First of all, let us assume without loss of generality that $x_0>0$ (implying that all further $x_n$ are themselves $>0$).
Indeed if $x_0<0$, we have completely symmetrical results.
In fact, this sequence can be "casted" into a Newton's method convergence:
$$x_{n+1}=x_n-\dfrac{f(x_n)}{f'(x_n)}=x_n-\dfrac{x_n^2-16}{2x_n}$$
with $f$ defined by $f(x)=x^2-16$ (roots of $f(x)=0$ are precisely $\pm 4$).
One of the essential properties of Newton's method is that it has a quadratic convergence. It means that
$$e_{n+1}=Ke_n^2 \ \ \text{where} \ \ e_n=|x_{n+1}-4| \ \ \text{and} \ \ K=\dfrac{f''(L)}{2f'(L)}=\dfrac18.$$
(where $L$ is the limit, with $L=4$ here).
for a certain $K$, which gives a fantastic speed of convergence (under the condition to be in a good vicinity of the root).
Therefore, the computation of $\lim_{n \to \infty} \frac{e_{n+1}}{e_{n}}$ i.e.
$$\lim_{n \to \infty} \frac{|x_{n+1}-4|}{{|x_{n}-4|}}$$
will give $0$ but gives no information, plainly because the convergence isn't linear as is the case for example for a fixed point method.