$100.00$ & $89.06$ & $87.50$\         
  ----------------------- --------------------------------------------------------------------------------- -- -- --

  : \[tab:2\]The filling percentage $\eta$ of the $\left( r\leftrightarrow p_{r}\leftrightarrow\theta\right)$ one-particle phase space maps at several multipolarities and frequencies of wall vibration

  ----------------------- ------------------------------------------------------------------------------------ -- -- --
   Oscillation frequency                            [UCE]{} & $L=0$ & $L=1$ & $L=2$\                                 
                            $\Omega \:_{ad} = 0.020\: c/\rm{fm}$ & $>10^{5}$ & $6,023$ & $6,359$ & $5,356$\          
                           $\Omega \:_{ad} = 0.050\: c/\rm{fm}$ & $>10^{5}$ & $1,618$ & $4,223$ & $>10^{5}$\         
                           $\Omega \:\;\ \   = 0.100\: c/\rm{fm}$ & $>10^{5}$ & $11,442$ & $3,241$ & $2,758$\        
                             $\Omega _{res} = 0.145\: c/\rm{fm}$ & $>10^{5}$ & $729$ & $1,887$ & $10,571$\           
  ----------------------- ------------------------------------------------------------------------------------ -- -- --

  : \[tab:3\]The time (in $\rm{fm}/c$) at which the informational entropies of the $\left( r\leftrightarrow p_{r}\leftrightarrow\theta\right)$ one-particle phase space maps at several multipolarities and frequencies of wall vibration have the maximum value (*i.e.* $\eta  = 100\ \%$)

We continue the analysis by further defining the Shannon entropy for a group of $w$ nearby orbits:

$$S_{traject.\ pack}\left(t\right)=ln\ N_{w}\left(t\right),$$

so that the number of occupied cells is:

$$1 \leq N_w(t) \leq w,$$

thus describing the spread of the trajectories at each moment of time $t$ (Figs. \[fig:13\]-\[fig:16\]). When reaching the maximum divergence, the entropy for five distinct phase space 