Transverse momentum dependepnce of $v_2$ for identified particle $\pi^-$.

Transverse momentum dependepnce of $v_2$ for identified particle $K^-$.

Transverse momentum dependepnce of $v_2$ for identified particle $\bar{p}$.

Transverse momentum dependepnce of $v_2$ for identified particle $\pi^+$.

Transverse momentum dependepnce of $v_2$ for identified particle $K$.

Transverse momentum dependepnce of $v_2$ for identified particle $p$.

Transverse momentum dependepnce of $v_2$ for combined particles $\pi^+$ and $\pi^-$.

Transverse momentum dependepnce of $v_2$ for combined particles $K^+$ and $K^-$.

Transverse momentum dependepnce of $v_2$ for combined particles $p$ and $\bar{p}$.

Transverse momentum dependepnce of $v_2$ for combined particles $\pi^+$ and $\pi^-$ scaled by quarks for each particle as motivated by a quark coalescence model.

Transverse momentum dependepnce of $v_2$ for combined particles $K^+$ and $K^-$ scaled by quarks for each particle as motivated by a quark coalescence model.

Transverse momentum dependepnce of $v_2$ for combined particles $p$ and $\bar{p}$ scaled by quarks for each particle as motivated by a quark coalescence model.

Transverse momentum dependence of $v_2$ for negative charged particle distributions at 0-20% centrality.

Transverse momentum dependence of $v_2$ for combined $\pi^-$ and $K^-$ at 0-20% centrality.

Transverse momentum dependence of $v_2$ for $\bar{p}$ at 0-20% centrality.

Transverse momentum dependence of $v_2$ for positive charged particle distributions at 0-20% centrality.

Transverse momentum dependence of $v_2$ for combined $\pi^+$ and $K^+$ at 0-20% centrality.

Transverse momentum dependence of $v_2$ for $p$ at 0-20% centrality.

Transverse momentum dependence of $v_2$ for negative charged particle distributions at 20-40% centrality.

Transverse momentum dependence of $v_2$ for combined $\pi^-$ and $K^-$ at 20-40% centrality.

Transverse momentum dependence of $v_2$ for $\bar{p}$ at 20-40% centrality.

Transverse momentum dependence of $v_2$ for positive charged particle distributions at 20-40% centrality.

Transverse momentum dependence of $v_2$ for combined $\pi^+$ and $K^+$ at 20-40% centrality.

Transverse momentum dependence of $v_2$ for $p$ at 20-40% centrality.

Transverse momentum dependence of $v_2$ for negative charged particle distributions at 40-60% centrality.

Transverse momentum dependence of $v_2$ for combined $\pi^-$ and $K^-$ at 40-60% centrality.

Transverse momentum dependence of $v_2$ for $\bar{p}$ at 40-60% centrality.

Transverse momentum dependence of $v_2$ for positive charged particle distributions at 40-60% centrality.

Transverse momentum dependence of $v_2$ for combined $\pi^+$ and $K^+$ at 40-60% centrality.

Transverse momentum dependence of $v_2$ for $p$ at 40-60% centrality.

Inclusive jet cross section DSIG/DETARAP for jets in the lab. frame. Data from the 1995-1997 data sample.

Inclusive jet cross section DSIG/DETARAP for jets in the lab. frame. Data from the 1999-2000 data sample.

Inclusive jet cross section DSIG/DETARAP for jets in the lab. frame. Data from the combined data sample.

Inclusive jet cross section DSIG/DET for jets in the lab. frame. Data from the 1995-1997 running period.

Inclusive jet cross section DSIG/DET for jets in the lab. frame. Data from the 1999-2000 running period.

Inclusive jet cross section DSIG/DET for jets in the lab. frame. Data from the combined running period.

Inclusive di-jet cross section DSIG/DQ**2 for jets in the lab. frame. Data from the 1995-1997 data sample.

Inclusive di-jet cross section DSIG/DQ**2 for jets in the lab. frame. Data from the 1999-2000 data sample.

Inclusive di-jet cross section DSIG/DQ**2 for jets in the lab. frame. Data from the combined data sample.

Inclusive di-jet cross section DSIG/DM for jets in the lab. frame. Data from the 1995-1997 sample.

Inclusive di-jet cross section DSIG/DM for jets in the lab. frame. Data from the 1999-2000 sample.

Inclusive di-jet cross section DSIG/DM for jets in the lab. frame. Data from the combined sample.

Mean subjet multiplicity as a function of the YCUT parameter used in defining the jet for the inclusive jet sample with ET 14 to 17 GeV and 17 to 21 GeV.

Mean subjet multiplicity as a function of the YCUT parameter used in defining the jet for the inclusive jet sample with ET 21 to 25 GeV and 25 to 35 GeV.

Mean subjet multiplicity as a function of the YCUT parameter used in defining the jet for the inclusive jet sample with ET 35 to 55 GeV and 55 to 119 GeV.

Measured values of the mean subjet multiplicity at YCUT = 0.01 as a function of Q**2.

Value of ALPHAS at the Z0 mass obtained from the data with ET(C=JET) > 25 GeV.. The second DSYS error is due to the uncertainty in the theory.

Nuclear modification factor $R_{AA}$ in 10% most central $Au$+$Au$ collisions.

Nuclear modification factor $R_{dA}$ for ($h^+$+$h^-$)/2 in minimum bias $d$+$Au$.

$R_{AA}$ in the 10% most central $Au$+$Au$ collisions.

$R_{dA}$ for ($h^+$+$h^-$)/2 measurement in $d$+$Au$.

$R_{dA}$ for $\pi^0$ measurement in $d$+$Au$.

Ratio of $R_{dA}$ in minimum bias $d$+$Au$ and $R_{pA}$ from neutron tagged $d$+$Au$ collisions for ($h^+$+$h^-$)/2.

Ratio of $R_{dA}$ in minimum bias $d$+$Au$ and $R_{pA}$ from neutron tagged $d$+$Au$ collisions for $\pi^0$

The differential cross section as a function of Y.

The reduced cross section as a function of Q**2 and X.

The reduced cross section as a function of Q**2 and X.

The reduced cross section as a function of Q**2 and X.

The reduced cross section as a function of Q**2 and X.

The reduced cross section as a function of Q**2 and X.

The reduced cross section as a function of Q**2 and X.

The reduced cross section as a function of Q**2 and X.

The reduced cross section as a function of Q**2 and X.

The differential cross section as a function of pseudorapidity.

The differential cross section as a function of log(M(P=5)**2).

The differential cross section as a function of X(C=D*).

The differential cross section as a function of BETA.

The differential cross section as a function of LOG(BETA).

The differential cross section as a function of LOG(Q**2).

The differential cross section as a function of W.

Overall ratio of diffractively produced D*+- mesons to inclusive D*+- mesons.

Ratio of diffractively produced D*+- mesons to inclusive D*+- mesons as a function of transverse momentum.

Ratio of diffractively produced D*+- mesons to inclusive D*+- mesons as a function of pseudorapidity.

Ratio of diffractively produced D*+- mesons to inclusive D*+- mesons as a function of X(C=D*).

Ratio of diffractively produced D*+- mesons to inclusive D*+- mesons as a function of LOG(Q**2).

Ratio of diffractively produced D*+- mesons to inclusive D*+- mesons as a function of W.

Differential cross section as a function of LOG(BETA) in different regions of Q**2 and X(NAME=POMERON).

The measured charm contribution to the diffractive structure function of the proton F2(C=D(3),CHARM).

Mean PT value for J/PSI production. The mean PT is obtained with a phenomonological fit of the J/PSI distribution in PT of the form (1/(2*PI*PT))*D(SIG)/DPT = A ( 1+(PT/B)^2)^-6 .The value given is a combined value of the mean PT for the electron channel results and the muon channel results. The systematic uncertainties were estimated from the spread in mean pt from a weighted mean of the binned data, the phenomenological fit and an exponential fit.An additionnal 3% incertainty is added in the systenatic error for the muon PT due to the incertainty in momentum scale.

Value of the total cross-section for J/PSI production. The total cross section is estimated using a pythia calculation, which reproduces the sigma distribution in rapidity the best, normalized to our data.The systematic error given is obtained by setting the measured cross sections to their upper and lower systematic error limits and noting how the total cross section changed.The choice of the PDF and model was estimated to have little impact in the value of the total cross section (~3%).In addition to the systematic error given, there is a +-40 microbarn error due to normalization.

Centrality dependence of the $p_{T}$ distribution for $K^{-}$ in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. Errors are statistical only.

Centrality dependence of the $p_{T}$ distribution for protons in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. Errors are statistical only.

Centrality dependence of the $p_{T}$ distribution for antiprotons in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. Errors are statistical only.

Centrality dependence of the $p_{T}$ distribution for antiprotons in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. Errors are statistical only.

Inverse slope parameters for $\pi^{+}$, $\pi^{-}$, $K^{+}$, $K^{-}$, proton, and antiproton for the 0-5%, 40-50%, and 60-92% centrality bins. Errors are statistical only.

Fit paramaters $T_{0}^{+}$ and $T_{0}^{-}$. Errors are statistical only.

Fit paramaters $u_{t}^{+}$ and $u_{t}^{-}$. Errors are statistical only.

Relationship between $N_{part}$ and centrality.

Mean transverse momentum as a function of centrality for pions, kaons, protons,and antiprotons in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. Errors are systematic only.

dN/dy as a function of centrality for pions, kaons, protons,and antiprotons in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. Errors are systematic only.

Particle ratios of $\pi^{-}$/$\pi^{+}$ for centrality 0-5% and 60-92%. Errors are statistical and systematic.

Particle ratios of $K^{-}$/$K^{+}$ for centrality 0-5% and 60-92%. Errors are statistical and systematic.

Particle ratios of antiprotons/protons for centrality 0-5%, 60-92%, and minimum bias. Errors are statistical and systematic.

Particle ratios of kaons/pions for centrality 0-5% and 60-92%. Errors are statistical and systematic.

Particle ratios of proton/$\pi^{+}$ and antiproton/$\pi^{-}$ for centrality 0-10%, 20-30%, and 60-92%. Errors are statistical and systematic.

Particle ratios of proton/$\pi^{0}$ and antiproton/$\pi^{0}$ for centrality 0-10%, 20-30%, and 60-92%. Errors are statistical and systematic.

Centrality dependence of particle ratios for $\pi^{-}$/$\pi^{+}$, $K^{-}$/$K^{+}$, and antiprotons/protons. Errors are statistical and systematic.

Rcp as a function of centrality 0-10% and 60-92% for ($\pi^{+}$ + $\pi^{-}$)/2. Errors are statistical only.

Rcp as a function of centrality 0-10% and 60-92% for ($K^{+}$ + $K^{-}$)/2. Errors are statistical only.

Rcp as a function of centrality 0-10% and 60-92% for charged (p+pbar)/2. Errors are statistical only.

Rcp as a function of centrality 0-10% and 60-92% for neutral pions. Errors are statistical only.

Integrated Rcp above $p_{T}$ = 1.5 GeV/c as a function of centrality 60-92% for pions, kaons, and (p+pbar)/2. Errors are statistical only.

The minimum $\chi^2$ and the parameters $T_{fo}$ and $\beta^{max}_T$ for each of the five centrality selections. The best fit parameters are determined by averaging all parameter pairs within the 1$\sigma$ contour. The errors correspond to the standard deviation of the parameter pairs within the 1$\sigma$ $\chi^2$ contour.

Fit parameters for each particle species using Equations $\frac{dN}{dy}$ = $C \cdot$ ($N_{part}$)$^{\alpha_{part}}$ and $\frac{dN}{dy}$ = $C^{\prime} \cdot$ ($N_{coll}$)$^{\alpha_{coll}}$.

Values of the parameters $n_{pp}$ and $x$ from fitting Equation $R \equiv \frac{dN/dy}{N_{part}}$ = (1-$x$) $\cdot n_{pp} \frac{1}{2}$ + $x \cdot n_{pp} \frac{N_{coll}}{N_{part}}$ = $n_{pp}$ [$\frac{1}{2}$ + $x$($\frac{N_{coll}}{N_{part}}$ - $\frac{1}{2})$]to the observed $dN$/$dy$ per $N_{part}$.

Invariant yields for $\pi^{\pm}$ measured in minimum-bias events at midrapidity and normalized to one rapidity unit.

Invariant yields for $K^{\pm}$ measured in minimum-bias events at midrapidity and normalized to one rapidity unit.

Invariant yields for (anti)$p$ measured in minimum-bias events at midrapidity and normalized to one rapidity unit.

Pion invariant yields in each event centrality and $p_T$ bin measured at midrapidity, normalized to one rapidity unit.

Pion invariant yields in each event centrality and $p_T$ bin measured at midrapidity, normalized to one rapidity unit.

Kaon invariant yields in each event centrality and $p_T$ bin measured at midrapidity, normalized to one rapidity unit.

Kaon invariant yields in each event centrality and $p_T$ bin measured at midrapidity, normalized to one rapidity unit.

(Anti)proton invariant yields in each event centrality and $p_T$ bin measured at midrapidity, normalized to one rapidity unit.

(Anti)proton invariant yields in each event centrality and $p_T$ bin measured at midrapidity, normalized to one rapidity unit.

(Anti)proton invariant yields in each event centrality and $p_T$ bin measured at midrapidity, normalized to one rapidity unit.

(Anti)proton invariant yields in each event centrality and $p_T$ bin measured at midrapidity, normalized to one rapidity unit.

(Anti)proton invariant yields in each event centrality and $p_T$ bin measured at midrapidity, normalized to one rapidity unit.

(Anti)proton invariant yields in each event centrality and $p_T$ bin measured at midrapidity, normalized to one rapidity unit.

(Anti)proton invariant yields in each event centrality and $p_T$ bin measured at midrapidity, normalized to one rapidity unit.

Minimum-bias invariant yields for $\pi^{\pm}$ in equal $p_T$ bins.

Minimum-bias invariant yields for $K^{\pm}$ in equal $p_T$ bins.

Minimum-bias invariant yields for (anti)$p$ in equal $p_T$ bins.

Pion invariant yields in each event centrality normalized to one rapidity unit at midrapidity.

Pion invariant yields in each event centrality normalized to one rapidity unit at midrapidity.

Kaon invariant yields in each event centrality normalized to one rapidity unit at midrapidity.

(Anti)proton invariant yields in each event centrality normalized to one rapidity unit at midrapidity.

(Anti)proton invariant yields in each event centrality normalized to one rapidity unit at midrapidity.

The integrated mean $p_T$ for pions, kaons, and (anti)protons produced in the five different classes of event centrality.

The expansion parameters $T_{fo}$ and $\beta^{max}_T$ as a function of the number of participants.

Measured cross section for TAU+ TAU- production. The data are corrected to no interference between initial and final state radiation.

Measured cross section for E+ E- production.

Measured cross section for E+ E- production.

Measured cross section for E+ E- production.

Measured forward backward asymmetries for MU+ MU- production. The data are corrected to no interference between initial and final state radiation.

Measured forward backward asymmetries for TAU+ TAU- production. The data are corrected to no interference between initial and final state radiation.

Measured forward backward asymmetries for E+ E- production.

Differential cross section (angular distribution) for QUARK QUARKBAR (HADRON) production. The data are corrected to no interference between initial and final state radiation. The systematic (DSYS) errors quoted here do not include the errors on the luminosity given above.

Differential cross section (angular distribution) for QUARK QUARKBAR (HADRON) production. The data are corrected to no interference between initial and final state radiation. The systematic (DSYS) errors quoted here do not include the errors on the luminosity given above.

Differential cross section (angular distribution) for MU+ MU- production. The data are corrected to no interference between initial and final state radiation. The systematic (DSYS) errors quoted here do not include the errors on the luminosity given above.

Differential cross section (angular distribution) for MU+ MU- production. The data are corrected to no interference between initial and final state radiation. The systematic (DSYS) errors quoted here do not include the errors on the luminosity given above.

Differential cross section (angular distribution) for TAU+ TAU- production.The data are corrected to no interference between initial and final state radia tion. The systematic (DSYS) errors quoted here do not include the errors on the luminosity given above.

Differential cross section (angular distribution) for TAU+ TAU- production.The data are corrected to no interference between initial and final state radia tion. The systematic (DSYS) errors quoted here do not include the errors on the luminosity given above.

Differential cross sections(angulardistribution) for E+ E- production.

Differential cross sections(angulardistribution) for E+ E- production.