It is now possible to assign a precise quantity to measure the strength of
attraction of an attractor. Two definitions are given, followed by a proof
that the two are really the same. The first, called here the
"intensity" ,
assigns to an attractor
the supremum over all values of
such
that
is an attractor block for
.
That is, every attractor
block
associated with
has the property that the minimum distance
from the image of
to its complement does not exceed the intensity of
. Furthermore, the intensity is the smallest such number. The second
definition, called here the "chain intensity"
,
assigns to an attractor
the supremum over all values of
such that every
-pseudo-orbit
starting in
stays in some compact
subset of the domain of attraction of
.
That is, every
-pseudo-orbit which starts in
and for which
does not
exceed the chain intensity of
remains inside the domain of attraction
of
. On the other hand, if
does exceed the chain
intensity of
, then one can find an
-pseudo-orbit
starting on
and
leaving every compact subset of the domain of attraction of
.
The next theorem states that the intensity and chain intensity is equal for a given attractor.
Conley was interested in the concept of "continuation" of an isolated invariant set in his study of the topological properties persisting under perturbation [3].
Given two different maps on the same space and an attractor for each map,
one attractor is said to "continue immediately" to the other if a common
attractor block can be found which is associated with each of the
attractors.
The notion of "continuation" is obtained from the notion of "immediate continuation" by completing it to a transitive relation. In other words, an attractor for a map is said to "continue" to an attractor for another map if a sequence of maps and attractors can be found, each continuing immediately to the next.
The notion of "immediate
continuation" of an attractor is closely related to its intensity of
attraction. It will be convenient to introduce some notation to be used
in the discussion of this relationship. If
is an attractor for the
map
, then the intensity depends not only on the set
but also
on the map
. If there is any doubt about which map is used in the
computation of the intensity, then it will be expicitly indicated. In
particular,
while
The standard
metric is used on the space of maps,
where
and
are both maps on
. The following property
is an immediate consequence of the definitions.
Theorem 5.2 If
is an attractor for
the map
and if the map
satisfies
, then there exists an attractor
for
such that
is an immediate continuation of
.
It is natural to ask whether there is some kind of converse to
Theorem 5.2. In other words, given an
attractor
for the map
and given an
, does
there exist a map
satisfying
such that
has no attractor which is an immediate continuation of
? The
answer, in this generality, is "no".
Although it would be interesting to explore the conditions under which
the answer is "yes", no such exploration will be undertaken here.
Copyright (c) 1998 by Richard
McGehee, all rights reserved.