emerged at $\Omega = 0.1\ c/\rm{fm}$:

$$E_{L_{UCE}} = 18.05 - E_r,$$

$$E_{L_{\Omega=0.1\: c/\rm{fm}}} = 18.09 - E_r.$$

Moreover, for the intermittency frequency of monopole oscillations, one can notice a second smaller segment with the same negative slope:

$$E_{L_{\Omega=0.1\: c/\rm{fm}}} = 5.87 - E_r.$$

For the uncoupled differential equations there are a couple of extreme values for the centrifugal kinetic energy: $E_{L_{min}}(UCE) = 1.02\ \rm{MeV}$, and $E_{L_{Max}}(UCE) = 18.05\ \rm{MeV}$, associated with $r_{Max}(UCE)$ and respectively, with $r_{min}(UCE)$ (left column of Fig. \[fig:3\] and Eq. (1)).

As for the monopolar intermittency, we can distinguish just five distinct values for the $E_{L}$: $1.32\ \rm{MeV}$, $2.13\ \rm{MeV}$, $3.01\ \rm{MeV}$, $5.87\ \rm{MeV}$, and $18.09\ \rm{MeV}$ (central plot of Fig. \[fig:3\]), correlated with stationary radii: $r_{1} \approx 5.26\ \rm{fm}$, $r_{2} %
\approx 4.14\ \rm{fm}$, $r_{3} \approx 3.49\ \rm{fm}$, $r_{4} \approx 2.51\ \rm{fm}$, and $r_{5} \approx %
1.43\ \rm{fm}$ (Eq. (1), Fig. 2 of [@felea-09a], and central plot of Fig. \[fig:2\]). Thus, the nucleonic motion for the intermittent case is composed of alternated revolutions about the force field centre, forming a cyclic symmetrical structure, for e.g., $r_{1}$, $r_{5}$, $r_{2}$, $r_{4}$, $r_{3}$, $r_{4}$, $r_{2}$, $r_{5}$, $r_{1}$, and so on (Fig. \[fig:2\]). This behaviour can be easily verified through 