The combined differential $D^{*\pm}$-production cross section as a function of $Q^2$, with its uncorrelated and correlated uncertainties.

The combined differential $D^{*\pm}$-production cross section as a function of $y$, with its uncorrelated and correlated uncertainties.

The combined double-differential $D^{*\pm}$-production cross section as a function of $Q^2$ and $y$, with its uncorrelated and correlated uncertainties.

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 $Q^2$.

Measured differential photoproduction cross sections as a function of the squared transverse momentum of the J/PSI in 4 bins of elasticity.

Measured differential photoproduction cross sections as a function of the elasticity of the J/PSI in 4 bins of transverse momentum.

Measured differential electroproduction cross section as a function of Q**2.

Measured differential electroproduction cross section as a function of the squared transverse momentum of the J/PSI in the GAMMA* P frame.

Measured differential electroproduction cross section as a function of the elasticity of the J/PSI.

Measured differential electroproduction cross section as a function of the photon-proton centre of mass energy W.

Measured differential electroproduction cross section as a function of the squared transverse momentum of the J/PSI in the GAMMA* P rest frame.

Measured differential electroproduction cross section as a function of the squared transverse momentum of the J/PSI in the GAMMA* P rest frame.

Measured differential electroproduction cross section as a function of the squared transverse momentum of the J/PSI in the GAMMA* P rest frame.

Measured differential electroproduction cross section as a function of the elasticity of the J/PSI.

Measured differential electroproduction cross section as a function of the elasticity of the J/PSI.

Measured differential electroproduction cross section as a function of the elasticity of the J/PSI.

Measured polarization parameter in the Helicity Frame. Here ALPHA is given by DSIG/DCOS(THETA) ~ 1+ ALPHA COS(THETA)**2 and NU is given by DSIG/DPHI ~ 1+ ALPHA/3 + (NU/3)*COS(2THETA).

Measured polarization parameter in the Collins-Soper Frame. Here ALPHA is given by DSIG/DCOS(THETA) ~ 1+ ALPHA COS(THETA)**2 and NU is given by DSIG/DPHI ~ 1+ ALPHA/3 + (NU/3)*COS(2THETA).

Measured polarization parameter in the Helicity Frame. Here ALPHA is given by DSIG/DCOS(THETA) ~ 1+ ALPHA COS(THETA)**2 and NU is given by DSIG/DPHI ~ 1+ ALPHA/3 + (NU/3)*COS(2THETA).

Measured polarization parameter in the Collins-Soper Frame. Here ALPHA is given by DSIG/DCOS(THETA) ~ 1+ ALPHA COS(THETA)**2 and NU is given by DSIG/DPHI ~ 1+ ALPHA/3 + (NU/3)*COS(2THETA).

Inclusive Jet Cross Section ${\rm\frac{d\sigma_{jet}}{dP_T}}$.

2-Jet Cross Section ${\rm\frac{d\sigma_{2-jet}}{d\langle P_T \rangle}}$.

3-Jet Cross Section ${\rm\frac{d\sigma_{3-jet}}{d\langle P_T \rangle}}$.

Inclusive Jet Cross Section ${\rm\frac{d^2\sigma_{jet}}{dQ^2dP_T}}$.

2-Jet Cross Section ${\rm\frac{d^2\sigma_{2-jet}}{dQ^2d\langle P_T \rangle}}$.

2-Jet Cross Section ${\rm\frac{d^2\sigma_{2-jet}}{dQ^2d\xi}}$.

3-Jet Cross Section ${\rm\frac{d^2\sigma_{3-jet}}{dQ^2d\langle P_T \rangle}}$.

3-Jet to 2-Jet Cross Sections Ratio ${\rm\frac{d\sigma_{3-jet}}{dQ^2}/\frac{d\sigma_{2-jet}}{dQ^2}}$.

3-Jet to 2-Jet Cross Sections Ratio ${\rm\frac{d\sigma_{3-jet}}{d\langle P_T \rangle}/\frac{d\sigma_{2-jet}}{d\langle P_T \rangle}}$.

3-Jet to 2-Jet Cross Sections Ratio ${\rm\frac{d^2\sigma_{3-jet}}{dQ^2d\langle P_T \rangle}/\frac{d^2\sigma_{2-jet}}{dQ^2d\langle P_T \rangle}}$.

Single differential cross section DSIG/DZ for D*+- production. The DSYS errors are the uncorrelated and correlated systematicuncertainties respectively.

Single differential cross section DSIG/DLOG(Q**2) for D*+- production. The DSYS errors are the uncorrelated and correlated systematicuncertainties respectively.

Single differential cross section DSIG/DX for D*+- production. The DSYS errors are the uncorrelated and correlated systematicuncertainties respectively.

Double differential cross section for D*+- production in the LOG(Q**2) binfrom 2.0 to 2.2. The DSYS errors are the uncorrelated and correlated systematicuncertainties respectively.

Double differential cross section for D*+- production in the LOG(Q**2) binfrom 2.2 to 2.4. The DSYS errors are the uncorrelated and correlated systematicuncertainties respectively.

Double differential cross section for D*+- production in the LOG(Q**2) binfrom 2.4 to 3.0. The DSYS errors are the uncorrelated and correlated systematicuncertainties respectively.

Measured values of the charm contributions to F2 for a mean Q**2 of 120GeV. The third DSYS error is the model uncertainty.

Measured values of the charm contributions to F2 for a mean Q**2 of 200GeV. The third DSYS error is the model uncertainty.

Measured values of the charm contributions to F2 for a mean Q**2 of 400GeV. The third DSYS error is the model uncertainty.

Differential cross section as a function of the photon ETARAP.

Differential cross section as a function of Q**2.

Differential cross section as a function of the photon ET in the ETARAP bins -1.2 to -0.6.

Differential cross section as a function of the photon ET in the ETARAP bins -0.6 to 0.2.

Differential cross section as a function of the photon ET in the ETARAP bins 0.2 to 0.9.

Differential cross section as a function of the photon ET in the ETARAP bins 0.9 to 1.4.

Differential cross section as a function of the photon ET in the ETARAP bins 1.4 to 1.8.

Differential cross section as a function of the photon ET in the higher Q**2 range > 40 GeV**2.

Differential cross section as a function of the photon ETARAP in the higher Q**2 range > 40 GeV**2.

Differential cross section for isolated photon production accompanied by non or at least 1-jet as a function of the photon ET.

Differential cross section for isolated photon production accompanied by non or at least 1-jet as a function of the photon ETARAP.

Differential cross section for isolated photon production accompanied by non or at least 1-jet as a function of Q**2.

The NC cross section DSIG/DX for Q**2 > 10000 GeV**2. There is an additional 1.5 PCT normalization uncertainty.

The CC cross section DSIG/DX for Q**2 > 1000 GeV**2. There is an additional 1.5 PCT normalization uncertainty.

The NC reduced cross section and the electromagnetic structure funcion F2 derived from the data. For Q**2 > 2000 GeV**2 the extraction of F2 is restricted to Y < 0.6.

The CC double differential cross section D2SIG/DX/DQ**2 and the structure function term PHI.

The NC E- P reduced cross section for the high-y analysis. All E- P data not previously reported in EPJ C19 (2001) 269 are given.. There is an additional 1.8 PCT normalization uncertainty.

The NC structure function term PHI and the structure function FL for the E-P data.

The NC structure function term PHI and the structure function FL for the E+P data.

The generalised structure function XF3.

The structure function XF3(C=GAMMA,Z) obtained by averaging over different Q**2 values and transforming to Q**2 = 1500 GeV**2.

Breakdown of errors from table 6, DSIG(C=NC)/DQ**2 as a function of Q**2. All errors are in PCT.

All errors are in PCT.

Breakdown of errors from table 8, DSIG(C=NC)/DX as a function of X. All errors are in PCT.

Breakdown of errors from table 9, DSIG(C=NC)/DX as a function of X. All errors are in PCT.

Breakdown of errors from table 10, DSIG(C=CC)/DX as a function of X. All errors are in PCT.

Breakdown of errors from table 11, F2 as a function of Q**2, X and Y. All errors are in PCT.

Breakdown of errors from table 11, F2 as a function of Q**2, X and Y. PHI(C=NC) is the NC structure function term.. Y+ = 1+(1-Y)**2. DEL(F2),DEL9F3) and DEL(FL) are the corrections to F2 as decribed in the text of the paper.

All errors are in PCT.

Breakdown of errors from table 12, SIG(C=REDUCED) as a function of Q**2 andX. All errors are in PCT.

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.

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).

Single differential visible cross section as a function of LOG(X).

Single differential visible cross section as a function of ETARAP.

Single differential visible cross section as a function of Q**2.

Single differential visible cross section as a function of Z.

Double differential visible cross section as a function of ETARAP and Q**2.

Double differential visible cross section as a function of PT and Q**2.

Double differential visible cross section as a function of ETARAP and Z.

Double differential visible cross section as a function of PT and ETARAP.

Double differential visible cross section as a function of PT and Z.

The inclusive visible D*+ cross section extracted in the DGLAP scheme.

The charm structure function extracted in both the DGLAP and CCFM scheme.

The inclusive 3-JET cross section as a function of Bjorken scaling variableX for the Q**2 range 150 to 5000 GeV**2.

The inclusive 3-JET cross section as a function of the invariant 3-JET massfor the Q**2 range 5 to 100 GeV**2.

The inclusive 3-JET cross section as a function of the invariant 3-JET massfor the Q**2 range 150 to 5000 GeV**2.

Distribution of jet energy fraction X3 = 2E(P=4)/M(P=4_5_6) in the 3 JET centre-of-mass frame for Q**2 from 5 to 100 GeV**2.

Distribution of jet energy fraction X3 = 2E(P=4)/M(P=4_5_6) in the 3 JET centre-of-mass frame for Q**2 from 150 to 5000 GeV**2.

Distribution of jet energy fraction X4 = 2E(P=5)/M(P=4_5_6) in the 3 JET centre-of-mass frame for Q**2 from 5 to 100 GeV**2.

Distribution of jet energy fraction X4 = 2E(P=5)/M(P=4_5_6) in the 3 JET centre-of-mass frame for Q**2 from 150 to 5000 GeV**2.

Distribution of COS(THETA(C=3)) in the 3 JET centre-of-mass frame at Q**2 from 5 to 100 GeV**2. THETA(C=3) is the angle of the most energetic jet with respect to the proton beam direction.

Distribution of COS(THETA(C=3)) in the 3 JET centre-of-mass frame at Q**2 from 150 to 5000 GeV**2. THETA(C=3) is the angle of the most energetic jet with respect to the proton beam direction.

Distribution of PSI(C=3)) in the 3 JET centre-of-mass frame at Q**2 from 5 to 100 GeV**2. PSI(C=3) is the angle between the plane spanned by the highest energy jet and the proton beam and the plane containing the 3 jets.

Distribution of COS(THETA(C=3)) in the 3 JET centre-of-mass frame at Q**2 from 150 to 5000 GeV**2. PSI(C=3) is the angle between the plane spanned by the highest energy jet and the proton beam and the plane containing the 3 jets.

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).

Inclusive di-jet cross section as a function of the di-jet mass M and Q**2.. Data are analysed in the Breit frame using the inclusive kT alogrithm.

Inclusive di-jet cross section as a function of XI (=XBJ/XP) and Q**2.. Data are analysed in the Breit frame using the inclusive kT alogrithm.

Inclusive di-jet cross section as a function of XI (=XBJ/XP) and Q**2.. Data are analysed in the Breit frame using the inclusive kT alogrithm.

Inclusive di-jet cross section as a function of XI (=XBJ/XP) and Q**2.. Data are analysed in the Breit frame using the inclusive kT alogrithm.

Inclusive di-jet cross section as a function of XI (=XBJ/XP) and Q**2.. Data are analysed in the Breit frame using the inclusive kT alogrithm.

Inclusive di-jet cross section as a function of XP and Q**2.. Data are analysed in the Breit frame using the inclusive kT alogrithm.

Inclusive di-jet cross section as a function of XP and Q**2.. Data are analysed in the Breit frame using the inclusive kT alogrithm.

Inclusive di-jet cross section as a function of XP and Q**2.. Data are analysed in the Breit frame using the inclusive kT alogrithm.

Inclusive di-jet cross section as a function of XP and Q**2.. Data are analysed in the Breit frame using the inclusive kT alogrithm.

Inclusive di-jet cross section as a function of X (=XBJ) and Q**2.. Data are analysed in the Breit frame using the inclusive kT alogrithm.

Inclusive di-jet cross section as a function of X (=XBJ) and Q**2.. Data are analysed in the Breit frame using the inclusive kT alogrithm.

Inclusive di-jet cross section as a function of X (=XBJ) and Q**2.. Data are analysed in the Breit frame using the inclusive kT alogrithm.

Inclusive di-jet cross section as a function of X (=XBJ) and Q**2.. Data are analysed in the Breit frame using the inclusive kT alogrithm.

Inclusive di-jet cross section as a function of Y (inelasticity) and Q**2.. Data are analysed in the Breit frame using the inclusive kT alogrithm.

Inclusive di-jet cross section as a function of ETAPRIME ((ETARAP(P=3)-ETARAP(P=4))/2) and ET.. Data are analysed in the Breit frame using the inclusive kT alogrithm.

Inclusive di-jet cross section as a function of ETAPRIME ((ETARAP(P=3)-ETARAP(P=4))/2) and Q**2.. Data are analysed in the Breit frame using the inclusive kT alogrithm.

Inclusive di-jet cross section as a function of ETARAP(forward jet in lab frame) and Q**2.. Data are analysed in the Breit frame using the inclusive kT alogrithm.

Inclusive di-jet cross section as a function of ETARAP(backward jet in lab frame) and Q**2.. Data are analysed in the Breit frame using the inclusive kT alogrithm.

Inclusive single jet cross section as a function of ET and Q**2.. Data are analysed in the Breit frame using the Aachen alogrithm.

Inclusive dijet cross section as a function Q**2.. Data are analysed in the Breit frame using the Aachen alogrithm.

Inclusive di-jet cross section as a function of ET and Q**2.. Data are analysed in the Breit frame using the Aachen alogrithm.

Inclusive di-jet cross section as a function of the di-jet mass M and Q**2.. Data are analysed in the Breit frame using the Aachen alogrithm.

Inclusive di-jet cross section as a function of XI (=XBJ/XP) and Q**2.. Data are analysed in the Breit frame using the Aachen alogrithm.

Inclusive di-jet cross section as a function of XI (=XBJ/XP) and Q**2.. Data are analysed in the Breit frame using the Aachen alogrithm.

Inclusive di-jet cross section as a function of XI (=XBJ/XP) and Q**2.. Data are analysed in the Breit frame using the Aachen alogrithm.

Inclusive di-jet cross section as a function of XI (=XBJ/XP) and Q**2.. Data are analysed in the Breit frame using the Aachen alogrithm.

Inclusive di-jet cross section as a function of XP and Q**2.. Data are analysed in the Breit frame using the Aachen alogrithm.

Inclusive di-jet cross section as a function of XP and Q**2.. Data are analysed in the Breit frame using the Aachen alogrithm.

Inclusive di-jet cross section as a function of XP and Q**2.. Data are analysed in the Breit frame using the Aachen alogrithm.

Inclusive di-jet cross section as a function of XP and Q**2.. Data are analysed in the Breit frame using the Aachen alogrithm.

Data are analysed in the Breit frame using the Aachen alogrithm.

Inclusive di-jet cross section as a function of X (=XBJ) and Q**2.. Data are analysed in the Breit frame using the Aachen alogrithm.

Inclusive di-jet cross section as a function of X (=XBJ) and Q**2.. Data are analysed in the Breit frame using the Aachen alogrithm.

Inclusive di-jet cross section as a function of X (=XBJ) and Q**2.. Data are analysed in the Breit frame using the Aachen alogrithm.

Inclusive di-jet cross section as a function of Y (inelasticity) and Q**2.. Data are analysed in the Breit frame using the Aachen alogrithm.

Inclusive di-jet cross section as a function of ETAPRIME ((ETARAP(P=3)-ETARAP(P=4))/2) and ET.. Data are analysed in the Breit frame using the Aachen alogrithm.

Inclusive di-jet cross section as a function of ETAPRIME ((ETARAP(P=3)-ETARAP(P=4))/2) and Q**2.. Data are analysed in the Breit frame using the Aachen alogrithm.

Data are analysed in the Breit frame using the Aachen alogrithm.

Inclusive di-jet cross section as a function of ETARAP(forward jet in lab frame) and Q**2.. Data are analysed in the Breit frame using the Aachen alogrithm.

Inclusive di-jet cross section as a function of ETARAP(backward jet in lab frame) and Q**2.. Data are analysed in the Breit frame using the Aachen alogrithm.

Inclusive dijet cross section as a function Q**2.. Data are analysed in the Breit frame using the exclusive kT alogrithm.

Inclusive di-jet cross section as a function of ET and Q**2.. Data are analysed in the Breit frame using the exclusive kT alogrithm.

Inclusive di-jet cross section as a function of the di-jet mass M and Q**2.. Data are analysed in the Breit frame using the exclusive kT alogrithm.

Inclusive di-jet cross section as a function of XI (=XBJ/XP) and Q**2.. Data are analysed in the Breit frame using the exclusive kT alogrithm.

Inclusive di-jet cross section as a function of XI (=XBJ/XP) and Q**2.. Data are analysed in the Breit frame using the exclusive kT alogrithm.

Inclusive di-jet cross section as a function of XI (=XBJ/XP) and Q**2.. Data are analysed in the Breit frame using the exclusive kT alogrithm.

Inclusive di-jet cross section as a function of XI (=XBJ/XP) and Q**2.. Data are analysed in the Breit frame using the exclusive kT alogrithm.

Inclusive di-jet cross section as a function of XP and Q**2.. Data are analysed in the Breit frame using the exclusive kT alogrithm.

Inclusive di-jet cross section as a function of XP and Q**2.. Data are analysed in the Breit frame using the exclusive kT alogrithm.

Inclusive di-jet cross section as a function of XP and Q**2.. Data are analysed in the Breit frame using the exclusive kT alogrithm.

Inclusive di-jet cross section as a function of XP and Q**2.. Data are analysed in the Breit frame using the exclusive kT alogrithm.

Inclusive di-jet cross section as a function of X (=XBJ) and Q**2.. Data are analysed in the Breit frame using the exclusive kT alogrithm.

Inclusive di-jet cross section as a function of X (=XBJ) and Q**2.. Data are analysed in the Breit frame using the exclusive kT alogrithm.

Inclusive di-jet cross section as a function of X (=XBJ) and Q**2.. Data are analysed in the Breit frame using the exclusive kT alogrithm.

Inclusive di-jet cross section as a function of X (=XBJ) and Q**2.. Data are analysed in the Breit frame using the exclusive kT alogrithm.

Inclusive di-jet cross section as a function of Y (inelasticity) and Q**2.. Data are analysed in the Breit frame using the exclusive kT alogrithm.

Inclusive di-jet cross section as a function of ETAPRIME ((ETARAP(P=3)-ETARAP(P=4))/2) and ET.. Data are analysed in the Breit frame using the exclusive kT alogrithm.

Inclusive di-jet cross section as a function of ETAPRIME ((ETARAP(P=3)-ETARAP(P=4))/2) and Q**2.. Data are analysed in the Breit frame using the exclusive kT alogrithm.

Inclusive di-jet cross section as a function of ETARAP(forward jet in lab frame) and Q**2.. Data are analysed in the Breit frame using the exclusive kT alogrithm.

Inclusive di-jet cross section as a function of ETARAP(backward jet in lab frame) and Q**2.. Data are analysed in the Breit frame using the exclusive kT alogrithm.

Inclusive dijet cross section as a function Q**2.. Data are analysed in the Breit frame using the Cambridge jet alogrithm.

Inclusive di-jet cross section as a function of ET and Q**2.. Data are analysed in the Breit frame using the Cambridge jet alogrithm.

Inclusive di-jet cross section as a function of the di-jet mass M and Q**2.. Data are analysed in the Breit frame using the Cambridge jet alogrithm.

Inclusive di-jet cross section as a function of XI (=XBJ/XP) and Q**2.. Data are analysed in the Breit frame using the Cambridge jet alogrithm.

Inclusive di-jet cross section as a function of XI (=XBJ/XP) and Q**2.. Data are analysed in the Breit frame using the Cambridge jet alogrithm.

Inclusive di-jet cross section as a function of XI (=XBJ/XP) and Q**2.. Data are analysed in the Breit frame using the Cambridge jet alogrithm.

Inclusive di-jet cross section as a function of XI (=XBJ/XP) and Q**2.. Data are analysed in the Breit frame using the Cambridge jet alogrithm.

Inclusive di-jet cross section as a function of XP and Q**2.. Data are analysed in the Breit frame using the Cambridge jet alogrithm.

Inclusive di-jet cross section as a function of XP and Q**2.. Data are analysed in the Breit frame using the Cambridge jet alogrithm.

Inclusive di-jet cross section as a function of XP and Q**2.. Data are analysed in the Breit frame using the Cambridge jet alogrithm.

Inclusive di-jet cross section as a function of XP and Q**2.. Data are analysed in the Breit frame using the Cambridge jet alogrithm.

Inclusive di-jet cross section as a function of X (=XBJ) and Q**2.. Data are analysed in the Breit frame using the Cambridge jet alogrithm.

Inclusive di-jet cross section as a function of X (=XBJ) and Q**2.. Data are analysed in the Breit frame using the Cambridge jet alogrithm.

Inclusive di-jet cross section as a function of X (=XBJ) and Q**2.. Data are analysed in the Breit frame using the Cambridge jet alogrithm.

Inclusive di-jet cross section as a function of X (=XBJ) and Q**2.. Data are analysed in the Breit frame using the Cambridge jet alogrithm.

Inclusive di-jet cross section as a function of Y (inelasticity) and Q**2.. Data are analysed in the Breit frame using the Cambridge jet alogrithm.

Inclusive di-jet cross section as a function of ETAPRIME ((ETARAP(P=3)-ETARAP(P=4))/2) and ET.. Data are analysed in the Breit frame using the Cambridge jet alogrithm.

Inclusive di-jet cross section as a function of ETAPRIME ((ETARAP(P=3)-ETARAP(P=4))/2) and Q**2.. Data are analysed in the Breit frame using the Cambridge jet alogrithm.

Inclusive di-jet cross section as a function of ETARAP(forward jet in lab frame) and Q**2.. Data are analysed in the Breit frame using the Cambridge jet alogrithm.

Inclusive di-jet cross section as a function of ETARAP(backward jet in lab frame) and Q**2.. Data are analysed in the Breit frame using the Cambridge jet alogrithm.

Axis error includes +- 5/5 contribution (Trigger efficiency).

Axis error includes +- 5/5 contribution (Trigger efficiency).

Axis error includes +- 5/5 contribution (Trigger efficiency).

Axis error includes +- 5/5 contribution (Trigger efficiency).

Axis error includes +- 5/5 contribution (Trigger efficiency).

Axis error includes +- 5/5 contribution (Trigger efficiency).

Axis error includes +- 5/5 contribution (Trigger efficiency).

Axis error includes +- 5/5 contribution (Trigger efficiency).

Axis error includes +- 5/5 contribution (Trigger efficiency).

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.

Total cross-section for E+P events.