Signal region detector-level distribution for the observable $p_{\mathrm{T}}^{\mathrm{lead}\, \ell}$.

Signal region detector-level distribution for the observable $m_{e\mu}$.

Signal region detector-level distribution for the observable $p_{\mathrm{T}}^{e\mu}$.

Measured fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $|y_{e\mu}|$

Relative systematic uncertainties for the fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $|y_{e\mu}|$

Measured fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $|\Delta \phi(e \mu)|$

Relative systematic uncertainties for the fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $|\Delta \phi(e \mu)|$

Measured fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $ \cos\theta^{\ast}$

Relative systematic uncertainties for the fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $ \cos\theta^{\ast}$

Measured fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $p_{\mathrm{T}}^{\mathrm{lead}\, \ell}$

Relative systematic uncertainties for the fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $p_{\mathrm{T}}^{\mathrm{lead}\, \ell}$

Measured fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $m_{e\mu}$

Relative systematic uncertainties for the fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $m_{e\mu}$

Measured fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $p_{\mathrm{T}}^{e\mu}$

Relative systematic uncertainties for the fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $p_{\mathrm{T}}^{e\mu}$

The statistical correlation coefficients (in percentage) between bins for the measured fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $|y_{e\mu}|$

The total correlation coefficients (in percentage) between bins for the measured fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $|y_{e\mu}|$

The statistical correlation coefficients (in percentage) between bins for the measured fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $|\Delta \phi(e \mu)|$

The total correlation coefficients (in percentage) between bins for the measured fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $|\Delta \phi(e \mu)|$

The statistical correlation coefficients (in percentage) between bins for the measured fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $ \cos\theta^{\ast}$

The total correlation coefficients (in percentage) between bins for the measured fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $ \cos\theta^{\ast}$

The statistical correlation coefficients (in percentage) between bins for the measured fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $p_{\mathrm{T}}^{\mathrm{lead}\, \ell}$

The total correlation coefficients (in percentage) between bins for the measured fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $p_{\mathrm{T}}^{\mathrm{lead}\, \ell}$

The statistical correlation coefficients (in percentage) between bins for the measured fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $m_{e\mu}$

The total correlation coefficients (in percentage) between bins for the measured fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $m_{e\mu}$

The statistical correlation coefficients (in percentage) between bins for the measured fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $p_{\mathrm{T}}^{e\mu}$

The total correlation coefficients (in percentage) between bins for the measured fiducial differential cross-section of $WW \rightarrow e^{\pm}\nu\mu^{\mp}\nu$ production for the observable $p_{\mathrm{T}}^{e\mu}$

The standard deviation (DISPERSION) of the subject multiplicity for gluon jets and quark jets for different values of the subject resolution parameter Y0.

The ratio of the multiplicities and their standard deviations for the subject in quark and gluon jets as a function of the subject resolution parameter Y0.

The measured fragmentation function for charged particles within quark and gluon jets.

The dsig/dpt**2 distribution was approximated by the expression: dsig /dpt**2 = CONST(C=1)*SLOPE(C=1)*EXP(-SLOPE(C1)*PT**2) + CONST(C=2)*SLOPE(C=2)* EXP(-SLOPE(C2)*PT**2).

No description provided.

No description provided.

No description provided.

No description provided.

Charged particle Thrust(minor) distribution.

Charged particle Two-jet resolution variable, Y3 distribution.

Charged particle Heavy Jet Mass distribution.

Charged particle C-Parameter distribution.

Charged particle Oblateness distribution.

Charged particle XP distribution.

Charged particle rapidity distribution.

Charged particle PTIN distribution.

Charged particle PTOUT distribution.

Measure n-jet rates using the Durham cluster algorithm as a function of thejet-resolution parameter YCUT.

Measure n-jet rates using the Durham cluster algorithm as a function of thejet-resolution parameter YCUT.

Measure n-jet rates using the Durham cluster algorithm as a function of thejet-resolution parameter YCUT.

Measure n-jet rates using the Durham cluster algorithm as a function of thejet-resolution parameter YCUT.

Charged particle inclusive distribution of -LN(1/X).

Unfolded charged particle multiplicity distribution giving the probability to have a hadronic Z0 decay with N charged particles.

Values of the mean values of the leading moments of the charged particle multiplicity distribution. R2 is the second binomial moment defined as MEAN(N*(N-1))/MULT**2.

Unfolded values of the the mean multiplicity and dispersion of the multiplicity distributions integaretd over the rapidity region -0.5 to 0.5.

Unfolded values of the the mean multiplicity and dispersion of the multiplicity distributions integrated over the rapidity region -1.0 to 1.0.

Unfolded values of the the mean multiplicity and dispersion of the multiplicity distributions integrated over the rapidity region -1.5 to 1.5.

Unfolded values of the the mean multiplicity and dispersion of the multiplicity distributions integrated over the rapidity region -2.0 to 2.0.

Unfolded values of the the mean multiplicity and dispersion of the multiplicity distribution integrated over the full rapidity region.

Differential cross sections for the inclusive production of PI+-. Additional 3pct systematic uncertainty.

Differential cross sections for the inclusive production of K+-. Additionalsystematic uncertainty 3% above and 5% below X = 0.010.

Differential cross sections for the inclusive production of P PBAR. Additional systematic uncertainty 3% above and 5% below X = 0.018.

Measured inclusive photon cross section. Errors contain both statistical and systematic uncertainties.

Measured differential cross section for PI0 production.

Measured fragmentation function at the ETA meson. Additional 6pct systematic error.

Measured fragmentation function at the ETAPRIME meson. Additional 8pct systematic error.

Inclusive K0 spectrum. Additional 2pct normalization error.

Inclusive LAMBDA spectrum. Additional 4pct normalization error.

Fragmentation distribution for XI production.

Fragmentation distribution for SIGMA(1385) production.

Fragmentation distribution for XI(1530) production.

Differential cross section for RHO0 production.

Differential cross section for OMEGA production.

Differential cross section for K*0 production.

Differential cross section for PHI production.

Differential cross section for K*0 production as a function of the transverse momentum with respect to the Thrust axis.

Differential cross section for PHI production as a function of the transverse momentum with respect to the Thrust axis.

Fragmentation distribution for K*+- production.

Mean Multiplicities. Where a second systematic error is given, this is due to the uncertainty in the extrapolation to X = 0. Note that the ETA and ETAPRIMEvalues are for X > 0.1.

PI0 cross sections as a function of the transverse momentum PTIN relative to the plane defined by the sphericity tensor.

Corrected production rates from the etaprime --> rho0 gamma decay mode. Extrapolation to full x range.

Differential cross section for inclusive omega production from the omega --> pi+ pi- p0 decay mode data. The mean x values are the appropriate x position to plot the data according to the method of Lafferty et al (NIM A 355(95)541).

Differential cross section for inclusive omega production from the omega --> pi+ pi- p0 decay mode data. The mean x values are the appropriate x position to plot the data according to the method of Lafferty et al (NIM A 355(95)541).

Differential cross section for inclusive etaprime production from the etaprime --> pi+ pi- eta decay mode data. The mean x values are the appropriate x position to plot the data according to the method of Lafferty et al (NIM A 355(95)541).

Differential cross section for inclusive etaprime production from the etaprime --> pi+ pi- eta decay mode data. The mean x values are the appropriate x position to plot the data according to the method of Lafferty et al (NIM A 355(95)541).

Differential cross section for inclusive etaprime production from the etaprime --> rho0 gamma decay mode data. The mean x values are the appropriate x position to plot the data according to the method of Lafferty et al (NIM A 355(95)541).

Differential cross section for inclusive etaprime production from the etaprime --> rho0 gamma decay mode data. The mean x values are the appropriate x position to plot the data according to the method of Lafferty et al (NIM A 355(95)541).

Differential cross section for inclusive etaprime production obtained by combining the two etaprime decay modes.

Differential cross section for inclusive etaprime production obtained by combining the two etaprime decay modes.

Inclusive charged particle distribution as a function of PT out of the event plane.

Mean charged particle multiplicity.

Inclusive charged particle distribution as a function of -LN(XP).

Distribution of Thrust.

Distribution of -LN(Y3).

No description provided.

XI multiplicity in direct upsilon(1S) decays.