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\section*{\usemenu{slac-pub-7172::context::slac-pub-7172-0-0-6u3}{Figure captions }}\label{section::slac-pub-7172-0-0-6u3}
\noindent
{\bf Figure 1}.
The distribution of the
number of tracks per hemisphere $n_{sig}$ that miss the interaction
point by more
than 3$\sigma$ in the $x$-$y$ plane.
The points represent the data distribution and
the solid histogram represents the
Monte Carlo simulated distribution.
The flavor composition of the Monte Carlo distribution is shown.
\vspace{5mm}
\noindent
{\bf Figure 2}.
The distributions of $\Delta M$ for
a) $D^0 \to K^-\pi^+$, b) $D^0 \to K^-\pi^+\pi^0$ and
c) $D^0 \to K^-\pi^+\pi^+\pi^-$;
d) $M(K^-\pi^+\pi^+)$ distribution for $D^+ \to K^-\pi^+\pi^+$ (see text).
The points represent the data distributions and
the solid histograms represent the Monte Carlo simulated distributions.
The flavor composition of the Monte Carlo distributions is shown.
\vspace{5mm}
\noindent
{\bf Figure 3}.
a)
Our measurements of $\aven_{uds}$ plotted at $W=M_{Z^0}$ and the
non-leading multiplicities $\aven^{nl}_c$ and $\aven^{nl}_b$
plotted at the appropriately reduced non-leading energy
$[1-\langle x_{E_Q}(W)\rangle ]W$.
Previous measurements of these quantities
\cite{1,6,7,8,9,10,27,28}
are also shown.
The solid curve is a fit \cite{27}
to $\aven_{uds}$ measured in the range 5 $