The measured fiducial cross section vs $E_{\mathrm{T}}^\gamma$. The central values are provided along with the statistical and systematic uncertainties together with the sign information. The statistical and "Uncor" uncertainty should be treated as uncorrelated bin-to-bin, while the rest are correlated between bins, and they are written as signed NP variations. The parton-to-particle correction factor $C_{theory}$ is the ratio of the cross-section predicted by Sherpa LO samples at particle level within the fiducial phase-space region defined in Table 4 to the predicted cross-section at parton level within the same fiducial region but with the smooth-cone isolation prescription defined above replacing the particle-level photon isolation criterion, and with Born-level leptons in place of dressed leptons. This correction should be applied on fixed order parton-level calculations. The systematic uncertainty is evaluated from a comparison with the correction factor obtained using events generated with SHERPA 2.2.2 at NLO. In the case that the calculations are valid for dressed leptons, a modified correction factor excluding the Born-to-dressed lepton correction should be applied instead. This correction only takes into account the particle-level isolation criteria, and is provided separately here. The Sherpa 2.2.8 NLO cross-sections given below include a small contribution from EW $Z\gamma jj$ production.

The measured fiducial cross section vs $|\eta^\gamma|$. The central values are provided along with the statistical and systematic uncertainties together with the sign information. The statistical and "Uncor" uncertainty should be treated as uncorrelated bin-to-bin, while the rest are correlated between bins, and they are written as signed NP variations. The parton-to-particle correction factor $C_{theory}$ is the ratio of the cross-section predicted by Sherpa LO samples at particle level within the fiducial phase-space region defined in Table 4 to the predicted cross-section at parton level within the same fiducial region but with the smooth-cone isolation prescription defined above replacing the particle-level photon isolation criterion, and with Born-level leptons in place of dressed leptons. This correction should be applied on fixed order parton-level calculations. The systematic uncertainty is evaluated from a comparison with the correction factor obtained using events generated with Sherpa 2.2.2 at NLO. The uncertainty is defined as Max(stat error, systematic difference between Sherpa LO and Sherpa 2.2.2 NLO), and cannot be considered correlated bin-to-bin. In the case that the calculations are valid for dressed leptons, a modified correction factor excluding the Born-to-dressed lepton correction should be applied instead. This correction only takes into account the particle-level isolation criteria, and is provided separately here. The Sherpa 2.2.8 NLO cross-sections given below include a small contribution from EW $Z\gamma jj$ production.

The measured fiducial cross section vs $|\eta^\gamma|$. The central values are provided along with the statistical and systematic uncertainties together with the sign information. The statistical and "Uncor" uncertainty should be treated as uncorrelated bin-to-bin, while the rest are correlated between bins, and they are written as signed NP variations. The parton-to-particle correction factor $C_{theory}$ is the ratio of the cross-section predicted by Sherpa LO samples at particle level within the fiducial phase-space region defined in Table 4 to the predicted cross-section at parton level within the same fiducial region but with the smooth-cone isolation prescription defined above replacing the particle-level photon isolation criterion, and with Born-level leptons in place of dressed leptons. This correction should be applied on fixed order parton-level calculations. The systematic uncertainty is evaluated from a comparison with the correction factor obtained using events generated with SHERPA 2.2.2 at NLO. In the case that the calculations are valid for dressed leptons, a modified correction factor excluding the Born-to-dressed lepton correction should be applied instead. This correction only takes into account the particle-level isolation criteria, and is provided separately here. The Sherpa 2.2.8 NLO cross-sections given below include a small contribution from EW $Z\gamma jj$ production.

The measured fiducial cross section vs $m(\ell\ell\gamma)$. The central values are provided along with the statistical and systematic uncertainties together with the sign information. The statistical and "Uncor" uncertainty should be treated as uncorrelated bin-to-bin, while the rest are correlated between bins, and they are written as signed NP variations. The parton-to-particle correction factor $C_{theory}$ is the ratio of the cross-section predicted by Sherpa LO samples at particle level within the fiducial phase-space region defined in Table 4 to the predicted cross-section at parton level within the same fiducial region but with the smooth-cone isolation prescription defined above replacing the particle-level photon isolation criterion, and with Born-level leptons in place of dressed leptons. This correction should be applied on fixed order parton-level calculations. The systematic uncertainty is evaluated from a comparison with the correction factor obtained using events generated with Sherpa 2.2.2 at NLO. The uncertainty is defined as Max(stat error, systematic difference between Sherpa LO and Sherpa 2.2.2 NLO), and cannot be considered correlated bin-to-bin. In the case that the calculations are valid for dressed leptons, a modified correction factor excluding the Born-to-dressed lepton correction should be applied instead. This correction only takes into account the particle-level isolation criteria, and is provided separately here. The Sherpa 2.2.8 NLO cross-sections given below include a small contribution from EW $Z\gamma jj$ production.

The measured fiducial cross section vs $m(\ell\ell\gamma)$. The central values are provided along with the statistical and systematic uncertainties together with the sign information. The statistical and "Uncor" uncertainty should be treated as uncorrelated bin-to-bin, while the rest are correlated between bins, and they are written as signed NP variations. The parton-to-particle correction factor $C_{theory}$ is the ratio of the cross-section predicted by Sherpa LO samples at particle level within the fiducial phase-space region defined in Table 4 to the predicted cross-section at parton level within the same fiducial region but with the smooth-cone isolation prescription defined above replacing the particle-level photon isolation criterion, and with Born-level leptons in place of dressed leptons. This correction should be applied on fixed order parton-level calculations. The systematic uncertainty is evaluated from a comparison with the correction factor obtained using events generated with SHERPA 2.2.2 at NLO. In the case that the calculations are valid for dressed leptons, a modified correction factor excluding the Born-to-dressed lepton correction should be applied instead. This correction only takes into account the particle-level isolation criteria, and is provided separately here. The Sherpa 2.2.8 NLO cross-sections given below include a small contribution from EW $Z\gamma jj$ production.

The measured fiducial cross section vs $p_{\mathrm{T}}^{\ell\ell\gamma}$. The central values are provided along with the statistical and systematic uncertainties together with the sign information. The statistical and "Uncor" uncertainty should be treated as uncorrelated bin-to-bin, while the rest are correlated between bins, and they are written as signed NP variations. The parton-to-particle correction factor $C_{theory}$ is the ratio of the cross-section predicted by Sherpa LO samples at particle level within the fiducial phase-space region defined in Table 4 to the predicted cross-section at parton level within the same fiducial region but with the smooth-cone isolation prescription defined above replacing the particle-level photon isolation criterion, and with Born-level leptons in place of dressed leptons. This correction should be applied on fixed order parton-level calculations. The systematic uncertainty is evaluated from a comparison with the correction factor obtained using events generated with Sherpa 2.2.2 at NLO. The uncertainty is defined as Max(stat error, systematic difference between Sherpa LO and Sherpa 2.2.2 NLO), and cannot be considered correlated bin-to-bin. In the case that the calculations are valid for dressed leptons, a modified correction factor excluding the Born-to-dressed lepton correction should be applied instead. This correction only takes into account the particle-level isolation criteria, and is provided separately here. The Sherpa 2.2.8 NLO cross-sections given below include a small contribution from EW $Z\gamma jj$ production.

The measured fiducial cross section vs $p_{\mathrm{T}}^{\ell\ell\gamma}$. The central values are provided along with the statistical and systematic uncertainties together with the sign information. The statistical and "Uncor" uncertainty should be treated as uncorrelated bin-to-bin, while the rest are correlated between bins, and they are written as signed NP variations. The parton-to-particle correction factor $C_{theory}$ is the ratio of the cross-section predicted by Sherpa LO samples at particle level within the fiducial phase-space region defined in Table 4 to the predicted cross-section at parton level within the same fiducial region but with the smooth-cone isolation prescription defined above replacing the particle-level photon isolation criterion, and with Born-level leptons in place of dressed leptons. This correction should be applied on fixed order parton-level calculations. The systematic uncertainty is evaluated from a comparison with the correction factor obtained using events generated with SHERPA 2.2.2 at NLO. In the case that the calculations are valid for dressed leptons, a modified correction factor excluding the Born-to-dressed lepton correction should be applied instead. This correction only takes into account the particle-level isolation criteria, and is provided separately here. The Sherpa 2.2.8 NLO cross-sections given below include a small contribution from EW $Z\gamma jj$ production.

The measured fiducial cross section vs $\Delta\phi(ll,\gamma)$. The central values are provided along with the statistical and systematic uncertainties together with the sign information. The statistical and "Uncor" uncertainty should be treated as uncorrelated bin-to-bin, while the rest are correlated between bins, and they are written as signed NP variations. The parton-to-particle correction factor $C_{theory}$ is the ratio of the cross-section predicted by Sherpa LO samples at particle level within the fiducial phase-space region defined in Table 4 to the predicted cross-section at parton level within the same fiducial region but with the smooth-cone isolation prescription defined above replacing the particle-level photon isolation criterion, and with Born-level leptons in place of dressed leptons. This correction should be applied on fixed order parton-level calculations. The systematic uncertainty is evaluated from a comparison with the correction factor obtained using events generated with Sherpa 2.2.2 at NLO. The uncertainty is defined as Max(stat error, systematic difference between Sherpa LO and Sherpa 2.2.2 NLO), and cannot be considered correlated bin-to-bin. In the case that the calculations are valid for dressed leptons, a modified correction factor excluding the Born-to-dressed lepton correction should be applied instead. This correction only takes into account the particle-level isolation criteria, and is provided separately here. The Sherpa 2.2.8 NLO cross-sections given below include a small contribution from EW $Z\gamma jj$ production.

The measured fiducial cross section vs $\Delta\phi(ll,\gamma)$. The central values are provided along with the statistical and systematic uncertainties together with the sign information. The statistical and "Uncor" uncertainty should be treated as uncorrelated bin-to-bin, while the rest are correlated between bins, and they are written as signed NP variations. The parton-to-particle correction factor $C_{theory}$ is the ratio of the cross-section predicted by Sherpa LO samples at particle level within the fiducial phase-space region defined in Table 4 to the predicted cross-section at parton level within the same fiducial region but with the smooth-cone isolation prescription defined above replacing the particle-level photon isolation criterion, and with Born-level leptons in place of dressed leptons. This correction should be applied on fixed order parton-level calculations. The systematic uncertainty is evaluated from a comparison with the correction factor obtained using events generated with SHERPA 2.2.2 at NLO. In the case that the calculations are valid for dressed leptons, a modified correction factor excluding the Born-to-dressed lepton correction should be applied instead. This correction only takes into account the particle-level isolation criteria, and is provided separately here. The Sherpa 2.2.8 NLO cross-sections given below include a small contribution from EW $Z\gamma jj$ production.

The measured fiducial cross section vs $p_{\mathrm{T}}^{\ell\ell\gamma}/m(\ell\ell\gamma)$. The central values are provided along with the statistical and systematic uncertainties together with the sign information. The statistical and "Uncor" uncertainty should be treated as uncorrelated bin-to-bin, while the rest are correlated between bins, and they are written as signed NP variations. The parton-to-particle correction factor $C_{theory}$ is the ratio of the cross-section predicted by Sherpa LO samples at particle level within the fiducial phase-space region defined in Table 4 to the predicted cross-section at parton level within the same fiducial region but with the smooth-cone isolation prescription defined above replacing the particle-level photon isolation criterion, and with Born-level leptons in place of dressed leptons. This correction should be applied on fixed order parton-level calculations. The systematic uncertainty is evaluated from a comparison with the correction factor obtained using events generated with Sherpa 2.2.2 at NLO. The uncertainty is defined as Max(stat error, systematic difference between Sherpa LO and Sherpa 2.2.2 NLO), and cannot be considered correlated bin-to-bin. In the case that the calculations are valid for dressed leptons, a modified correction factor excluding the Born-to-dressed lepton correction should be applied instead. This correction only takes into account the particle-level isolation criteria, and is provided separately here. The Sherpa 2.2.8 NLO cross-sections given below include a small contribution from EW $Z\gamma jj$ production.

The measured fiducial cross section vs $p_{\mathrm{T}}^{\ell\ell\gamma}/m(\ell\ell\gamma)$. The central values are provided along with the statistical and systematic uncertainties together with the sign information. The statistical and "Uncor" uncertainty should be treated as uncorrelated bin-to-bin, while the rest are correlated between bins, and they are written as signed NP variations. The parton-to-particle correction factor $C_{theory}$ is the ratio of the cross-section predicted by Sherpa LO samples at particle level within the fiducial phase-space region defined in Table 4 to the predicted cross-section at parton level within the same fiducial region but with the smooth-cone isolation prescription defined above replacing the particle-level photon isolation criterion, and with Born-level leptons in place of dressed leptons. This correction should be applied on fixed order parton-level calculations. The systematic uncertainty is evaluated from a comparison with the correction factor obtained using events generated with SHERPA 2.2.2 at NLO. In the case that the calculations are valid for dressed leptons, a modified correction factor excluding the Born-to-dressed lepton correction should be applied instead. This correction only takes into account the particle-level isolation criteria, and is provided separately here. The Sherpa 2.2.8 NLO cross-sections given below include a small contribution from EW $Z\gamma jj$ production.

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.

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.

Differential cross sections as a function of X(C=GAMMA) from beauty and charm quarks.

Differential cross sections for the most energetic jet as a function of ET from beauty and charm quarks.

Differential cross sections for the most energetic jet as a function of ET from beauty and charm quarks.

Differential cross sections as a function of the electron ET for the jet associated to the electron from beauty or charm decays.

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.

Differential cross section DSIG/DZ(NAME=POMERON) for diffractive photoproduction of dijets as a function of Z(NAME=POMERON).

Differential cross section for the diffractive photoproduction of dijets as a function of ET of the highest jet.

Differential cross section for the diffractive photoproduction of dijets as a function of pseudorapidity (ETARAP) of the highest ET jet.

Differential cross section for the diffractive photoproduction of dijets as a function of X(C=GAMMA,OBS).

Differential cross section DSIG/DY for diffractive photoproduction of dijets as a function of Y for X(C=GAMMA,OBS) > 0.75.

Differential cross section DSIG/DM(P=5_6_7) for diffractive photoproduction of dijets as a function of M(P=5_6_7) for X(C=GAMMA,OBS) > 0.75.

Differential cross section DSIG/DX(NAME=POMERON) for diffractive photoproduction of dijets as a function of X(NAME=POMERON) for X(C=GAMMA,OBS) > 0.75.

Differential cross section DSIG/DZ(NAME=POMERON) for diffractive photoproduction of dijets as a function of Z(NAME=POMERON) for X(C=GAMMA,OBS) > 0.75.

Differential cross section DSIG/DY for diffractive photoproduction of dijets as a function of Y for X(C=GAMMA,OBS) < 0.75.

Differential cross section DSIG/DM(P=5_6_7) for diffractive photoproduction of dijets as a function of M(P=5_6_7) for X(C=GAMMA,OBS) < 0.75.

Differential cross section DSIG/DX(NAME=POMERON) for diffractive photoproduction of dijets as a function of X(NAME=POMERON) for X(C=GAMMA,OBS) < 0.75.

Differential cross section DSIG/DZ(NAME=POMERON) for diffractive photoproduction of dijets as a function of Z(NAME=POMERON) for X(C=GAMMA,OBS) < 0.75.

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 .