$K^{+}$ signal and the corresponding background fit for the region covering mid-rapidity and $m_{t}−m_{0}$ between 25 and 50 $MeV/c^{2}$.

$K^{+}$ signal and the corresponding background fit for the region covering mid-rapidity and $m_{t}−m_{0}$ between 25 and 50 $MeV/c^{2}$.

$K^{+}$ signal and the corresponding background fit for the region covering mid-rapidity and $m_{t}−m_{0}$ between 25 and 50 $MeV/c^{2}$.

$K^{-}$ signal and the corresponding background fit for the region covering mid-rapidity and $m_{t}−m_{0}$ between 50 and 75 $MeV/c^{2}$.

$K^{-}$ signal and the corresponding background fit for the region covering mid-rapidity and $m_{t}−m_{0}$ between 50 and 75 $MeV/c^{2}$.

$K^{-}$ signal and the corresponding background fit for the region covering mid-rapidity and $m_{t}−m_{0}$ between 50 and 75 $MeV/c^{2}$.

$K^{+}K^{-}$ invariant mass distribution for the mid-rapidity region and $m_{t}−m_{0}$ between 0 and 100 $MeV/c^{2}$ after subtraction of the background.

$K^{+}K^{-}$ invariant mass distribution for the mid-rapidity region and $m_{t}−m_{0}$ between 0 and 100 $MeV/c^{2}$ after subtraction of the background.

$K^{+}K^{-}$ invariant mass distribution for the mid-rapidity region and $m_{t}−m_{0}$ between 0 and 100 $MeV/c^{2}$ after subtraction of the background.

Rapidity distributions of $K^{-}$ and $\phi$ as well as extracted inverse slope parameters obtained from the Boltzmann fits to the the $m_{t}$ spectra.

Rapidity distributions of $K^{-}$ and $\phi$ as well as extracted inverse slope parameters obtained from the Boltzmann fits to the the $m_{t}$ spectra.

Rapidity distributions of $K^{-}$ and $\phi$ as well as extracted inverse slope parameters obtained from the Boltzmann fits to the the $m_{t}$ spectra.

$K^{-}$ transverse-mass spectrum around mid-rapidity

$K^{-}$ transverse-mass spectrum around mid-rapidity

$K^{-}$ transverse-mass spectrum around mid-rapidity

Multiplicity ratio $\phi/K^{-}$ as function of $\sqrt{s_{NN}}$ for central heavy-ion collisions.

Multiplicity ratio $\phi/K^{-}$ as function of $\sqrt{s_{NN}}$ for central heavy-ion collisions.

Multiplicity ratio $\phi/K^{-}$ as function of $\sqrt{s_{NN}}$ for central heavy-ion collisions.

Multiplicities and effective inverse slopes $T_{eff}$ at mid-rapidity for given centrality classes.

Multiplicities and effective inverse slopes $T_{eff}$ at mid-rapidity for given centrality classes.

Multiplicities and effective inverse slopes $T_{eff}$ at mid-rapidity for given centrality classes.

Multiplicity ratios for given centrality classes.

Multiplicity ratios for given centrality classes.

Multiplicity ratios for given centrality classes.

Reduced transverse mass ($m_{t}-m_{0}$) spectra of $K^{+}$ for the 0-40% most central events.

Reduced transverse mass ($m_{t}-m_{0}$) spectra of $K^{+}$ for the 0-40% most central events.

Reduced transverse mass ($m_{t}-m_{0}$) spectra of $K^{+}$ for the 0-40% most central events.

Reduced transverse mass ($m_{t}-m_{0}$) spectra of $K^{-}$ for the 0-40% most central events.

Reduced transverse mass ($m_{t}-m_{0}$) spectra of $K^{-}$ for the 0-40% most central events.

Reduced transverse mass ($m_{t}-m_{0}$) spectra of $K^{-}$ for the 0-40% most central events.

Reduced transverse mass ($m_{t}-m_{0}$) spectra of $\phi$ for the 0-40% most central events.

Reduced transverse mass ($m_{t}-m_{0}$) spectra of $\phi$ for the 0-40% most central events.

Reduced transverse mass ($m_{t}-m_{0}$) spectra of $\phi$ for the 0-40% most central events.

Rapidity distribution of $K^{+}$ for the 0-40% most central events.

The integrated number of LAMBDA/C+'s per UPSILON(4S) event at cm energy 10.58 GeV.

Distribution of the invariant mass of the P-LAMBDA subsystem at beam momentum 2.75 GeV.

Distribution of the invariant mass of the K-LAMBDA subsystem at beam momentum 2.75 GeV.

Angular distributions of the LAMBDA in reference to the proton direction inthe K-LAMBDA cm system for a beam momentum of 2.85 GeV.

Angular distributions of the LAMBDA in reference to the proton direction inthe K-LAMBDA cm system for a beam momentum of 2.85 GeV.

Measured yields as a function of Q**2.

Measured yields as a function the Bjorken X variable.

Measured yields as a function the Bjorken Y variable. Note: this data was not in the paper.

Ratios of measured yields for K0S/LAMBDA and LAMBDA/LAMBDABAR as a functionof E, the neutrino energy.

Ratios of measured yields for K0S/LAMBDA and LAMBDABAR/LAMBDA as a functionof W**2.

Ratios of measured yields for K0S/LAMBDA and LAMBDABAR/LAMBDA as a functionof Q**2.

Ratios of measured yields for K0S/LAMBDA and LAMBDABAR/LAMBDA as a functionof the Bjorken X variable.

Efficiency corrected Feynman X distributions.

Efficiency corrected Z distributions.

Efficiency corrected Z distributions for K0S production in two Feynman X regions.

Efficiency corrected Z distributions for LAMDBA production in two Feynman Xregions.

Efficiency corrected Z distributions for LAMDBABAR production in two Feynman X regions.

Efficiency corrected PT**2 distributions.

Efficiency corrected PT**2 distributions for K0S production in two Feynman X regions. Note: this data does not appear in the paper.

Efficiency corrected PT**2 distributions for LAMBDA production in two Feynman X regions. Note: this data does not appear in the paper.

Efficiency corrected PT**2 distributions for LAMBDABAR production in two Feynman X regions. Note: this data does not appear in the paper.

Efficiency corrected mean PT**2 versus Feynman X distributions.

Inclusive pi0 spectra in the UPSILON (1S).

Inclusive eta spectra in the continuum.

Inclusive eta spectra in the UPSILON (1S).

Data read from graph.. Event distributions uncorrected for angular acceptance and the efficiency with energy of the detector RE = GAMMA GAMMA --> PI0 PI0.

Data read from graph.

Data read from graph.. Event distributions uncorrected for angular acceptance and the efficiency with energy of the detector RE = GAMMA GAMMA --> PI0 PI0.