Revista Matemática Iberoamericana

Full-Text PDF (365 KB) | Metadata | Table of Contents | RMI summary
Volume 22, Issue 1, 2006, pp. 131–180
DOI: 10.4171/RMI/452

Published online: 2006-04-30

Wavelets on Fractals

Dorin E. Dutkay[1] and Palle E.T. Jorgensen[2]

(1) Rutgers University, Piscataway, USA
(2) University of Iowa, Iowa City, USA

We show that there are Hilbert spaces constructed from the Hausdorff measures $\mathcal{H}^{s}$ on the real line $\mathbb{R}$ with $0 < s < 1$ which admit multiresolution wavelets. For the case of the middle-third Cantor set $\mathbf{C}\subset \lbrack 0,1]$, the Hilbert space is a separable subspace of $L^{2}(\mathbb{R},(dx)^{s})$ where $s=\log _{3}(2)$. While we develop the general theory of multi-resolutions in fractal Hilbert spaces, the emphasis is on the case of scale $3$ which covers the traditional Cantor set $\mathbf{C}$. Introducing \begin{equation*} \psi_{1}(x)=\sqrt{2}\chi _{\mathbf{C}}(3x-1) \qquad\mbox{and}\qquad \psi _{2}(x)=\chi _{\mathbf{C}}(3x)- \chi_{\mathbf{C}}(3x-2) \end{equation*} we first describe the subspace in $L^{2}(\mathbb{R},(dx)^{s})$ which has the following family as an orthonormal basis (ONB): \begin{equation*} \psi_{i,j,k}(x)=2^{j/2}\psi_{i}(3^{j}x-k)\text{,} \end{equation*} where $i=1,2,j$, $k\in \mathbb{Z}$. Since the affine iteration systems of Cantor type arise from a certain algorithm in $\mathbb{R}^d$ which leaves gaps at each step, our wavelet bases are in a sense gap-filling constructions.

Keywords: Hausdorff measure, Cantor sets, iterated function systems (IFS), fractal, wavelets, Hilbert space, unitary operators, orthonormal basis (ONB), spectrum, transfer operator, cascade approximation, scaling, translation

Dutkay Dorin, Jorgensen Palle: Wavelets on Fractals. Rev. Mat. Iberoamericana 22 (2006), 131-180. doi: 10.4171/RMI/452