Signal region detector-level distribution for the observable $p_{\mathrm{T}}^{\mathrm{lead}\, \ell}$.

Signal region detector-level distribution for the observable $m_{e\mu}$.

Signal region detector-level distribution for the observable $p_{\mathrm{T}}^{e\mu}$.

Measured fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $|y_{e\mu}|$

Relative systematic uncertainties for the fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $|y_{e\mu}|$

Measured fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $|\Delta \phi(e \mu)|$

Relative systematic uncertainties for the fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $|\Delta \phi(e \mu)|$

Measured fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $ \cos\theta^{\ast}$

Relative systematic uncertainties for the fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $ \cos\theta^{\ast}$

Measured fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $p_{\mathrm{T}}^{\mathrm{lead}\, \ell}$

Relative systematic uncertainties for the fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $p_{\mathrm{T}}^{\mathrm{lead}\, \ell}$

Measured fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $m_{e\mu}$

Relative systematic uncertainties for the fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $m_{e\mu}$

Measured fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $p_{\mathrm{T}}^{e\mu}$

Relative systematic uncertainties for the fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $p_{\mathrm{T}}^{e\mu}$

The statistical correlation coefficients (in percentage) between bins for the measured fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $|y_{e\mu}|$

The total correlation coefficients (in percentage) between bins for the measured fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $|y_{e\mu}|$

The statistical correlation coefficients (in percentage) between bins for the measured fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $|\Delta \phi(e \mu)|$

The total correlation coefficients (in percentage) between bins for the measured fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $|\Delta \phi(e \mu)|$

The statistical correlation coefficients (in percentage) between bins for the measured fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $ \cos\theta^{\ast}$

The total correlation coefficients (in percentage) between bins for the measured fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $ \cos\theta^{\ast}$

The statistical correlation coefficients (in percentage) between bins for the measured fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $p_{\mathrm{T}}^{\mathrm{lead}\, \ell}$

The total correlation coefficients (in percentage) between bins for the measured fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $p_{\mathrm{T}}^{\mathrm{lead}\, \ell}$

The statistical correlation coefficients (in percentage) between bins for the measured fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $m_{e\mu}$

The total correlation coefficients (in percentage) between bins for the measured fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $m_{e\mu}$

The statistical correlation coefficients (in percentage) between bins for the measured fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $p_{\mathrm{T}}^{e\mu}$

The total correlation coefficients (in percentage) between bins for the measured fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $p_{\mathrm{T}}^{e\mu}$

Statistical correlation between bins in data for the differential cross sections for the production of W⁺ bosons as a function of the inclusive jet multiplicity.

Statistical correlation between bins in data for the differential cross sections for the production of W^- bosons as a function of the inclusive jet multiplicity.

Differential cross section for the production of W bosons as a function of H_T for events with N_jets ≥ 1.

Statistical correlation between bins in data for the differential cross section for the production of W bosons as a function of H_T for events with N_jets ≥ 1.

Differential cross sections for the production of W⁺ bosons, W^- bosons and the W⁺/W^- cross section ratio as a function of the H_T for events with N_jets ≥ 1.

Statistical correlation between bins in data for the differential cross sections for the production of W⁺ bosons as a function of the H_T for events with N_jets ≥ 1.

Statistical correlation between bins in data for the differential cross sections for the production of W^- bosons as a function of the H_T for events with N_jets ≥ 1.

Differential cross section for the production of W bosons as a function of the W p_T for events with N_jets ≥ 1.

Statistical correlation between bins in data for the differential cross section for the production of W bosons as a function of the W p_T for events with N_jets ≥ 1.

Differential cross sections for the production of W⁺ bosons, W^- bosons and the W⁺/W^- cross section ratio as a function of the W p_T for events with N_jets ≥ 1.

Statistical correlation between bins in data for the differential cross sections for the production of W⁺ bosons as a function of the W p_T for events with N_jets ≥ 1.

Statistical correlation between bins in data for the differential cross sections for the production of W^- bosons as a function of the W p_T for events with N_jets ≥ 1.

Differential cross section for the production of W bosons as a function of the leading jet p_T for events with N_jets ≥ 1.

Statistical correlation between bins in data for the differential cross section for the production of W bosons as a function of the leading jet p_T for events with N_jets ≥ 1.

Differential cross sections for the production of W⁺ bosons, W^- bosons and the W⁺/W^- cross section ratio as a function of the leading jet p_T for events with N_jets ≥ 1.

Statistical correlation between bins in data for the differential cross sections for the production of W⁺ bosons as a function of the leading jet p_T for events with N_jets ≥ 1.

Statistical correlation between bins in data for the differential cross sections for the production of W^- bosons as a function of the leading jet p_T for events with N_jets ≥ 1.

Differential cross section for the production of W bosons as a function of the leading jet rapidity for events with N_jets ≥ 1.

Statistical correlation between bins in data for the differential cross section for the production of W bosons as a function of the leading jet rapidity for events with N_jets ≥ 1.

Differential cross sections for the production of W⁺ bosons, W^- bosons and the W⁺/W^- cross section ratio as a function of the leading jet rapidity for events with N_jets ≥ 1.

Statistical correlation between bins in data for the differential cross sections for the production of W⁺ bosons as a function of the leading jet rapidity for events with N_jets ≥ 1.

Statistical correlation between bins in data for the differential cross sections for the production of W^- bosons as a function of the leading jet rapidity for events with N_jets ≥ 1.

Differential cross section for the production of W bosons as a function of second leading jet p_T for events with N_jets ≥ 2.

Statistical correlation between bins in data for the differential cross section for the production of W bosons as a function of second leading jet p_T for events with N_jets ≥ 2.

Differential cross section for the production of W bosons as a function of second leading jet rapidity for events with N_jets ≥ 2.

Statistical correlation between bins in data for the differential cross section for the production of W bosons as a function of second leading jet rapidity for events with N_jets ≥ 2.

Differential cross section for the production of W bosons as a function of Δ R_jet1,jet2 for events with N_jets ≥ 2.

Statistical correlation between bins in data for the differential cross section for the production of W bosons as a function of Δ R_jet1,jet2 for events with N_jets ≥ 2.

Differential cross section for the production of W bosons as a function of dijet invariant mass for events with N_jets ≥ 2.

Statistical correlation between bins in data for the differential cross section for the production of W bosons as a function of dijet invariant mass for events with N_jets ≥ 2.

Cross section for the production of W bosons as a function of exclusive jet multiplicity.

Statistical correlation between bins in data for the cross section for the production of W bosons as a function of exclusive jet multiplicity.

Differential cross section for the production of W bosons as a function of the H_T for events with N_jets ≥ 2.

Statistical correlation between bins in data for the differential cross section for the production of W bosons as a function of the H_T for events with N_jets ≥ 2.

Differential cross sections for the production of W⁺ bosons, W^- bosons and the W⁺/W^- cross section ratio as a function of the H_T for events with N_jets ≥ 2.

Statistical correlation between bins in data for the differential cross sections for the production of W⁺ bosons as a function of the H_T for events with N_jets ≥ 2.

Statistical correlation between bins in data for the differential cross sections for the production of W^- bosons as a function of the H_T for events with N_jets ≥ 2.

Differential cross section for the production of W bosons as a function of the W p_T for events with N_jets ≥ 2.

Statistical correlation between bins in data for the differential cross section for the production of W bosons as a function of the W p_T for events with N_jets ≥ 2.

Differential cross sections for the production of W⁺ bosons, W^- bosons and the W⁺/W^- cross section ratio as a function of the W p_T for events with N_jets ≥ 2.

Statistical correlation between bins in data for the differential cross sections for the production of W⁺ bosons as a function of the W p_T for events with N_jets ≥ 2.

Statistical correlation between bins in data for the differential cross sections for the production of W^- bosons as a function of the W p_T for events with N_jets ≥ 2.

Differential cross section for the production of W bosons as a function of the leading jet p_T for events with N_jets ≥ 2.

Statistical correlation between bins in data for the differential cross section for the production of W bosons as a function of the leading jet p_T for events with N_jets ≥ 2.

Differential cross sections for the production of W⁺ bosons, W^- bosons and the W⁺/W^- cross section ratio as a function of the leading jet p_T for events with N_jets ≥ 2.

Statistical correlation between bins in data for the differential cross sections for the production of W⁺ bosons as a function of the leading jet p_T for events with N_jets ≥ 2.

Statistical correlation between bins in data for the differential cross sections for the production of W^- bosons as a function of the leading jet p_T for events with N_jets ≥ 2.

Differential cross section for the production of W bosons as a function of the electron η for events with N_jets ≥ 0.

Statistical correlation between bins in data for the differential cross section for the production of W bosons as a function of the electron η for events with N_jets ≥ 0.

Differential cross sections for the production of W⁺ bosons, W^- bosons and the W⁺/W^- cross section ratio as a function of the electron η for events with N_jets ≥ 0.

Statistical correlation between bins in data for the differential cross sections for the production of W⁺ bosons as a function of the electron η for events with N_jets ≥ 0.

Statistical correlation between bins in data for the differential cross sections for the production of W^- bosons as a function of the electron η for events with N_jets ≥ 0.

Differential cross section for the production of W bosons as a function of the electron η for events with N_jets ≥ 1.

Statistical correlation between bins in data for the differential cross section for the production of W bosons as a function of the electron η for events with N_jets ≥ 1.

Differential cross sections for the production of W⁺ bosons, W^- bosons and the W⁺/W^- cross section ratio as a function of the electron η for events with N_jets ≥ 1.

Statistical correlation between bins in data for the differential cross sections for the production of W⁺ bosons as a function of the electron η for events with N_jets ≥ 1.

Statistical correlation between bins in data for the differential cross sections for the production of W^- bosons as a function of the electron η for events with N_jets ≥ 1.

List of experimentally considered systematic uncertainties for the W+jets cross section measurement

Non-perturbative corrections for the cross section for the production of W bosons for different inclusive jet multiplicities.

Non-perturbative corrections for the differential cross sections for the production of W⁺ bosons and W^- bosons as a function of the inclusive jet multiplicity.

Non-perturbative corrections for the differential cross section for the production of W bosons as a function of H_T for events with N_jets ≥ 1.

Non-perturbative corrections for the differential cross sections for the production of W⁺ bosons and W^- bosons as a function of the H_T for events with N_jets ≥ 1.

Non-perturbative corrections for the differential cross section for the production of W bosons as a function of the W p_T for events with N_jets ≥ 1.

Non-perturbative corrections for the differential cross sections for the production of W⁺ bosons and W^- bosons as a function of the W p_T for events with N_jets ≥ 1.

Non-perturbative corrections for the differential cross section for the production of W bosons as a function of the leading jet p_T for events with N_jets ≥ 1.

Non-perturbative corrections for the differential cross sections for the production of W⁺ bosons and W^- bosons as a function of the leading jet p_T for events with N_jets ≥ 1.

Non-perturbative corrections for the differential cross section for the production of W bosons as a function of the leading jet rapidity for events with N_jets ≥ 1.

Non-perturbative corrections for the differential cross sections for the production of W⁺ bosons and W^- bosons as a function of the leading jet rapidity for events with N_jets ≥ 1.

Non-perturbative corrections for the differential cross section for the production of W bosons as a function of second leading jet p_T for events with N_jets ≥ 2.

Non-perturbative corrections for the differential cross section for the production of W bosons as a function of second leading jet rapidity for events with N_jets ≥ 2.

Non-perturbative corrections for the differential cross section for the production of W bosons as a function of Δ R_jet1,jet2 for events with N_jets ≥ 2.

Non-perturbative corrections for the differential cross section for the production of W bosons as a function of dijet invariant mass for events with N_jets ≥ 2.

Non-perturbative corrections for the cross section for the production of W bosons as a function of exclusive jet multiplicity.

Non-perturbative corrections for the differential cross section for the production of W bosons as a function of the H_T for events with N_jets ≥ 2.

Non-perturbative corrections for the differential cross sections for the production of W⁺ bosons and W^- bosons as a function of the H_T for events with N_jets ≥ 2.

Non-perturbative corrections for the differential cross section for the production of W bosons as a function of the W p_T for events with N_jets ≥ 2.

Non-perturbative corrections for the differential cross sections for the production of W⁺ bosons and W^- bosons as a function of the W p_T for events with N_jets ≥ 2.

Non-perturbative corrections for the differential cross section for the production of W bosons as a function of the leading jet p_T for events with N_jets ≥ 2.

Non-perturbative corrections for the differential cross sections for the production of W⁺ bosons and W^- bosons as a function of the leading jet p_T for events with N_jets ≥ 2.

NNLO/NLO k-factors determined with NNLO Njetti for the differential cross sections for the production of W⁺ bosons and W^- bosons as a function of the H_T for events with N_jets ≥ 1. These numbers were obtained with code described in Phys. Rev. Lett. 115 (2015) 062002 [arXiv:1504.02131].

NNLO/NLO k-factors determined with NNLO Njetti for the differential cross sections for the production of W⁺ bosons and W^- bosons as a function of the W p_T for events with N_jets ≥ 1. These numbers were obtained with code described in Phys. Rev. Lett. 115 (2015) 062002 [arXiv:1504.02131].

NNLO/NLO k-factors determined with NNLO Njetti for the differential cross sections for the production of W⁺ bosons and W^- bosons as a function of the leading jet p_T for events with N_jets ≥ 1. These numbers were obtained with code described in Phys. Rev. Lett. 115 (2015) 062002 [arXiv:1504.02131].

NNLO/NLO k-factors determined with NNLO Njetti for the differential cross sections for the production of W⁺ bosons and W^- bosons as a function of the leading jet rapidity for events with N_jets ≥ 1. These numbers were obtained with code described in Phys. Rev. Lett. 115 (2015) 062002 [arXiv:1504.02131].

The cross section differential in the fraction of the proton four-momentum carried by the Pomeron, LOG10(C=XI), for events with at least two jets of pt > 20 GeV found by the anti-kt jet algorithm with R=0.4.

The cross section differential in the fraction of the proton four-momentum carried by the Pomeron, LOG10(C=XI), for events with at least two jets of pt > 20 GeV found by the anti-kt jet algorithm with R=0.6 and after requiring that the pseudorapidity gap > 2.

The cross section differential in the fraction of the proton four-momentum carried by the Pomeron, LOG10(C=XI), for events with at least two jets of pt > 20 GeV found by the anti-kt jet algorithm with R=0.4 and after requiring that the pseudorapidity gap > 2.

The differential cross section of $Z$ boson production scaled by 1/$p_\mathrm{T}^{Z}$, (1/$p_\mathrm{T}^{Z}$) $d\sigma /dp_\mathrm{T}^{Z}$, for $-3<y^\mathrm{*}_{Z}<2$.

The differential cross section of $Z$ boson production scaled by 1/$p_\mathrm{T}^{Z}$, (1/$p_\mathrm{T}^{Z}$) $d\sigma /dp_\mathrm{T}^{Z}$, for $-2<y^\mathrm{*}_{Z}<0$ and $0<y^\mathrm{*}_{Z}<2.

Centrality bias corrected $Z$ boson yields per event for $-3<y^\mathrm{*}_{Z}<2$ scaled by by $\langle N_{coll}\rangle$. (To remove the centrality bias correction each value may be multiplied by the approriate correction value found in arXiv:1412.0976.).

The rapidity differential Z boson yields per event scaled by $\langle N_{coll}\rangle$ for three centrality ranges.

The inclusive PI0 cross section as a function of the Bjorken X.

The inclusive PI0 cross section as a function of the Bjorken X.

The inclusive PI0 cross section as a function of the Bjorken X.

The inclusive PI0 cross section as a function of the transverse momentum of the PI0 in the photon-proton c.m. system (PT*).

The inclusive PI0 cross section as a function of the transverse momentum of the PI0 in the photon-proton c.m. system (PT*).

The inclusive PI0 cross section as a function of the transverse momentum of the PI0 in the photon-proton c.m. system (PT*).

The inclusive PI0 cross section as a function of the scaled pion energy in 3 regions of Bjorken X.

The inclusive PI0 cross section as a function of the scaled pion energy in 3 regions of Q**2.

XP distribution at c.m. energy 172.0 GeV.

XP distribution at c.m. energy 183.0 GeV.

XP distribution at c.m. energy 189.0 GeV.

XP distribution at c.m. energy 196.0 GeV.

XP distribution at c.m. energy 200.0 GeV.

XP distribution at c.m. energy 206.0 GeV.

Peak position in XI distribution for different c.m. energies.

XI distribution at c.m. energy 133.0 GeV.

XI distribution at c.m. energy 161.0 GeV.

XI distribution at c.m. energy 172.0 GeV.

XI distribution at c.m. energy 183.0 GeV.

XI distribution at c.m. energy 189.0 GeV.

XI distribution at c.m. energy 196.0 GeV.

XI distribution at c.m. energy 200.0 GeV.

XI distribution at c.m. energy 206.0 GeV.

XE distribution at c.m. energy 133.0 GeV.

XE distribution at c.m. energy 161.0 GeV.

XE distribution at c.m. energy 172.0 GeV.

XE distribution at c.m. energy 183.0 GeV.

XE distribution at c.m. energy 189.0 GeV.

XE distribution at c.m. energy 196.0 GeV.

XE distribution at c.m. energy 200.0 GeV.

XE distribution at c.m. energy 206.0 GeV.

PTIN distribution at c.m. energy 133.0 GeV.

PTIN distribution at c.m. energy 161.0 GeV.

PTIN distribution at c.m. energy 172.0 GeV.

PTIN distribution at c.m. energy 183.0 GeV.

PTIN distribution at c.m. energy 189.0 GeV.

PTIN distribution at c.m. energy 196.0 GeV.

PTIN distribution at c.m. energy 200.0 GeV.

PTIN distribution at c.m. energy 206.0 GeV.

PTOUT distribution at c.m. energy 206.0 GeV.

RAPIDITY W.R.T THRUST AXIS distribution at c.m. energy 133.0 GeV.

RAPIDITY W.R.T THRUST AXIS distribution at c.m. energy 161.0 GeV.

RAPIDITY W.R.T THRUST AXIS distribution at c.m. energy 172.0 GeV.

RAPIDITY W.R.T THRUST AXIS distribution at c.m. energy 183.0 GeV.

RAPIDITY W.R.T THRUST AXIS distribution at c.m. energy 189.0 GeV.

RAPIDITY W.R.T THRUST AXIS distribution at c.m. energy 196.0 GeV.

RAPIDITY W.R.T THRUST AXIS distribution at c.m. energy 200.0 GeV.

RAPIDITY W.R.T THRUST AXIS distribution at c.m. energy 206.0 GeV.

RAPIDITY W.R.T. SPHERICITY AXIS distribution at c.m. energy 133.0 GeV.

RAPIDITY W.R.T. SPHERICITY AXIS distribution at c.m. energy 161.0 GeV.

RAPIDITY W.R.T. SPHERICITY AXIS distribution at c.m. energy 172.0 GeV.

RAPIDITY W.R.T. SPHERICITY AXIS distribution at c.m. energy 183.0 GeV.

RAPIDITY W.R.T. SPHERICITY AXIS distribution at c.m. energy 189.0 GeV.

RAPIDITY W.R.T. SPHERICITY AXIS distribution at c.m. energy 196.0 GeV.

RAPIDITY W.R.T. SPHERICITY AXIS distribution at c.m. energy 200.0 GeV.

RAPIDITY W.R.T. SPHERICITY AXIS distribution at c.m. energy 206.0 GeV.

Combined results for ALPHAS.

Event shape means.

THRUST distribution at c.m. energy 91.20 GeV.

1-THRUST distribution at c.m. energy 133.00 GeV.

1-THRUST distribution at c.m. energy 161.00 GeV.

1-THRUST distribution at c.m. energy 172.00 GeV.

1-THRUST distribution at c.m. energy 183.00 GeV.

1-THRUST distribution at c.m. energy 189.00 GeV.

1-THRUST distribution at c.m. energy 200.00 GeV.

1-THRUST distribution at c.m. energy 206.00 GeV.

Heavy Jet Mass (RHO) distribution at c.m. energy 91.20 GeV.

Heavy Jet Mass (RHO) distribution at c.m. energy 133.00 GeV.

Heavy Jet Mass (RHO) distribution at c.m. energy 161.00 GeV.

Heavy Jet Mass (RHO) distribution at c.m. energy 172.00 GeV.

Heavy Jet Mass (RHO) distribution at c.m. energy 183.00 GeV.

Heavy Jet Mass (RHO) distribution at c.m. energy 189.00 GeV.

Heavy Jet Mass (RHO) distribution at c.m. energy 200.00 GeV.

Heavy Jet Mass (RHO) distribution at c.m. energy 206.00 GeV.

Total jet broadening distribution at c.m. energy 91.20 GeV.

Total jet broadening distribution at c.m. energy 133.00 GeV.

Total jet broadening distribution at c.m. energy 161.00 GeV.

Total jet broadening distribution at c.m. energy 172.00 GeV.

Total jet broadening distribution at c.m. energy 183.00 GeV.

Total jet broadening distribution at c.m. energy 189.00 GeV.

Total jet broadening distribution at c.m. energy 200.00 GeV.

Total jet broadening distribution at c.m. energy 206.00 GeV.

Wide jet broadening distribution at c.m. energy 91.20 GeV.

Wide jet broadening distribution at c.m. energy 133.00 GeV.

Wide jet broadening distribution at c.m. energy 161.00 GeV.

Wide jet broadening distribution at c.m. energy 172.00 GeV.

Wide jet broadening distribution at c.m. energy 183.00 GeV.

Wide jet broadening distribution at c.m. energy 189.00 GeV.

Wide jet broadening distribution at c.m. energy 200.00 GeV.

Wide jet broadening distribution at c.m. energy 206.00 GeV.

C-PARAMETER distribution at c.m. energy 91.20 GeV.

C-PARAMETER distribution at c.m. energy 133.00 GeV.

C-PARAMETER distribution at c.m. energy 161.00 GeV.

C-PARAMETER distribution at c.m. energy 172.00 GeV.

C-PARAMETER distribution at c.m. energy 183.00 GeV.

C-PARAMETER distribution at c.m. energy 189.00 GeV.

C-PARAMETER distribution at c.m. energy 200.00 GeV.

C-PARAMETER distribution at c.m. energy 206.00 GeV.

Thrust Major distribution at c.m. energy 91.20 GeV.

Thrust Major distribution at c.m. energy 133.00 GeV.

Thrust Major distribution at c.m. energy 161.00 GeV.

Thrust Major distribution at c.m. energy 172.00 GeV.

Thrust Major distribution at c.m. energy 183.00 GeV.

Thrust Major distribution at c.m. energy 189.00 GeV.

Thrust Major distribution at c.m. energy 200.00 GeV.

Thrust Major distribution at c.m. energy 206.00 GeV.

Thrust Minor distribution at c.m. energy 91.20 GeV.

Thrust Minor distribution at c.m. energy 133.00 GeV.

Thrust Minor distribution at c.m. energy 161.00 GeV.

Thrust Minor distribution at c.m. energy 172.00 GeV.

Thrust Minor distribution at c.m. energy 183.00 GeV.

Thrust Minor distribution at c.m. energy 189.00 GeV.

Thrust Minor distribution at c.m. energy 200.00 GeV.

Thrust Minor distribution at c.m. energy 206.00 GeV.

Jet Mass Difference distribution at c.m. energy 91.20 GeV.

Jet Mass Difference distribution at c.m. energy 133.00 GeV.

Jet Mass Difference distribution at c.m. energy 161.00 GeV.

Jet Mass Difference distribution at c.m. energy 172.00 GeV.

Jet Mass Difference distribution at c.m. energy 183.00 GeV.

Jet Mass Difference distribution at c.m. energy 189.00 GeV.

Jet Mass Difference distribution at c.m. energy 200.00 GeV.

Jet Mass Difference distribution at c.m. energy 206.00 GeV.

Aplanarity distribution at c.m. energy 91.20 GeV.

Aplanarity distribution at c.m. energy 133.00 GeV.

Aplanarity distribution at c.m. energy 161.00 GeV.

Aplanarity distribution at c.m. energy 172.00 GeV.

Aplanarity distribution at c.m. energy 183.00 GeV.

Aplanarity distribution at c.m. energy 189.00 GeV.

Aplanarity distribution at c.m. energy 200.00 GeV.

Aplanarity distribution at c.m. energy 206.00 GeV.

Planarity distribution at c.m. energy 133.00 GeV.

Planarity distribution at c.m. energy 161.00 GeV.

Planarity distribution at c.m. energy 172.00 GeV.

Planarity distribution at c.m. energy 183.00 GeV.

Planarity distribution at c.m. energy 189.00 GeV.

Planarity distribution at c.m. energy 200.00 GeV.

Planarity distribution at c.m. energy 206.00 GeV.

Oblateness distribution at c.m. energy 91.20 GeV.

Oblateness distribution at c.m. energy 133.00 GeV.

Oblateness distribution at c.m. energy 161.00 GeV.

Oblateness distribution at c.m. energy 172.00 GeV.

Oblateness distribution at c.m. energy 183.00 GeV.

Oblateness distribution at c.m. energy 189.00 GeV.

Oblateness distribution at c.m. energy 200.00 GeV.

Oblateness distribution at c.m. energy 206.00 GeV.

Sphericity distribution at c.m. energy 91.20 GeV.

Sphericity distribution at c.m. energy 133.00 GeV.

Sphericity distribution at c.m. energy 161.00 GeV.

Sphericity distribution at c.m. energy 172.00 GeV.

Sphericity distribution at c.m. energy 183.00 GeV.

Sphericity distribution at c.m. energy 189.00 GeV.

Sphericity distribution at c.m. energy 200.00 GeV.

Sphericity distribution at c.m. energy 206.00 GeV.

LN(Y12) distribution at c.m. energy 91.20 GeV.

LN(Y12) distribution at c.m. energy 133.00 GeV.

LN(Y12) distribution at c.m. energy 161.00 GeV.

LN(Y12) distribution at c.m. energy 172.00 GeV.

LN(Y12) distribution at c.m. energy 183.00 GeV.

LN(Y12) distribution at c.m. energy 189.00 GeV.

LN(Y12) distribution at c.m. energy 200.00 GeV.

LN(Y12) distribution at c.m. energy 206.00 GeV.

LN(Y23) distribution at c.m. energy 91.20 GeV.

LN(Y23) distribution at c.m. energy 133.00 GeV.

LN(Y23) distribution at c.m. energy 161.00 GeV.

LN(Y23) distribution at c.m. energy 172.00 GeV.

LN(Y23) distribution at c.m. energy 183.00 GeV.

LN(Y23) distribution at c.m. energy 189.00 GeV.

LN(Y23) distribution at c.m. energy 200.00 GeV.

LN(Y23) distribution at c.m. energy 206.00 GeV.

LN(Y34) distribution at c.m. energy 91.20 GeV.

LN(Y34) distribution at c.m. energy 133.00 GeV.

LN(Y34) distribution at c.m. energy 161.00 GeV.

LN(Y34) distribution at c.m. energy 172.00 GeV.

LN(Y34) distribution at c.m. energy 183.00 GeV.

LN(Y34) distribution at c.m. energy 189.00 GeV.

LN(Y34) distribution at c.m. energy 200.00 GeV.

LN(Y34) distribution at c.m. energy 206.00 GeV.

LN(Y45) distribution at c.m. energy 91.20 GeV.

LN(Y45) distribution at c.m. energy 133.00 GeV.

LN(Y45) distribution at c.m. energy 161.00 GeV.

LN(Y45) distribution at c.m. energy 172.00 GeV.

LN(Y45) distribution at c.m. energy 183.00 GeV.

LN(Y45) distribution at c.m. energy 189.00 GeV.

LN(Y45) distribution at c.m. energy 206.00 GeV.

LN(Y56) distribution at c.m. energy 91.20 GeV.

LN(Y56) distribution at c.m. energy 133.00 GeV.

LN(Y56) distribution at c.m. energy 161.00 GeV.

LN(Y56) distribution at c.m. energy 172.00 GeV.

LN(Y56) distribution at c.m. energy 183.00 GeV.

LN(Y56) distribution at c.m. energy 189.00 GeV.

LN(Y56) distribution at c.m. energy 206.00 GeV.

1-jet fraction at c.m. energy 91.20 GeV.

1-jet fraction at c.m. energy 133.00 GeV.

1-jet fraction at c.m. energy 161.00 GeV.

1-jet fraction at c.m. energy 172.00 GeV.

1-jet fraction at c.m. energy 183.00 GeV.

1-jet fraction at c.m. energy 189.00 GeV.

1-jet fraction at c.m. energy 200.00 GeV.

1-jet fraction at c.m. energy 206.00 GeV.

2-jet fraction at c.m. energy 91.20 GeV.

2-jet fraction at c.m. energy 133.00 GeV.

2-jet fraction at c.m. energy 161.00 GeV.

2-jet fraction at c.m. energy 172.00 GeV.

2-jet fraction at c.m. energy 183.00 GeV.

2-jet fraction at c.m. energy 189.00 GeV.

2-jet fraction at c.m. energy 200.00 GeV.

2-jet fraction at c.m. energy 206.00 GeV.

3-jet fraction at c.m. energy 91.20 GeV.

3-jet fraction at c.m. energy 133.00 GeV.

3-jet fraction at c.m. energy 161.00 GeV.

3-jet fraction at c.m. energy 172.00 GeV.

3-jet fraction at c.m. energy 183.00 GeV.

3-jet fraction at c.m. energy 189.00 GeV.

3-jet fraction at c.m. energy 200.00 GeV.

3-jet fraction at c.m. energy 206.00 GeV.

4-jet fraction at c.m. energy 91.20 GeV.

4-jet fraction at c.m. energy 133.00 GeV.

4-jet fraction at c.m. energy 161.00 GeV.

4-jet fraction at c.m. energy 172.00 GeV.

4-jet fraction at c.m. energy 183.00 GeV.

4-jet fraction at c.m. energy 189.00 GeV.

4-jet fraction at c.m. energy 200.00 GeV.

4-jet fraction at c.m. energy 206.00 GeV.

5-jet fraction at c.m. energy 91.20 GeV.

5-jet fraction at c.m. energy 133.00 GeV.

5-jet fraction at c.m. energy 161.00 GeV.

5-jet fraction at c.m. energy 172.00 GeV.

5-jet fraction at c.m. energy 183.00 GeV.

5-jet fraction at c.m. energy 189.00 GeV.

5-jet fraction at c.m. energy 200.00 GeV.

5-jet fraction at c.m. energy 206.00 GeV.

>=6-jet fraction at c.m. energy 91.20 GeV.

>=6-jet fraction at c.m. energy 133.00 GeV.

>=6-jet fraction at c.m. energy 161.00 GeV.

>=6-jet fraction at c.m. energy 172.00 GeV.

>=6-jet fraction at c.m. energy 183.00 GeV.

>=6-jet fraction at c.m. energy 189.00 GeV.

>=6-jet fraction at c.m. energy 200.00 GeV.

>=6-jet fraction at c.m. energy 206.00 GeV.

Differential cross section as a function of the ratio of the virtualities of the two photons.

Differential cross section as a function of the acolinearity angle PHI between the scattered electrons.

Differential cross section as a function of the acolinearity angle DEL(PHI) between the scattered electrons.

Differential cross section as a function of W of the hadronic system.

Differential cross section as a function of the Bjorken X.

Differential cross section as a function of the DIS Y variable.

Differential cross section as a function of LOG(S/S0).

The NC cross section DSIG/DX for Q**2 > 10000 GeV**2. There is an additional 1.5 PCT normalization uncertainty.

The CC cross section DSIG/DX for Q**2 > 1000 GeV**2. There is an additional 1.5 PCT normalization uncertainty.

The NC reduced cross section and the electromagnetic structure funcion F2 derived from the data. For Q**2 > 2000 GeV**2 the extraction of F2 is restricted to Y < 0.6.

The CC double differential cross section D2SIG/DX/DQ**2 and the structure function term PHI.

The NC E- P reduced cross section for the high-y analysis. All E- P data not previously reported in EPJ C19 (2001) 269 are given.. There is an additional 1.8 PCT normalization uncertainty.

The NC structure function term PHI and the structure function FL for the E-P data.

The NC structure function term PHI and the structure function FL for the E+P data.

The generalised structure function XF3.

The structure function XF3(C=GAMMA,Z) obtained by averaging over different Q**2 values and transforming to Q**2 = 1500 GeV**2.

Breakdown of errors from table 6, DSIG(C=NC)/DQ**2 as a function of Q**2. All errors are in PCT.

All errors are in PCT.

Breakdown of errors from table 8, DSIG(C=NC)/DX as a function of X. All errors are in PCT.

Breakdown of errors from table 9, DSIG(C=NC)/DX as a function of X. All errors are in PCT.

Breakdown of errors from table 10, DSIG(C=CC)/DX as a function of X. All errors are in PCT.

Breakdown of errors from table 11, F2 as a function of Q**2, X and Y. All errors are in PCT.

Breakdown of errors from table 11, F2 as a function of Q**2, X and Y. PHI(C=NC) is the NC structure function term.. Y+ = 1+(1-Y)**2. DEL(F2),DEL9F3) and DEL(FL) are the corrections to F2 as decribed in the text of the paper.

All errors are in PCT.

Breakdown of errors from table 12, SIG(C=REDUCED) as a function of Q**2 andX. All errors are in PCT.

The inelastic dijet cross section as a function of the ET gap.

The dijet cross sections as a function of the rapidity gap with the requirement that ET(C=GAP) is less than ET(C=CUT).

The dijet cross sections as a function of the rapidity gap with the requirement that ET(C=GAP) is less than ET(C=CUT).

The gap fraction defined as the fraction of all dijet events with ET(C= GAP)<ET(C=CUT).

The gap fraction defined as the fraction of all dijet events with ET(C= GAP)<ET(C=CUT).

The dijet cross sections as a function of X(C=GAMMA) with the requirement that ET(C=GAP) is less than ET(C=CUT).

The dijet cross sections as a function of X(C=GAMMA) with the requirement that ET(C=GAP) is less than ET(C=CUT).

The gap fraction defined as the fraction of all dijet events with ET(C= GAP)<ET(C=CUT).

The gap fraction defined as the fraction of all dijet events with ET(C= GAP)<ET(C=CUT).

The dijet cross sections as a function of XP with the requirement that ET(C=GAP) is less than ET(C=CUT).

The dijet cross sections as a function of XP with the requirement that ET(C=GAP) is less than ET(C=CUT).

The gap fraction defined as the fraction of all dijet events with ET(C= GAP)<ET(C=CUT).

The gap fraction defined as the fraction of all dijet events with ET(C= GAP)<ET(C=CUT).

Differential ep cross section for dijet production as a function of the average pseudorapidity the two jets in two transverse energy regions and in the Y region 0.1 to 0.5.

Differential ep cross section for dijet production as a function of the average pseudorapidity the two jets in two transverse energy regions and in the Y region 0.5 to 0.9.

Differential ep cross section for dijet production as a function of the photon momentum fraction X(C=GAMMA) in two regions of proton fractional momentum XP.

Differential ep cross section for dijet production as a function of the proton momentum fraction XP in two regions of photon fractional momentum X(C=GAMMA).

Differential ep cross section for dijet production as a function of the photon momentum fraction X(C=GAMMA) in two regions maximum jet transverseenergy.

Differential ep cross section for dijet production as a function of COS(THETA*) in two regions of fractional photon momentum fraction X(C=GAMMA).

Differential ep cross section for dijet production as a function of COS(THETA*) for dijet masses > 65 GeV in two regions of fractional photon momentum fraction X(C=GAMMA).