Sample correlations in $\Delta\phi$ ($|\Delta\eta|<$ 1.78) for 3 $<$ $p_T^{trigger}$ $<$ 6 GeV/$c$ and 1.5 GeV/$c$ $<$ $p_T^{associated}$ $<$ $p_T^{trigger}$ for 0-60% Cu+Cu at $\sqrt{s_{NN}}$ = 62.4 GeV, 0-80% Au+Au at $\sqrt{s_{NN}}$ = 62.4 GeV, 0-95% $d$+Au at $\sqrt{s_{NN}}$ = 200 GeV, 0-60% Cu+Cu at $\sqrt{s_{NN}}$ = 200 GeV, 40-80% Au+Au at $\sqrt{s_{NN}}$ = 200 GeV, and 0-12% central Au+Au at $\sqrt{s_{NN}}$ = 200 GeV. The data are averaged between positive and negative $\Delta\phi$ and reflected in the plot.

Background subtracted sample correlations for 3 $<$ $p_T^{trigger}$ $<$ 6 GeV/$c$ and 1.5 GeV/$c$ $<$ $p_T^{associated}$ $<$ $p_T^{trigger}$ on the near-side for 0-60% Cu+Cu at $\sqrt{s_{NN}}$ = 62.4 GeV, 0-80% Au+Au at $\sqrt{s_{NN}}$ = 62.4 GeV, 0-95% $d$+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV, 0-60% Cu+Cu at $\sqrt{s_{NN}}$ = 200 GeV, 40-80% Au+Au at $\sqrt{s_{NN}}$ = 200 GeV and 0-12% central Au+Au at $\sqrt{s_{NN}}$ = 200 GeV. The dependence of the jet-like correlation is shown as a function of $\Delta\eta$ ($|\Delta\phi|<$ 0.78). The data are averaged between positive and negative $\Delta\eta$.

Background subtracted sample correlations for 3 $<$ $p_T^{trigger}$ $<$ 6 GeV/$c$ and 1.5 GeV/$c$ $<$ $p_T^{associated}$ $<$ $p_T^{trigger}$ on the near-side for 0-60% Cu+Cu at $\sqrt{s_{NN}}$ = 62.4 GeV, 0-80% Au+Au at $\sqrt{s_{NN}}$ = 62.4 GeV, 0-95% $d$+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV, 0-60% Cu+Cu at $\sqrt{s_{NN}}$ = 200 GeV, 40-80% Au+Au at $\sqrt{s_{NN}}$ = 200 GeV and 0-12% central Au+Au at $\sqrt{s_{NN}}$ = 200 GeV. The dependence of the jet-like correlation is shown as a function of $\Delta\phi$ ($|\Delta\eta|<$ 1.78). The data are averaged between positive and negative $\Delta\phi$.

Dependence of jet-like yield on $N_{part}$ for 3 $<$ $p_T^{trigger}$ $<$ 6 GeV/$c$ and 1.5 GeV/$c$ $<$ $p_T^{associated}$ $<$ $p_T^{trigger}$ for Cu+Cu at $\sqrt{s_{NN}}$ = 62.4 GeV. 5% systematic error due to the uncertainty on the associated particle's efficiency is not shown.

Dependence of jet-like yield on $N_{part}$ for 3 $<$ $p_T^{trigger}$ $<$ 6 GeV/$c$ and 1.5 GeV/$c$ $<$ $p_T^{associated}$ $<$ $p_T^{trigger}$ for Au+Au at $\sqrt{s_{NN}}$ = 62.4 GeV. 5% systematic error due to the uncertainty on the associated particle's efficiency is not shown.

Dependence of jet-like yield on $N_{part}$ for 3 $<$ $p_T^{trigger}$ $<$ 6 GeV/$c$ and 1.5 GeV/$c$ $<$ $p_T^{associated}$ $<$ $p_T^{trigger}$ for $d$+Au at $\sqrt{s_{NN}}$ = 200 GeV. 5% systematic error due to the uncertainty on the associated particle's efficiency is not shown.

Dependence of jet-like yield on $N_{part}$ for 3 $<$ $p_T^{trigger}$ $<$ 6 GeV/$c$ and 1.5 GeV/$c$ $<$ $p_T^{associated}$ $<$ $p_T^{trigger}$ for Cu+Cu at $\sqrt{s_{NN}}$ = 200 GeV. 5% systematic error due to the uncertainty on the associated particle's efficiency is not shown.

Dependence of jet-like yield on $N_{part}$ for 3 $<$ $p_T^{trigger}$ $<$ 6 GeV/$c$ and 1.5 GeV/$c$ $<$ $p_T^{associated}$ $<$ $p_T^{trigger}$ for Au+Au at $\sqrt{s_{NN}}$ = 200 GeV. 5% systematic error due to the uncertainty on the associated particle's efficiency is not shown.

Dependence of jet-like yield on $p_T^{\mathrm{trigger}}$ for 0-60% Cu+Cu at $\sqrt{s_{NN}}$ = 62.4 GeV, 0-80% Au+Au at $\sqrt{s_{NN}}$ = 62.4 GeV, 0-95% $d$+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV, 0-60% Cu+Cu at $\sqrt{s_{NN}}$ = 200 GeV, 40-80% Au+Au at $\sqrt{s_{NN}}$ = 200 GeV and 0-12% central Au+Au at $\sqrt{s_{NN}}$ = 200 GeV. The 5% systematic error due to the uncertainty on the associated particle's efficiency is not shown.

Dependence of jet-like yield on $p_T^{\mathrm{associated}}$ for 3 $<$ $p_T^{trigger}$ $<$ 6 GeV/$c$ for 0-60% Cu+Cu and 0-80% Au+Au collisions at $\sqrt{s_{NN}}$ = 62.4 GeV and 0-95% $d$+Au, 0-60% Cu+Cu, 0-12% Au+Au and 40-80% Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. The 5% systematic error due to the uncertainty on the associated particle's efficiency is not shown.

Dependence of the widths in $\Delta\phi$ on $p_T^{\mathrm{trigger}}$ for 1.5 GeV/$c$ $<$ $p_T^{associated}$ $<$ $p_T^{trigger}$ for 0-95% $d$+Au, 0-60% Cu+Cu at $\sqrt{s_{NN}}$ = 62.4 GeV and $\sqrt{s_{NN}}$ = 200 GeV, 0-80% Au+Au at $\sqrt{s_{NN}}$ = 62.4 GeV, and 0-12% and 40-80% Au+Au at $\sqrt{s_{NN}}$ = 200 GeV.

Dependence of the widths in $\Delta\phi$ on $p_T^{\mathrm{associated}}$ for 3 $<$ $p_T^{trigger}$ $<$ 6 GeV/$c$ for 0-95% $d$+Au, 0-60% Cu+Cu at $\sqrt{s_{NN}}$ = 62.4 GeV and $\sqrt{s_{NN}}$ = 200 GeV, 0-80% Au+Au at $\sqrt{s_{NN}}$ = 62.4 GeV, and 0-12% and 40-80% Au+Au at $\sqrt{s_{NN}}$ = 200 GeV.

Dependence of the widths in $\Delta\phi$ on $N_{part}$ for 3 $<$ $p_T^{trigger}$ $<$ 6 GeV/$c$ and 1.5 GeV/$c$ $<$ $p_T^{associated}$ $<$ $p_T^{trigger}$ for 0-60% Cu+Cu at $\sqrt{s_{NN}}$ = 62.4 GeV.

Dependence of the widths in $\Delta\phi$ on $N_{part}$ for 3 $<$ $p_T^{trigger}$ $<$ 6 GeV/$c$ and 1.5 GeV/$c$ $<$ $p_T^{associated}$ $<$ $p_T^{trigger}$ for 0-80% Au+Au at $\sqrt{s_{NN}}$ = 62.4 GeV.

Dependence of the widths in $\Delta\phi$ on $N_{part}$ for 3 $<$ $p_T^{trigger}$ $<$ 6 GeV/$c$ and 1.5 GeV/$c$ $<$ $p_T^{associated}$ $<$ $p_T^{trigger}$ for 0-95% $d$+Au at $\sqrt{s_{NN}}$ = 200 GeV.

Dependence of the widths in $\Delta\phi$ on $N_{part}$ for 3 $<$ $p_T^{trigger}$ $<$ 6 GeV/$c$ and 1.5 GeV/$c$ $<$ $p_T^{associated}$ $<$ $p_T^{trigger}$ for 0-60% Cu+Cu at $\sqrt{s_{NN}}$ = 200 GeV.

Dependence of the widths in $\Delta\phi$ on $N_{part}$ for 3 $<$ $p_T^{trigger}$ $<$ 6 GeV/$c$ and 1.5 GeV/$c$ $<$ $p_T^{associated}$ $<$ $p_T^{trigger}$ for Au+Au at $\sqrt{s_{NN}}$ = 200 GeV.

Dependence of the widths in $\Delta\eta$ on $p_T^{\mathrm{trigger}}$ for 1.5 GeV/$c$ $<$ $p_T^{associated}$ $<$ $p_T^{trigger}$ for 0-95% $d$+Au, 0-60% Cu+Cu at $\sqrt{s_{NN}}$ = 62.4 GeV and $\sqrt{s_{NN}}$ = 200 GeV, 0-80% Au+Au at $\sqrt{s_{NN}}$ = 62.4 GeV, and 0-12% and 40-80% Au+Au at $\sqrt{s_{NN}}$ = 200 GeV.

Dependence of the widths in $\Delta\eta$ on $p_T^{\mathrm{associated}}$ for 3 $<$ $p_T^{trigger}$ $<$ 6 GeV/$c$ for 0-95% $d$+Au, 0-60% Cu+Cu at $\sqrt{s_{NN}}$ = 62.4 GeV and $\sqrt{s_{NN}}$ = 200 GeV, 0-80% Au+Au at $\sqrt{s_{NN}}$ = 62.4 GeV, and 0-12% and 40-80% Au+Au at $\sqrt{s_{NN}}$ = 200 GeV.

Dependence of the widths in $\Delta\eta$ on $N_{part}$ for 3 $<$ $p_T^{trigger}$ $<$ 6 GeV/$c$ and 1.5 GeV/$c$ $<$ $p_T^{associated}$ $<$ $p_T^{trigger}$ for 0-60% Cu+Cu at $\sqrt{s_{NN}}$ = 62.4 GeV.

Dependence of the widths in $\Delta\eta$ on $N_{part}$ for 3 $<$ $p_T^{trigger}$ $<$ 6 GeV/$c$ and 1.5 GeV/$c$ $<$ $p_T^{associated}$ $<$ $p_T^{trigger}$ for 0-80% Au+Au at $\sqrt{s_{NN}}$ = 62.4 GeV.

Dependence of the widths in $\Delta\eta$ on $N_{part}$ for 3 $<$ $p_T^{trigger}$ $<$ 6 GeV/$c$ and 1.5 GeV/$c$ $<$ $p_T^{associated}$ $<$ $p_T^{trigger}$ for 0-95% $d$+Au at $\sqrt{s_{NN}}$ = 200 GeV.

Dependence of the widths in $\Delta\eta$ on $N_{part}$ for 3 $<$ $p_T^{trigger}$ $<$ 6 GeV/$c$ and 1.5 GeV/$c$ $<$ $p_T^{associated}$ $<$ $p_T^{trigger}$ for 0-60% Cu+Cu at $\sqrt{s_{NN}}$ = 200 GeV.

Dependence of the widths in $\Delta\eta$ on $N_{part}$ for 3 $<$ $p_T^{trigger}$ $<$ 6 GeV/$c$ and 1.5 GeV/$c$ $<$ $p_T^{associated}$ $<$ $p_T^{trigger}$ for Au+Au at $\sqrt{s_{NN}}$ = 200 GeV.

Dependence of ridge yield on $N_{part}$ for 3 $<$ $p_T^{trigger}$ $<$ 6 GeV/$c$ and 1.5 GeV/$c$ $<$ $p_T^{associated}$ $<$ $p_T^{trigger}$ for Cu+Cu at $\sqrt{s_{NN}}$ = 62.4 GeV.

Dependence of ridge yield on $N_{part}$ for 3 $<$ $p_T^{trigger}$ $<$ 6 GeV/$c$ and 1.5 GeV/$c$ $<$ $p_T^{associated}$ $<$ $p_T^{trigger}$ for Au+Au at $\sqrt{s_{NN}}$ = 62.4 GeV.

Dependence of ridge yield on $N_{part}$ for 3 $<$ $p_T^{trigger}$ $<$ 6 GeV/$c$ and 1.5 GeV/$c$ $<$ $p_T^{associated}$ $<$ $p_T^{trigger}$ for Cu+Cu at $\sqrt{s_{NN}}$ = 200 GeV.

Dependence of ridge yield on $N_{part}$ for 3 $<$ $p_T^{trigger}$ $<$ 6 GeV/$c$ and 1.5 GeV/$c$ $<$ $p_T^{associated}$ $<$ $p_T^{trigger}$ for Au+Au at $\sqrt{s_{NN}}$ = 200 GeV.

Ratio of the ridge and jet-like yields on $N_{part}$ for 3 $<$ $p_T^{trigger}$ $<$ 6 GeV/$c$ and 1.5 GeV/$c$ $<$ $p_T^{associated}$ $<$ $p_T^{trigger}$ for Cu+Cu at $\sqrt{s_{NN}}$ = 62.4 GeV.

Ratio of the ridge and jet-like yields on $N_{part}$ for 3 $<$ $p_T^{trigger}$ $<$ 6 GeV/$c$ and 1.5 GeV/$c$ $<$ $p_T^{associated}$ $<$ $p_T^{trigger}$ for Au+Au at $\sqrt{s_{NN}}$ = 62.4 GeV.

Ratio of the ridge and jet-like yields on $N_{part}$ for 3 $<$ $p_T^{trigger}$ $<$ 6 GeV/$c$ and 1.5 GeV/$c$ $<$ $p_T^{associated}$ $<$ $p_T^{trigger}$ for Cu+Cu at $\sqrt{s_{NN}}$ = 200 GeV.

Ratio of the ridge and jet-like yields on $N_{part}$ for 3 $<$ $p_T^{trigger}$ $<$ 6 GeV/$c$ and 1.5 GeV/$c$ $<$ $p_T^{associated}$ $<$ $p_T^{trigger}$ for Au+Au at $\sqrt{s_{NN}}$ = 200 GeV.

Dependence of $V_{3\Delta}/V_{2\Delta}$ on $N_{part}$ for 3 $<$ $p_T^{trigger}$ $<$ 6 GeV/$c$ and 1.5 GeV/$c$ $<$ $p_T^{associated}$ $<$ $p_T^{trigger}$ for Cu+Cu at $\sqrt{s_{NN}}$ = 62.4 GeV.

Dependence of $V_{3\Delta}/V_{2\Delta}$ on $N_{part}$ for 3 $<$ $p_T^{trigger}$ $<$ 6 GeV/$c$ and 1.5 GeV/$c$ $<$ $p_T^{associated}$ $<$ $p_T^{trigger}$ for Au+Au at $\sqrt{s_{NN}}$ = 62.4 GeV.

Dependence of $V_{3\Delta}/V_{2\Delta}$ on $N_{part}$ for 3 $<$ $p_T^{trigger}$ $<$ 6 GeV/$c$ and 1.5 GeV/$c$ $<$ $p_T^{associated}$ $<$ $p_T^{trigger}$ for $d$+Au at $\sqrt{s_{NN}}$ = 200 GeV.

Dependence of $V_{3\Delta}/V_{2\Delta}$ on $N_{part}$ for 3 $<$ $p_T^{trigger}$ $<$ 6 GeV/$c$ and 1.5 GeV/$c$ $<$ $p_T^{associated}$ $<$ $p_T^{trigger}$ for Cu+Cu at $\sqrt{s_{NN}}$ = 200 GeV.

Dependence of $V_{3\Delta}/V_{2\Delta}$ on $N_{part}$ for 3 $<$ $p_T^{trigger}$ $<$ 6 GeV/$c$ and 1.5 GeV/$c$ $<$ $p_T^{associated}$ $<$ $p_T^{trigger}$ for Au+Au at $\sqrt{s_{NN}}$ = 200 GeV.

Normalized Delta_Phi distributions for events with a maximum jet pT between 200 and 300 GeV.

Normalized Delta_Phi distributions for events with a maximum jet pT > 300 GeV.

Single differential cross section DSIG/DCOS(THETA).

Double differential cross section D2SIG/DM/DPT in the diphoton mass range 30 TO 50 GeV.

Double differential cross section D2SIG/DM/DPHI in the diphoton mass range 30 TO 50 GeV.

Double differential cross section D2SIG/DM/DCOS(THETA) in the diphoton mass range 30 TO 50 GeV.

Double differential cross section D2SIG/DM/DPT in the diphoton mass range 50 TO 80 GeV.

Double differential cross section D2SIG/DM/DPHI in the diphoton mass range 50 TO 80 GeV.

Double differential cross section D2SIG/DM/DCOS(THETA) in the diphoton mass range 50 TO 80 GeV.

Double differential cross section D2SIG/DM/DPT in the diphoton mass range 80 TO 350 GeV.

Double differential cross section D2SIG/DM/DPHI in the diphoton mass range 80 TO 350 GeV.

Double differential cross section D2SIG/DM/DCOS(THETA) in the diphoton mass range 80 TO 350 GeV.

The average multiplicity and average scalar sum of transverse momenta of charge particles per unit of pseudorapidity and per radian as a function of the leading track-jet transverse momenta. Statistical errors only. Typical systematic error of 1.8 PCT at a leading track-jet PT of 3.5 GeV.

The normalized multiplicity distribution (PROB) of charged particles. Statistical error only. Typical systematic error of 2.3 PCT at a multiplicity of 4.

The normalized distribution of the scalar sum of the transverse momenta of charged particles. Statistical errors only. Typical systematic error of 1.6 PCT at a SUM(PT) of 4.5 GeV.

The transverse momenta spectrum of charged particles. Statistical error only. Typical systematic error of 2.0 PCT at a PT of 1 GeV.

The fitted exponential slope of the T distribution as a function of X(NAME=POMERON).

The fitted exponential slope of the T distribution as a function of X(NAME=POMERON).

The fitted exponential slope of the T distribution as a function of X(NAME=POMERON).

The fitted exponential slope of the T distribution as a function of X(NAME=POMERON).

The fitted exponential slope of the T distribution as a function of X(NAME=POMERON).

The fitted exponential slope of the T distribution as a function of X(NAME=POMERON).

The fitted exponential slope of the T distribution as a function of X(NAME=POMERON).

The differential cross section as a function of PHI, the angle between the positron scattering plane and the proton scattering plane for the LRG and the LPS data samples.

The azimuthal asymmetries ALT and ATT as a function of X(NAME=POMERON).

The azimuthal asymmetries ALT and ATT as a function of BETA.

The azimuthal asymmetries ALT and ATT as a function of ABS(T).

The azimuthal asymmetries ALT and ATT as a function of Q**2.

The reduced diffractive cross sections obtained from the LPS data as a function of X(NAME=POMERON) for Q**2 = 2.5 GeV**2 and ABS(T) = 0.09 to 0.19 GeV**2 for M(X) values of 3, 7, 15 and 30 GeV.

The reduced diffractive cross sections obtained from the LPS data as a function of X(NAME=POMERON) for Q**2 = 3.9 GeV**2 and ABS(T) = 0.09 to 0.19 GeV**2 for M(X) values of 3, 7, 15 and 30 GeV.

The reduced diffractive cross sections obtained from the LPS data as a function of X(NAME=POMERON) for Q**2 = 7.1 GeV**2 and ABS(T) = 0.09 to 0.19 GeV**2 for M(X) values of 3, 7, 15 and 30 GeV.

The reduced diffractive cross sections obtained from the LPS data as a function of X(NAME=POMERON) for Q**2 = 14 GeV**2 and ABS(T) = 0.09 to 0.19 GeV**2 for M(X) values of 3, 7, 15 and 30 GeV.

The reduced diffractive cross sections obtained from the LPS data as a function of X(NAME=POMERON) for Q**2 = 40 GeV**2 and ABS(T) = 0.09 to 0.19 GeV**2 for M(X) values of 3, 7, 15 and 30 GeV.

The reduced diffractive cross sections obtained from the LPS data as a function of X(NAME=POMERON) for Q**2 = 2.5 GeV**2 and ABS(T) = 0.19 to 0.55 GeV**2 for M(X) values of 3, 7, 15 and 30 GeV.

The reduced diffractive cross sections obtained from the LPS data as a function of X(NAME=POMERON) for Q**2 = 3.9 GeV**2 and ABS(T) = 0.19 to 0.55 GeV**2 for M(X) values of 3, 7, 15 and 30 GeV.

The reduced diffractive cross sections obtained from the LPS data as a function of X(NAME=POMERON) for Q**2 = 7.1 GeV**2 and ABS(T) = 0.19 to 0.55 GeV**2 for M(X) values of 3, 7, 15 and 30 GeV.

The reduced diffractive cross sections obtained from the LPS data as a function of X(NAME=POMERON) for Q**2 = 14 GeV**2 and ABS(T) = 0.19 to 0.55 GeV**2 for M(X) values of 3, 7, 15 and 30 GeV.

The reduced diffractive cross sections obtained from the LPS data as a function of X(NAME=POMERON) for Q**2 = 40 GeV**2 and ABS(T) = 0.19 to 0.55 GeV**2 for M(X) values of 3, 7, 15 and 30 GeV.

The reduced diffractive cross sections obtained from the LPS data as a function of X(NAME=POMERON) for Q**2 = 2.5 GeV**2 and M(X) values of 3, 6, 11, 19 and 32 GeV.

The reduced diffractive cross sections obtained from the LPS data as a function of X(NAME=POMERON) for Q**2 = 3.9 GeV**2 and M(X) values of 3, 6, 11, 19 and 32 GeV.

The reduced diffractive cross sections obtained from the LPS data as a function of X(NAME=POMERON) for Q**2 = 7.1 GeV**2 and M(X) values of 3, 6, 11, 19 and 32 GeV.

The reduced diffractive cross sections obtained from the LPS data as a function of X(NAME=POMERON) for Q**2 = 14 GeV**2 and M(X) values of 3, 6, 11, 19 and 32 GeV.

The reduced diffractive cross sections obtained from the LPS data as a function of X(NAME=POMERON) for Q**2 = 40 GeV**2 and M(X) values of 3, 6, 11, 19 and 32 GeV.

The reduced diffractive cross sections obtained from the LRG data as a function of X(NAME=POMERON) for Q**2 = 2.5 GeV**2 and M(X) values of 3, 6, 11, 19 and 32 GeV.

The reduced diffractive cross sections obtained from the LRG data as a function of X(NAME=POMERON) for Q**2 = 3.5 GeV**2 and M(X) values of 3, 6, 11, 19 and 32 GeV.

The reduced diffractive cross sections obtained from the LRG data as a function of X(NAME=POMERON) for Q**2 = 4.5 GeV**2 and M(X) values of 3, 6, 11, 19 and 32 GeV.

The reduced diffractive cross sections obtained from the LRG data as a function of X(NAME=POMERON) for Q**2 = 5.5 GeV**2 and M(X) values of 3, 6, 11, 19 and 32 GeV.

The reduced diffractive cross sections obtained from the LRG data as a function of X(NAME=POMERON) for Q**2 = 6.5 GeV**2 and M(X) values of 3, 6, 11, 19 and 32 GeV.

The reduced diffractive cross sections obtained from the LRG data as a function of X(NAME=POMERON) for Q**2 = 8.5 GeV**2 and M(X) values of 3, 6, 11, 19 and 32 GeV.

The reduced diffractive cross sections obtained from the LRG data as a function of X(NAME=POMERON) for Q**2 = 12 GeV**2 and M(X) values of 3, 6, 11, 19 and 32 GeV.

The reduced diffractive cross sections obtained from the LRG data as a function of X(NAME=POMERON) for Q**2 = 16 GeV**2 and M(X) values of 3, 6, 11, 19 and 32 GeV.

The reduced diffractive cross sections obtained from the LRG data as a function of X(NAME=POMERON) for Q**2 = 22 GeV**2 and M(X) values of 3, 6, 11, 19 and 32 GeV.

The reduced diffractive cross sections obtained from the LRG data as a function of X(NAME=POMERON) for Q**2 = 30 GeV**2 and M(X) values of 3, 6, 11, 19 and 32 GeV.

The reduced diffractive cross sections obtained from the LRG data as a function of X(NAME=POMERON) for Q**2 = 40 GeV**2 and M(X) values of 3, 6, 11, 19 and 32 GeV.

The reduced diffractive cross sections obtained from the LRG data as a function of X(NAME=POMERON) for Q**2 = 50 GeV**2 and M(X) values of 3, 6, 11, 19 and 32 GeV.

The reduced diffractive cross sections obtained from the LRG data as a function of X(NAME=POMERON) for Q**2 = 65 GeV**2 and M(X) values of 3, 6, 11, 19 and 32 GeV.

The reduced diffractive cross sections obtained from the LRG data as a function of X(NAME=POMERON) for Q**2 = 85 GeV**2 and M(X) values of 3, 6, 11, 19 and 32 GeV.

The reduced diffractive cross sections obtained from the LRG data as a function of X(NAME=POMERON) for Q**2 = 110 GeV**2 and M(X) values of 3, 6, 11, 19 and 32 GeV.

The reduced diffractive cross sections obtained from the LRG data as a function of X(NAME=POMERON) for Q**2 = 140 GeV**2 and M(X) values of 3, 6, 11, 19 and 32 GeV.

The reduced diffractive cross sections obtained from the LRG data as a function of X(NAME=POMERON) for Q**2 = 185 GeV**2 and M(X) values of 3, 6, 11, 19 and 32 GeV.

The reduced diffractive cross sections obtained from the LRG data as a function of X(NAME=POMERON) for Q**2 = 255 GeV**2 and M(X) values of 3, 6, 11, 19 and 32 GeV.

Cross section D(SIG)/ET(P=4) as a function of ET(P=4) for X(C=GAMMA,OBS) <= 0.75 .

Cross section D(SIG)/(ETARAP(P=4)+ETARAP(P=5))/2 as a function of (ETARAP(P=4)+ETARAP(P=5))/2 for X(C=GAMMA,OBS) > 0.75 .

Cross section D(SIG)/(ETARAP(P=4)+ETARAP(P=5))/2 as a function of (ETARAP(P=4)+ETARAP(P=5))/2 for X(C=GAMMA,OBS) <= 0.75 .

Cross section D(SIG)/X(C=P,OBS) as a function of X(C=P,OBS) for X(C=GAMMA,OBS) > 0.75 .

Cross section D(SIG)/X(C=P,OBS) as a function of X(C=P,OBS) for X(C=GAMMA,OBS) <= 0.75 .

Cross section D(SIG)/(PHI(P=4)-PHI(P=5))/2 as a function of (PHI(P=4)-PHI(P=5))/2 for X(C=GAMMA,OBS) > 0.75 .

Cross section D(SIG)/(PHI(P=4)-PHI(P=5))/2 as a function of (PHI(P=4)-PHI(P=5))/2 for X(C=GAMMA,OBS) <= 0.75 .

Cross section D(SIG)/X(C=P,OBS) as a function of X(C=P,OBS) for X(C=GAMMA,OBS) > 0.75 for the High X(C=GAMMA,OBS) 1 optimized set.

Cross section D(SIG)/X(C=P,OBS) as a function of X(C=P,OBS) for X(C=GAMMA,OBS) > 0.75 for the High X(C=GAMMA,OBS) 2 optimized set.

Cross section D(SIG)/X(C=P,OBS) as a function of X(C=P,OBS) for X(C=GAMMA,OBS) > 0.75 for the High X(C=GAMMA,OBS) 3 optimized set.

Cross section D(SIG)/X(C=P,OBS) as a function of X(C=P,OBS) for X(C=GAMMA,OBS) > 0.75 for the High X(C=GAMMA,OBS) 4 optimized set.

Cross section D(SIG)/X(C=P,OBS) as a function of X(C=P,OBS) for X(C=GAMMA,OBS) <= 0.75 for the Low X(C=GAMMA,OBS) 1 optimized set.

Cross section D(SIG)/X(C=P,OBS) as a function of X(C=P,OBS) for X(C=GAMMA,OBS) <= 0.75 for the Low X(C=GAMMA,OBS) 2 optimized set.

Cross section D(SIG)/X(C=P,OBS) as a function of X(C=P,OBS) for X(C=GAMMA,OBS) <= 0.75 for the Low X(C=GAMMA,OBS) 3 optimized set.

Cross section D(SIG)/X(C=P,OBS) as a function of X(C=P,OBS) for X(C=GAMMA,OBS) <= 0.75 for the Low X(C=GAMMA,OBS) 4 optimized set.

Cross section D(SIG)/X(C=GAMMA,OBS) as a function of X(C=GAMMA,OBS) .

Two jet cross section D(SIG)/DET(P=5,RF=CM) as a function of ET(P=5,RF=CM).

Two jet cross section D(SIG)/DETARAP(P=4,RF=LAB) as a function of ETARAP(P=4,RF=LAB).

Two jet cross section D(SIG)/DETARAP(P=5,RF=LAB) as a function of ETARAP(P=5,RF=LAB).

Two jet cross section D(SIG)/D(ETARAP(P=4,RF=CM)-ETARAP(P=5,RF=CM)) as a function of ETARAP(P=4,RF=LAB)-ETARAP(P=5,RF=LAB).

Two jet cross section D2(SIG)/D(ET(P=4,RF=CM)-ET(P=5,RF=CM))/DX as a function of ET(P=4,RF=CM)-ET(P=5,RF=CM).

Two jet cross section D2(SIG)/D(ET(P=4,RF=CM)-ET(P=5,RF=CM))/DX as a function of ET(P=4,RF=CM)-ET(P=5,RF=CM).

Two jet cross section D2(SIG)/D(ET(P=4,RF=CM)-ET(P=5,RF=CM))/DX as a function of ET(P=4,RF=CM)-ET(P=5,RF=CM).

Two jet cross section D2(SIG)/D(ET(P=4,RF=CM)-ET(P=5,RF=CM))/DX as a function of ET(P=4,RF=CM)-ET(P=5,RF=CM).

Two jet cross section D2(SIG)/D(ET(P=4,RF=CM)-ET(P=5,RF=CM))/DX as a function of ET(P=4,RF=CM)-ET(P=5,RF=CM).

Two jet cross section D2(SIG)/D(PT(P=4,RF=CM)-PT(P=5,RF=CM))/DX as a function of PT(P=4,RF=CM)-PT(P=5,RF=CM).

Two jet cross section D2(SIG)/D(PT(P=4,RF=CM)-PT(P=5,RF=CM))/DX as a function of PT(P=4,RF=CM)-PT(P=5,RF=CM).

Two jet cross section D2(SIG)/D(PT(P=4,RF=CM)-PT(P=5,RF=CM))/DX as a function of PT(P=4,RF=CM)-PT(P=5,RF=CM).

Two jet cross section D2(SIG)/D(PT(P=4,RF=CM)-PT(P=5,RF=CM))/DX as a function of PT(P=4,RF=CM)-PT(P=5,RF=CM).

Two jet cross section D2(SIG)/D(PT(P=4,RF=CM)-PT(P=5,RF=CM))/DX as a function of PT(P=4,RF=CM)-PT(P=5,RF=CM).

Two jet cross section D2(SIG)/DABS((PT(P=4,RF=CM)-PT(P=5,RF=CM))/2*ET(P=4,RF=CM))/DX as a function of ABS(PT(P=4,RF=CM)-PT(P=5,RF=CM))/2*ET(P=4,RF=CM).

Two jet cross section D2(SIG)/DABS((PT(P=4,RF=CM)-PT(P=5,RF=CM))/2*ET(P=4,RF=CM))/DX as a function of ABS(PT(P=4,RF=CM)-PT(P=5,RF=CM))/2*ET(P=4,RF=CM).

Two jet cross section D2(SIG)/DABS((PT(P=4,RF=CM)-PT(P=5,RF=CM))/2*ET(P=4,RF=CM))/DX as a function of ABS(PT(P=4,RF=CM)-PT(P=5,RF=CM))/2*ET(P=4,RF=CM).

Two jet cross section D2(SIG)/DABS((PT(P=4,RF=CM)-PT(P=5,RF=CM))/2*ET(P=4,RF=CM))/DX as a function of ABS(PT(P=4,RF=CM)-PT(P=5,RF=CM))/2*ET(P=4,RF=CM).

Two jet cross section D2(SIG)/DABS((PT(P=4,RF=CM)-PT(P=5,RF=CM))/2*ET(P=4,RF=CM))/DX as a function of ABS(PT(P=4,RF=CM)-PT(P=5,RF=CM))/2*ET(P=4,RF=CM).

Two jet cross section D2(SIG)/D(PHI(P=4,RF=CM)-PHI(P=5,RF=CM))/DX as a function of PHI(P=4,RF=CM)-PHI(P=5,RF=CM).

Two jet cross section D2(SIG)/D(PHI(P=4,RF=CM)-PHI(P=5,RF=CM))/DX as a function of PHI(P=4,RF=CM)-PHI(P=5,RF=CM).

Two jet cross section D2(SIG)/D(PHI(P=4,RF=CM)-PHI(P=5,RF=CM))/DX as a function of PHI(P=4,RF=CM)-PHI(P=5,RF=CM).

Two jet cross section D2(SIG)/D(PHI(P=4,RF=CM)-PHI(P=5,RF=CM))/DX as a function of PHI(P=4,RF=CM)-PHI(P=5,RF=CM).

Two jet cross section D2(SIG)/D(PHI(P=4,RF=CM)-PHI(P=5,RF=CM))/DX as a function of PHI(P=4,RF=CM)-PHI(P=5,RF=CM).

Two jet cross section D2(SIG)/DQ**2/DX as a function of X.

Two jet cross section D2(SIG)/DQ**2/DX as a function of X.

Two jet cross section D2(SIG)/DQ**2/DX as a function of X.

Two jet cross section D2(SIG)/DQ**2/DX as a function of X.

Two jet cross section D2(SIG)/DQ**2/DX as a function of X.

Three jet cross section D(SIG)/DQ**2 as a function of Q**2.

Three jet cross section D(SIG)/DX as a function of X.

Three jet cross section D(SIG)/DET(P=4,RF=CM) as a function of ET(P=4,RF=CM).

Three jet cross section D(SIG)/DET(P=5,RF=CM) as a function of ET(P=5,RF=CM).

Three jet cross section D(SIG)/DET(P=6,RF=CM) as a function of ET(P=6,RF=CM).

Three jet cross section D(SIG)/DETARAP(P=4,RF=LAB) as a function of ETARAP(P=4,RF=LAB).

Three jet cross section D(SIG)/DETARAP(P=5,RF=LAB) as a function of ETARAP(P=5,RF=LAB).

Three jet cross section D(SIG)/DETARAP(P=6,RF=LAB) as a function of ETARAP(P=6,RF=LAB).

Three jet cross section D(SIG)/D(ETARAP(P=4,RF=CM)-ETARAP(P=5,RF=CM)) as a function of ETARAP(P=4,RF=LAB)-ETARAP(P=5,RF=LAB).

Three jet cross section D2(SIG)/D(ET(P=4,RF=CM)-ET(P=5,RF=CM))/DX as a function of ET(P=4,RF=CM)-ET(P=5,RF=CM).

Three jet cross section D2(SIG)/D(ET(P=4,RF=CM)-ET(P=5,RF=CM))/DX as a function of ET(P=4,RF=CM)-ET(P=5,RF=CM).

Three jet cross section D2(SIG)/D(ET(P=4,RF=CM)-ET(P=5,RF=CM))/DX as a function of ET(P=4,RF=CM)-ET(P=5,RF=CM).

Three jet cross section D2(SIG)/D(ET(P=4,RF=CM)-ET(P=5,RF=CM))/DX as a function of ET(P=4,RF=CM)-ET(P=5,RF=CM).

Three jet cross section D2(SIG)/D(ET(P=4,RF=CM)-ET(P=5,RF=CM))/DX as a function of ET(P=4,RF=CM)-ET(P=5,RF=CM).

Three jet cross section D2(SIG)/D(PT(P=4,RF=CM)-PT(P=5,RF=CM))/DX as a function of PT(P=4,RF=CM)-PT(P=5,RF=CM).

Three jet cross section D2(SIG)/D(PT(P=4,RF=CM)-PT(P=5,RF=CM))/DX as a function of PT(P=4,RF=CM)-PT(P=5,RF=CM).

Three jet cross section D2(SIG)/D(PT(P=4,RF=CM)-PT(P=5,RF=CM))/DX as a function of PT(P=4,RF=CM)-PT(P=5,RF=CM).

Three jet cross section D2(SIG)/D(PT(P=4,RF=CM)-PT(P=5,RF=CM))/DX as a function of PT(P=4,RF=CM)-PT(P=5,RF=CM).

Three jet cross section D2(SIG)/D(PT(P=4,RF=CM)-PT(P=5,RF=CM))/DX as a function of PT(P=4,RF=CM)-PT(P=5,RF=CM).

Three jet cross section D2(SIG)/DABS((PT(P=4,RF=CM)-PT(P=5,RF=CM))/2*ET(P=4,RF=CM))/DX as a function of (PT(P=4,RF=CM)-PT(P=5,RF=CM))/2*ET(P=4,RF=CM).

Three jet cross section D2(SIG)/DABS((PT(P=4,RF=CM)-PT(P=5,RF=CM))/2*ET(P=4,RF=CM))/DX as a function of (PT(P=4,RF=CM)-PT(P=5,RF=CM))/2*ET(P=4,RF=CM).

Three jet cross section D2(SIG)/DABS((PT(P=4,RF=CM)-PT(P=5,RF=CM))/2*ET(P=4,RF=CM))/DX as a function of (PT(P=4,RF=CM)-PT(P=5,RF=CM))/2*ET(P=4,RF=CM).

Three jet cross section D2(SIG)/DABS((PT(P=4,RF=CM)-PT(P=5,RF=CM))/2*ET(P=4,RF=CM))/DX as a function of (PT(P=4,RF=CM)-PT(P=5,RF=CM))/2*ET(P=4,RF=CM).

Three jet cross section D2(SIG)/DABS((PT(P=4,RF=CM)-PT(P=5,RF=CM))/2*ET(P=4,RF=CM))/DX as a function of (PT(P=4,RF=CM)-PT(P=5,RF=CM))/2*ET(P=4,RF=CM).

Three jet cross section D2(SIG)/D(PHI(P=4,RF=CM)-PHI(P=5,RF=CM))/DX as a function of PHI(P=4,RF=CM)-PHI(P=5,RF=CM).

Three jet cross section D2(SIG)/D(PHI(P=4,RF=CM)-PHI(P=5,RF=CM))/DX as a function of PHI(P=4,RF=CM)-PHI(P=5,RF=CM).

Three jet cross section D2(SIG)/D(PHI(P=4,RF=CM)-PHI(P=5,RF=CM))/DX as a function of PHI(P=4,RF=CM)-PHI(P=5,RF=CM).

Three jet cross section D2(SIG)/D(PHI(P=4,RF=CM)-PHI(P=5,RF=CM))/DX as a function of PHI(P=4,RF=CM)-PHI(P=5,RF=CM).

Three jet cross section D2(SIG)/D(PHI(P=4,RF=CM)-PHI(P=5,RF=CM))/DX as a function of PHI(P=4,RF=CM)-PHI(P=5,RF=CM).

Three jet cross section D2(SIG)/DQ**2/DX as a function of X.

Three jet cross section D2(SIG)/DQ**2/DX as a function of X.

Three jet cross section D2(SIG)/DQ**2/DX as a function of X.

Three jet cross section D2(SIG)/DQ**2/DX as a function of X.

Three jet cross section D2(SIG)/DQ**2/DX as a function of X.

Cross section as a function of the jet transverse energy for INCLUSIVE events containing at least one D* meson in different jet pseudorapidity regions.

Cross section as a function of the jet transverse energy for INCLUSIVE events containing at least one D* meson in different jet pseudorapidity regions.

Cross section as a function of the jet pseudorapidity for INCLUSIVE events containing at least one D* meson in different jet transverse energy regions.

Cross section as a function of the jet pseudorapidity for INCLUSIVE events containing at least one D* meson in different jet transverse energy regions.

Cross section as a function of the jet pseudorapidity for INCLUSIVE events containing at least one D* meson in different jet transverse energy regions.

Cross section as a function of the jet transverse energy for D*-TAGGED and UNTAGGED jets in the jet pseudorapidity region -1.5 TO 2.4.

Cross section as a function of the jet pseudorapidity for D*-TAGGED and UNTAGGED jets in 3 regions of jet transverse energy.

Cross section as a function of the jet pseudorapidity for D*-TAGGED and UNTAGGED jets in 3 regions of jet transverse energy.

Cross section as a function of the jet pseudorapidity for D*-TAGGED and UNTAGGED jets in 3 regions of jet transverse energy.

Cross section as a function of the jet transverse energy in 3 regions of transverse momentum of the D*.

Cross section as a function of the jet transverse energy in 3 regions of transverse momentum of the D*.

Cross section as a function of the jet transverse energy in 3 regions of transverse momentum of the D*.

Cross section as a function of the jet pseudorapidity in 3 regions of transverse momentum of the D*.

Cross section as a function of the jet pseudorapidity in 3 regions of transverse momentum of the D*.

Cross section as a function of the jet pseudorapidity in 3 regions of transverse momentum of the D*.

Cross section as a function of XOBS(C=GAMMA,D*,JET) where the jet here is the UNTAGGED jet with the lightest ET.

The dijet cross section as a function of XOBS(C=GAMMA) for events containing at least one D* meson.

The dijet cross section as a function of the PHI angle difference in JET1 and JET2 for events containing at least one D* meson in different XOBS(C=GAMMA) regions.

The dijet cross section as a function of the PHI angle difference in JET1 and JET2 for events containing at least one D* meson in different XOBS(C=GAMMA) regions.

The dijet cross section as a function of the PHI angle difference in JET1 and JET2 for events containing at least one D* meson in different XOBS(C=GAMMA) regions.

The dijet cross section as a function of the 2-jet transverse momentum for events containing at least one D* meson in different XOBS(C=GAMMA) regions.

The dijet cross section as a function of the 2-jet transverse momentum for events containing at least one D* meson in different XOBS(C=GAMMA) regions.

The dijet cross section as a function of the 2-jet transverse momentum for events containing at least one D* meson in different XOBS(C=GAMMA) regions.

The dijet cross section as a function of the the 2-jet mass for events containing at least one D* meson in different XOBS(C=GAMMA) regions.

The dijet cross section as a function of the the 2-jet mass for events containing at least one D* meson in different XOBS(C=GAMMA) regions.

The dijet cross section as a function of the the 2-jet mass for events containing at least one D* meson in different XOBS(C=GAMMA) regions.

Distribution for the maxPT jet above 180 GeV.