Cross section for elastic J/PSI photoproduction as a function of W in Q**2 bins for ABS(T) < 1.2 GeV**2.

Cross section for elastic J/PSI photoproduction as a function of W in Q**2 bins for ABS(T) < 1.2 GeV**2.

Parameters of the fits of the cross section as W**POWER and slope of the D(SIG)/DT distribution.

Differential cross section for the elastic process GAMMA P --> J/PSI P as a function of T in Q**2 bins in the W range 40 to 160 GeV.

Differential cross section for the elastic process GAMMA P --> J/PSI P as a function of T in Q**2 bins in the W range 40 to 160 GeV.

Differential cross section for the elastic process GAMMA P --> J/PSI P as a function of T in Q**2 bins in the W range 40 to 160 GeV.

Differential cross section for the elastic process GAMMA P --> J/PSI P as a function of T in Q**2 bins in the W range 40 to 160 GeV.

Differential photoproduction cross section for the elastic process GAMMA P --> J/PSI P as a function of W in bins of ABS(T).

Differential electroproduction cross section for the elastic process GAMMA P --> J/PSI P as a function of W in bins of ABS(T).

Slope parameter derived from the one dimensional fit to the DSIG/DT differential distribution as a function of W in Q**2 bins in the electroproduction region.

Slope parameter derived from the one dimensional fit to the DSIG/DT differential distribution as a function of W in Q**2 bins in the photoproduction region.

Spin density matrices and ratio R of cross sections of longitudinal and polarized photons as a function of Q**2 for ABS(T) < 5 GeV**2 and W from 40 to 160 GeV.

Spin density matrices as a function of Q**2 for ABS(T) < 5 GeV**2 and W from 40 to 160 GeV.

Spin density matrix elements as a function of ABS(T) for photoproduction data in the W region 40 to 160 GeV.

Spin density matrix elements as a function of ABS(T) for electroproduction data in the W region 40 to 160 GeV.

Spin density matrix elements as a function of ABS(T) in the W range 40 to 160 GeV for the electroproduction region.

Nuclear modification factor as a function of PT, for 10-20% central reactions Note that the systematic error given is related to the the uncertainties in the p+p measurements.An additional systematic error, symmetrical on the + and - side, related to the uncertainties in the Au+Au measurement, is given in the second column. Another, PT-independant, 13%systematic error due to the uncertainty on the overlap function and the Pi0 yield normalization is to add.

Nuclear modification factor as a function of PT, for 20-40% central reactions Note that the systematic error given is related to the the uncertainties in the p+p measurements.An additional systematic error, symmetrical on the + and - side, related to the uncertainties in the Au+Au measurement, is given in the second column. Another, PT-independant, 13%systematic error due to the uncertainty on the overlap function and the Pi0 yield normalization is to add.

Nuclear modification factor as a function of PT, for 40-60% central reactions Note that the systematic error given is related to the the uncertainties in the p+p measurements.An additional systematic error, symmetrical on the + and - side, related to the uncertainties in the Au+Au measurement, is given in the second column. Another, PT-independant, 13%systematic error due to the uncertainty on the overlap function and the Pi0 yield normalization is to add.

Directed flow of charged particles as a function of pseudorapidity, for centrality 10%-70%.

Directed flow of charged particles as a function of pseudorapidity, for centrality 10%-70%.

Directed flow of charged particles as a function of pseudorapidity, for centrality 10%-70%.

$v_1$ versus rapidity for charged particles.

$v_1$ versus rapidity for pions.

$v_1$ versus rapidity for protons.

Directed flow of charged particles as a function of pseudorapidity for the 60-70% and 70-80% centrality classes.

Directed flow of charged particles as a function of pseudorapidity for the 10-20%, 20-30%, 30-40%, 40-50% and 50-60% centrality classes.

Directed flow of charged particles as a function of pseudorapidity for the 5-10% centrality class.

Directed flow of charged particles as a function of pseudorapidity for the 0-5% centrality class.

$v_1${3} versus $p_t$ measured in the main TPC (|$\eta$| < 1.3), for centrality 10%-70%.

$v_1${3} versus $p_t$ measured in the Forward TPC (2.5 < |$\eta$| < 4.0), for different centralities.

Directed flow of charged particles as a function of impact parameter for the mid-pseudorapidity region (|$\eta$| < 1.3) and the forward pseudorapidity region (2.5 < |$\eta$| < 4.0.

Charged particle $v_1$ for Au+Au collisions (10%-70%) at 200 GeV as a function of $\eta-y_{beam}$.

Charged particle $v_1$ for Au+Au collisions (10%-70%) at 62.4 GeV as a function of $\eta-y_{beam}$.

Charged particle $v_1$ for Pb+Pb collisions (12.5%-33.5%) at 17.2 GeV as a function of $y-y_{beam}$.

Fully corrected assorted $\pi^{0}$-hadron conditional pair distributions for $d$+Au collisions centrality 0-88% and $p$+$p$ collisions. The trigger $\pi^0$s are within 5 < $p_{T,trig}$ < 10 GeV/$c$ and are correlated with hadrons with $p_{T,assoc}$ of 1.5-2 GeV/$c$, 2-3GeV/$c$, 3-4 GeV/$c$, and 4-5 GeV/$c$.

Near- and far-side widths as a function of $p_{T, assoc}$ for charged hadron azimuthal correlations from minimumbias $d$+Au collisions.

Near-side width, far-side width as a function of $p_{T,assoc}$ for a charged pion and neutral pion triggers from the $p_{T,trig}$ range of 5-10 GeV/$c$ in minimum bias $d$+Au collisions.

Near-side width, far-side width as a function of $p_{T,assoc}$ for a charged pion and neutral pion triggers from the $p_{T,trig}$ range of 5-10 GeV/$c$ in minimum bias $d$+Au collisions.

Near- and far-side conditional yields as a function of $p_{T, assoc}$ for charged hadron triggers (2.5−4 GeV/$c$) and associated charged hadrons from $d$+Au collisions.

Near- and far-side conditional yields as a function of $p_{T, assoc}$ for charged hadron triggers (4−6 GeV/$c$) and associated charged hadrons from $d$+Au collisions.

Near- and far-side conditional yields as a function of $p_{T, assoc}$ for charged pion triggers (5−10 GeV/$c$) and associated charged hadrons from minimum-bias $d$+Au collisions.

Near- and far-side conditional yields as a function of $p_{T, assoc}$ for neutral pion triggers (5−10 GeV/$c$) and associated charged hadrons from minimum-bias $d$+Au collisions.

Near- and far-side widths and conditional yields as a function of $N_{coll}$ for charged hadron triggers (2.5−4 GeV/$c$) and associated charged hadrons (1–2.5 GeV/$c$) from $d$+Au collisions.

Near- and far-side widths and conditional yields as a function of centrality for neutral pion triggers (5−10 GeV/$c$) and associated charged hadrons (2–3 GeV/$c$) from $d$+Au collisions.

The extracted $\sqrt{<j^2_T>}$ for minimum-bias $d$+Au collisions from all four dihadron correlations. The trigger $p_T$ ranges are 3 - 5 GeV/$c$, 5 - 10 GeV/$c$ and 5 - 10 GeV/$c$ for $h^{\pm}$ - $h^{\pm}$, $\pi^0$ - $h^{\pm}$ and $\pi^{\pm}$ - $h^{\pm}$ assorted-$p_T$ correlations.

The extracted $\sqrt{<j^2_T>}$ for minimum-bias $d$+Au collisions from all four dihadron correlations. The trigger $p_T$ ranges are 3 - 5 GeV/$c$, 5 - 10 GeV/$c$ and 5 - 10 GeV/$c$ for $h^{\pm}$ - $h^{\pm}$, $\pi^0$ - $h^{\pm}$ and $\pi^{\pm}$ - $h^{\pm}$ assorted-$p_T$ correlations.

The extracted $\sqrt{<j^2_T>}$ for minimum-bias $d$+Au collisions from all four dihadron correlations. The trigger $p_T$ ranges are 3 - 5 GeV/$c$, 5 - 10 GeV/$c$ and 5 - 10 GeV/$c$ for $h^{\pm}$ - $h^{\pm}$, $\pi^0$ - $h^{\pm}$ and $\pi^{\pm}$ - $h^{\pm}$ assorted-$p_T$ correlations.

The extracted $\sqrt{<j^2_T>}$ for minimum-bias $d$+Au collisions from all four dihadron correlations. The trigger $p_T$ ranges are 3 - 5 GeV/$c$, 5 - 10 GeV/$c$ and 5 - 10 GeV/$c$ for $h^{\pm}$ - $h^{\pm}$, $\pi^0$ - $h^{\pm}$ and $\pi^{\pm}$ - $h^{\pm}$ assorted-$p_T$ correlations.

$<sin^2(\phi_{jj})>$ for minimum bias $d$+Au collisions as function of associated particle $p_T$ for $\pi^{\pm}$ - $h^{\pm}$ and $\pi^0$ - $h^{\pm}$ correlations where the trigger particles have a $p_T$ between 5 - 10 GeV/$c$.

$<sin^2(\phi_{jj})>$ for minimum bias $d$+Au collisions as function of associated particle $p_T$ for $\pi^{\pm}$ - $h^{\pm}$ and $\pi^0$ - $h^{\pm}$ correlations where the trigger particles have a $p_T$ between 5 - 10 GeV/$c$.

$<sin^2(\phi_{jj})>$ for minimum bias $d$+Au collisions as function of trigger particle $p_T$ for $\pi^{\pm}$ - $h^{\pm}$ and $\pi^0$ - $h^{\pm}$ correlations.

$<sin^2(\phi_{jj})>$ for minimum bias $d$+Au collisions as function of trigger particle $p_T$ for $\pi^{\pm}$ - $h^{\pm}$ and $\pi^0$ - $h^{\pm}$ correlations.

Near-side and far-side $p_{out}$ distributions for minimum bias $d$+Au collisions obtained from $\pi^{\pm}$ - $h^{\pm}$ correlation. The trigger is 5 < $p_{T,trig}$ < 10 GeV/$c$, the associated particle is 0.5 < $p_{T,assoc}$ < 5.0 GeV/$c$.

Conditional yield as a function of $x_E$ for near-side and far-side for $\pi^{\pm}$ - $h^{\pm}$ and $\pi^0$ - $h^{\pm}$ from minimum-bias $d$+Au collisions.

Conditional yield as a function of $x_E$ for near-side and far-side for $\pi^{\pm}$ - $h^{\pm}$ and $\pi^0$ - $h^{\pm}$ from minimum-bias $d$+Au collisions.

Conditional yield as a function of $x_E$ for near-side and far-side correlations for $\pi^{\pm}$ - $h^{\pm}$ correlations from minimum-bias $d$+Au collisions. The trigger pions are 5 < $p_{T,trig}$ < 6 GeV/$c$.

Conditional yield as a function of $x_E$ for near-side and far-side correlation for $\pi^{\pm}$ - $h^{\pm}$ correlation for several different trigger $p_T$s for minimum-bias $d$+Au collisions.

Far-side conditional yield as a function of $p_{T,trig}$ for different ranges of $x_E$ for $\pi^{\pm}$ - $h^{\pm}$ correlation for minimum-bias $d$+Au collisions.

Far-side conditional yield as a function of $p_{T,trig}$ for different ranges of $x_E$ for $\pi^{\pm}$ - $h^{\pm}$ correlation for minimum-bias $d$+Au collisions.

Far-side conditional yield as a function of $p_{T,trig}$ for different ranges of $x_E$ for $\pi^{\pm}$ - $h^{\pm}$ correlation for minimum-bias $d$+Au collisions.

Far-side conditional yield as a function of $p_{T,trig}$ for different ranges of $x_E$ for $\pi^{\pm}$ - $h^{\pm}$ correlation for minimum-bias $d$+Au collisions.

The comparison of the $\sqrt{<j^2_T>}$ values between $d$+Au and $p$+$p$ for the $\pi^{\pm}$ - $h^{\pm}$ correlations and $\pi^0$ - $h^{\pm}$ correlations. The trigger pion range is 5 - 10 GeV/$c$.

The comparison of the $\sqrt{<j^2_T>}$ values between $d$+Au and $p$+$p$ for the $\pi^{\pm}$ - $h^{\pm}$ correlations and $\pi^0$ - $h^{\pm}$ correlations. The trigger pion range is 5 - 10 GeV/$c$.

Quadrature difference between minimum-bias $d$+Au and $p$+$p$ $<sin^2(\phi_{jj})>$ values.

Quadrature difference between minimum-bias $d$+Au and $p$+$p$ $<sin^2(\phi_{jj})>$ values.

The comparison of the $p_{out}$ distribution at the near-side and far-side between central $d$+Au collisions and $p$+$p$ collisions. Results are obtained for $\pi^{\pm}$ - $h^{\pm}$ correlations with the associated hadron range 0.5 < $p_{T,assoc}$ < 5 GeV/$c$ and trigger pion range of 5 < $p_{T,trig}$ < 10 GeV/$c$.

The comparison of the $x_E$ distribution from $\pi^{\pm}$ - $h^{\pm}$ correlation at the near-side and far-side between minimum bias $d$+Au collisions and $p$+$p$ collisions. The trigger $\pi^{\pm}$ are from 5 - 10 GeV/$c$.

Far-side conditional yield as a function of $p_{T,trig}$ for different ranges of $x_E$ from $p$+$p$ collisions, triggers are $\pi^{\pm}$ from 5 - 10 GeV/$c$.

Far-side conditional yield as a function of $p_{T,trig}$ for different ranges of $x_E$ from $p$+$p$ collisions, triggers are $\pi^{\pm}$ from 5 - 10 GeV/$c$.

Far-side conditional yield as a function of $p_{T,trig}$ for different ranges of $x_E$ from $p$+$p$ collisions, triggers are $\pi^{\pm}$ from 5 - 10 GeV/$c$.

The fitted fractional change in $dN/d_{x_E}$ per unit $p_{T,trig}$ of the far-side conditional yield for different ranges of $x_E$.

Centrality dependent near and far $CY(p_T)$ for $\pi^{\pm}$ - $h^{\pm}$ correlations and $\pi^0$ - $h^{\pm}$ correlations.

Centrality dependent near and far $CY(p_T)$ for $\pi^{\pm}$ - $h^{\pm}$ correlations and $\pi^0$ - $h^{\pm}$ correlations.

Centrality dependence to the ratio of near and far $CY(p_T)$ for $d$+Au to $p$+$p$.

Centrality dependence to the ratio of near and far $CY(p_T)$ for $d$+Au to $p$+$p$.

Near- and far-side widths as a function of $p_{T, trig}$ for charged pion triggers and associated charged hadrons (2–4.5 Gev/$c$) from minimum-bias $d$+Au collisions.

Near- and far-side widths as a function of $p_{T, trig}$ for neutral pion triggers and associated charged hadrons (2–4.5 Gev/$c$) from minimum-bias $d$+Au collisions.

Measurement of F2 at X = 0.125.

Measurement of F2 at X = 0.175.

Measurement of F2 at X = 0.225.

Measurement of F2 at X = 0.275.

Measurement of F2 at X = 0.350.

Measurement of F2 at X = 0.450.

Measurement of F2 at X = 0.550.

Measurement of F2 at X = 0.650.

Measurement of F2 at X = 0.750.

Measurement of XF3 at X = 0.015.

Measurement of XF3 at X = 0.045.

Measurement of XF3 at X = 0.080.

Measurement of XF3 at X = 0.125.

Measurement of XF3 at X = 0.175.

Measurement of XF3 at X = 0.225.

Measurement of XF3 at X = 0.275.

Measurement of XF3 at X = 0.350.

Measurement of XF3 at X = 0.450.

Measurement of XF3 at X = 0.550.

Measurement of XF3 at X = 0.650.

Measurement of XF3 at X = 0.750.

Differential cross sections at neutrino energy 35.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at neutrino energy 35.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at neutrino energy 35.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at neutrino energy 35.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at neutrino energy 45.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at neutrino energy 45.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at neutrino energy 45.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at neutrino energy 45.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at neutrino energy 55.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at neutrino energy 55.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at neutrino energy 55.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at neutrino energy 55.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at neutrino energy 65.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at neutrino energy 65.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at neutrino energy 65.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at neutrino energy 65.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at neutrino energy 75.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at neutrino energy 75.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at neutrino energy 75.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at neutrino energy 75.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at neutrino energy 85.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at neutrino energy 85.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at neutrino energy 85.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at neutrino energy 85.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at neutrino energy 95.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at neutrino energy 95.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at neutrino energy 95.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at neutrino energy 95.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at neutrino energy 110.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at neutrino energy 110.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at neutrino energy 110.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at neutrino energy 110.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at neutrino energy 130.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at neutrino energy 130.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at neutrino energy 130.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at neutrino energy 130.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at neutrino energy 150.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at neutrino energy 150.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at neutrino energy 150.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at neutrino energy 150.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at neutrino energy 170.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at neutrino energy 170.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at neutrino energy 170.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at neutrino energy 170.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at neutrino energy 190.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at neutrino energy 190.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at neutrino energy 190.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at neutrino energy 190.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at neutrino energy 215.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at neutrino energy 215.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at neutrino energy 215.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at neutrino energy 215.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at neutrino energy 245.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at neutrino energy 245.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at neutrino energy 245.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at neutrino energy 245.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at neutrino energy 275.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at neutrino energy 275.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at neutrino energy 275.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at neutrino energy 275.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at neutrino energy 305.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at neutrino energy 305.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at neutrino energy 305.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at neutrino energy 305.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at neutrino energy 340.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at neutrino energy 340.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at neutrino energy 340.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at neutrino energy 340.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at antineutrino energy 35.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at antineutrino energy 35.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at antineutrino energy 35.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at antineutrino energy 35.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at antineutrino energy 45.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at antineutrino energy 45.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at antineutrino energy 45.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at antineutrino energy 45.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at antineutrino energy 55.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at antineutrino energy 55.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at antineutrino energy 55.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at antineutrino energy 55.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at antineutrino energy 65.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at antineutrino energy 65.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at antineutrino energy 65.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at antineutrino energy 65.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at antineutrino energy 75.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at antineutrino energy 75.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at antineutrino energy 75.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at antineutrino energy 75.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at antineutrino energy 85.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at antineutrino energy 85.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at antineutrino energy 85.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at antineutrino energy 85.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at antineutrino energy 95.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at antineutrino energy 95.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at antineutrino energy 95.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at antineutrino energy 95.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at antineutrino energy 110.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at antineutrino energy 110.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at antineutrino energy 110.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at antineutrino energy 110.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at antineutrino energy 130.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at antineutrino energy 130.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at antineutrino energy 130.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at antineutrino energy 130.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at antineutrino energy 150.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at antineutrino energy 150.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at antineutrino energy 150.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at antineutrino energy 150.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at antineutrino energy 170.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at antineutrino energy 170.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at antineutrino energy 170.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at antineutrino energy 170.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at antineutrino energy 190.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at antineutrino energy 190.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at antineutrino energy 190.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at antineutrino energy 190.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at antineutrino energy 215.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at antineutrino energy 215.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at antineutrino energy 215.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at antineutrino energy 215.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at antineutrino energy 245.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at antineutrino energy 245.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at antineutrino energy 245.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at antineutrino energy 245.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at antineutrino energy 275.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at antineutrino energy 275.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at antineutrino energy 275.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at antineutrino energy 275.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at antineutrino energy 305.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at antineutrino energy 305.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at antineutrino energy 305.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at antineutrino energy 305.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at antineutrino energy 340.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at antineutrino energy 340.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at antineutrino energy 340.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Triple differential cross section.

Cross sections for di-jet and forward jet data.. The jets are ordered such that:-. ETARAP(P=4) > ETARAP(P=5) > ETARAP(P=6).. The first jet (P=4) is the forward jet.

Cross sections for di-jet and forward jet data.. The jets are ordered such that:-. ETARAP(P=4) > ETARAP(P=5) > ETARAP(P=6).. The first jet (P=4) is the forward jet.

Cross sections for di-jet and forward jet data.. The jets are ordered such that:-. ETARAP(P=4) > ETARAP(P=5) > ETARAP(P=6).. The first jet (P=4) is the forward jet.