A survey of weighted substitution operators and generalizations of Banach‐stone theorem

Singh, Raj

doi:10.1155/ijmms.2005.937

Cited by 2 publications

(2 citation statements)

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“…They are algebras on generators and relations; and often, as is the case in the present paper, the generators may be identified as substitution operators [Jor04]. However, these substitution operators and their adjoints (often called transfer operators) are of independent interest; see, e.g., [JP96,Sin05,KS93,Kwa04].…”

Section: Introduction: Ifss and Operator Theorymentioning

confidence: 90%

Harmonic analysis of iterated function systems with overlap

Jørgensen

Kornelson

Shuman

2007

Journal of Mathematical Physics

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Abstract. An iterated function system (IFS) is a system of contractive mappings τ i : Y → Y , i = 1, . . . , N (finite) where Y is a complete metric space. Every such IFS has a unique (up to scale) equilibrium measure (also called the Hutchinson measure µ), and we study the Hilbert space L 2 (µ).In this paper we extend previous work on IFSs without overlap. Our method involves systems of operators generalizing the more familiar Cuntz relations from operator algebra theory, and from subband filter operators in signal processing.These Cuntz-like operator systems were used in recent papers on wavelets analysis by Baggett, Jorgensen, Merrill and Packer, where they serve as a first step to generating wavelet bases of Parseval type (alias normalized tight frames), i.e., wavelet bases with redundancy.Similarly, it was shown in work by Dutkay and Jorgensen that the iterative operator approach works well for generating wavelets on fractals from IFSs without overlap. But so far the more general and more difficult case of essential overlap has resisted previous attempts at a harmonic analysis, and explicit basis constructions in particular.The operators generating the appropriate Cuntz relations are composition operators, e.g., F i : f → f • τ i where (τ i ) is the given IFS. If the particular IFS is essentially non-overlapping, it is relatively easy to compute the adjoint operators S i = F * i , and the S i operators will be isometries in L 2 (µ) with orthogonal ranges. For the case of essential overlap, we can use the extra terms entering in the computation of the operators F * i as a "measure" of the essential overlap for the particular IFS we study. Here the adjoint operators F * i refers to the Hilbert space L 2 (µ) where µ is the equilibrium measure µ for the given IFS (τ i ).

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