phase space is not covered up by all five trajectories for the whole range of $10,000\ \rm{fm}/c$ considered, when analyzing $S_{traject.\ pack}$ (Fig. \[fig:13\] and Table \[tab:4\]).

For the dipole oscillations mode, at $\Omega_{ad} = 0.05\ c/\rm{fm}$, it appears that, after only $800\ \rm{fm}/c$, the entropy closes in upon its maximum value: $S_{Max} = ln\ N_{total\ cells} = 4.1589$ (Fig. \[fig:11\] and Table \[tab:1\]). However, on long periods of time, the real tendency is towards filling up the nucleonic phase space as rapid as the vibrational frequency is increased (Table \[tab:3\]). The exact pattern is repeated when studying the Shannon entropy for closeby nucleonic trajectories (Fig. \[fig:15\] and Table \[tab:4\]).

We found quite the same feature for the monopole case, with exception for the intermittent “window” at $\Omega=0.1\ c/\rm{fm}$ (Tables \[tab:1\], \[tab:2\] and Fig. \[fig:10\]). The occupying rate is so small in the intermittent zone, that just at $11,442\ \rm{fm}/c$, the particle would have covered the whole phase space (see Table \[tab:3\]). A similar conclusion can be drawn from Table \[tab:4\] and Fig. \[fig:14\] (with a double temporal scale scanned for the intermittent frequency). The trajectory pack informational entropy reaches its highest value after the longest one-particle evolution time of 