are thus aperiodic. We
examine some beautiful examples, beginning with one due to Euler:
.
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.
, then
which has very large entries placed irregularly throughout. This
intermittency is a typical feature of a chaotic system [10].
is not known, in the sense that no pattern has
been identified. It begins
and some 17,000,000 elements of this continued fraction have been computed
by Gosper (see [4]). There are many open questions
about this continued fraction---for example, it is not known if the
elements of the continued fraction are bounded.