$T=2\pi /3$, $p_0=0.0$

Figures C.18-C.28.

While I do not discuss explicitly each of the figures of this section, attention should be called to figure C.20: there, for smaller values of $n$ ( $n{ {\protect\begin{array}{c} <\protect\\ [-0.3cm]\sim \protect\end{array}} }300$), no regular structure of the HUSIMI distribution seems to develop, as a consequence of the quite large values of $V_0=20.0$ and $\hbar =1.0$. But the sub-figures for larger $n$ indicate that this absence of a regular pattern is a transitional feature of the dynamics: for $n{ {\protect\begin{array}{c} >\protect\\ [-0.3cm]\sim \protect\end{array}} }1000$, a relatively regular hexagonal pattern has been generated around the position of the initial state.