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.

Distribution of D(SIG)/DM(P=6) as a function of M(P=6) .

Distribution of D(SIG)/DBETA as a function of BETA .

Distribution of D(SIG)/DX(NAME=POMERON) as a function of X(NAME=POMERON) .

Distribution of D(SIG)/DET(P=4,5,RF=CM) as a function of ET(P=4,5,RF=CM) .

Distribution of D(SIG)/DETARAP(P=4,5,RF=CM) as a function of ETARAP(P=4,5,RF=CM) .

Distribution of D(SIG)/DZ(NAME=POMERON) as a function of Z(NAME=POMERON) .

Distribution of D(SIG)/DX(NAME=GAMMA) as a function of X(NAME=GAMMA) .

Distribution of D2(SIG)/DZ(NAME=POMERON)/DET(P=4,RF=CM) as a function of Z(NAME=POMERON) for ET(P=4,RF=CM) from 5 to 6.5 GeV). .

Distribution of D2(SIG)/DZ(NAME=POMERON)/DET(P=4,RF=CM) as a function of Z(NAME=POMERON) for ET(P=4,RF=CM) from 6.5 to 8 GeV). .

Distribution of D2(SIG)/DZ(NAME=POMERON)/DET(P=4,RF=CM) as a function of Z(NAME=POMERON) for ET(P=4,RF=CM) from 8 to 16 GeV). .

Distribution of D2(SIG)/DZ(NAME=POMERON)/DQ**2) as a function of Z(NAME=POMERON) for Q**2 from 5 to 12 GeV**2). .

Distribution of D2(SIG)/DZ(NAME=POMERON)/DQ**2) as a function of Z(NAME=POMERON) for Q**2 from 12 to 25 GeV**2). .

Distribution of D2(SIG)/DZ(NAME=POMERON)/DQ**2) as a function of Z(NAME=POMERON) for Q**2 from 25 to 50 GeV**2). .

Distribution of D2(SIG)/DZ(NAME=POMERON)/DQ**2) as a function of Z(NAME=POMERON) for Q**2 from 50 to 100 GeV**2). .

Differential cross section DSIG/DETARAP(P=4) in bins of ETARAP(P=4) .

Differential cross section DSIG/D(ETARAP(P=5)-ETARAP(P=6)) in bins of ETARAP(P=5)-ETARAP(P=6) .

Differential cross section DSIG/D(ETARAP(P=5)-ETARAP(P=6)) in bins of ETARAP(P=4)-ETARAP(P=5) .

Differential cross section DSIG/D(ETARAP(P=5)-ETARAP(P=6)) in bins of ETARAP(P=4)-ETARAP(P=5) .

Differential cross section DSIG/D(ETARAP(P=5)-ETARAP(P=6)) in bins of ETARAP(P=4)-ETARAP(P=5) .

Differential cross section D3SIG/DQ**2/DET(P=4)**2/DETARAP(P=4) in bins of ETARAP(P=4) for Q**2 from 20 TO 40 GeV*2 and ET(P=4)**2 range from 25 to 35 GeV**2 .

Differential cross section D3SIG/DQ**2/DET(P=4)**2/DETARAP(P=4) in bins of ETARAP(P=4) for Q**2 from 20 TO 40 GeV*2 and ET(P=4)**2 range from 36 to 100 GeV**2 .

Differential cross section D3SIG/DQ**2/DET(P=4)**2/DETARAP(P=4) in bins of ETARAP(P=4) for Q**2 from 20 TO 40 GeV*2 and ET(P=4)**2 range from 100 to 400 GeV**2 .

Differential cross section D3SIG/DQ**2/DET(P=4)**2/DETARAP(P=4) in bins of ETARAP(P=4) for Q**2 from 40 to 100 GeV*2 and ET(P=4)**2 range from 25 to 35 GeV**2 .

Differential cross section D3SIG/DQ**2/DET(P=4)**2/DETARAP(P=4) in bins of ETARAP(P=4) for Q**2 from 40 to 100 GeV*2 and ET(P=4)**2 range from 36 to 100 GeV**2 .

Differential cross section D3SIG/DQ**2/DET(P=4)**2/DETARAP(P=4) in bins of ETARAP(P=4) for Q**2 from 40 to 100 GeV*2 and ET(P=4)**2 range from 100 to 400 GeV**2 .

Cross section D(SIG)/X(C=GAMMA,OBS) as a function of X(C=GAMMA,OBS) in two jet invariant mass regions, 25 to 50 and > 50 GeV .

Cross section D(SIG)/Y as a function of Y in two jet invariant mass regions, 25 to 50 and > 50 GeV .

Cross section D(SIG)/Y as a function of Y in two jet invariant mass regions, 25 to 50 and > 50 GeV .

Cross section D(SIG)/ET(P=4) as a function of ET(P=4) in two jet invariant mass regions, 25 to 50 and > 50 GeV .

Cross section D(SIG)/ET(P=5) as a function of ET(P=5) in two jet invariant mass regions, 25 to 50 and > 50 GeV .

Cross section D(SIG)/ET(P=6) as a function of ET(P=6) in two jet invariant mass regions, 25 to 50 and > 50 GeV .

Cross section D(SIG)/ET(P=4) as a function of ET(P=4) in two jet invariant mass regions, 25 to 50 and > 50 GeV .

Cross section D(SIG)/ET(P=5) as a function of ET(P=5) in two jet invariant mass regions, 25 to 50 and > 50 GeV .

Cross section D(SIG)/ET(P=6) as a function of ET(P=6) in two jet invariant mass regions, 25 to 50 and > 50 GeV .

Cross section D(SIG)/ET(P=7) as a function of ET(P=7) in two jet invariant mass regions, 25 to 50 and > 50 GeV .

Cross section D(SIG)/ETARAP(P=4) as a function of ETARAP(P=4) in two jet invariant mass regions, 25 to 50 and > 50 GeV .

Cross section D(SIG)/ETARAP(P=5) as a function of ETARAP(P=5) in two jet invariant mass regions, 25 to 50 and > 50 GeV .

Cross section D(SIG)/ETARAP(P=6) as a function of ETARAP(P=6) in two jet invariant mass regions, 25 to 50 and > 50 GeV .

Cross section D(SIG)/ETARAP(P=4) as a function of ETARAP(P=4) in two jet invariant mass regions, 25 to 50 and > 50 GeV .

Cross section D(SIG)/ETARAP(P=5) as a function of ETARAP(P=5) in two jet invariant mass regions, 25 to 50 and > 50 GeV .

Cross section D(SIG)/ETARAP(P=6) as a function of ETARAP(P=6) in two jet invariant mass regions, 25 to 50 and > 50 GeV .

Cross section D(SIG)/ETARAP(P=7) as a function of ETARAP(P=7) in two jet invariant mass regions, 25 to 50 and > 50 GeV .

Cross section D(SIG)/COS(PSI(3)) as a function of COS(PSI(3)) in two jet invariant mass regions, 25 to 50 and > 50 GeV . PSI(3) is the angle in the 3-jet CM frame between the plane containing the highest energy jet (P=4) and the beam, and the plane containing the three jets .

Cross section D(SIG)/ET(P=4) as a function of ET(P=4) for X(C=GAMMA,OBS) <= 0.75 .

Cross section D(SIG)/(ETARAP(P=4)+ETARAP(P=5))/2 as a function of (ETARAP(P=4)+ETARAP(P=5))/2 for X(C=GAMMA,OBS) > 0.75 .

Cross section D(SIG)/(ETARAP(P=4)+ETARAP(P=5))/2 as a function of (ETARAP(P=4)+ETARAP(P=5))/2 for X(C=GAMMA,OBS) <= 0.75 .

Cross section D(SIG)/X(C=P,OBS) as a function of X(C=P,OBS) for X(C=GAMMA,OBS) > 0.75 .

Cross section D(SIG)/X(C=P,OBS) as a function of X(C=P,OBS) for X(C=GAMMA,OBS) <= 0.75 .

Cross section D(SIG)/(PHI(P=4)-PHI(P=5))/2 as a function of (PHI(P=4)-PHI(P=5))/2 for X(C=GAMMA,OBS) > 0.75 .

Cross section D(SIG)/(PHI(P=4)-PHI(P=5))/2 as a function of (PHI(P=4)-PHI(P=5))/2 for X(C=GAMMA,OBS) <= 0.75 .

Cross section D(SIG)/X(C=P,OBS) as a function of X(C=P,OBS) for X(C=GAMMA,OBS) > 0.75 for the High X(C=GAMMA,OBS) 1 optimized set.

Cross section D(SIG)/X(C=P,OBS) as a function of X(C=P,OBS) for X(C=GAMMA,OBS) > 0.75 for the High X(C=GAMMA,OBS) 2 optimized set.

Cross section D(SIG)/X(C=P,OBS) as a function of X(C=P,OBS) for X(C=GAMMA,OBS) > 0.75 for the High X(C=GAMMA,OBS) 3 optimized set.

Cross section D(SIG)/X(C=P,OBS) as a function of X(C=P,OBS) for X(C=GAMMA,OBS) > 0.75 for the High X(C=GAMMA,OBS) 4 optimized set.

Cross section D(SIG)/X(C=P,OBS) as a function of X(C=P,OBS) for X(C=GAMMA,OBS) <= 0.75 for the Low X(C=GAMMA,OBS) 1 optimized set.

Cross section D(SIG)/X(C=P,OBS) as a function of X(C=P,OBS) for X(C=GAMMA,OBS) <= 0.75 for the Low X(C=GAMMA,OBS) 2 optimized set.

Cross section D(SIG)/X(C=P,OBS) as a function of X(C=P,OBS) for X(C=GAMMA,OBS) <= 0.75 for the Low X(C=GAMMA,OBS) 3 optimized set.

Cross section D(SIG)/X(C=P,OBS) as a function of X(C=P,OBS) for X(C=GAMMA,OBS) <= 0.75 for the Low X(C=GAMMA,OBS) 4 optimized set.

Cross section D(SIG)/X(C=GAMMA,OBS) as a function of X(C=GAMMA,OBS) .

Production cross section for D/S+ mesons.

Measured differential cross sections for D0 (not coming from D*+ decay) and D+.

Measured differential cross sections for D0 (not coming from D*+ decay) and D+.

Measured differential cross sections for D0 (not coming from D*+ decay) and D+.

Measured differential cross sections for D0 (not coming from D*+ decay) and D+.

Measured differential cross sections for D/S+.

Measured differential cross sections for D/S+.

Measured differential cross sections for D/S+.

Measured differential cross sections for D/S+.

Measured cross sections for D0 not coming fom a D*+ decay, and D+ as a function of Y.

Measured cross sections for D0 not coming fom a D*+ decay, and D+ as a function of Y.

Measured cross sections for D0 not coming fom a D*+ decay, and D+ as a function of Y.

Measured cross sections for D/S+ as a function of Y.

Measured cross sections for D/S+ as a function of Y.

Measured cross sections for D/S+ as a function of Y.

The extracted values of F2(CC) from the production cross section of D0 (not coming from D*+ decay), D_ and D/S+.

The extracted values of F2(CC) from the production cross section of D0 (not coming from D*+ decay), D_ and D/S+.

The extracted values of F2(CC) from the production cross section of D0 (not coming from D*+ decay), D_ and D/S+.

The extracted values of F2(CC) from a combination of the production cross section of D0 (not coming from D*+ decay), D_ and D/S+.

The extracted values of F2(CC) from a combination of the production cross section of D0 (not coming from D*+ decay), D_ and D/S+.

The extracted values of F2(CC) from a combination of the production cross section of D0 (not coming from D*+ decay), D_ and D/S+.