all: $4,133\ \rm{fm}/c$.

The quadrupole oscillation also reveals an apparent intermittent pattern, this time at $\Omega_{ad} = %
0.05\ c/\rm{fm}$. We call it intermittent because after $800\ \rm{fm}/c$ the nucleon fills in only $42.19\ \%$ of the total number of bins (Figure \[fig:12\] and Table \[tab:2\]), and a longer time than $100,000\ \rm{fm}/c$ is required to get to $\eta  = 100\ \%$ (Table \[tab:3\]). However, this behaviour can be a misleading one, the Shannon entropy for a trajectory bunch showing exactly the opposite (see Fig. \[fig:16\] and Table \[tab:4\]), after $122\ \rm{fm}/c$ the orbits being completely dispersed.

Lyapunov exponents
------------------

We furthermore presented another quantitative analysis: the temporal evolution of the Lyapunov exponents, $\lambda\left(t\right)$. As previously shown, initial adjacent points in the phase space $\Delta x_{0} (t=0)$, can generate in time separated trajectories $\Delta x\left(t\right)$. When studying the evolution of a single phase space parameter, the one-dimensional Lyapunov exponent takes the form:

$$\lambda\left(t\right)=\lim_{\left|\Delta x_{0}\right|\rightarrow 0} ln\left|\frac{\Delta x\left(t\right)}{\Delta x_{0}}\right|.$$

The generalization for obtaining the multi-dimensional Lyapunov exponent is then straightforward:

$$\lambda\left(t\right)=ln\frac{\left(\sum_{k=1}^{m}\left[x_{k}\left(t\right)-x_{k0}\right]^{2}\right)^{\frac{1}{2}}}{0.01},$$

where the sum is taken over all $m = 4$ squared differences between final $x_{k}\left(t\right)$ and initial $x_{k0}$ one-nucleon phase space variables. Integration times of the order of $10^{3}$ [fm]{}/c 