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\begin{document}
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\begin{figure}
\begin{flushleft}
Fig. 1: Hadronic current for the process (a) $\tau \to \nu_{\tau}
\rho, \rho \to a_1 \pi, a_1 \to \rho \pi, \rho \to \pi \pi $ and (b)
$\tau \to \nu_{\tau} \rho, \rho \to (\pi \pi)_s \rho, \rho \to
\pi \pi $
\end{flushleft}
\begin{center}
\mbox{\epsfig{figure=tau1.ps,width=15.8cm,%
bbllx=2.cm,bblly=6.cm,bburx=20.cm,bbury=20.cm}}
\unitlength1.0cm
\end{center}
\end{figure}
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\begin{figure}
\begin{flushleft}
Fig. 2: Hadronic current of the anomalous part
\end{flushleft}
\begin{center}
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bbllx=2.cm,bblly=6.cm,bburx=20.cm,bbury=20.cm}}
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\end{center}
\end{figure}         
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%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%                Fig plot1a
\begin{figure}
\begin{flushleft}
Fig. 4(a): Cross section for $e^+ e^- \to 2 \pi^+ 2 \pi^-$: Data
from Nowosibirsk (dots with error bars) [12] ,
from Frascati (triangles) [13] and
from Orsay (crosses) [14], and the result of our model (solid line).
\end{flushleft}
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%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%                Fig plot1b
\begin{figure}
\begin{flushleft}
Fig. 4(b): Cross section for $e^+ e^- \to \pi^+ \pi^- 2 \pi^0$: Data
from Nowosibirsk (dots with error bars) [12] ,
from Frascati (triangles) [13] and
from Orsay (crosses) [14], and the result of our model (solid line).
\end{flushleft}
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%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%                Fig plot2
\begin{figure}
\begin{flushleft}
Fig. 5: Distribution of the invariant mass of the four pion system
in the decay $\tau^- \to \nu_\tau 2\pi^-\pi^+\pi^0$:
Data from Argus (dots with error bars) [4], the result of our model 
(lego plot with solid lines) and the one of Tauola 2.4 (lego plot 
with dotted lines). 
\end{flushleft}
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$ }}
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{dm_{4\pi}}   \, [\mbox{GeV}^{-1}]$}}
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  \end{center}
\end{figure}
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%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%                Fig plot3
\begin{figure}
\begin{flushleft}
Fig. 6: Distribution of the invariant mass of the $\pi^+\pi^-\pi^0$ 
subsystem
in the decay $\tau^- \to \nu_\tau 2\pi^-\pi^+\pi^0$: (two entries 
per event).
Data from Argus (dots with error bars) [4], the result of our model 
(lego plot with solid lines) 
and the one of Tauola 2.4 (lego plot with dotted lines).
\end{flushleft}
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{dm_{3\pi}}   \, [\mbox{GeV}^{-1}]$}}
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  \end{center}
\end{figure}
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%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%                Fig plot4
\begin{figure}
\begin{flushleft}
Fig. 7: Distribution of the invariant mass of various two-pion 
subsystems in the decay $\tau^- \to \nu_\tau 2\pi^-\pi^+\pi^0$:
Data from Argus (dots with error bars) [4], the result of our model 
(lego plots with solid lines) 
and the one of Tauola 2.4 (lego plots with dotted lines).
\end{flushleft}

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    (a) $\pi^+\pi^-$         %%%%%%%%%%%%%%%%%  4a
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\end{figure}
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\begin{figure}
\begin{center}
     (b) $\pi^\pm \pi^0$ \par
      (sum of (c) and (d))
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%%%%%%%%%%%%%%%%%%%%%%%%%%%              4c
\begin{figure}
\begin{center}
     (c) $\pi^- \pi^0$
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\end{figure}
%%%%%%%%%%%%%%%%%%%%%%%%%%%              4d
\begin{figure}
\begin{center}
     (d) $\pi^+ \pi^0$
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\end{figure}
%%%%%%%%%%%%%%%%%%%%%%%%%%%            4e
\begin{figure}
\begin{center}
     (e) $\pi^\pm \pi^\pm$
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\end{figure}
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\end{document}

