much as $226$ bins occupied out of a total of $1,728$ (*i.e.* $\eta = 13.08\ \%$).

At a first glance one can identify a series of entropy plateaus, which could be put in correspondence with stationary or quasi-stationary thermodynamic values of the system if a large number of particles would be under study. Some of them will vanish when considering a large number of bins. However, those surviving for $N_{b} \rightarrow \infty$ could be associated with stationary nucleonic states in the chosen potential well in the limit of a large number of degrees of freedom.

For a given 2D phase space lattice formed of $N_{b}=4^3$ bins we present in Figures \[fig:9\]-\[fig:12\] a comparison between the informational entropies of the physical system in study, starting from the adiabatic stage of interaction and gradually increasing the vibrational wall frequency towards the dipole resonance value, $\Omega _{res}=0.145\ c/\rm{fm}$. The slopes for the resonance frequency case were found to be significantly higher than for the adiabatic one ($\Omega _{ad}=0.02\ c/\rm{fm}$) for all multipolarities involved.

Another comparison revealed significant differences between the onset times of the quasi-constant Shannon entropy values for all cases taken into consideration. Thus, for four vibrational radian frequencies and for four 