Intensity

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" [More], assigns to an attractor Inten1.jpg [More] the supremum over all values of Inten2.jpg [More] such that Inten3.jpg is an attractor block for Inten4.jpg [More]. That is, every attractor block Inten5.jpg associated with Inten6.jpg has the property that the minimum distance from the image of Inten7.jpg to its complement does not exceed the intensity of Inten8.jpg . Furthermore, the intensity is the smallest such number. The second definition, called here the "chain intensity" [More], assigns to an attractor Inten9.jpg the supremum over all values of Inten10.jpg such that every Inten11.jpg -pseudo-orbit [More] starting in Inten12.jpg stays in some compact subset of the domain of attraction of Inten13.jpg [More]. That is, every Inten14.jpg -pseudo-orbit which starts in Inten15.jpg and for which Inten16.jpg does not exceed the chain intensity of Inten17.jpg remains inside the domain of attraction of Inten18.jpg . On the other hand, if Inten19.jpg does exceed the chain intensity of Inten20.jpg , then one can find an Inten21.jpg -pseudo-orbit starting on Inten22.jpg and leaving every compact subset of the domain of attraction of Inten23.jpg .

The next theorem states that the intensity and chain intensity is equal for a given attractor.

Theorem 5.1 Inten24.jpg .

Proof.

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. [More]

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 Inten25.jpg is an attractor for the map Inten26.jpg , then the intensity depends not only on the set Inten27.jpg but also on the map Inten28.jpg . If there is any doubt about which map is used in the computation of the intensity, then it will be expicitly indicated. In particular,

Inten29.jpg

while

Inten30.jpg

The standard Inten31.jpg metric is used on the space of maps,

Inten32.jpg

where Inten33.jpg and Inten34.jpg are both maps on Inten35.jpg . The following property is an immediate consequence of the definitions.

(5-1) Inten36.jpg

Theorem 5.2 If Inten37.jpg is an attractor for the map Inten38.jpg and if the map Inten39.jpg satisfies Inten40.jpg , then there exists an attractor Inten41.jpg for Inten42.jpg such that Inten43.jpg is an immediate continuation of Inten44.jpg .

Proof.

It is natural to ask whether there is some kind of converse to Theorem 5.2. In other words, given an attractor Inten45.jpg for the map Inten46.jpg and given an Inten47.jpg , does there exist a map Inten48.jpg satisfying Inten49.jpg such that Inten50.jpg has no attractor which is an immediate continuation of Inten51.jpg ? The answer, in this generality, is "no". [More] Although it would be interesting to explore the conditions under which the answer is "yes", no such exploration will be undertaken here.


[Left] Pseudo-orbits
[Right] Discrete approximations
[Up] Main entry point

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Copyright (c) 1998 by Richard McGehee, all rights reserved.
Last modified: July 31, 1998.