In Fig. 4.3 we show a phase space which is part of
the real line. It is divided into three subintervals
(
). The return map is shown. This return map
shows that the interval
is mapped onto
the interval
. Similarly,
is mapped onto
, and
is mapped onto all three intervals.
More mathematically, we could write
. These
relations are summarized on the right in a
transition graph. The arrow from
to
says
that
covers
, or that
is in the image of
(under
).
Mathematically we write
, and similarly for the
arrow from
to
. Since the image of
covers everything, there are arrows from
to everybody. These relations are also very
conveniently summarized in a (Markov) transition
matrix. The rows and columns are labeled by the
indices for the partition (e.g.,
).
The matrix element
if
does
not cover
. If
,
.
The first row (
) of the
transition matrix
for the return map of Fig. 4.3 is
. The
entire matrix is
![]() |
(3) |
Another example is given in Fig. 4.4. In this case
the partition has four components. The return map
is shown on the left and the transition graph
is shown on the right. The Markov transition
matrix is
![]() |
(4) |
|
|