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 $p_{\mathrm{T}}^{e\mu}$

Differential polarized inclusive jet cross sections as a function of jet transverse energy.

Differential polarized inclusive jet cross sections as a function of photon virtuality, Q**2.

Differential polarized inclusive jet cross sections as a function of photon virtuality, Q**2.

Differential polarized inclusive jet cross sections as a function of X. Update: contrary to the publication, this is D(SIG)/DLOG10(X) not D(SIG)/DX.

Differential polarized inclusive jet cross sections as a function of X. Update: contrary to the publication, this is D(SIG)/DLOG10(X) not D(SIG)/DX.

Integrated polarized inclusive-jet cross section in the given kinematical range for the E- beam.

Integrated polarized inclusive-jet cross section in the given kinematical range for the E+ beam.

Differential unpolarized cross section for single jet production as a function of the jet pseudorapidity.

Differential unpolarized cross section for two jet production as a function of the mean jet pseudorapidity.

Differential unpolarized cross section for three jet production as a function of the mean jet pseudorapidity.

Differential unpolarized cross section for single jet production as a function of the jet transverse energy.

Differential unpolarized cross section for two jet production as a function of the mean jet transverse energy.

Differential unpolarized cross section for three jet production as a function of the mean jet transverse energy.

Differential unpolarized cross section for single jet production as a function of photon virtuality, Q**2.

Differential unpolarized cross section for two jet production as a function of photon virtuality, Q**2.

Differential unpolarized cross section for three jet production as a function of photon virtuality, Q**2.

Differential unpolarized inclusive-jet cross section as a function of X. Update: contrary to the publication, this is D(SIG)/DLOG10(X) not D(SIG)/DX.

Integrated unpolarized jet cross section in the given kinemetical region.

Differential unpolarized dijet cross section as a function of the dijet mass.

Differential unpolarized three-jet cross section as a function of the three-jet mass.

Data from Figure 3b on charged pion production. Data correspond to charged particle production, corrected to the contribution from (PI+ + PI-)/2.

Data from Figure 3b on charged pion production. Data correspond to charged particle production, corrected to the contribution from (PI+ + PI-)/2.

Data from Figure 3c on charged pion production. Data correspond to charged particle production, corrected to the contribution from (PI+ + PI-)/2.

Data from Figure 3d on charged pion production. Data correspond to charged particle production, corrected to the contribution from (PI+ + PI-)/2.

Data from Figure 4a on forward jet production differential in x, low PT

Data from Figure 4a on forward jet production differential in x, high PT

Data from Figure 5a on forward jet production differential in delta(phi), low x

Data from Figure 5b on forward jet production differential in delta(phi), high x

Inclusive dijet cross-sections ${d\sigma/dM_{jj}}$. Other details as in the caption to Table 1.

Inclusive dijet cross-sections ${d\sigma/d\eta^{*}}$. Other details as in the caption to Table 1.

Inclusive dijet cross-sections ${d\sigma/d\log_{10}\left(\xi\right)}$. Other details as in the caption to Table 1.

Inclusive dijet cross-sections ${d\sigma/d\log_{10}\left(\xi\right)}$ for ${Q^{2}}$ between 125 and 250 GeV$^2$. Other details as in the caption to Table 1.

Inclusive dijet cross-sections ${d\sigma/d\log_{10}\left(\xi\right)}$ for ${Q^{2}}$ between 250 and 500 GeV$^2$. Other details as in the caption to Table 1.

Inclusive dijet cross-sections ${d\sigma/d\log_{10}\left(\xi\right)}$ for ${Q^{2}}$ between 500 and 1000 GeV$^2$. Other details as in the caption to Table 1.

Inclusive dijet cross-sections ${d\sigma/d\log_{10}\left(\xi\right)}$ for ${Q^{2}}$ between 1000 and 2000 GeV$^2$. Other details as in the caption to Table 1.

Inclusive dijet cross-sections ${d\sigma/d\log_{10}\left(\xi\right)}$ for ${Q^{2}}$ between 2000 and 5000 GeV$^2$. Other details as in the caption to Table 1.

Inclusive dijet cross-sections ${d\sigma/d\log_{10}\left(\xi\right)}$ for ${Q^{2}}$ between 5000 and 20000 GeV$^2$. Other details as in the caption to Table 1.

Inclusive dijet cross-sections ${d\sigma/d\overline{E^{jet}_{T,B}}}$ for ${Q^{2}}$ between 125 and 250 GeV$^2$. Other details as in the caption to Table 1.

Inclusive dijet cross-sections ${d\sigma/d\overline{E^{jet}_{T,B}}}$ for ${Q^{2}}$ between 250 and 500 GeV$^2$. Other details as in the caption to Table 1.

Inclusive dijet cross-sections ${d\sigma/d\overline{E^{jet}_{T,B}}}$ for ${Q^{2}}$ between 500 and 1000 GeV$^2$. Other details as in the caption to Table 1.

Inclusive dijet cross-sections ${d\sigma/d\overline{E^{jet}_{T,B}}}$ for ${Q^{2}}$ between 1000 and 2000 GeV$^2$. Other details as in the caption to Table 1.

Inclusive dijet cross-sections ${d\sigma/d\overline{E^{jet}_{T,B}}}$ for ${Q^{2}}$ between 2000 and 5000 GeV$^2$. Other details as in the caption to Table 1.

Inclusive dijet cross-sections ${d\sigma/d\overline{E^{jet}_{T,B}}}$ for ${Q^{2}}$ between 5000 and 20000 GeV$^2$. Other details as in the caption to Table 1.

Total visible cross section for LAMBDA/C+ production for the two decay channels combined. The second systematic error reflects the uncertainty in the branching ratios.

Measured D+ cross section as a function of the D+ transverse momentum.

Measured D+ cross section as a function of the D+ pseudorapidity.

Measured D+ cross section as a function of Q**2.

Measured D+ cross section as a function of the Bjorken X.

Differential cross section w.r.t. the muon transverse momentum.

Differential cross section w.r.t. the muon pseudorapidity.

Differential cross section w.r.t. the JET transverse energy.

Measured differential cross section DSIG/DQ**2.

Measured differential cross section DSIG/DX.

Pseudorapidity distribution with additional kinematical restraints on Q**2 and ET.

Double differential cross sections as a funtion of PT**2 for the XL range 0.50 TO 0.56. The methods S123 and S456 are the results using different stations of the silicon microstrip detectors.

Double differential cross sections as a funtion of PT**2 for the XL range 0.56 TO 0.62. The methods S123 and S456 are the results using different stations of the silicon microstrip detectors.

Double differential cross sections as a funtion of PT**2 for the XL range 0.62 TO 0.65. The methods S123 and S456 are the results using different stations of the silicon microstrip detectors.

Double differential cross sections as a funtion of PT**2 for the XL range 0.65 TO 0.68. The methods S123 and S456 are the results using different stations of the silicon microstrip detectors.

Double differential cross sections as a funtion of PT**2 for the XL range 0.68 TO 0.71. The methods S123 and S456 are the results using different stations of the silicon microstrip detectors.

Double differential cross sections as a funtion of PT**2 for the XL range 0.71 TO 0.74. The methods S123 and S456 are the results using different stations of the silicon microstrip detectors.

Double differential cross sections as a funtion of PT**2 for the XL range 0.74 TO 0.77. The methods S123 and S456 are the results using different stations of the silicon microstrip detectors.

Double differential cross sections as a funtion of PT**2 for the XL range 0.77 TO 0.80. The methods S123 and S456 are the results using different stations of the silicon microstrip detectors.

Double differential cross sections as a funtion of PT**2 for the XL range 0.80 TO 0.83. The methods S123 and S456 are the results using different stations of the silicon microstrip detectors.

Double differential cross sections as a funtion of PT**2 for the XL range 0.83 TO 0.86. The methods S123 and S456 are the results using different stations of the silicon microstrip detectors.

Double differential cross sections as a funtion of PT**2 for the XL range 0.86 TO 0.89. The methods S123 and S456 are the results using different stations of the silicon microstrip detectors.

Double differential cross sections as a funtion of PT**2 for the XL range 0.89 TO 0.92. The methods S123 and S456 are the results using different stations of the silicon microstrip detectors.

Double differential cross sections as a funtion of PT**2 for the XL range 0.92 TO 0.95. The methods S123 and S456 are the results using different stations of the silicon microstrip detectors.

Double differential cross sections as a funtion of PT**2 for the XL range 0.95 TO 0.98. The methods S123 and S456 are the results using different stations of the silicon microstrip detectors.

Double differential cross sections as a funtion of PT**2 for the XL range 0.98 TO 1.00. The methods S123 and S456 are the results using different stations of the silicon microstrip detectors.

Leading proton production rate as a funtion of XL in 3 PT**2 ranges.

Leading proton production rate as a funtion of XL for the PT**2 region < 0.5 GeV**2.

Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 9.6E-5 and mean Q**2 of 4.2 GeV**2.

Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 1.7E-4 and mean Q**2 of 4.2 GeV**2.

Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 3.5E-4 and mean Q**2 of 4.2 GeV**2.

Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 6.9E-4 and mean Q**2 of 4.2 GeV**2.

Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 1.46E-3 and mean Q**2 of 4.2 GeV**2.

Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 1.9E-4 and mean Q**2 of 7.3 GeV**2.

Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 3.4E-4 and mean Q**2 of 7.3 GeV**2.

Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 6.9E-4 and mean Q**2 of 7.3 GeV**2.

Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 1.36E-3 and mean Q**2 of 7.3 GeV**2.

Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 2.67E-3 and mean Q**2 of 7.3 GeV**2.

Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 2.6E-4 and mean Q**2 of 11 GeV**2.

Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 4.6E-4 and mean Q**2 of 11 GeV**2.

Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 9.2E-4 and mean Q**2 of 11 GeV**2.

Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 1.83E-3 and mean Q**2 of 11 GeV**2.

Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 3.98E-3 and mean Q**2 of 11 GeV**2.

Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 5.1E-4 and mean Q**2 of 22 GeV**2.

Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 9.2E-4 and mean Q**2 of 22 GeV**2.

Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 1.84E-3 and mean Q**2 of 22 GeV**2.

Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 3.66E-3 and mean Q**2 of 22 GeV**2.

Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 7.83E-3 and mean Q**2 of 22 GeV**2.

Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 1.03E-3 and mean Q**2 of 44 GeV**2.

Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 1.86E-3 and mean Q**2 of 44 GeV**2.

Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 3.68E-3 and mean Q**2 of 44 GeV**2.

Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 7.33E-3 and mean Q**2 of 44 GeV**2.

Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 1.54E-2 and mean Q**2 of 44 GeV**2.

Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 2.00E-3 and mean Q**2 of 88 GeV**2.

Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 3.59E-3 and mean Q**2 of 88 GeV**2.

Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 7.37E-3 and mean Q**2 of 88 GeV**2.

Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 1.42E-2 and mean Q**2 of 88 GeV**2.

Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 3.01E-2 and mean Q**2 of 88 GeV**2.

Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 4.00E-3 and mean Q**2 of 237 GeV**2.

Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 7.52E-3 and mean Q**2 of 237 GeV**2.

Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 1.47E-2 and mean Q**2 of 237 GeV**2.

Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 3.25E-2 and mean Q**2 of 237 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.

Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.

Leading proton production rate as a function of X in Q**2 bins for protons with XL in the range 0.32 to 0.92 and PT**2 < 0.5 GeV**2.

Leading proton production rate as a function of X in Q**2 bins for protons with XL in the range 0.32 to 0.92 and PT**2 < 0.5 GeV**2.

Leading proton production rate as a function of X in Q**2 bins for protons with XL in the range 0.32 to 0.92 and PT**2 < 0.5 GeV**2.

Leading proton production rate as a function of X in Q**2 bins for protons with XL in the range 0.32 to 0.92 and PT**2 < 0.5 GeV**2.

Leading proton production rate as a function of X in Q**2 bins for protons with XL in the range 0.32 to 0.92 and PT**2 < 0.5 GeV**2.

Leading proton production rate as a function of X in Q**2 bins for protons with XL in the range 0.32 to 0.92 and PT**2 < 0.5 GeV**2.

Leading proton production rate as a function of X in Q**2 bins for protons with XL in the range 0.32 to 0.92 and PT**2 < 0.5 GeV**2.

Leading proton production rate, averaged over X, as a function of Q**2 for protons with PT**2 < 0.5 GeV**2 in two XL ranges.

Leading proton production structure function F2(C=Lp) as a fujnction of X in Q**2 bins for protons with XL in the range 0.32 to 0.92 and PT**2 < 0.5 GeV**2.

Leading proton production structure function F2(C=Lp) as a fujnction of X in Q**2 bins for protons with XL in the range 0.32 to 0.92 and PT**2 < 0.5 GeV**2.

Leading proton production structure function F2(C=Lp) as a fujnction of X in Q**2 bins for protons with XL in the range 0.32 to 0.92 and PT**2 < 0.5 GeV**2.

Leading proton production structure function F2(C=Lp) as a fujnction of X in Q**2 bins for protons with XL in the range 0.32 to 0.92 and PT**2 < 0.5 GeV**2.

Leading proton production structure function F2(C=Lp) as a fujnction of X in Q**2 bins for protons with XL in the range 0.32 to 0.92 and PT**2 < 0.5 GeV**2.

Leading proton production structure function F2(C=Lp) as a fujnction of X in Q**2 bins for protons with XL in the range 0.32 to 0.92 and PT**2 < 0.5 GeV**2.

Leading proton production structure function F2(C=Lp) as a fujnction of X in Q**2 bins for protons with XL in the range 0.32 to 0.92 and PT**2 < 0.5 GeV**2.

Measured D+- cross section as a function of X.

Measured D+- cross section as a function of the transverse momentum of the D meson.

Measured D+- cross section as a function of the pseudorapidity of the D meson.

Measured D0/DBAR0 cross section as a function of Q**2.

Measured D0/DBAR0 cross section as a function of X.

Measured D0/DBAR0 cross section as a function of the transverse momentum of the D meson.

Measured D0/DBAR0 cross section as a function of the pseudorapidity of the D meson.

Measured cross section for D+- mesons in Q**2 and Y bins.

Measured cross section for D0/DBAR0 mesons in Q**2 and Y bins.

The extracted values of the F2(NAME=CHARM) structure function from the production cross section of D+- mesons.. The second systematic error is from the extrapolation to the full phase space.

The extracted values of the F2(NAME=CHARM) structure function from the production cross section of D+- mesons.. The second systematic error is from the extrapolation to the full phase space.

The extracted values of the F2(NAME=CHARM) structure function from the production cross section of D+- mesons.. The second systematic error is from the extrapolation to the full phase space.

The extracted values of the F2(NAME=CHARM) structure function from the production cross section of D0/DBAR0 mesons not coming from D*+- decays.. The second systematic error is from the extrapolation to the full phase space.

The extracted values of the F2(NAME=CHARM) structure function from the production cross section of D0/DBAR0 mesons not coming from D*+- decays.. The second systematic error is from the extrapolation to the full phase space.

The extracted values of the F2(NAME=CHARM) structure function from the production cross section of D0/DBAR0 mesons not coming from D*+- decays.. The second systematic error is from the extrapolation to the full phase space.

The combined F2(NAME=CHARM) structure function from the production cross section of D+- and D0/DBAR0 mesons.. The second systematic error is from the extrapolation to the full phase space.. The additional error from the branching ratio is 3.3 PCT.

The combined F2(NAME=CHARM) structure function from the production cross section of D+- and D0/DBAR0 mesons.. The second systematic error is from the extrapolation to the full phase space.. The additional error from the branching ratio is 3.3 PCT.

The combined F2(NAME=CHARM) structure function from the production cross section of D+- and D0/DBAR0 mesons.. The second systematic error is from the extrapolation to the full phase space.. The additional error from the branching ratio is 3.3 PCT.

Differential cross section DSIG/DX for the two values of longitudinal polarization of the electron beam.

Differential cross section DSIG/DY for the two values of longitudinal polarization of the electron beam.

Values of the differential cross section DSIG/DQ**2 with detailed statistical and systematic errors.. The first DSYS is the uncorrelated systematic error and the second is the calorimeter energy scale uncertainty which has significant correlation between cross section bins.

Values of the differential cross section DSIG/DX with detailed statistical and systematic errors.. The first DSYS is the uncorrelated systematic error and the second is the calorimeter energy scale uncertainty which has significant correlation between cross section bins.

Values of the differential cross section DSIG/DY with detailed statistical and systematic errors.. The first DSYS is the uncorrelated systematic error and the second is the calorimeter energy scale uncertainty which has significant correlation between cross section bins.

Values of the differential cross section DSIG/DQ**2 with detailed statistical and systematic errors.. The first DSYS is the uncorrelated systematic error and the second is the calorimeter energy scale uncertainty which has significant correlation between cross section bins.

Values of the differential cross section DSIG/DX with detailed statistical and systematic errors.. The first DSYS is the uncorrelated systematic error and the second is the calorimeter energy scale uncertainty which has significant correlation between cross section bins.

Values of the differential cross section DSIG/DY with detailed statistical and systematic errors.. The first DSYS is the uncorrelated systematic error and the second is the calorimeter energy scale uncertainty which has significant correlation between cross section bins.

Values of the reduced cross section for 3 values of longitudinal polarization of the electron beam for Q**2 = 280 GeV**2.

Values of the reduced cross section for 3 values of longitudinal polarization of the electron beam for Q**2 = 530 GeV**2.

Values of the reduced cross section for 3 values of longitudinal polarization of the electron beam for Q**2 = 950 GeV**2.

Values of the reduced cross section for 3 values of longitudinal polarization of the electron beam for Q**2 = 1700 GeV**2.

Values of the reduced cross section for 3 values of longitudinal polarization of the electron beam for Q**2 = 3000 GeV**2.

Values of the reduced cross section for 3 values of longitudinal polarization of the electron beam for Q**2 = 5300 GeV**2.

Values of the reduced cross section for 3 values of longitudinal polarization of the electron beam for Q**2 = 9500 GeV**2.

Values of the reduced cross section for 3 values of longitudinal polarization of the electron beam for Q**2 = 17000 GeV**2.

Values of the reduced cross section for 3 values of longitudinal polarization of the electron beam for Q**2 = 30000 GeV**2.

Values of the reduced cross section with detailed statistical and systematic errors.. The first DSYS is the uncorrelated systematic error and the second is the calorimeter energy scale uncertainty which has significant correlationS between cross section bins.

Values of the reduced cross section with detailed statistical and systematic errors.. The first DSYS is the uncorrelated systematic error and the second is the calorimeter energy scale uncertainty which has significant correlationS between cross section bins.

Values of the reduced cross section with detailed statistical and systematic errors.. The first DSYS is the uncorrelated systematic error and the second is the calorimeter energy scale uncertainty which has significant correlationS between cross section bins.

Values of the reduced cross section with detailed statistical and systematic errors.. The first DSYS is the uncorrelated systematic error and the second is the calorimeter energy scale uncertainty which has significant correlationS between cross section bins.

Values of the reduced cross section with detailed statistical and systematic errors.. The first DSYS is the uncorrelated systematic error and the second is the calorimeter energy scale uncertainty which has significant correlationS between cross section bins.

Values of the reduced cross section with detailed statistical and systematic errors.. The first DSYS is the uncorrelated systematic error and the second is the calorimeter energy scale uncertainty which has significant correlationS between cross section bins.

Values of the reduced cross section with detailed statistical and systematic errors.. The first DSYS is the uncorrelated systematic error and the second is the calorimeter energy scale uncertainty which has significant correlationS between cross section bins.

Values of the reduced cross section with detailed statistical and systematic errors.. The first DSYS is the uncorrelated systematic error and the second is the calorimeter energy scale uncertainty which has significant correlationS between cross section bins.

Values of the reduced cross section with detailed statistical and systematic errors.. The first DSYS is the uncorrelated systematic error and the second is the calorimeter energy scale uncertainty which has significant correlationS between cross section bins.

Values of the reduced cross section with detailed statistical and systematic errors.. The first DSYS is the uncorrelated systematic error and the second is the calorimeter energy scale uncertainty which has significant correlationS between cross section bins.

Values of the reduced cross section with detailed statistical and systematic errors.. The first DSYS is the uncorrelated systematic error and the second is the calorimeter energy scale uncertainty which has significant correlationS between cross section bins.

Values of the reduced cross section with detailed statistical and systematic errors.. The first DSYS is the uncorrelated systematic error and the second is the calorimeter energy scale uncertainty which has significant correlationS between cross section bins.

Values of the reduced cross section with detailed statistical and systematic errors.. The first DSYS is the uncorrelated systematic error and the second is the calorimeter energy scale uncertainty which has significant correlationS between cross section bins.

Values of the reduced cross section with detailed statistical and systematic errors.. The first DSYS is the uncorrelated systematic error and the second is the calorimeter energy scale uncertainty which has significant correlationS between cross section bins.

Values of the reduced cross section with detailed statistical and systematic errors.. The first DSYS is the uncorrelated systematic error and the second is the calorimeter energy scale uncertainty which has significant correlationS between cross section bins.

Values of the reduced cross section with detailed statistical and systematic errors.. The first DSYS is the uncorrelated systematic error and the second is the calorimeter energy scale uncertainty which has significant correlationS between cross section bins.

Values of the reduced cross section with detailed statistical and systematic errors.. The first DSYS is the uncorrelated systematic error and the second is the calorimeter energy scale uncertainty which has significant correlationS between cross section bins.

Values of the reduced cross section with detailed statistical and systematic errors.. The first DSYS is the uncorrelated systematic error and the second is the calorimeter energy scale uncertainty which has significant correlationS between cross section bins.