with the property that, given
,
there is a set U of positive Lebesgue measure in the
-neighbourhood of
such that if x is in U then the
-limit set of orb(x)
is contained in
and the orbit of x is contained in U [10].
has positive Lyapunov exponent and is
thus sensitive to initial conditions but is not chaotic, while
bounded orbits that don't diverge from one another are too regular
to be called `chaotic'. There is a more mathematically flavoured
definition, usually attributed to Devaney, which uses transitivity.
This is, to my mind, not the essence of chaos, though it allows
precise discussion.
.
In this paper we use the term loosely, forgetting about the smoothness
and invertibility (see map).
. Put
and
. Define
, for
where
terminates the process. Then the gcd of a and b is
.
For more details, and to investigate the connection to continued
fractions, see [20]. For a deeper discussion see [16].
(the floor function), towards 0 (the truncate function),
or towards the nearest integer (the round function). By `integer
part' I mean the `floor' function, so that the fractional part
is always nonnegative.
are called fixed points
of the map.
.
.
-limit set of orb(
) is the set
of all initial points whose orbits approach orb(
) as ``time''
increases; to be precise, an initial point
is in the
-limit
set of orb(
) if there exist m and n such that for all
there exists K such that
implies
.
The
-limit set of orb(
) is the set of accumulation
points of orb(
).
, we can
look at the induced map
in the tangent space, formed
by computing the Jacobian matrix
of f. We can then look at
how a unit ball in the tangent space at
evolves under iteration
of this tangent space map, which measures in some sense the
growth of small initial errors as the map is iterated. We can then
look at the `average' rate of growth of the images of this unit ball,
by considering the SVD of the product of
(equivalently, the square roots of the eigenvalues of
). The limiting exponential rate of growth of these singular values (which Osledec [21] showed existed for almost
all initial points, for regular dynamical systems f) are called
the Lyapunov exponents of the map. In our one-dimensional case,
this amounts to computing the limit
where
gives the orbit of G
starting at
.
That is the definition, but it doesn't really tell you what
the Lyapunov exponents are good for.
Click here for a tutorial that will explore Lyapunov exponents further.
to define an orbit
,
.
if the measure of a set A
is the same as the sum of the measures of all the pre-images of A
under f: that is,
. Since f may
be many-to-one, this is a different definition than would result if
we asked for
.
For the Gauss map
frac
, we can fairly easily show
that it preserves the Gauss measure
by considering the so-called basic sets
for
.
The pre-image of the set
is the set of intervals
for
. The measures of these intervals add up
to
Other sets in
may be formed by countable unions and
intersections of these sets, and hence the Gauss measure is preserved
by the Gauss map. The only difficult part of this computation is the
evaluation of the sum in the middle, and this is tedious but straightforward.
In passing I note that Maple can evaluate this sum, when properly coached.
.
of a (here discrete) dynamical
system. Strictly speaking, we allow negative k (because f is
invertible), but in this paper I loosely refer to a `forward' orbit, with
nonnegative k only, simply as an `orbit'. We denote this by
orb
.
where
then x is called a periodic point of the map.
If N is the least such number n, then as usual we say x has
period N.
whose
conjugate (i.e. the other root of the quadratic polynomial with
integer coefficients that
satisfies) lies in the interval
.
grow like
for
some base b, at least initially. Another, more
rigorous, definition of this is that the Lyapunov exponent of
one or both orbits is positive.
Still another
definition is that points that are
close initially will, after
iterations of the
map, be
apart.
) or bi-infinite
(
, with a reference point in the middle).
The `shift map' is a map which moves each
entry in the
sequence one entry to the left:
. See [8] for discussion and application.
where
is an integer and all the other
are positive
integers. See [20] for more details. The
are
called the partial quotients.
.