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:
1. 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 , , or , which tend to 1, 0, and , respectively. Thus the -limit set of this orbit is the set , which, unlike the - limit sets of continuous maps, is not invariant 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.
2. Stark [26]. 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 [10].
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