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NOTE THAT THE DATA HAVE BEEN CHANGED FROM THE PUBLISHED FIGURE.

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.

Normalised inclusive single-particle distributions of charged hadrons in different intervals of W and Q**2 with corresponding values of X(Bjorken). Additional systematic error of 4 PCT.

Normalised inclusive single-particle distributions of charged hadrons in different intervals of W and Q**2 with corresponding values of X(Bjorken). Additional systematic error of 4 PCT.

Normalised inclusive single-particle distributions of charged hadrons in different intervals of W and Q**2 with corresponding values of X(Bjorken). Additional systematic error of 4 PCT.

Normalised inclusive single-particle distributions of charged hadrons in different intervals of W and Q**2 with corresponding values of X(Bjorken). Additional systematic error of 4 PCT.

Normalised inclusive single-particle distributions of charged hadrons in different intervals of W and Q**2 with corresponding values of X(Bjorken). Additional systematic error of 4 PCT.

Normalised inclusive single-particle distributions of charged hadrons in different intervals of W and Q**2 with corresponding values of X(Bjorken). Additional systematic error of 4 PCT.

Normalised inclusive single-particle distributions of charged hadrons in different intervals of W and Q**2 with corresponding values of X(Bjorken). Additional systematic error of 4 PCT.

Normalised inclusive single-particle distributions of charged hadrons in different intervals of W and Q**2 with corresponding values of X(Bjorken). Additional systematic error of 4 PCT.

Normalised inclusive single-particle distributions of charged hadrons in different intervals of W and Q**2 with corresponding values of X(Bjorken). Additional systematic error of 4 PCT.

Additional inclusive single-particle distributions of charged hadrons as a function of XL and PT**2 in different intervals of W. Additional systematic error 4 PCT.

Additional inclusive single-particle distributions of charged hadrons as a function of XL and PT**2 in different intervals of W. Additional systematic error 4 PCT.

Additional inclusive single-particle distributions of charged hadrons as a function of XL and PT**2 in different intervals of W. Additional systematic error 4 PCT.

Additional inclusive single-particle distributions of charged hadrons as a function of XL and PT**2 in different intervals of W. Additional systematic error 4 PCT.

Additional inclusive single-particle distributions of charged hadrons as a function of XL and PT**2 in different intervals of W. Additional systematic error 4 PCT.

Additional inclusive single-particle distributions of charged hadrons as a function of XL and PT**2 in different intervals of W. Additional systematic error 4 PCT.

Normalised inclusive single-particle distributions of charged hadrons as a function of XL and PT**2 in different intervals of Q**2. Additional systematic error 4 PCT.

Normalised inclusive single-particle distributions of charged hadrons as a function of XL and PT**2 in different intervals of Q**2. Additional systematic error 4 PCT.

Normalised inclusive single-particle distributions of charged hadrons as a function of XL and PT**2 in different intervals of Q**2. Additional systematic error 4 PCT.

Normalised inclusive single-particle distributions of charged hadrons as a function of XL and PT**2 in different intervals of Q**2. Additional systematic error 4 PCT.

Normalised inclusive single-particle distributions of charged hadrons as a function of XL and PT**2 in different intervals of Q**2. Additional systematic error 4 PCT.

Normalised inclusive single-particle distributions of charged hadrons as a function of XL and PT**2 in different intervals of Q**2. Additional systematic error 4 PCT.

Mean values of PT**2 in different XL intervals in different regions of W**2. Additional systematic error 2 PCT.

Mean values of PT**2 in different XL intervals in different Q**2 regions. Additional systematic error 2 PCT.

Mean value of PT**2 in different XL intervals in different intervals of W**2 and Q**2. Corresponding values of X(Bjorken) as shown. Additional systematic error 2 PCT.

Mean value of PT**2 in different XL intervals in different intervals of W**2 and Q**2. Corresponding values of X(Bjorken) as shown. Additional systematic error 2 PCT.

Mean value of PT**2 in different XL intervals in different intervals of W**2 and Q**2. Corresponding values of X(Bjorken) as shown. Additional systematic error 2 PCT.

Mean value of PT**2 in different XL intervals in different intervals of W**2 and Q**2. Corresponding values of X(Bjorken) as shown. Additional systematic error 2 PCT.

Mean value of PT**2 in different XL intervals in different intervals of W**2 and Q**2. Corresponding values of X(Bjorken) as shown. Additional systematic error 2 PCT.

Mean value of PT**2 in different XL intervals in different intervals of W**2 and Q**2. Corresponding values of X(Bjorken) as shown. Additional systematic error 2 PCT.

Average forward multipicities for positive, negative and all charged hadrons. Additional systematic error 1 PCT.

Average forward multipicities for positive, negative and all charged hadrons. Additional systematic error 1 PCT.

Average forward multipicities for positive, negative and all charged hadrons. Additional systematic error 1 PCT.

Normalizef multiplicity distribution of charged particle in the central region as a function of the KNO variable. Note that the different energies have not been separated here.