Fit of elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\pi^{+}\pi^{-}$ photoproduction off protons with a Soeding-inspired analytic function --- statistical correlations only. Only one half of the (symmetric) matrix is stored.

Elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\pi^{+}\pi^{-}$ photoproduction off protons, differential in the dipion mass and in bins of $W$. The tabulated cross sections are $\gamma p$ cross sections but can be converted to $ep$ cross sections using the effective photon flux $\Phi_{\gamma/e}$.

Elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\pi^{+}\pi^{-}$ photoproduction off protons, differential in the dipion mass and in bins of $W$ --- statistical correlations coefficients $\rho_{ij}$ only. Only one half of the (symmetric) matrix is stored. Bins are identified by their global bin number.

Elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\rho^0(770)$ photoproduction off protons, in bins of the photon-proton energy $W$. The cross section is defined as the integral of the relativistic Breit Wigner resonance in the dipion mass over the range $2m_\pi<m_{\pi\pi}<1.53$ GeV. The tabulated cross sections are $\gamma p$ cross sections but can be converted to $ep$ cross sections using the effective photon flux $\Phi_{\gamma/e}$.

Elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\rho^0(770)$ photoproduction off protons in bins of the photon-proton energy $W$ --- statistical correlations coefficients $\rho_{ij}$ only. Only one half of the (symmetric) matrix is stored. Bins are identified by their global bin number.

Fit of elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\rho^0(770)$ photoproduction cross sections off protons as a function of energy. Parameters with subscript "el" and "pd" correspond to elastic and proton-dissociative cross sections, respectively.

Fit of elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\rho^0(770)$ photoproduction cross sections off protons as a function of energy --- statistical correlations coefficients $\rho_{ij}$ only. Only one half of the (symmetric) matrix is stored. Bins are identified by their global bin number.

Fit of elastic $\rho^0(770)$ photoproduction cross section off protons as a function of energy (various experiments)

Fit of elastic $\rho^0(770)$ photoproduction cross sections off protons as a function of energy (various experiments) --- statistical correlations coefficients $\rho_{ij}$ only. Only one half of the (symmetric) matrix is stored. Bins are identified by their global bin number.

Elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\pi^{+}\pi^{-}$ photoproduction cross section off protons, double-differential in the dipion mass and the momentum transfer $\vert t\vert$. The tabulated cross sections are $\gamma p$ cross sections but can be converted to $ep$ cross sections using the effective photon flux $\Phi_{\gamma/e}$.

Elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\pi^{+}\pi^{-}$ photoproduction cross section off protons, double-differential in the dipion mass and the momentum transfer $\vert t\vert$ --- statistical correlations coefficients $\rho_{ij}$ only. Only one half of the (symmetric) matrix is stored. Bins are identified by their global bin number.

Elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\rho^0(770)$ photoproduction off protons, single-differential in the momentum transfer $\vert t\vert$. The cross section is defined as the integral of the relativistic Breit Wigner resonance in the dipion mass over the range $2m_\pi<m_{\pi\pi}<1.53$ GeV. The tabulated cross sections are $\gamma p$ cross sections but can be converted to $ep$ cross sections using the effective photon flux $\Phi_{\gamma/e}$.

Elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\rho^0(770)$ photoproduction off protons, single differential in the momentum transfer $\vert t\vert$ --- statistical correlations coefficients $\rho_{ij}$ only. Only one half of the (symmetric) matrix is stored. Bins are identified by their global bin number.

Fit of elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\rho^0(770)$ photoproduction single-differential cross sections off protons as a function of momentum transfer $t$. Parameters with subscript "el" and "pd" correspond to elastic and proton-dissociative cross sections, respectively.

Fit of elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\rho^0(770)$ photoproduction single-differential cross sections off protons as a function of momentum transfer $t$ --- statistical correlations coefficients $\rho_{ij}$ only. Only one half of the (symmetric) matrix is stored. Bins are identified by their global bin number.

Elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\pi^{+}\pi^{-}$ photoproduction double-differenial cross section off protons, as a function of the dipion mass and the momentum transfer $\vert t\vert$, in bins of the photon-proton energy $W$ The tabulated cross sections are $\gamma p$ cross sections but can be converted to $ep$ cross sections using the effective photon flux $\Phi_{\gamma/e}$.

Elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\pi^{+}\pi^{-}$ photoproduction double-differenial cross section off protons, as a function of the dipion mass and the momentum transfer $\vert t\vert$, in bins of the photon-proton energy $W$ --- statistical correlations coefficients $\rho_{ij}$ only. Only one half of the (symmetric) matrix is stored. Bins are identified by their global bin number.

Elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\rho^0(770)$ photoproduction off protons, single-differential in the momentum transfer $\vert t\vert$, in bins of the photon-proton energy $W$. The cross section is defined as the integral of the relativistic Breit Wigner resonance in the dipion mass over the range $2m_\pi<m_{\pi\pi}<1.53$ GeV. The tabulated cross sections are $\gamma p$ cross sections but can be converted to $ep$ cross sections using the effective photon flux $\Phi_{\gamma/e}$.

Elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\rho^0(770)$ photoproduction cross section off protons, single differential in the momentum transfer $\vert t\vert$ and in bins of the photon-proton energy $W$ --- statistical correlations coefficients $\rho_{ij}$ only. Only one half of the (symmetric) matrix is stored. Bins are identified by their global bin number.

Regge fit of elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\rho^0(770)$ photoproduction single-differential cross sections off protons as a function of momentum transfer $t$ and photon-proton energy $W$. Parameters with subscript "el" and "pd" correspond to elastic and proton-dissociative cross sections, respectively.

Regge fit of elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\rho^0(770)$ photoproduction single-differential cross sections off protons as a function of momentum transfer $t$ and photon-proton energy $W$ --- statistical correlations coefficients $\rho_{ij}$ only. Only one half of the (symmetric) matrix is stored. Bins are identified by their global bin number.

Fit of $b$-slopes in elastic ($m_Y=m_p$) $\rho^0(770)$ photoproduction single-differential cross sections off protons as a function of momentum transfer $t$ in bins of photon-proton energy $W$.

Fit of $b$-slopes in elastic ($m_Y=m_p$) $\rho^0(770)$ photoproduction single-differential cross sections off protons as a function of momentum transfer $t$ in bins of photon-proton energy $W$ --- statistical correlations coefficients $\rho_{ij}$ only. Only one half of the (symmetric) matrix is stored. Bins are identified by their global bin number.

Fit of Pomeron trajectories in elastic ($m_Y=m_p$) $\rho^0(770)$ photoproduction single-differential cross sections off protons as a function of momentum transfer $t$ in bins of photon-proton energy $W$.

Fit of Pomeron trajectories in elastic ($m_Y=m_p$) $\rho^0(770)$ photoproduction single-differential cross sections off protons as a function of momentum transfer $t$ in bins of photon-proton energy $W$ --- statistical correlations coefficients $\rho_{ij}$ only. Only one half of the (symmetric) matrix is stored. Bins are identified by their global bin number.

The inclusive doubly differential cross section for K0S production with a Ctarget.

The inclusive doubly differential cross section for K0S production with a TI target.

The inclusive doubly differential cross section for K0S production with a WT target.

The inclusive doubly differential cross section for LAMBDA production with a C target.

The inclusive doubly differential cross section for LAMBDA production with a TI target.

The inclusive doubly differential cross section for LAMBDA production with a WT target.

The inclusive doubly differential cross section for LAMBDABAR production with a C target.

The inclusive doubly differential cross section for LAMBDABAR production with a TI target.

The inclusive doubly differential cross section for LAMBDABAR production with a WT target.

Antineutrino forward dimuon cross sections for Y bins 0.35, 0.58 and 0.78 as a function of X for neutrino energy 78.

Antineutrino forward dimuon cross sections for Y bins 0.35, 0.58 and 0.78 as a function of X for neutrino energy 144.

Antineutrino forward dimuon cross sections for Y bins 0.35, 0.58 and 0.78 as a function of X for neutrino energy 227.

Normalized double differential cross sections for leading neutron production for the full DIS sample. Statistical errors only are given.

Normalized double differential cross sections for leading neutron production for the full DIS sample. Statistical errors only are given.

Normalized double differential cross sections for leading neutron production for the full DIS sample. Statistical errors only are given.

Normalized double differential cross sections for leading neutron production for the full DIS sample. Statistical errors only are given.

Normalized double differential cross sections for leading neutron production for the full DIS sample. Statistical errors only are given.

Normalized double differential cross sections for leading neutron production for the full DIS sample. Statistical errors only are given.

Normalized double differential cross sections for leading neutron production for the full DIS sample. Statistical errors only are given.

Normalized double differential cross sections for leading neutron production for the full DIS sample. Statistical errors only are given.

Normalized double differential cross sections for leading neutron production for the full DIS sample. Statistical errors only are given.

Normalized double differential cross sections for leading neutron production for the full DIS sample. Statistical errors only are given.

Normalized double differential cross sections for leading neutron production for the full DIS sample. Statistical errors only are given.

Normalized double differential cross sections for leading neutron production for the full DIS sample. Statistical errors only are given.

Normalized double differential cross sections for leading neutron production for the full DIS sample. Statistical errors only are given.

The intercepts and slope for the exponential parameterisation of the differential cross section of the form A exp(-B*PT**2). Errors do not contain additional 2.1 PCT uncertainty on the intercepts.

Normalized double differential cross sections for leading neutron production in the photoproduction sample. Statistical errors only are given.

Normalized double differential cross sections for leading neutron production in the photoproduction sample. Statistical errors only are given.

Normalized double differential cross sections for leading neutron production in the photoproduction sample. Statistical errors only are given.

Normalized double differential cross sections for leading neutron production in the photoproduction sample. Statistical errors only are given.

Normalized double differential cross sections for leading neutron production in the photoproduction sample. Statistical errors only are given.

Normalized double differential cross sections for leading neutron production in the photoproduction sample. Statistical errors only are given.

Normalized double differential cross sections for leading neutron production in the photoproduction sample. Statistical errors only are given.

Normalized double differential cross sections for leading neutron production in three regions of Q**2. Statistical errors only are given.

Normalized double differential cross sections for leading neutron production in three regions of Q**2. Statistical errors only are given.

Normalized double differential cross sections for leading neutron production in three regions of Q**2. Statistical errors only are given.

Normalized double differential cross sections for leading neutron production in three regions of Q**2. Statistical errors only are given.

Normalized double differential cross sections for leading neutron production in three regions of Q**2. Statistical errors only are given.

Normalized double differential cross sections for leading neutron production in three regions of Q**2. Statistical errors only are given.

Normalized double differential cross sections for leading neutron production in three regions of Q**2. Statistical errors only are given.

The intercepts and slope for the exponential parameterisation of the differential cross section of the form Aexp(-B*PT**2) for the photoproduction sample. The errors do not contain the additional 2.1 PCT uncertainty on the DIS intercepts, nor the additional 5.1 PCT uncertainty on the photoproduction intercepts.

The intercept and slope for the exponential parameterisation of the differential cross section of the form Aexp(-B*PT**2) for the low-Q**2 DIS sample. The errors do not contain the additional 2.1 PCT uncertainty on the DIS intercepts, nor the additional 5.1 PCT uncertainty on the photoproduction intercepts.

The intercept and slope for the exponential parameterisation of the differential cross section of the form Aexp(-B*PT**2) for the mid-Q**2 DIS sample. The errors do not contain the additional 2.1 PCT uncertainty on the DIS intercepts, nor the additional 5.1 PCT uncertainty on the photoproduction intercepts.

The intercept and slope for the exponential parameterisation of the differential cross section of the form Aexp(-B*PT**2) for the high-Q**2 DIS sample. The errors do not contain the additional 2.1 PCT uncertainty on the DIS intercepts, nor the additional 5.1 PCT uncertainty on the photoproduction intercepts.

The measured F2 and xF3 at X = 0.125.

The measured F2 and xF3 at X = 0.175.

The measured F2 and xF3 at X = 0.225.

The measured F2 and xF3 at X = 0.275.

The measured F2 and xF3 at X = 0.350.

The measured F2 and xF3 at X = 0.450.

The measured F2 and xF3 at X = 0.550.

The measured F2 and xF3 at X = 0.650.

The measured R (=sigL/sigT)) at X = 0.020.

The measured R (=sigL/sigT)) at X = 0.045.

The measured R (=sigL/sigT)) at X = 0.080.

The measured R (=sigL/sigT)) at X = 0.125.

The measured R (=sigL/sigT)) at X = 0.175.

The measured R (=sigL/sigT)) at X = 0.225.

The measured R (=sigL/sigT)) at X = 0.275.

The measured R (=sigL/sigT)) at X = 0.350.

The measured R (=sigL/sigT)) at X = 0.450.

The measured R (=sigL/sigT)) at X = 0.550.

The measured R (=sigL/sigT)) at X = 0.650.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 25.0 GeV and X =0.020.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 25.0 GeV and X =0.045.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 25.0 GeV and X =0.080.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 25.0 GeV and X =0.125.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 25.0 GeV and X =0.175.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 25.0 GeV and X =0.225.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 25.0 GeV and X =0.275.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 25.0 GeV and X =0.350.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 25.0 GeV and X =0.450.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 25.0 GeV and X =0.550.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 25.0 GeV and X =0.650.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 35.0 GeV and X =0.020.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 35.0 GeV and X =0.045.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 35.0 GeV and X =0.080.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 35.0 GeV and X =0.125.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 35.0 GeV and X =0.175.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 35.0 GeV and X =0.225.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 35.0 GeV and X =0.275.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 35.0 GeV and X =0.350.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 35.0 GeV and X =0.450.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 35.0 GeV and X =0.550.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 35.0 GeV and X =0.650.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 45.0 GeV and X =0.020.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 45.0 GeV and X =0.045.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 45.0 GeV and X =0.080.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 45.0 GeV and X =0.125.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 45.0 GeV and X =0.175.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 45.0 GeV and X =0.225.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 45.0 GeV and X =0.275.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 45.0 GeV and X =0.350.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 45.0 GeV and X =0.450.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 45.0 GeV and X =0.550.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 45.0 GeV and X =0.650.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 55.0 GeV and X =0.020.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 55.0 GeV and X =0.045.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 55.0 GeV and X =0.080.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 55.0 GeV and X =0.125.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 55.0 GeV and X =0.175.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 55.0 GeV and X =0.225.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 55.0 GeV and X =0.275.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 55.0 GeV and X =0.350.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 55.0 GeV and X =0.450.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 55.0 GeV and X =0.550.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 55.0 GeV and X =0.650.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 70.0 GeV and X =0.020.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 70.0 GeV and X =0.045.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 70.0 GeV and X =0.080.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 70.0 GeV and X =0.125.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 70.0 GeV and X =0.175.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 70.0 GeV and X =0.225.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 70.0 GeV and X =0.275.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 70.0 GeV and X =0.350.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 70.0 GeV and X =0.450.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 70.0 GeV and X =0.550.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 70.0 GeV and X =0.650.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 90.0 GeV and X =0.020.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 90.0 GeV and X =0.045.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 90.0 GeV and X =0.080.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 90.0 GeV and X =0.125.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 90.0 GeV and X =0.175.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 90.0 GeV and X =0.225.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 90.0 GeV and X =0.275.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 90.0 GeV and X =0.350.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 90.0 GeV and X =0.450.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 90.0 GeV and X =0.550.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 90.0 GeV and X =0.650.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 110.0 GeV and X =0.020.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 110.0 GeV and X =0.045.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 110.0 GeV and X =0.080.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 110.0 GeV and X =0.125.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 110.0 GeV and X =0.175.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 110.0 GeV and X =0.225.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 110.0 GeV and X =0.275.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 110.0 GeV and X =0.350.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 110.0 GeV and X =0.450.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 110.0 GeV and X =0.550.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 110.0 GeV and X =0.650.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 130.0 GeV and X =0.020.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 130.0 GeV and X =0.045.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 130.0 GeV and X =0.080.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 130.0 GeV and X =0.125.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 130.0 GeV and X =0.175.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 130.0 GeV and X =0.225.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 130.0 GeV and X =0.275.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 130.0 GeV and X =0.350.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 130.0 GeV and X =0.450.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 130.0 GeV and X =0.550.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 130.0 GeV and X =0.650.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 170.0 GeV and X =0.020.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 170.0 GeV and X =0.045.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 170.0 GeV and X =0.080.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 170.0 GeV and X =0.125.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 170.0 GeV and X =0.175.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 170.0 GeV and X =0.225.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 170.0 GeV and X =0.275.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 170.0 GeV and X =0.350.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 170.0 GeV and X =0.450.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 170.0 GeV and X =0.550.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 170.0 GeV and X =0.650.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

PT integrated invariant cross sections and density distributions together with mean values of PT and PT**2 as a function of Feynman X for positive pion production.

PT integrated invariant cross sections and density distributions together with mean values of PT and PT**2 as a function of Feynman X for negative pion production.

PT integrated rapidity distribution.

Measured differential E+ P cross section DSIG/DETARAP for inclusive jet photoproduction(Q**2 < 1 GeV**2) integrated over the ET range 21 to 75 GeV and the W(C=GAMMA P) range 95 to 285 GeV.

Measured differential E+ P cross section DSIG/DETARAP for inclusive jet photoproduction(Q**2 < 1 GeV**2) integrated over the ET range 21 to 35 GeV and the W(C=GAMMA P) range 95 to 285 GeV.

Measured differential E+ P cross section DSIG/DETARAP for inclusive jet photoproduction(Q**2 < 1 GeV**2) integrated over the ET range 35 to 52 GeV and the W(C=GAMMA P) range 95 to 285 GeV.

Measured differential E+ P cross section DSIG/DETARAP for inclusive jet photoproduction(Q**2 < 1 GeV**2) integrated over the ET range 52 to 75 GeV and the W(C=GAMMA P) range 95 to 285 GeV.

Measured differential E+ P cross section DSIG/DETARAP for inclusive jet photoproduction(Q**2 < 1 GeV**2) integrated over the ET range 21 to 35 GeV and the W(C=GAMMA P) range 95 to 212 GeV.

Measured differential E+ P cross section DSIG/DETARAP for inclusive jet photoproduction(Q**2 < 1 GeV**2) integrated over the ET range 21 to 35 GeV and the W(C=GAMMA P) range 212 to 285 GeV.

Measured differential E+ P cross section DSIG/DETARAP for inclusive jet photoproduction(Q**2 < 1 GeV**2) integrated over the ET range 35 to 52 GeV and the W(C=GAMMA P) range 95 to 212 GeV.

Measured differential E+ P cross section DSIG/DETARAP for inclusive jet photoproduction(Q**2 < 1 GeV**2) integrated over the ET range 35 to 52 GeV and the W(C=GAMMA P) range 212 to 285 GeV.

Measured differential E+ P cross section DSIG/DETARAP for inclusive jet photoproduction(Q**2 < 1 GeV**2) integrated over the ET range 52 to 75 GeV and the W(C=GAMMA P) range 212 to 285 GeV.

Measured differential E+ P cross section DSIG/DETARAP for inclusive jet photoproduction(Q**2 < 0.01 GeV**2) integrated over the ET ranges 5 to 12 GeV and 12 to 21 GeV and the W(C=GAMMA P) range 164 to 242 GeV.

Measured differential E+ P cross section DSIG/DET for inclusive jet photoproductionm, with jets defined by the cone algorithm with R = 1, for the two Q**2 ranges integrated over the jet pseudorapidity range -1 to 2.5 in the W(C=GAMMA P) range 164 to 242 GeV.

The scaled GAMMA P cross section at a mean W of 200 GeV as a function of the jet XT for the jet CM rapidity range -0.5 to 0.5. Jets are defined by the conealgorithm with R = 1.

The differential cross section dsig/dmx measured with the LPS method for the Q**2 range 0.17 to 0.70.

The differential cross section dsig/dmx measured with the LPS method for the Q**2 range 3 to 9.

The differential cross section dsig/dmx measured with the LPS method for the Q**2 range 9 to 80.

The differential cross section dsig/dmx measured with the M_X**2 method forthe Q**2 range 0.220 to 0.324 in two M_X**2 ranges.

The differential cross section dsig/dmx measured with the M_X**2 method forthe Q**2 range 0.324 to 0.476 in two M_X**2 ranges.

The differential cross section dsig/dmx measured with the M_X**2 method forthe Q**2 range 0.476 to 0.700 in two M_X**2 ranges.

J/PSI leptoproduction differential cross section as a function of the laboratory frame PT**2.

J/PSI leptoproduction differential cross section as a function of the centre-of-mass frame rapidity Y*.

J/PSI leptoproduction differential cross section as a function of the centre-of-mass frame PT**2.

J/PSI leptoproduction differential cross section as a function of the laboratory frame rapidity Y.

J/PSI leptoproduction differential cross section as a function of Q**2 for laboratory PT**2 > 6.4 GeV**2 and Q**2 > 12 GeV**2.

J/PSI leptoproduction differential cross section as a function of Z for laboratory PT**2 > 6.4 GeV**2 and Q**2 > 12 GeV**2.

J/PSI leptoproduction differential cross section as a function of W for laboratort PT**2 > 6.4 GeV**2 and Q**2 > 12 GeV**2.

J/PSI leptoproduction differential cross section as a function of the laboratory frame PT**2 for laboratory PT**2 > 6.4 GeV**2 and Q**2 > 12 GeV**2.

J/PSI leptoproduction differential cross section as a function of the centre-of-mass frame rapidity Y* for laboratory PT**2 > 6.4 GeV**2 and Q**2 > 12 GeV**2.

J/PSI leptoproduction differential cross section as a function of the centre-of-mass frame PT**2 for laboratory PT**2 > 6.4 GeV**2 and Q**2 > 12 GeV**2.

J/PSI leptoproduction double differential cross section as a function of the centre-of-mass frame PT**2 and Z for the Z range 0.3 to 0.6.

J/PSI leptoproduction double differential cross section as a function of the centre-of-mass frame PT**2 and Z for the Z range 0.6 to 0.75.

J/PSI leptoproduction double differential cross section as a function of the centre-of-mass frame PT**2 and Z for Z range 0.75 to 0.9.

J/PSI leptoproduction double differential cross section as a function of Q**2 and Z for the Z range 0.3 to 0.6.

J/PSI leptoproduction double differential cross section as a function of Q**2 and Z for the Z range 0.6 to 0.75.

J/PSI leptoproduction double differential cross section as a function of Q**2 and Z for the Z range 0.75 to 0.9.

J/PSI photoproduction cross section at a mean Q**2 of 10.6 GeV**2.

J/PSI leptoproduction differential cross section as a function of COS(THETA*). for the Z range 0.75 to 0.9.

J/PSI leptoproduction differential cross section as a function of COS(THETA*) in the Q**2 range 2 to 6.5 GeV**2.

J/PSI leptoproduction differential cross section as a function of COS(THETA*) in the Q**2 range 6.5 to 100 GeV**2.