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.