jets for the region where either X(C=GAMMA+) or X(C=GAMMA-) are < 0.75.

The di-jet cross section as a function of the absolute pseudorapidity difference of the two leading jets for the region where both X(C=GAMMA+) and X(C=GAMMA-) are < 0.75.

The di-jet cross section as a function of the pseudorapidity of the jet with the lower pseudorapidity in the region where either X(C=GAMMA+) or X(C=GAMMA-)are < 0.75.

The di-jet cross section as a function of the pseudorapidity of the jet with the lower pseudorapidity in the region where both X(C=GAMMA+) and X(C=GAMMA-) are < 0.75.

The di-jet cross section as a function of the pseudorapidity of the jet with the lower pseudorapidity in the region where either X(C=GAMMA+) or X(C=GAMMA-)are < 0.75.

The di-jet cross section as a function of the pseudorapidity of the jet with the lower pseudorapidity in the region where both X(C=GAMMA+) and X(C=GAMMA-) are < 0.75.

The forward-backward asymmetry in muon- and tau-pair production in the two sprime/s regions.

The forward-backward asymmetry in electron-pair production for cos(theta_e) <0.7.

The angular distribution for hadron production. The errors include statistical and systematic effects combined.

The angular distribution for electron-pair production. The errors include statistical and systematic effects combined.

The angular distribution for muon- and tau-pair production. The errors include statistical and systematic effects combined.

Results of fits to the data for the Electromagnetic Coupling Constant.

The asymmetries have been corrected for interference between initial- and final-state radiation. The errors shown are the combined statistical and systematic errors.

The asymmetries have been corrected for interference between initial- and final-state radiation. The errors shown are the combined statistical and systematic errors.

The asymmetries have been corrected for interference between initial- and final-state radiation. The errors shown are the combined statistical and systematic errors.

The asymmetries have been corrected for interference between initial- and final-state radiation. The errors shown are the combined statistical and systematic errors. Combined data from MU+ MU- and TAU+ TAU-.

The data have been corrected for interference between initial- and final-state radiation. The errors shown are the combined statistical and systematic errors, with the former dominant.

The data have been corrected for interference between initial- and final-state radiation. The errors shown are the combined statistical and systematic errors, with the former dominant.

The data have been corrected for interference between initial- and final-state radiation. The errors shown are the combined statistical and systematic errors, with the former dominant.

The data have been corrected for interference between initial- and final-state radiation. The errors shown are the combined statistical and systematic errors, with the former dominant.

No description provided.

The contribution of interference between initial- and final-state radiationhas been removed.. The data are combined with previously published, see EPJ C2, 441.

The contribution of interference between initial- and final-state radiationhas been removed.. The data are combined with previously published, see EPJ C2, 441.

The contribution of interference between initial- and final-state radiationhas been removed.. The data are combined with previously published, see EPJ C2, 441.

The contribution of interference between initial- and final-state radiationhas been removed.. The data are combined with previously published, see EPJ C2, 441.

The contribution of interference between initial- and final-state radiationhas been removed.. The data are combined with previously published, see EPJ C2, 441.

The asymmetries have been corrected for interference between initial- and final-state radiation. The errors shown are the combined statistical and systematic errors. The data are combined with previously published, see EPJ C2, 441.

The asymmetries have been corrected for interference between initial- and final-state radiation. The errors shown are the combined statistical and systematic errors.

The asymmetries have been corrected for interference between initial- and final-state radiation. The errors shown are the combined statistical and systematic errors.

The asymmetries have been corrected for interference between initial- and final-state radiation. The errors shown are the combined statistical and systematic errors. Combination of MU+MU- and TAU+TAU- data.

No description provided.

No description provided.

Transverse energy flow outside the jets in the rapidity region abs(etarap*)<1.

Measured jet shape (PSI), corrected to the hadron level for each of the two highest ET jets as a function of the cone radius R in the region of mean ET from 3 to 6 GeV.

Measured jet shape (PSI), corrected to the hadron level for each of the two highest ET jets as a function of the cone radius R in the region of mean ET from 6 to 9 GeV.

Measured jet shape (PSI), corrected to the hadron level for each of the two highest ET jets as a function of the cone radius R in the region of mean ET from 9 to 12 GeV.

Measured jet shape (PSI), corrected to the hadron level for each of the two highest ET jets as a function of the cone radius R in the region of mean ET from 12 to 20 GeV.

Fraction of the transverse energy of the jets inside a cone of radious 0.5 around the jet axis as a function of the mean ET of the jets.

Fraction of the transverse energy of the jets inside a cone of radious 0.5 around the jet axis as a function of the jet rapidity.

Measured jet shape (PSI), corrected to the hadron level for each of the two highest ET jets as a function of the cone radius R for X(C=GAMMA)+- <0.8.

Measured jet shape (PSI), corrected to the hadron level for each of the two highest ET jets as a function of the cone radius R for X(C=GAMMA)+- > 0.8.