Hutchinson operator: Difference between revisions
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In [[mathematics]], in the study of [[fractal]]s, a '''Hutchinson operator''' is a collection of functions on an underlying space ''E''. The [[Iterated function|iteration]] on these functions gives rise to an [[iterated function system]], for which the fixed set is [[self-similar]]. | In [[mathematics]], in the study of [[fractal]]s, a '''Hutchinson operator''' is a collection of functions on an underlying space ''E''. The [[Iterated function|iteration]] on these functions gives rise to an [[iterated function system]], for which the fixed set is [[self-similar]]. | ||
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* {{cite journal | last=Hutchinson | first=John E. | title=Fractals and self similarity | journal=Indiana Univ. Math. J. | volume=30 | year=1981 | pages=713–747 | doi=10.1512/iumj.1981.30.30055 }} | * {{cite journal | last=Hutchinson | first=John E. | title=Fractals and self similarity | journal=Indiana Univ. Math. J. | volume=30 | year=1981 | pages=713–747 | doi=10.1512/iumj.1981.30.30055 }} | ||
* {{cite book | title=Chaos and Fractals: New Frontiers of Science | author=Heinz-Otto Peitgen | authorlink=Heinz-Otto Peitgen | coauthors=Hartmut Jürgens, Dietmar Saupe | year=2004 | puclisher=[[Springer-Verlag]] | isbn=0387202293 | pages=84,225 }} | * {{cite book | title=Chaos and Fractals: New Frontiers of Science | author=Heinz-Otto Peitgen | authorlink=Heinz-Otto Peitgen | coauthors=Hartmut Jürgens, Dietmar Saupe | year=2004 | puclisher=[[Springer-Verlag]] | isbn=0387202293 | pages=84,225 }} | ||
Latest revision as of 14:52, 27 October 2008
In mathematics, in the study of fractals, a Hutchinson operator is a collection of functions on an underlying space E. The iteration on these functions gives rise to an iterated function system, for which the fixed set is self-similar.
Definition
Formally, let fi be a finite set of N functions from a set X to itself. We may regard this as defining an operator H on the power set P X as
where A is any subset of X.
A key question in the theory is to describe the fixed sets of the operator H. One way of constructing such a fixed set is to start with an initial point or set S0 and iterate the actions of the fi, taking Sn+1 to be the union of the images of Sn under the operator H; then taking S to be the union of the Sn, that is,
and
Properties
Hutchinson (1981) considered the case when the fi are contraction mappings on a Euclidean space X = Rd. He showed that such a system of functions has a unique compact (closed and bounded) fixed set S.
The collection of functions together with composition form a monoid. With N functions, then one may visualize the monoid as a full N-ary tree or a Cayley tree.
References
- Hutchinson, John E. (1981). "Fractals and self similarity". Indiana Univ. Math. J. 30: 713–747. DOI:10.1512/iumj.1981.30.30055. Research Blogging.
- Heinz-Otto Peitgen; Hartmut Jürgens, Dietmar Saupe (2004). Chaos and Fractals: New Frontiers of Science, 84,225. ISBN 0387202293.