LAMBDA spectrum (1/SIG(had))*D(SIG)/D(X) for UPSILON (2S) direct decays, with X = P/Pmax.

LAMBDA spectrum (1/SIG(had))*D(SIG)/D(X) for continuum data, with X = P/Pmax.

LAMBDA spectrum (1/BETA*SIG(had))*D(SIG)/D(Z) for continuum data, with Z = 2*E/SQRT(S).

XI- spectrum (1/SIG(had))*D(SIG)/D(X) for UPSILON (1S) direct decays, with X = P/Pmax.

XI- spectrum (1/SIG(had))*D(SIG)/D(X) for UPSILON (2S) direct decays, with X = P/Pmax.

XI- spectrum (1/BETA*SIG)*D(SIG)/D(Z) for continuum data, with Z = 2*E/SQRT(S).

LAMBDA spectrum for continuum data.

LAMBDA dsig/dz spectrum from continuum data.

XI- Spectrum from UPSI(1S) direct decays.

XI- Spectrum for continuum data.

XI- dsig/dz spectrum for continuum data.

No description provided.

No description provided.

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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.

Diffractive DIS dijet cross section measured differentially as a function of $\log x_P$. The global normalisation uncertainty of $7.8\%$ is not listed explicitly but is included in the total systematic uncertainty. The last two column show the correction factors for hadronisation and QED radiation, respectively. (Note: assume typo in Table 2 that $x_P$ really means $\log x_P$.).

Diffractive DIS dijet cross section measured differentially as a function of $z_P$. The global normalisation uncertainty of $7.8\%$ is not listed explicitly but is included in the total systematic uncertainty. The last two column show the correction factors for hadronisation and QED radiation, respectively.

Diffractive DIS dijet cross section measured differentially as a function of $p^{\ast}_{T,1}$.

Diffractive DIS dijet cross section measured differentially as a function of $p^{\ast}_{T,2}$.

Diffractive DIS dijet cross section measured differentially as a function of $\langle p^{\ast}_{T}\rangle$.

Diffractive DIS dijet cross section measured differentially as a function of $\Delta\eta^{\ast}$.

Diffractive DIS dijet cross section measured differentially as a function of $z_P$ and $Q^2$.

Diffractive DIS dijet cross section measured differentially as a function of $p^{\ast}_{\rm T,1}$ and $Q^2$.

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.

Differential cross sections for diffractive photoproduction of D*+- mesons as a function of M(C=X).

Differential cross sections for diffractive photoproduction of D*+- mesons as a function of PT(C=D*).

Ratio of cross sections for Diffractive to Inclusive photoproduction of D*+- mesons as a function of PT(C=D*).

Differential cross sections for diffractive photoproduction of D*+- mesons as a function of ETARAP(C=D*).

Ratio of cross sections for Diffractive to Inclusive photoproduction of D*+- mesons as a function of ETARAP(C=D*).

Differential cross sections for diffractive photoproduction of D*+- mesons as a function of Z(C=D*).

Ratio of cross sections for Diffractive to Inclusive photoproduction of D*+- mesons as a function of Z(C=D*).

Differential cross sections for diffractive photoproduction of D*+- mesons as a function of W.

Ratio of cross sections for Diffractive to Inclusive photoproduction of D*+- mesons as a function of W.

Differential cross section for diffractive D*+- production in the DIS region as a function of the inelasticity Y.

Differential cross section for diffractive D*+- production in the DIS region as a function of Q**2.

Differential cross section for diffractive D*+- production in the DIS region as a function of X(NAME=POMERON).

Differential cross section for diffractive D*+- production in the DIS region as a function of Z(NAME=POMERON).

Differential cross section for diffractive D*+- production in the DIS region as a function of BETA.

Differential cross section for diffractive D*+- production in the Photoproduction region as a function of PT of the D*.

Differential cross section for diffractive D*+- production in the Photoproduction region as a function of ETARAP of the D*.

Differential cross section for diffractive D*+- production in the Photoproduction region as a function of the inlasticity Y.

Differential cross section for diffractive D*+- production in the Photoproduction region as a function of X(NAME=POMERON).

Differential cross section for diffractive D*+- production in the Photoproduction region as a function of Z(NAME=POMERON).

Differential cross section for diffractive D*+- production in the DIS region as a function of PT of the D* for the region X(NAME=POMERON) < 0.01.

Differential cross section for diffractive D*+- production in the DIS region as a function of ETARAP of the D*.for the region X(NAME=POMERON) < 0.01.

Differential cross section for diffractive D*+- production in the DIS region as a function of X(NAME=POMERON) for the region X(NAME=POMERON) < 0.01.

Differential cross section for diffractive D*+- production in the DIS region as a function of Z(NAME=POMERON) for the region X(NAME=POMERON) < 0.01.

Reduced cross section for diffractive D*+- production measured in the DIS region from the displaced track analysis.

Differential cross section for diffractive D*+- production measured in the Q**2 region 15 to 100 GeV**2 region as a function of M(X).

Fractional charm contribution to the diffractive cross section obtained from the displaced track method.

Cross section as a function of Z(NAME=POMERON,C=OBSERVED).

Cross section as a function of LOG10(Q**2).

Cross section as a function of PT(P=4,RF=CM).

Cross section as a function of ETARAP(P=4).

Average values, over the specified interval, of the differential hadron level dijet cross section as a function of the invariant mass of the diffractive system (X).

Average values, over the specified interval, of the differential hadron level dijet cross section as a function of W.

Average values, over the specified interval, of the differential hadron level dijet cross section as a function of X(NAME=POMERON).

Average values, over the specified interval, of the differential hadron level dijet cross section as a function of BETA=X/X(NAME=POMERON).

Average values, over the specified interval, of the differential hadron level dijet cross section as a function of Z(NAME=POMERON,C=JETS), the fraction of the hadronic final state energy of the DD system which is contained in the two jets.

Average values, over the specified interval, of the differential hadron level dijet cross section as a function of X(NAME=GAMMA,C=JETS), the fraction ofthe photon momentum which enters the hard scattering.

Average values, over the specified interval, of the differential hadron level dijet cross section as a function of E(NAME=REM,C=GAMMA), the energy sum of all final state hadrons in the photon hemisphere (ETARAP<0) which lie outside the two hightest PT(RF=CM) jet cones.

Average values, over the specified interval, of the differential hadron level dijet cross section as a function of Z(NAME=POMERON,C=JETS), for the LOG10(X(NAME=POMERON)) range -1.5 TO -1.3.

Average values, over the specified interval, of the differential hadron level dijet cross section as a function of Z(NAME=POMERON,C=JETS), for the LOG10(X(NAME=POMERON)) range -1.75 TO -1.5.

Average values, over the specified interval, of the differential hadron level dijet cross section as a function of Z(NAME=POMERON,C=JETS), for the LOG10(X(NAME=POMERON)) range -2.0 TO -1.75.

Average values, over the specified interval, of the differential hadron level dijet cross section as a function of Z(NAME=POMERON,C=JETS), for the LOG10(X(NAME=POMERON)) range < -2.0.

Average values, over the specified interval, of the differential hadron level dijet cross section as a function of Z(NAME=POMERON,C=JETS), for the Q**2 + PT**2 range 20 TO 35 GEV**2.

Average values, over the specified interval, of the differential hadron level dijet cross section as a function of Z(NAME=POMERON,C=JETS), for the Q**2 + PT**2 range 35 TO 45 GEV**2.

Average values, over the specified interval, of the differential hadron level dijet cross section as a function of Z(NAME=POMERON,C=JETS), for the Q**2 + PT**2 range 45 TO 60 GEV**2.

Average values, over the specified interval, of the differential hadron level dijet cross section as a function of Z(NAME=POMERON,C=JETS), for the Q**2 + PT**2 range > 60 GEV**2.

Average values, over the specified interval, of the differential hadron level dijet cross section as a function of Q**2 for the restricted interval X(NAME=POMERON) < 0.01.

Average values, over the specified interval, of the differential hadron level dijet cross section as a function of the average transverse momentum of the two jets in the c.m.frame for the restricted interval X(NAME=POMERON) < 0.01.

Average values, over the specified interval, of the differential hadron level dijet cross section as a function of Z(NAME=POMERON,C=JETS), the fraction of the hadronic final state energy of the DD system which is contained in the two jets for the restricted interval X(NAME=POMERON) < 0.01.

Average values, over the specified interval, of the differential hadron level dijet cross section as a function of PT(NAME=REM,C=POMERON), the PT sum of all final state hadrons in the pomeron hemisphere (ETARAP>0) which lie outside the two hightest PT(RF=CM) jet cones.

Average values, over the specified interval, of the differential hadron level three-jet cross section as a function of the invariant mass of the 3 jet system.

Average values, over the specified interval, of the differential hadron level three-jet cross section as a function of Z(NAME=POMERON,C=3-JETS).

Q**2 dependence of the elastic J/PSI photoproduction cross section.

Slope of the elastic J/PSI photoproduction T distribution.

Slope of the elastic J/PSI photoproduction T distribution.

Spin density matrices of the angular distribution in J/PSI electroproduction.

Ratio of longitudinal to transverse J/PSI electroproduction cross section determined under the assumption of SCHC.

Inclusive and inelastic (MX>10) J/PSI electroproduction cross sections.

Inclusive and inelastic (MX>10) J/PSI electroproduction cross sections.

Inclusive and inelastic (MX>10) J/PSI electroproduction cross sections.

Inclusive and inelastic (MX>10) J/PSI electroproduction cross sections.

Inclusive and inelastic (MX>10) J/PSI electroproduction cross sections.

Inclusive and inelastic (MX>10GEV) differential cross section for J/PSI electroproduction.

Inclusive and inelastic (MX>10GEV) differential cross section for J/PSI electroproduction.

Inclusive and inelastic (MX>10GEV) differential cross section for J/PSI electroproduction.

W dependence of the inclusive and inelastic (Z<0.9) J/PSI photoproduction cross section.

No description provided.

No description provided.

No description provided.