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.

Exclusive RHO0 electro- and photo- production cross sections as a function of W from the DIS data set.

Exclusive RHO0 electro- and photo- production cross sections as a function of W from the DIS data set.

Exclusive RHO0 electro- and photo- production cross sections as a function of W from the DIS data set.

Exclusive J/PSI electro-production cross sections as a function of W from the DIS data set.

Exclusive J/PSI photo-production cross sections as a function of W from theDIS data set.

The powers of W found from the fit of the W dependence of the exclusive RHO0 photoproduction cross section to the W distributiuons in various Q**2 regions.

The ratio of the J/PSI and RHO0 cross sections at two Q**2 values.

Differential cross section for RHO0 production from the BPC data.

Differential cross section for RHO0 production from the DIS data.

Differential cross section for J/PSI production from the DIS data.

The slope of the RHO0 dsig/dt distribution from the BPC data. The first point is the fit over the full data sample.. The second systematic (DSYS) error is the uncertainty arising from the subtraction of the proton dissiciation background.

The slope of the RHO0 dsig/dt distribution from the BPC data. The second systematic (DSYS) error is the uncertainty arising from the subtraction of the proton dissiciation background.

The slope of the RHO0 dsig/dt distribution from the BPC data. The second systematic (DSYS) error is the uncertainty arising from the subtraction of the proton dissiciation background.

The slope of the RHO0 dsig/dt distribution from the DIS data. The first point is the fit over the full data sample.. The second systematic (DSYS) error is the uncertainty arising from the subtraction of the proton dissiciation background.

The slope of the RHO0 dsig/dt distribution from the DIS data. The second systematic (DSYS) error is the uncertainty arising from the subtraction of the proton dissiciation background.

The slope of the RHO0 dsig/dt distribution from the DIS data. The second systematic (DSYS) error is the uncertainty arising from the subtraction of the proton dissiciation background.

The slope of the RHO0 dsig/dt distribution from the DIS data. The second systematic (DSYS) error is the uncertainty arising from the subtraction of the proton dissiciation background.

The spin-density martix elements deletermined for various values of W and Q**2 for the RHO0 BPC sample.

The spin-density martix elements deletermined for various values of W and Q**2 for the RHO0 BPC sample.

The spin-density martix elements deletermined for various values of W and Q**2 for the RHO0 DIS sample.

The spin-density martix elements deletermined for various values of W and Q**2 for the RHO0 DIS sample.

Ratio of the cross sections for longitudinal and transverse photons from the DIS data as a function of Q**2.

Ratio of the cross sections for longitudinal and transverse photons from the BPC data as a function of Q**2.

Ratio of the cross sections for longitudinal and transverse photons from the BPC data as a function of W.

Ratio of the cross sections for longitudinal and transverse photons from the DIS data as a function of W.

The measured forward longitudinal cross section as a function of x for the DIS RHO0 data sample. NOTE FROM THE AUTHORS about figure 19_21:. Please note that the positive and negative error bars in the publication Eur.Phys.J. C6 (1999) 603 were inadvertently exchanged. In this table we give thetotal systematic uncertainty on each point as the quadratic sum of the correlat ed systematic error, shown as shaded bands in the publication, and the systematic error bars.

The measured forward longitudinal cross section as a function of x for the DIS RHO0 data sample. See note above from the authors.

The measured forward longitudinal cross section as a function of x for the DIS RHO0 data sample. See note above from the authors.

The measured forward longitudinal cross section as a function of x for the DIS RHO0 data sample. See note above from the authors.

Differential T distribution. Statistical errors only.

DSIG/DT distribution fit with the expression A*EXP(-B*ABS(T) + C*T**2).

SLOPE (B) of the DSIG/DT distribution keeping c fixed at 2.8 (see previous table).

DSIG/DT distribution fit with the expression A* EXP(-B*ABS(T) + C *T**2).

SLOPE (B) as a function of M(P=1_2) keeping C constant at 2.7 (see previoustable).

Acceptance corrected distribution of THETA, the polar angle of the decay ofthe PI+ in the RHO0 helicity frame where the RHO0 is at rest. THETA is defined as the angle between the direction opposite to that of the outgoing PROTON and the direction of the PI+. Statistical errors only.

Acceptance corrected PHI angular distribution, where PHI is angle between the decay plane and the RHO0 production plane. Stastistical errors only.

Result of two dimensional least-square fit to the accertance corrected angular distributions to give spin density matrices.

Spin density matrices as function of the two pion mass.

Spin density matrices as function of the two pion mass.

Spin density matrices as function of the two pion mass.

Spin density matrices as a function of M(P=1_2).

Spin density matrices as a function of M(P=1_2).

Spin density matrices as a function of M(P=1_2).

DSIG/DT distribution for the proton dissociative events tagged with the PRT1. Statistical errors only.

DSIG/DT distribution for the proton dissociative events tagged with the LPS(X<0.98). Statistical errors only.