Ratio of prompt J/PSI to B-BBAR production cross section in P NUCLEON interactions in the Feynmann X range -0.35 to 0.15 for the E+ E- and MU+ MU- channels separately and combined.

Ratio of combined prompt J/PSI to B-BBAR production cross section in P NUCLEON interactions in the Feynmann X range -0.35 to 0.15. including 2000 measurements.

Measured value of the B-BBAR cross section extrapolated to the full phase space.

Measured value of the B-BBAR cross section extrapolated to the full phase space. including 2000 measurements.

The purity and momentum-resolution corrected correlation functions $C_{true}(k^{*})$ for $p-\Lambda$, $\bar{p}-\bar{\Lambda}$ (a), $\bar{p}-\Lambda$, $p-\bar{\Lambda}$ (b). Curves correspond to fits done using the Lednicky and Lyuboshitz analytical model [12].

$(p-\Lambda) \oplus (\bar{p}-\bar{\Lambda})$ and $(\bar{p}-\Lambda) \oplus (p-\bar{\Lambda})$ combined correlation functions. Correlation functions are corrected for purity and momentum resolution. Curves correspond to fits done using the Lednicky and Lyuboshitz analytical model [12].

The combined $(\bar{p}-\Lambda) \oplus (p-\bar{\Lambda})$ spin-averaged $s$-wave scattering length compared with the previous measurements for the $p-\bar{p}$ system [24-27]. The curves show the one standard deviation contours. Note that for $(\bar{p}-\Lambda) \oplus (p-\bar{\Lambda})$ only, one should read $0.1973 \times \mbox{Im}f_{0}$ instead of $\mbox{Im}f_{0}$ on the x-axis.

The combined $(\bar{p}-\Lambda) \oplus (p-\bar{\Lambda})$ spin-averaged $s$-wave scattering length compared with the previous measurements for the $p-\bar{p}$ system [24-27]. The curves show the one standard deviation contours. Note that for $(\bar{p}-\Lambda) \oplus (p-\bar{\Lambda})$ only, one should read $0.1973 \times \mbox{Im}f_{0}$ instead of $\mbox{Im}f_{0}$ on the x-axis.

Pion source size [5] compared with proton and lambda source sizes as a function of the mean transverse mass $(\langle m_{t}\rangle)$ The curve shows the $\langle m_{t}\rangle^{-1/2}$ dependence with an arbitrary normalization.

(Color Online) Variation of $N_{ch}$ normalized to the number of collisions in the FTPC coverage $(2.9 \leq \eta \leq 3.9)$ and $N_{\gamma}$ normalized to number of collisions, in the PMD coverage $(2.3 \leq \eta \leq 3.7)$ as a function of $N_{coll}$. The lower band shows the uncertainty in the ratio due to uncertainties in $N_{coll}$ calculations.

(Color Online) $dN/d\eta$ for charged particles and photons for Au + Au collisions at $\sqrt{s_{NN}}$ = 62.4 GeV for various event centrality classes.

(Color Online) $dN/d\eta$ for charged particles and photons for Au + Au collisions at $\sqrt{s_{NN}}$ = 62.4 GeV for various event centrality classes.

(Color Online) Half width at half maximum of the pseudorapidity distributions ($\eta_{h}$) of charged particles as a function of total charged particle multiplicity ($N_{T}$) normalized to the center of mass energy. The Au + Au collision data are from the PHOBOS [8] experiment and p + p collision data are from the ISR [31] experiments.

(Color Online) Half width at half maximum of the pseudorapidity distributions ($\eta_{h}$) of charged particles as a function of total charged particle multiplicity ($N_{T}$) normalized to the center of mass energy. The Au + Au collision data are from the PHOBOS [8] experiment and p + p collision data are from the ISR [31] experiments.

(Color Online) Variation of $dN_{ch}/d\eta$ normalized to $N_{part}$ with $\eta – y_{beam}$ for central and peripheral collisions for positively charged hadrons ($h^{+}$) and negatively charged hadrons ($h^{−}$).

(Color Online) The top panel shows the variation of pion rapidity density normalized to $N_{part}$ with $y – y_{beam}$ for central collisions at various collision energies. Also shown is the estimated $dN_{\pi^{0}}/dy$ obtained from $dN\_{\gamma}/dy$ normalized to $N_{part}$. The bottom panel shows the variation of net proton rapidity density normalized to $N_{part}$ with $y – y_{beam}$ for central collisions at various collision energies.

(Color Online) The top panel shows the variation of pion rapidity density normalized to $N_{part}$ with $y – y_{beam}$ for central collisions at various collision energies. Also shown is the estimated $dN_{\pi^{0}}/dy$ obtained from $dN\_{\gamma}/dy$ normalized to $N_{part}$. The bottom panel shows the variation of net proton rapidity density normalized to $N_{part}$ with $y – y_{beam}$ for central collisions at various collision energies.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

PT integrated invariant cross sections and density distributions together with mean values of PT and PT**2 as a function of Feynman X for positive pion production.

PT integrated invariant cross sections and density distributions together with mean values of PT and PT**2 as a function of Feynman X for negative pion production.

PT integrated rapidity distribution.

Double differential PI+ production cross section in the angular range 120 to 150 mrad.. Errors shown are point-to-point only.

Double differential PI+ production cross section in the angular range 150 to 180 mrad.. Errors shown are point-to-point only.

Double differential PI+ production cross section in the angular range 180 to 210 mrad.. Errors shown are point-to-point only.

The measured F2 and xF3 at X = 0.125.

The measured F2 and xF3 at X = 0.175.

The measured F2 and xF3 at X = 0.225.

The measured F2 and xF3 at X = 0.275.

The measured F2 and xF3 at X = 0.350.

The measured F2 and xF3 at X = 0.450.

The measured F2 and xF3 at X = 0.550.

The measured F2 and xF3 at X = 0.650.

The measured R (=sigL/sigT)) at X = 0.020.

The measured R (=sigL/sigT)) at X = 0.045.

The measured R (=sigL/sigT)) at X = 0.080.

The measured R (=sigL/sigT)) at X = 0.125.

The measured R (=sigL/sigT)) at X = 0.175.

The measured R (=sigL/sigT)) at X = 0.225.

The measured R (=sigL/sigT)) at X = 0.275.

The measured R (=sigL/sigT)) at X = 0.350.

The measured R (=sigL/sigT)) at X = 0.450.

The measured R (=sigL/sigT)) at X = 0.550.

The measured R (=sigL/sigT)) at X = 0.650.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 25.0 GeV and X =0.020.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 25.0 GeV and X =0.045.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 25.0 GeV and X =0.080.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 25.0 GeV and X =0.125.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 25.0 GeV and X =0.175.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 25.0 GeV and X =0.225.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 25.0 GeV and X =0.275.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 25.0 GeV and X =0.350.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 25.0 GeV and X =0.450.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 25.0 GeV and X =0.550.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 25.0 GeV and X =0.650.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 35.0 GeV and X =0.020.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 35.0 GeV and X =0.045.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 35.0 GeV and X =0.080.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 35.0 GeV and X =0.125.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 35.0 GeV and X =0.175.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 35.0 GeV and X =0.225.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 35.0 GeV and X =0.275.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 35.0 GeV and X =0.350.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 35.0 GeV and X =0.450.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 35.0 GeV and X =0.550.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 35.0 GeV and X =0.650.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 45.0 GeV and X =0.020.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 45.0 GeV and X =0.045.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 45.0 GeV and X =0.080.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 45.0 GeV and X =0.125.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 45.0 GeV and X =0.175.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 45.0 GeV and X =0.225.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 45.0 GeV and X =0.275.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 45.0 GeV and X =0.350.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 45.0 GeV and X =0.450.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 45.0 GeV and X =0.550.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 45.0 GeV and X =0.650.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 55.0 GeV and X =0.020.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 55.0 GeV and X =0.045.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 55.0 GeV and X =0.080.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 55.0 GeV and X =0.125.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 55.0 GeV and X =0.175.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 55.0 GeV and X =0.225.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 55.0 GeV and X =0.275.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 55.0 GeV and X =0.350.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 55.0 GeV and X =0.450.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 55.0 GeV and X =0.550.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 55.0 GeV and X =0.650.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 70.0 GeV and X =0.020.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 70.0 GeV and X =0.045.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 70.0 GeV and X =0.080.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 70.0 GeV and X =0.125.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 70.0 GeV and X =0.175.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 70.0 GeV and X =0.225.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 70.0 GeV and X =0.275.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 70.0 GeV and X =0.350.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 70.0 GeV and X =0.450.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 70.0 GeV and X =0.550.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 70.0 GeV and X =0.650.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 90.0 GeV and X =0.020.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 90.0 GeV and X =0.045.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 90.0 GeV and X =0.080.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 90.0 GeV and X =0.125.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 90.0 GeV and X =0.175.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 90.0 GeV and X =0.225.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 90.0 GeV and X =0.275.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 90.0 GeV and X =0.350.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 90.0 GeV and X =0.450.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 90.0 GeV and X =0.550.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 90.0 GeV and X =0.650.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 110.0 GeV and X =0.020.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 110.0 GeV and X =0.045.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 110.0 GeV and X =0.080.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 110.0 GeV and X =0.125.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 110.0 GeV and X =0.175.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 110.0 GeV and X =0.225.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 110.0 GeV and X =0.275.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 110.0 GeV and X =0.350.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 110.0 GeV and X =0.450.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 110.0 GeV and X =0.550.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 110.0 GeV and X =0.650.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 130.0 GeV and X =0.020.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 130.0 GeV and X =0.045.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 130.0 GeV and X =0.080.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 130.0 GeV and X =0.125.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 130.0 GeV and X =0.175.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 130.0 GeV and X =0.225.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 130.0 GeV and X =0.275.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 130.0 GeV and X =0.350.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 130.0 GeV and X =0.450.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 130.0 GeV and X =0.550.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 130.0 GeV and X =0.650.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 170.0 GeV and X =0.020.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 170.0 GeV and X =0.045.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 170.0 GeV and X =0.080.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 170.0 GeV and X =0.125.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 170.0 GeV and X =0.175.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 170.0 GeV and X =0.225.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 170.0 GeV and X =0.275.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 170.0 GeV and X =0.350.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 170.0 GeV and X =0.450.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 170.0 GeV and X =0.550.

Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 170.0 GeV and X =0.650.

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.

Measured MU+ MU- cross section for the high-energy data sample.

Measured TAU+ TAU- cross section for the inclusive data sample.

Measured TAU+ TAU- cross section for the high-energy data sample.

Measured E+ E- --> E+ E- cross section for the inclusive data sample.

Measured E+ E- --> E+ E- cross section for the high-energy data sample.

Measured Forward-Backward asymmetry in MU+ MU- production from the inclusive data sample.

Measured Forward-Backward asymmetry in MU+ MU- production from the high-energy data sample.

Measured Forward-Backward asymmetry in TAU+ TAU- production from the inclusive data sample.

Measured Forward-Backward asymmetry in TAU+ TAU- production from the high-energy data sample.

Measured Forward-Backward asymmetry in E+ E- production for the inclusive data sample.

Measured Forward-Backward asymmetry in E+ E- production for the high-energy data sample.

Differential cross sections for E+ E- production as a function of the scattering angle for the high-energy data sample for centre of mass energy 192 GeV.

Differential cross sections for E+ E- production as a function of the scattering angle for the high-energy data sample for centre of mass energy 196 GeV.

Differential cross sections for E+ E- production as a function of the scattering angle for the high-energy data sample for centre of mass energy 200 GeV.

Differential cross sections for E+ E- production as a function of the scattering angle for the high-energy data sample for centre of mass energy 202 GeV.

Differential cross sections for E+ E- production as a function of the scattering angle for the high-energy data sample for centre of mass energy 205 GeV.

Differential cross sections for E+ E- production as a function of the scattering angle for the high-energy data sample for centre of mass energy 207 GeV.

Differential cross sections for E+ E- production as a function of the scattering angle for the high-energy data sample for centre of mass energy 208 GeV.