paths gets its highest value (Table \[tab:4\]).

  ----------------------- ------------------------------------------------------------------------------- -- -- --
   Oscillation frequency                         [UCE]{} & $L=0$ & $L=1$ & $L=2$\                               
                            $\Omega \:_{ad} = 0.020\: c/\rm{fm}$ & $>10^{4}$ & $1,095$ & $555$ & $688$\         
                             $\Omega \:_{ad} = 0.050\: c/\rm{fm}$ & $>10^{4}$ & $855$ & $476$ & $122$\          
                           $\Omega \:\;\ \   = 0.100\: c/\rm{fm}$ & $>10^{4}$ & $4,133$ & $333$ & $395$\        
                             $\Omega _{res} = 0.145\: c/\rm{fm}$ & $>10^{4}$ & $279$ & $327$ & $469$\           
  ----------------------- ------------------------------------------------------------------------------- -- -- --

  : \[tab:4\]The time (in $\rm{fm}/c$) at which the one-particle Shannon entropies of a pack of $w=5$ close orbits begin having the maximum value (*i.e.* $S_{traject.\ pack} = 1.60944$) for various coupling degrees between the one-nucleon and the collective *d.o.f.* and for the standard chosen wall frequencies

We begin the analysis with the [UCE]{} case. The single and collective uncoupled *d.o.f.* give birth to a quasi-laminar behaviour with a weak development of chaotic states. The one-particle informational entropy shows an identical evolution, no matter the frequency chosen. The orbit covers, after $800\ \rm{fm}/c$, only $62.50\ \%$ of the entire lattice (Table \[tab:2\] and Figure \[fig:9\]) and does not reach $100\ \%$, even after $\Delta t = 100,000\ \rm{fm}/c$ (Table \[tab:3\]). Also, the 