Of course, non-quadratic irrationals have continued fraction expansions,
too. By Lagrange's theorem, these continued fractions are aperiodic,
and hence the orbit of these initial points under the Gauss map is
aperiodic. Note that most numbers in are thus aperiodic. We
examine some beautiful examples, beginning with one due to Euler:
e (the base of the natural logarithms) has an aperiodic continued
fraction expansion .
The elements of the orbit of this initial point are always of the form
which tend to 1, 0, and , respectively. Thus the
of this orbit is the set , which, unlike the -
limit sets of continuous maps, is notinvariant
under the Gauss
map since so G applied to this set simply gives
0. In other words, we have an
asymptotically periodic orbit which is
not asymptotic to a real orbit of the map. This cannot happen for a
discrete dynamical system with a continuous map.
Stark . If x is the positive root of , then
which has very large entries placed irregularly throughout. This
intermittency is a typical feature of a chaotic system .