Exclusive J/psi photoproduction cross section in gamma-p.

Dissociative J/psi photoproduction gamma-p.

Cross section ratio, dissociative J/psi photoproduction gamma-p over exclusive J/psi photoproduction gamma-p.

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deviation from phase space in arb. units.

Bin averaged hadron level differential cross sections as a function of the variable $z_{I\!\!P}$ for diffractive dijet DIS. The hadronisation correction factors ($1+\delta_{\text{hadr}}$) applied to the NLO calculations and the radiative corrections ($1+\delta_{\text{rad}}$) are also listed. The overall normalisation uncertainty of $6\%$ is not included in the table.

Bin averaged hadron level differential cross sections as a function of the variable $x_{I\!\!P}$ for diffractive dijet DIS. The hadronisation correction factors ($1+\delta_{\text{hadr}}$) applied to the NLO calculations and the radiative corrections ($1+\delta_{\text{rad}}$) are also listed. The overall normalisation uncertainty of $6\%$ is not included in the table.

Bin averaged hadron level differential cross sections as a function of the variable $y$ for diffractive dijet DIS. The hadronisation correction factors ($1+\delta_{\text{hadr}}$) applied to the NLO calculations and the radiative corrections ($1+\delta_{\text{rad}}$) are also listed. The overall normalisation uncertainty of $6\%$ is not included in the table.

Bin averaged hadron level differential cross sections as a function of the variable $Q^2$ for diffractive dijet DIS. The hadronisation correction factors ($1+\delta_{\text{hadr}}$) applied to the NLO calculations and the radiative corrections ($1+\delta_{\text{rad}}$) are also listed. The overall normalisation uncertainty of $6\%$ is not included in the table.

Bin averaged hadron level differential cross sections for diffractive dijet DIS as a function of the variable $E_T^{*\text{jet1}}$. The hadronisation correction factors ($1+\delta_{\text{hadr}}$) applied to the NLO calculations and the the radiative corrections ($1+\delta_{\text{rad}}$) are also listed. The overall normalisation uncertainty of $6\%$ is not included in the table.

Bin averaged hadron level differential cross sections for diffractive dijet DIS as a function of the variable $M_X$. The hadronisation correction factors ($1+\delta_{\text{hadr}}$) applied to the NLO calculations and the the radiative corrections ($1+\delta_{\text{rad}}$) are also listed. The overall normalisation uncertainty of $6\%$ is not included in the table.

Bin averaged hadron level differential cross sections for diffractive dijet DIS as a function of the variable $\vert\Delta\eta^{\text{jets}}\vert$. The hadronisation correction factors ($1+\delta_{\text{hadr}}$) applied to the NLO calculations and the the radiative corrections ($1+\delta_{\text{rad}}$) are also listed. The overall normalisation uncertainty of $6\%$ is not included in the table.

Bin averaged hadron level differential cross sections for diffractive dijet DIS as a function of the variable $\langle\eta^{\text{jets}}\rangle$. The hadronisation correction factors ($1+\delta_{\text{hadr}}$) applied to the NLO calculations and the the radiative corrections ($1+\delta_{\text{rad}}$) are also listed. The overall normalisation uncertainty of $6\%$ is not included in the table.

Bin averaged hadron level differential diffractive dijet $ep$ cross sections as a function of the variable $z_{I\!\!P}$ for the dijet photoproduction kinematic range. The hadronisation correction factors ($1+\delta_{\text{hadr}}$) applied to the NLO calculations are given. The overall normalisation uncertainty of $6\%$ is not included in the table.

Bin averaged hadron level differential diffractive dijet $ep$ cross sections as a function of the variable $x_{I\!\!P}$ for the dijet photoproduction kinematic range. The hadronisation correction factors ($1+\delta_{\text{hadr}}$) applied to the NLO calculations are given. The overall normalisation uncertainty of $6\%$ is not included in the table.

Bin averaged hadron level differential diffractive dijet $ep$ cross sections as a function of the variable $y$ for the dijet photoproduction kinematic range. The hadronisation correction factors ($1+\delta_{\text{hadr}}$) applied to the NLO calculations are given. The overall normalisation uncertainty of $6\%$ is not included in the table.

Bin averaged hadron level differential diffractive dijet $ep$ cross sections as a function of the variable $x_\gamma$ for the dijet photoproduction kinematic range. The hadronisation correction factors ($1+\delta_{\text{hadr}}$) applied to the NLO calculations are given. The overall normalisation uncertainty of $6\%$ is not included in the table.

Bin averaged hadron level differential diffractive dijet $ep$ cross sections in the photoproduction kinematic range as a function of the variable $E_T^{*\text{jet1}}$. The hadronisation correction factors ($1+\delta_{\text{hadr}}$) applied to the NLO calculations are given. The overall normalisation uncertainty of $6\%$ is not included in the table.

Bin averaged hadron level differential diffractive dijet $ep$ cross sections in the photoproduction kinematic range as a function of the variable $M_X$. The hadronisation correction factors ($1+\delta_{\text{hadr}}$) applied to the NLO calculations are given. The overall normalisation uncertainty of $6\%$ is not included in the table.

Bin averaged hadron level differential diffractive dijet $ep$ cross sections in the photoproduction kinematic range as a function of the variable $\vert\Delta\eta^{\text{jets}}\vert$. The hadronisation correction factors ($1+\delta_{\text{hadr}}$) applied to the NLO calculations are given. The overall normalisation uncertainty of $6\%$ is not included in the table.

Bin averaged hadron level differential diffractive dijet $ep$ cross sections in the photoproduction kinematic range as a function of the variable $\langle\eta^{\text{jets}}\rangle$. The hadronisation correction factors ($1+\delta_{\text{hadr}}$) applied to the NLO calculations are given. The overall normalisation uncertainty of $6\%$ is not included in the table.

Ratios of differential diffractive dijet $ep$ cross sections, measured in photoproduction, to measurements in DIS as a function of the variable $\vert\Delta\eta^{\text{jets}}\vert$. The hadronisation correction factors ($1+\delta_{\text{hadr}}$) applied to the NLO calculations are given.

Ratios of differential diffractive dijet $ep$ cross sections, measured in photoproduction, to measurements in DIS as a function of the variable $y$. The hadronisation correction factors ($1+\delta_{\text{hadr}}$) applied to the NLO calculations are given.

Ratios of differential diffractive dijet $ep$ cross sections, measured in photoproduction, to measurements in DIS as a function of the variable $z_{I\!\!P}$. The hadronisation correction factors ($1+\delta_{\text{hadr}}$) applied to the NLO calculations are given.

Ratios of differential diffractive dijet $ep$ cross sections, measured in photoproduction, to measurements in DIS as a function of the variable $E_T^{*\text{jet1}}$. The hadronisation correction factors ($1+\delta_{\text{hadr}}$) applied to the NLO calculations are given.

Invariant mass distributions of the three SIGMA-PI combinations for centre-of-mass energies, W, from 2.25 to 2.35 GeV corresponding to incident photon energies from 2.23 to 2.47 GeV.

Invariant mass distributions of the three SIGMA-PI combinations for centre-of-mass energies, W, from 2.35 to 2.45 GeV corresponding to incident photon energies from 2.47 to 2.73 GeV.

Invariant mass distributions of the three SIGMA-PI combinations for centre-of-mass energies, W, from 2.45 to 2.55 GeV corresponding to incident photon energies from 2.73 to 3.00 GeV.

Invariant mass distributions of the three SIGMA-PI combinations for centre-of-mass energies, W, from 2.55 to 2.65 GeV corresponding to incident photon energies from 3.00 to 3.27 GeV.

Invariant mass distributions of the three SIGMA-PI combinations for centre-of-mass energies, W, from 2.65 to 2.75 GeV corresponding to incident photon energies from 3.27 to 3.56 GeV.

Invariant mass distributions of the three SIGMA-PI combinations for centre-of-mass energies, W, from 2.75 to 2.84 GeV corresponding to incident photon energies from 3.56 to 3.83 GeV.

Distribution of the invariant mass of the N N system.

Distribution of the invariant mass of the N PI system.

Distribution of the invariant mass of the N N PI system.

Distribution of the invariant mass of the N PI PI system.

Distribution of the PI+ angle in the centre-of-mass system.

Distribution of the angle of the N-N system in the centre-of-mass system.

PI0_PI0 invariant mass distribution at an incident kinetic energy of 1200 MeV.

PI0_PI0 invariant mass distribution at an incident kinetic energy of 1300 MeV.

Distribution of the cosine of the PI0_PI0 opening angle (DELTA) at an incident kinetic energy of 1000 MeV.

Distribution of the cosine of the PI0_PI0 opening angle (DELTA) at an incident kinetic energy of 1100 MeV.

Distribution of the cosine of the PI0_PI0 opening angle (DELTA) at an incident kinetic energy of 1200 MeV.

Distribution of the cosine of the PI0_PI0 opening angle (DELTA) at an incident kinetic energy of 1300 MeV.

P_PI0 invariant mass distribution at an incident kinetic energy of 1000 MeV.

P_PI0 invariant mass distribution at an incident kinetic energy of 1100 MeV.

P_PI0 invariant mass distribution at an incident kinetic energy of 1200 MeV.

P_PI0 invariant mass distribution at an incident kinetic energy of 1300 MeV.

P_PI0_PI0 invariant mass distribution at an incident kinetic energy of 1000 MeV.

P_PI0_PI0 invariant mass distribution at an incident kinetic energy of 1100 MeV.

P_PI0_PI0 invariant mass distribution at an incident kinetic energy of 1200 MeV.

P_PI0_PI0 invariant mass distribution at an incident kinetic energy of 1300 MeV.

Distribution of the cosine of the Proton centre-of-mass angle at an incident kinetic energy of 1000 MeV.

Distribution of the cosine of the Proton centre-of-mass angle at an incident kinetic energy of 1100 MeV.

Distribution of the cosine of the Proton centre-of-mass angle at an incident kinetic energy of 1200 MeV.

Distribution of the cosine of the Proton centre-of-mass angle at an incident kinetic energy of 1300 MeV.

Distribution of the cosine of the PI0 centre-of-mass angle at an incident kinetic energy of 1000 MeV.

Distribution of the cosine of the PI0 centre-of-mass angle at an incident kinetic energy of 1100 MeV.

Distribution of the cosine of the PI0 centre-of-mass angle at an incident kinetic energy of 1200 MeV.

Distribution of the cosine of the PI0 centre-of-mass angle at an incident kinetic energy of 1300 MeV.

Distribution of the cosine of the PI0_PI0 centre-of-mass angle at an incident kinetic energy of 1000 MeV.

Distribution of the cosine of the PI0_PI0 centre-of-mass angle at an incident kinetic energy of 1100 MeV.

Distribution of the cosine of the PI0_PI0 centre-of-mass angle at an incident kinetic energy of 1200 MeV.

Distribution of the cosine of the PI0_PI0 centre-of-mass angle at an incident kinetic energy of 1300 MeV.

Distribution of the cosine of the PI0 angle in the PI0_PI0 subsystem at an incident kinetic energy of 1000 MeV.

Distribution of the cosine of the PI0 angle in the PI0_PI0 subsystem at an incident kinetic energy of 1100 MeV.

Distribution of the cosine of the PI0 angle in the PI0_PI0 subsystem at an incident kinetic energy of 1200 MeV.

Distribution of the cosine of the PI0 angle in the PI0_PI0 subsystem at an incident kinetic energy of 1300 MeV.

Bin averaged hadron level differential cross section for diffractive dijet production as a function of X(C=POMERON). The first systematic error is the uncorrelated and the second the correlated uncertainty.

Bin averaged hadron level differential cross section for diffractive dijet production as a function of Z(C=POMERON). The first systematic error is the uncorrelated and the second the correlated uncertainty.

Bin averaged hadron level differential cross section for diffractive dijet production as a function of the average pseudorapidity of the dijet system. The first systematic error is the uncorrelated and the second the correlated uncertainty.

Bin averaged hadron level differential cross section for diffractive dijet production as a function of the absolute difference of the pseudorapidities of the two jets. The first systematic error is the uncorrelated and the second the correlated uncertainty.

Bin averaged hadron level differential cross section for diffractive dijet production as a function of W. The first systematic error is the uncorrelated and the second the correlated uncertainty.

Bin averaged hadron level differential cross section for diffractive dijet production as a function of the dijet invariant mass. The first systematic error is the uncorrelated and the second the correlated uncertainty.

Bin averaged hadron level differential cross section for diffractive dijet production as a function of mass of the diffractive system. The first systematic error is the uncorrelated and the second the correlated uncertainty.

Bin averaged hadron level double-differential cross section for diffractive dijet production as a function of X(GAMMA) for 3 ranges of ET of jet 1. The first systematic error is the uncorrelated and the second the correlated uncertainty.

Bin averaged hadron level double-differential cross section for diffractive dijet production as a function of Z(POMERON) for 2 ranges of X(GAMMA). The first systematic error is the uncorrelated and the second the correlated uncertainty.

Ratios of the diffractive to the inclusive single-differential hadron level dijet cross sections as a function of X(C=GAMMA). The first systematic error is the uncorrelated and the second the correlated uncertainty.

Ratios of the diffractive to the inclusive single-differential hadron level dijet cross sections as a function of ET of jet 1. The first systematic error is the uncorrelated and the second the correlated uncertainty.

Ratios of the diffractive to the inclusive single-differential hadron level dijet cross sections as a function of the average pseudorapidity of the dijet system. The first systematic error is the uncorrelated and the second the correlated uncertainty.

Ratios of the diffractive to the inclusive single-differential hadron level dijet cross sections as a function of the absolute difference in the pseudorapidities of the 2 jets. The first systematic error is the uncorrelated and the second the correlated uncertainty.

Ratios of the diffractive to the inclusive single-differential hadron level dijet cross sections as a function of the invariant mass of the dijet system. The first systematic error is the uncorrelated and the second the correlated uncertainty.

Ratios of the diffractive to the inclusive single-differential hadron level dijet cross sections as a function of W. The first systematic error is the uncorrelated and the second the correlated uncertainty.

Invariant HE4 PI0 mass distribution at deuteron kinetic energy 1.029 GeV.

Invariant HE4 PI+ mass distribution at deuteron kinetic energy 1.029 GeV.

Invariant HE4 PI- mass distribution at deuteron kinetic energy 1.029 GeV.

Angular distributions of HE4 at incident deuteron energy of 1.029 GeV in the neutral pion channel.

Angular distributions of PI0 at incident deuteron energy of 1.029 GeV in the neutral pion channel.

Angular distributions of PI0 at incident deuteron energy of 1.029 GeV in the neutral pion channel.

Angular distributions of PI0 at incident deuteron energy of 1.029 GeV in the neutral pion channel.

Angular distributions of HE4 at incident deuteron energy of 1.029 GeV in the charged pion channel.

Angular distributions of PI+ at incident deuteron energy of 1.029 GeV in the charged pion channel.

Angular distributions of PI- at incident deuteron energy of 1.029 GeV in the charged pion channel.

Angular distributions of PI+ PI- at incident deuteron energy of 1.029 GeV in the charged pion channel.

Angular distributions of PI+ PI- at incident deuteron energy of 1.029 GeV in the charged pion channel.

Angular distributions of protons in the centre of mass system for the P P --> P N PI+ process.

Angular distributions of pions in the centre of mass system for the P P -->P N PI+ process.

Distribution in the planarity angle DEL(PHI) defined as the projection of the opening angle between two tracks onto the plane normal to the beam vector.