The measured differential branching fractions as a function of the invariant hadronic mass squared of the $X_u$ system ($M_X^2$).

The measured differential branching fractions as a function of the light-cone momenta of the hadronic $X_u$ system [$P_+ = (E_X^B - |old{p}_X^B|)$].

The measured differential branching fractions as a function of the light-cone momenta of the hadronic $X_u$ system [$P_- = (E_X^B + |old{p}_X^B|)$].

The background-subtracted yields as a function of $E_\ell^B$.

The background-subtracted yields as a function of $q^2$.

The background-subtracted yields as a function of $M_X$.

The background-subtracted yields as a function of $M_X^2$.

The background-subtracted yields as a function of $P_+$. [$P_+ = (E_X^B - |P_X^B|)$]

The background-subtracted yields as a function of $P_-$. [$P_- = (E_X^B + |P_X^B|)$].

The full experimental correlation matrix for the background-subtracted spectrum of the lepton energy in the $B$ rest frame ($E_\ell^B$).

The full experimental correlation matrix for the background-subtracted spectrum of $q^2$).

The full experimental correlation matrix for the background-subtracted spectrum of $M_X$.

The full experimental correlation matrix for the background-subtracted spectrum of $M_X^2$.

The full experimental correlation matrix for the background-subtracted spectrum of $P_+$.

The full experimental correlation matrix for the background-subtracted spectrum of $P_-$.

Migration matrix of $E_\ell^B$ [in %].

Migration matrix of $q^2$ [in %].

Migration matrix of $M_X$ [in %].

Migration matrix of $M_X^2$ [in %].

Migration matrix of $P_+$ [in %].

Migration matrix of $P_-$ [in %].

The total correction factors and phase space acceptance as a function of the invariant hadronic mass of the $X_u$ system ($M_X$).

The total correction factors and phase space acceptance as a function of the invariant hadronic mass squared of the $X_u$ system ($M_X^2$).

The total correction factors and phase space acceptance as a function of the lepton energy in the $B$ rest frame ($E_\ell^B$).

The total correction factors and phase space acceptance as a function of the four-momentum-transfer squared of the $B$ to the $X_u$ system ($q^2$).

The total correction factors and phase space acceptance as a function of $P_+$.

The total correction factors and phase space acceptance as a function of $P_-$.

The statistical correlations of the differential branching fractions are shown. The matrix elements are ordered for $M_{X}$, $M_{X}^{2}$, $q^{2}$, $E_{\ell}^{B}$, $P_{+}$ and $P_{-}$.

The full experimental (statistical and systematical) correlations of the differential branching fractions are shown. The matrix elements are ordered for $M_{X}$, $M_{X}^{2}$, $q^{2}$, $E_{\ell}^{B}$, $P_{+}$ and $P_{-}$.

The total partial branching fraction with $E_{\ell}^{B} > 1$ GeV. The order of entries is: the 2D fit result of Phys. Rev. D 104, 012008 (2021), the results calcuated with the differential branching fractions of $M_{X}$, $M_{X}^{2}$, $q^{2}$, $E_{\ell}^{B}$, $P_{+}$ and $P_{-}$

The full experimental correlations between the total partial branching fractions from summing the individual bins are shown. The matrix elements are saved in the order of $M_{X}$, $M_{X}^{2}$, $q^{2}$, $E_{\ell}^{B}$, $P_{+}$ and $P_{-}$.

The first moment of the measured differential branching fraction of the lepton energy in the $B$ rest frame ($E_\ell^B$).

The second moment of the measured differential branching fraction of the lepton energy in the $B$ rest frame ($E_\ell^B$).

The third moment of the measured differential branching fraction of the lepton energy in the $B$ rest frame ($E_\ell^B$).

The first moment of the measured differential branching fraction of $q^2$.

The second moment of the measured differential branching fraction of $q^2$.

The third moment of the measured differential branching fraction of $q^2$.

The first moment of the measured differential branching fraction of $M_{X}$.

The second moment of the measured differential branching fraction of $M_{X}$.

The third moment of the measured differential branching fraction of $M_{X}$.

The first moment of the measured differential branching fraction of $P_{+}$.

The second moment of the measured differential branching fraction of $P_{+}$.

The third moment of the measured differential branching fraction of $P_{+}$.

The first moment of the measured differential branching fraction of $P_{-}$.

The second moment of the measured differential branching fraction of $P_{-}$.

The third moment of the measured differential branching fraction of $P_{-}$.

The matrix elements are saved in the order of $M_{X}$, $q^{2}$, $E_{\ell}^{B}$, $P_{+}$ and $P_{-}$. For each variable, the entries is ordered for the first, second and third moments.

Flux-integrated differential $\nu_{e}$ CCQE-like cross section versus electron angle.

Covariance matrix for flux-integrated differential $\nu_{e}$ CCQE-like cross section versus electron angle.

The flux-integrated differential $\nu_{e}$ CCQE-like cross section versus $Q^{2}_{\rm QE}$.

Covariance matrix for the flux-integrated differential $\nu_{e}$ CCQE-like cross section versus $Q^{2}_{\rm QE}$.

The ratio of the MINERvA $\nu_{e}$ CCQE differential cross section as a function of $Q^2_{\rm QE}$ to the analogous result from MINERvA for $\nu_{\mu}$ [Phys.Rev.Lett. 111 (2013) 022502].

Covariance matrix for the ratio of the MINERvA $\nu_{e}$ CCQE differential cross section as a function of $Q^2_{\rm QE}$ to the analogous result from MINERvA for $\nu_{\mu}$ [Phys.Rev.Lett. 111 (2013) 022502].

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 $Q^2$.

Differential cross sections for inclusive jet production in charm events as a function of ETARAP(JET) for -1.6 < ETARAP(JET) < 2.2. The measurements are given together with their statistical and systematic uncertainties. Hadronisation and QED radiative corrections, CHAD and CRAD, respectively, are also shown.

Differential cross sections for inclusive jet production in beauty events as a function of Q**2 for 5 < Q**2 < 1000 GeV**2. The measurements are given together with their statistical and systematic uncertainties. Hadronisation and QED radiative corrections, CHAD and CRAD, respectively, are also shown.

Differential cross sections for inclusive jet production in beauty events as a function of Q**2 for 5 < Q**2 < 1000 GeV**2. The measurements are given together with their statistical and systematic uncertainties. Hadronisation and QED radiative corrections, CHAD and CRAD, respectively, are also shown.

Differential cross sections for inclusive jet production in beauty events as a function of XB. The measurements are given together with their statistical and systematic uncertainties. Hadronisation and QED radiative corrections, CHAD and CRAD, respectively, are also shown.

Differential cross sections for inclusive jet production in charm events as a function of XB. The measurements are given together with their statistical and systematic uncertainties. Hadronisation and QED radiative corrections, CHAD and CRAD, respectively, are also shown.

Double-differential cross sections for inclusive jet production in beauty events as a function of XB for 5 < Q**2 < 20 GeV**2. The measurements are given together with their statistical and systematic uncertainties. Hadronisation and QED radiative corrections, CHAD and CRAD, respectively, are also shown.

Double-differential cross sections for inclusive jet production in beauty events as a function of XB for 20 < Q**2 < 60 GeV**2. The measurements are given together with their statistical and systematic uncertainties. Hadronisation and QED radiative corrections, CHAD and CRAD, respectively, are also shown.

Double-differential cross sections for inclusive jet production in beauty events as a function of XB for 60 < Q**2 < 120 GeV**2. The measurements are given together with their statistical and systematic uncertainties. Hadronisation and QED radiative corrections, CHAD and CRAD, respectively, are also shown.

Double-differential cross sections for inclusive jet production in beauty events as a function of XB for 120 < Q**2 < 400 GeV**2. The measurements are given together with their statistical and systematic uncertainties. Hadronisation and QED radiative corrections, CHAD and CRAD, respectively, are also shown.

Double-differential cross sections for inclusive jet production in beauty events as a function of XB for 400 < Q**2 < 1000 GeV**2. The measurements are given together with their statistical and systematic uncertainties. Hadronisation and QED radiative corrections, CHAD and CRAD, respectively, are also shown.

Double-differential cross sections for inclusive jet production in charm events as a function of XB for 5 < Q**2 < 20 GeV**2. The measurements are given together with their statistical and systematic uncertainties. Hadronisation and QED radiative corrections, CHAD and CRAD, respectively, are also shown.

Double-differential cross sections for inclusive jet production in charm events as a function of XB for 20 < Q**2 < 60 GeV**2. The measurements are given together with their statistical and systematic uncertainties. Hadronisation and QED radiative corrections, CHAD and CRAD, respectively, are also shown.

Double-differential cross sections for inclusive jet production in charm events as a function of XB for 60 < Q**2 < 120 GeV**2. The measurements are given together with their statistical and systematic uncertainties. Hadronisation and QED radiative corrections, CHAD and CRAD, respectively, are also shown.

Double-differential cross sections for inclusive jet production in charm events as a function of XB for 120 < Q**2 < 400 GeV**2. The measurements are given together with their statistical and systematic uncertainties. Hadronisation and QED radiative corrections, CHAD and CRAD, respectively, are also shown.

Double-differential cross sections for inclusive jet production in charm events as a function of XB for 400 < Q**2 < 1000 GeV**2. The measurements are given together with their statistical and systematic uncertainties. Hadronisation and QED radiative corrections, CHAD and CRAD, respectively, are also shown.

The structure function F2(BOTTOM BOTTOMBAR) and the reduced beauty cross sections SIGR(BOTTOM BOTTOMBAR), both as functions of XB and Q**2. The measurements are given together with their statistical, systematic and extrapolation uncertainties.

The structure function F2(BOTTOM BOTTOMBAR) and the reduced beauty cross sections SIGR(BOTTOM BOTTOMBAR), both as functions of XB and Q**2. The measurements are given together with their statistical, systematic and extrapolation uncertainties.

The structure function F2(BOTTOM BOTTOMBAR) and the reduced beauty cross sections SIGR(BOTTOM BOTTOMBAR), both as functions of XB and Q**2. The measurements are given together with their statistical, systematic and extrapolation uncertainties.

The structure function F2(BOTTOM BOTTOMBAR) and the reduced beauty cross sections SIGR(BOTTOM BOTTOMBAR), both as functions of XB and Q**2. The measurements are given together with their statistical, systematic and extrapolation uncertainties.

The structure function F2(BOTTOM BOTTOMBAR) and the reduced beauty cross sections SIGR(BOTTOM BOTTOMBAR), both as functions of XB and Q**2. The measurements are given together with their statistical, systematic and extrapolation uncertainties.

The structure function F2(CHARM CHARMBAR) and the reduced charm cross sections SIGR(CHARM CHARMBAR), both as functions of XB and Q**2. The measurements are given together with their statistical, systematic and extrapolation uncertainties.

The structure function F2(CHARM CHARMBAR) and the reduced charm cross sections SIGR(CHARM CHARMBAR), both as functions of XB and Q**2. The measurements are given together with their statistical, systematic and extrapolation uncertainties.

The structure function F2(CHARM CHARMBAR) and the reduced charm cross sections SIGR(CHARM CHARMBAR), both as functions of XB and Q**2. The measurements are given together with their statistical, systematic and extrapolation uncertainties.

The structure function F2(CHARM CHARMBAR) and the reduced charm cross sections SIGR(CHARM CHARMBAR), both as functions of XB and Q**2. The measurements are given together with their statistical, systematic and extrapolation uncertainties.

The structure function F2(CHARM CHARMBAR) and the reduced charm cross sections SIGR(CHARM CHARMBAR), both as functions of XB and Q**2. The measurements are given together with their statistical, systematic and extrapolation uncertainties.

Double differential cross section for Q^2=1200 GeV^2.

Double differential cross section for Q^2=1400 GeV^2.

Double differential cross section for Q^2=1650 GeV^2.

Double differential cross section for Q^2=1950 GeV^2.

Double differential cross section for Q^2=2250 GeV^2.

Double differential cross section for Q^2=2600 GeV^2.

Double differential cross section for Q^2=3000 GeV^2.

Double differential cross section for Q^2=3500 GeV^2.

Double differential cross section for Q^2=4150 GeV^2.

Double differential cross section for Q^2=5250 GeV^2.

Double differential cross section for Q^2=7000 GeV^2.

Double differential cross section for Q^2=9500 GeV^2.

Double differential cross section for Q^2=15500 GeV^2.

Cross section integrated in X over the region Xedge-1.

The predicted CC1$\pi^{-}$ background in units of fb/GeV $(10^{-39}~\mbox{cm}^2)/\mbox{GeV}$ . This background corresponds to an empirical adjustment of the Rein-Sehgal calculation based on the MiniBooNE CC1$\pi^{+}$ data.

The MiniBooNE numub single differential cross section $\frac{d\sigma}{dQ^2_{QE}}$ on mineral oil, shape error, and the predicted CCQE-like and CC1$\pi^{-}$ backgrounds in units of fb $(10^{-39} \mbox{cm}^2)$. Not included in the table is the total normalization error of 13.0$\%$.

The MiniBooNE $\bar{\nu}_\mu$ CCQE total cross section on mineral oil, total and shape errors, and predicted CCQE-like and CC1$\pi^{-}$ backgrounds in bins of $E_\nu^{\textrm{QE,RFG}}$ and units of fb $(10^{-39} \mbox{cm}^2)$. The total error includes both the shape and normalization uncertainties. Note that the total error is incorrectly quoted as a power of 10 too low in the paper and the preprint. It is corrected in the resource file from which these data here are taken.

The MiniBooNE $\bar{\nu}_\mu$ CCQE double-differential cross section, with the shape uncertainty, on carbon. The units are fb/GeV $(10^{-39} \mbox{cm}^2/\mbox{GeV})$. Not included in the table is the total normalization uncertainty of 17.4%.

The QE-like $\bar{\nu}_\mu$ background subtracted from the double-differential cross section on carbon. The $\bar{\nu}_\mu$ CCQE interactions with hydrogen are treated as background in this calculation, and so their contribution is included here. The units are fb/GeV $(10^{-39} \mbox{cm}^2/\mbox{GeV})$ .

The MiniBooNE $\bar{\nu}_\mu$ CCQE single differential cross section $\frac{d\sigma}{dQ^2_{QE}}$ on carbon, shape error, and CCQE-like background in units of fb/GeV$^2$ $(10^{-39} \mbox{cm}^2/\mbox{GeV}^2)$ . The $\bar{\nu}_\mu$ CCQE content is treated as background. Not included in the table is the total normalization error of 17.4%.

The MiniBooNE $\bar{\nu}_\mu$ CCQE total cross section on carbon, total and shape errors, and predicted CCQE-like background in bins of $E_\nu^{\textrm{QE,RFG}}$ and units of fb $(10^{-39} \mbox{cm}^2)$. The total error includes both the shape and normalization uncertainties.

The single-differential cross section DSIG/DX (Y<0.9,Y(1-x)**2>0.004) at Q^2=3000 GeV^2, corrected to the electroweak Born level, for zero (Pe=0), positive (Pe=+0.32) and negative (Pe=-0.36) polarisations.

The single-differential cross section DSIG/DY (Y<0.9,Y(1-x)**2>0.004) at Q^2=185 GeV^2, corrected to the electroweak Born level, for zero (Pe=0), positive (Pe=+0.32) and negative (Pe=-0.36) polarisations.

The single-differential cross section DSIG/DY (Y<0.9,Y(1-x)**2>0.004) at Q^2=3000 GeV^2, corrected to the electroweak Born level, for zero (Pe=0), positive (Pe=+0.32) and negative (Pe=-0.36) polarisations.

The reduced cross section SIG(Reduced) at Q^2=200 GeV^2, corrected to the electroweak Born level, for zero (Pe=0), positive (Pe=+0.32) and negative (Pe=-0.36) polarisations.

The reduced cross section SIG(Reduced) at Q^2=250 GeV^2, corrected to the electroweak Born level, for zero (Pe=0), positive (Pe=+0.32) and negative (Pe=-0.36) polarisations.

The reduced cross section SIG(Reduced) at Q^2=350 GeV^2, corrected to the electroweak Born level, for zero (Pe=0), positive (Pe=+0.32) and negative (Pe=-0.36) polarisations.

The reduced cross section SIG(Reduced) at Q^2=450 GeV^2, corrected to the electroweak Born level, for zero (Pe=0), positive (Pe=+0.32) and negative (Pe=-0.36) polarisations.

The reduced cross section SIG(Reduced) at Q^2=650 GeV^2, corrected to the electroweak Born level, for zero (Pe=0), positive (Pe=+0.32) and negative (Pe=-0.36) polarisations.

The reduced cross section SIG(Reduced) at Q^2=800 GeV^2, corrected to the electroweak Born level, for zero (Pe=0), positive (Pe=+0.32) and negative (Pe=-0.36) polarisations.

The reduced cross section SIG(Reduced) at Q^2=1200 GeV^2, corrected to the electroweak Born level, for zero (Pe=0), positive (Pe=+0.32) and negative (Pe=-0.36) polarisations.

The reduced cross section SIG(Reduced) at Q^2=1500 GeV^2, corrected to the electroweak Born level, for zero (Pe=0), positive (Pe=+0.32) and negative (Pe=-0.36) polarisations.

The reduced cross section SIG(Reduced) at Q^2=2000 GeV^2, corrected to the electroweak Born level, for zero (Pe=0), positive (Pe=+0.32) and negative (Pe=-0.36) polarisations.

The reduced cross section SIG(Reduced) at Q^2=3000 GeV^2, corrected to the electroweak Born level, for zero (Pe=0), positive (Pe=+0.32) and negative (Pe=-0.36) polarisations.

The reduced cross section SIG(Reduced) at Q^2=5000 GeV^2, corrected to the electroweak Born level, for zero (Pe=0), positive (Pe=+0.32) and negative (Pe=-0.36) polarisations.

The reduced cross section SIG(Reduced) at Q^2=8000 GeV^2, corrected to the electroweak Born level, for zero (Pe=0), positive (Pe=+0.32) and negative (Pe=-0.36) polarisations.

The reduced cross section SIG(Reduced) at Q^2=12000 GeV^2, corrected to the electroweak Born level, for zero (Pe=0), positive (Pe=+0.32) and negative (Pe=-0.36) polarisations.

The reduced cross section SIG(Reduced) at Q^2=20000 GeV^2, corrected to the electroweak Born level, for zero (Pe=0), positive (Pe=+0.32) and negative (Pe=-0.36) polarisations.

The reduced cross section SIG(Reduced) at Q^2=30000 GeV^2, corrected to the electroweak Born level, for zero (Pe=0), positive (Pe=+0.32) and negative (Pe=-0.36) polarisations.

The structure function xF3 at Q^2=1500, 2000 and 3000 GeV^2 extracted using this data at Pe=0 and previously published NC E-P DIS data.

The structure function xF3 at Q^2=5000, 8000 and 12000 GeV^2 extracted using this data at Pe=0 and previously published NC E-P DIS data.

The structure function xF3 at Q^2=20000 and 30000 GeV^2 extracted using this data at Pe=0 and previously published NC E-P DIS data.

The interference structure function XF3(gammaZ) evaulated at Q^2=1500 GeV^2 in X centred bins.

The polarisation asymmetry measured using the positively and negatively polarised positron beams.

The measured differential cross section as a function of the pseudorapidity of the photon.

The measured differential cross section as a function of the transverse energy of the jet.

The measured differential cross section as a function of the pseudorapidity of the jet.

Total visible cross section for LAMBDA/C+ production for the two decay channels combined. The second systematic error reflects the uncertainty in the branching ratios.

Measured D+ cross section as a function of the D+ transverse momentum.

Measured D+ cross section as a function of the D+ pseudorapidity.

Measured D+ cross section as a function of Q**2.

Measured D+ cross section as a function of the Bjorken X.

The measured differential cross section DSIG/DQ**2 for inclusive jet production using the SIScone jet algorithm.

The measured differential cross section DSIG/DET for inclusive jet production in the Q**2 region 125 to 250 GeV for the anti-KT jet algorithm.

The measured differential cross section DSIG/DET for inclusive jet production in the Q**2 region 250 to 500 GeV for the anti-KT jet algorithm.

The measured differential cross section DSIG/DET for inclusive jet production in the Q**2 region 500 to 1000 GeV for the anti-KT jet algorithm.

The measured differential cross section DSIG/DET for inclusive jet production in the Q**2 region 1000 to 2000 GeV for the anti-KT jet algorithm.

The measured differential cross section DSIG/DET for inclusive jet production in the Q**2 region 2000 to 5000 GeV for the anti-KT jet algorithm.

The measured differential cross section DSIG/DET for inclusive jet production in the Q**2 region 5000 to 100000 GeV for the anti-KT jet algorithm.

The measured differential cross section DSIG/DET for inclusive jet production in the Q**2 region 125 to 250 GeV for the SIScone jet algorithm.

The measured differential cross section DSIG/DET for inclusive jet production in the Q**2 region 250 to 500 GeV for the SIScone jet algorithm.

The measured differential cross section DSIG/DET for inclusive jet production in the Q**2 region 500 to 1000 GeV for the SIScone jet algorithm.

The measured differential cross section DSIG/DET for inclusive jet production in the Q**2 region 1000 to 2000 GeV for the SIScone jet algorithm.

The measured differential cross section DSIG/DET for inclusive jet production in the Q**2 region 2000 to 5000 GeV for the SIScone jet algorithm.

The measured differential cross section DSIG/DET for inclusive jet production in the Q**2 region 5000 to 100000 GeV for the SIScone jet algorithm.

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 dijet cross-sections ${d\sigma/dM_{jj}}$. Other details as in the caption to Table 1.

Inclusive dijet cross-sections ${d\sigma/d\eta^{*}}$. Other details as in the caption to Table 1.

Inclusive dijet cross-sections ${d\sigma/d\log_{10}\left(\xi\right)}$. Other details as in the caption to Table 1.

Inclusive dijet cross-sections ${d\sigma/d\log_{10}\left(\xi\right)}$ for ${Q^{2}}$ between 125 and 250 GeV$^2$. Other details as in the caption to Table 1.

Inclusive dijet cross-sections ${d\sigma/d\log_{10}\left(\xi\right)}$ for ${Q^{2}}$ between 250 and 500 GeV$^2$. Other details as in the caption to Table 1.

Inclusive dijet cross-sections ${d\sigma/d\log_{10}\left(\xi\right)}$ for ${Q^{2}}$ between 500 and 1000 GeV$^2$. Other details as in the caption to Table 1.

Inclusive dijet cross-sections ${d\sigma/d\log_{10}\left(\xi\right)}$ for ${Q^{2}}$ between 1000 and 2000 GeV$^2$. Other details as in the caption to Table 1.

Inclusive dijet cross-sections ${d\sigma/d\log_{10}\left(\xi\right)}$ for ${Q^{2}}$ between 2000 and 5000 GeV$^2$. Other details as in the caption to Table 1.

Inclusive dijet cross-sections ${d\sigma/d\log_{10}\left(\xi\right)}$ for ${Q^{2}}$ between 5000 and 20000 GeV$^2$. Other details as in the caption to Table 1.

Inclusive dijet cross-sections ${d\sigma/d\overline{E^{jet}_{T,B}}}$ for ${Q^{2}}$ between 125 and 250 GeV$^2$. Other details as in the caption to Table 1.

Inclusive dijet cross-sections ${d\sigma/d\overline{E^{jet}_{T,B}}}$ for ${Q^{2}}$ between 250 and 500 GeV$^2$. Other details as in the caption to Table 1.

Inclusive dijet cross-sections ${d\sigma/d\overline{E^{jet}_{T,B}}}$ for ${Q^{2}}$ between 500 and 1000 GeV$^2$. Other details as in the caption to Table 1.

Inclusive dijet cross-sections ${d\sigma/d\overline{E^{jet}_{T,B}}}$ for ${Q^{2}}$ between 1000 and 2000 GeV$^2$. Other details as in the caption to Table 1.

Inclusive dijet cross-sections ${d\sigma/d\overline{E^{jet}_{T,B}}}$ for ${Q^{2}}$ between 2000 and 5000 GeV$^2$. Other details as in the caption to Table 1.

Inclusive dijet cross-sections ${d\sigma/d\overline{E^{jet}_{T,B}}}$ for ${Q^{2}}$ between 5000 and 20000 GeV$^2$. Other details as in the caption to Table 1.

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

Measured differential cross section as a function of the muon pseudorapidity.

Measured differential cross section as a function of the jet transverse momentum.

Measured differential cross section as a function of the jet pseudorapidity.

Measured cross sections for beauty production with a muon and jet for the Q**2 bin 2 to 4 GeV**2.

Measured cross sections for beauty production with a muon and jet for the Q**2 bin 4 to 20 GeV**2.

Measured cross sections for beauty production with a muon and jet for the Q**2 bin 20 to 45 GeV**2.

Measured cross sections for beauty production with a muon and jet for the Q**2 bin 45 to 100 GeV**2.

Measured cross sections for beauty production with a muon and jet for the Q**2 bin 100 to 250 GeV**2.

Measured cross sections for beauty production with a muon and jet for the Q**2 bin 250 to 3000 GeV**2.

Extracted values of F2 for B-BBAR production at an X value of 0.00013. The second systematic error is the uncertainty on the extrapolation to the full muon and jet phase space.

Extracted values of F2 for B-BBAR production at an X value of 0.0002. The second systematic error is the uncertainty on the extrapolation to the full muon and jet phase space.

Extracted values of F2 for B-BBAR production at an X value of 0.0005. The second systematic error is the uncertainty on the extrapolation to the full muon and jet phase space.

Extracted values of F2 for B-BBAR production at an X value of 0.002. The second systematic error is the uncertainty on the extrapolation to the full muon and jet phase space.

Extracted values of F2 for B-BBAR production at an X value 0.005.

Extracted values of F2 for B-BBAR production at an X value of 0.013. The second systematic error is the uncertainty on the extrapolation to the full muon and jet phase space.

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.

Measured differential cross section DSIG/DQ**2.

Measured differential cross section DSIG/DX.

Pseudorapidity distribution with additional kinematical restraints on Q**2 and ET.

Differential cross section DSIG/DX for the two values of longitudinal polarization of the electron beam.

Differential cross section DSIG/DY for the two values of longitudinal polarization of the electron beam.

Values of the differential cross section DSIG/DQ**2 with detailed statistical and systematic errors.. The first DSYS is the uncorrelated systematic error and the second is the calorimeter energy scale uncertainty which has significant correlation between cross section bins.

Values of the differential cross section DSIG/DX with detailed statistical and systematic errors.. The first DSYS is the uncorrelated systematic error and the second is the calorimeter energy scale uncertainty which has significant correlation between cross section bins.

Values of the differential cross section DSIG/DY with detailed statistical and systematic errors.. The first DSYS is the uncorrelated systematic error and the second is the calorimeter energy scale uncertainty which has significant correlation between cross section bins.

Values of the differential cross section DSIG/DQ**2 with detailed statistical and systematic errors.. The first DSYS is the uncorrelated systematic error and the second is the calorimeter energy scale uncertainty which has significant correlation between cross section bins.

Values of the differential cross section DSIG/DX with detailed statistical and systematic errors.. The first DSYS is the uncorrelated systematic error and the second is the calorimeter energy scale uncertainty which has significant correlation between cross section bins.

Values of the differential cross section DSIG/DY with detailed statistical and systematic errors.. The first DSYS is the uncorrelated systematic error and the second is the calorimeter energy scale uncertainty which has significant correlation between cross section bins.

Values of the reduced cross section for 3 values of longitudinal polarization of the electron beam for Q**2 = 280 GeV**2.

Values of the reduced cross section for 3 values of longitudinal polarization of the electron beam for Q**2 = 530 GeV**2.

Values of the reduced cross section for 3 values of longitudinal polarization of the electron beam for Q**2 = 950 GeV**2.

Values of the reduced cross section for 3 values of longitudinal polarization of the electron beam for Q**2 = 1700 GeV**2.

Values of the reduced cross section for 3 values of longitudinal polarization of the electron beam for Q**2 = 3000 GeV**2.

Values of the reduced cross section for 3 values of longitudinal polarization of the electron beam for Q**2 = 5300 GeV**2.

Values of the reduced cross section for 3 values of longitudinal polarization of the electron beam for Q**2 = 9500 GeV**2.

Values of the reduced cross section for 3 values of longitudinal polarization of the electron beam for Q**2 = 17000 GeV**2.

Values of the reduced cross section for 3 values of longitudinal polarization of the electron beam for Q**2 = 30000 GeV**2.

Values of the reduced cross section with detailed statistical and systematic errors.. The first DSYS is the uncorrelated systematic error and the second is the calorimeter energy scale uncertainty which has significant correlationS between cross section bins.

Values of the reduced cross section with detailed statistical and systematic errors.. The first DSYS is the uncorrelated systematic error and the second is the calorimeter energy scale uncertainty which has significant correlationS between cross section bins.

Values of the reduced cross section with detailed statistical and systematic errors.. The first DSYS is the uncorrelated systematic error and the second is the calorimeter energy scale uncertainty which has significant correlationS between cross section bins.

Values of the reduced cross section with detailed statistical and systematic errors.. The first DSYS is the uncorrelated systematic error and the second is the calorimeter energy scale uncertainty which has significant correlationS between cross section bins.

Values of the reduced cross section with detailed statistical and systematic errors.. The first DSYS is the uncorrelated systematic error and the second is the calorimeter energy scale uncertainty which has significant correlationS between cross section bins.

Values of the reduced cross section with detailed statistical and systematic errors.. The first DSYS is the uncorrelated systematic error and the second is the calorimeter energy scale uncertainty which has significant correlationS between cross section bins.

Values of the reduced cross section with detailed statistical and systematic errors.. The first DSYS is the uncorrelated systematic error and the second is the calorimeter energy scale uncertainty which has significant correlationS between cross section bins.

Values of the reduced cross section with detailed statistical and systematic errors.. The first DSYS is the uncorrelated systematic error and the second is the calorimeter energy scale uncertainty which has significant correlationS between cross section bins.

Values of the reduced cross section with detailed statistical and systematic errors.. The first DSYS is the uncorrelated systematic error and the second is the calorimeter energy scale uncertainty which has significant correlationS between cross section bins.

Values of the reduced cross section with detailed statistical and systematic errors.. The first DSYS is the uncorrelated systematic error and the second is the calorimeter energy scale uncertainty which has significant correlationS between cross section bins.

Values of the reduced cross section with detailed statistical and systematic errors.. The first DSYS is the uncorrelated systematic error and the second is the calorimeter energy scale uncertainty which has significant correlationS between cross section bins.

Values of the reduced cross section with detailed statistical and systematic errors.. The first DSYS is the uncorrelated systematic error and the second is the calorimeter energy scale uncertainty which has significant correlationS between cross section bins.

Values of the reduced cross section with detailed statistical and systematic errors.. The first DSYS is the uncorrelated systematic error and the second is the calorimeter energy scale uncertainty which has significant correlationS between cross section bins.

Values of the reduced cross section with detailed statistical and systematic errors.. The first DSYS is the uncorrelated systematic error and the second is the calorimeter energy scale uncertainty which has significant correlationS between cross section bins.

Values of the reduced cross section with detailed statistical and systematic errors.. The first DSYS is the uncorrelated systematic error and the second is the calorimeter energy scale uncertainty which has significant correlationS between cross section bins.

Values of the reduced cross section with detailed statistical and systematic errors.. The first DSYS is the uncorrelated systematic error and the second is the calorimeter energy scale uncertainty which has significant correlationS between cross section bins.

Values of the reduced cross section with detailed statistical and systematic errors.. The first DSYS is the uncorrelated systematic error and the second is the calorimeter energy scale uncertainty which has significant correlationS between cross section bins.

Values of the reduced cross section with detailed statistical and systematic errors.. The first DSYS is the uncorrelated systematic error and the second is the calorimeter energy scale uncertainty which has significant correlationS between cross section bins.

Differential K0S cross section as a function of Q**2 in the laboratory frame.

Differential K0S cross section as a function of X in the laboratory frame.

Differential K0S cross section as a function of PT in the laboratory frame.

Differential K0S cross section as a function of ETARAP in the laboratory frame.

Differential LAMBDA cross section as a function of Q**2 in the laboratory frame.

Differential LAMBDA cross section as a function of X in the laboratory frame.

Differential LAMBDA cross section as a function of PT in the laboratory frame.

Differential LAMBDA cross section as a function of ETARAP in the laboratoryframe.

Differential K0S cross section as a function of PT in the target hemisphere of the Breit frame.

Differential K0S cross section as a function of PT in the current hemisphere of the Breit frame.

Differential K0S cross section as a function of XP(Breit) in the target hemisphere of the Breit frame.

Differential K0S cross section as a function of XP(Breit) in the current hemisphere of the Breit frame.

Differential LAMBDA cross section as a function of PT in the target hemisphere of the Breit frame.

Differential LAMBDA cross section as a function of PT in the current hemisphere of the Breit frame.

Differential LAMBDA cross section as a function of XP(Breit) in the target hemisphere of the Breit frame.

Differential LAMBDA cross section as a function of XP(Breit) in the currenthemisphere of the Breit frame.

Value of the LAMBDA/K0S cross section ratio as a function of Q**2.

Value of the LAMBDA/K0S cross section ratio as a function of X.

Value of the LAMBDA/K0S cross section ratio as a function of PT.

Value of the LAMBDA/K0S cross section ratio as a function of ETARAP.

Value of the LAMBDA/K0S cross section ratio as a function of PT in the target hemisphere of the Breit frame.

Value of the LAMBDA/K0S cross section ratio as a function of PT in the current hemisphere of the Breit frame.

Value of the LAMBDA/K0S cross section ratio as a function of X in the target hemisphere of the Breit frame.

Value of the LAMBDA/K0S cross section ratio as a function of X in the current hemisphere of the Breit frame.

Value of the HADRON+-/K0S cross section ratio as a function of Q**2.

Value of the HADRON+-/K0S cross section ratio as a function of X.

Value of the HADRON+-/K0S cross section ratio as a function of PT.

Value of the HADRON+-/K0S cross section ratio as a function of ETARAP.

Measured D+- cross section as a function of X.

Measured D+- cross section as a function of the transverse momentum of the D meson.

Measured D+- cross section as a function of the pseudorapidity of the D meson.

Measured D0/DBAR0 cross section as a function of Q**2.

Measured D0/DBAR0 cross section as a function of X.

Measured D0/DBAR0 cross section as a function of the transverse momentum of the D meson.

Measured D0/DBAR0 cross section as a function of the pseudorapidity of the D meson.

Measured cross section for D+- mesons in Q**2 and Y bins.

Measured cross section for D0/DBAR0 mesons in Q**2 and Y bins.

The extracted values of the F2(NAME=CHARM) structure function from the production cross section of D+- mesons.. The second systematic error is from the extrapolation to the full phase space.

The extracted values of the F2(NAME=CHARM) structure function from the production cross section of D+- mesons.. The second systematic error is from the extrapolation to the full phase space.

The extracted values of the F2(NAME=CHARM) structure function from the production cross section of D+- mesons.. The second systematic error is from the extrapolation to the full phase space.

The extracted values of the F2(NAME=CHARM) structure function from the production cross section of D0/DBAR0 mesons not coming from D*+- decays.. The second systematic error is from the extrapolation to the full phase space.

The extracted values of the F2(NAME=CHARM) structure function from the production cross section of D0/DBAR0 mesons not coming from D*+- decays.. The second systematic error is from the extrapolation to the full phase space.

The extracted values of the F2(NAME=CHARM) structure function from the production cross section of D0/DBAR0 mesons not coming from D*+- decays.. The second systematic error is from the extrapolation to the full phase space.

The combined F2(NAME=CHARM) structure function from the production cross section of D+- and D0/DBAR0 mesons.. The second systematic error is from the extrapolation to the full phase space.. The additional error from the branching ratio is 3.3 PCT.

The combined F2(NAME=CHARM) structure function from the production cross section of D+- and D0/DBAR0 mesons.. The second systematic error is from the extrapolation to the full phase space.. The additional error from the branching ratio is 3.3 PCT.

The combined F2(NAME=CHARM) structure function from the production cross section of D+- and D0/DBAR0 mesons.. The second systematic error is from the extrapolation to the full phase space.. The additional error from the branching ratio is 3.3 PCT.

3-jet cross section normalised to 2-jet cross section in bins of $Q^{2}$.

Normalised inclusive jet cross section in bins of $Q^{2}$ and $P_{T}$.

Normalised 2-jet cross section in bins of $Q^{2}$ and $\langle P_{T} \rangle$.

Normalised 2-jet cross sections in bins of $Q^2$ and $\xi$.

Differential polarized inclusive jet cross sections as a function of jet transverse energy.

Differential polarized inclusive jet cross sections as a function of photon virtuality, Q**2.

Differential polarized inclusive jet cross sections as a function of photon virtuality, Q**2.

Differential polarized inclusive jet cross sections as a function of X. Update: contrary to the publication, this is D(SIG)/DLOG10(X) not D(SIG)/DX.

Differential polarized inclusive jet cross sections as a function of X. Update: contrary to the publication, this is D(SIG)/DLOG10(X) not D(SIG)/DX.

Integrated polarized inclusive-jet cross section in the given kinematical range for the E- beam.

Integrated polarized inclusive-jet cross section in the given kinematical range for the E+ beam.

Differential unpolarized cross section for single jet production as a function of the jet pseudorapidity.

Differential unpolarized cross section for two jet production as a function of the mean jet pseudorapidity.

Differential unpolarized cross section for three jet production as a function of the mean jet pseudorapidity.

Differential unpolarized cross section for single jet production as a function of the jet transverse energy.

Differential unpolarized cross section for two jet production as a function of the mean jet transverse energy.

Differential unpolarized cross section for three jet production as a function of the mean jet transverse energy.

Differential unpolarized cross section for single jet production as a function of photon virtuality, Q**2.

Differential unpolarized cross section for two jet production as a function of photon virtuality, Q**2.

Differential unpolarized cross section for three jet production as a function of photon virtuality, Q**2.

Differential unpolarized inclusive-jet cross section as a function of X. Update: contrary to the publication, this is D(SIG)/DLOG10(X) not D(SIG)/DX.

Integrated unpolarized jet cross section in the given kinemetical region.

Differential unpolarized dijet cross section as a function of the dijet mass.

Differential unpolarized three-jet cross section as a function of the three-jet mass.

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.

Distribution of D(SIG)/DM(P=6) as a function of M(P=6) .

Distribution of D(SIG)/DBETA as a function of BETA .

Distribution of D(SIG)/DX(NAME=POMERON) as a function of X(NAME=POMERON) .

Distribution of D(SIG)/DET(P=4,5,RF=CM) as a function of ET(P=4,5,RF=CM) .

Distribution of D(SIG)/DETARAP(P=4,5,RF=CM) as a function of ETARAP(P=4,5,RF=CM) .

Distribution of D(SIG)/DZ(NAME=POMERON) as a function of Z(NAME=POMERON) .

Distribution of D(SIG)/DX(NAME=GAMMA) as a function of X(NAME=GAMMA) .

Distribution of D2(SIG)/DZ(NAME=POMERON)/DET(P=4,RF=CM) as a function of Z(NAME=POMERON) for ET(P=4,RF=CM) from 5 to 6.5 GeV). .

Distribution of D2(SIG)/DZ(NAME=POMERON)/DET(P=4,RF=CM) as a function of Z(NAME=POMERON) for ET(P=4,RF=CM) from 6.5 to 8 GeV). .

Distribution of D2(SIG)/DZ(NAME=POMERON)/DET(P=4,RF=CM) as a function of Z(NAME=POMERON) for ET(P=4,RF=CM) from 8 to 16 GeV). .

Distribution of D2(SIG)/DZ(NAME=POMERON)/DQ**2) as a function of Z(NAME=POMERON) for Q**2 from 5 to 12 GeV**2). .

Distribution of D2(SIG)/DZ(NAME=POMERON)/DQ**2) as a function of Z(NAME=POMERON) for Q**2 from 12 to 25 GeV**2). .

Distribution of D2(SIG)/DZ(NAME=POMERON)/DQ**2) as a function of Z(NAME=POMERON) for Q**2 from 25 to 50 GeV**2). .

Distribution of D2(SIG)/DZ(NAME=POMERON)/DQ**2) as a function of Z(NAME=POMERON) for Q**2 from 50 to 100 GeV**2). .