Affine fractals as boundaries and their harmonic analysis

preprint2010arXivOpen access

Abstract

We introduce the notion of boundary representation for fractal Fourier expansions, starting with a familiar notion of spectral pairs for affine fractal measures. Specializing to one dimension, we establish boundary representations for these fractals. We prove that as sets these fractals arise as boundaries of functions in closed subspaces of the Hardy space H2H^2. By this we mean that there are lacunary subsets ΓΓ of the non-negative integers, and associated closed ΓΓ-subspace in the Hardy space $H^2(\bd)$, $\bd$ denoting the disk, such that for every function ff in in H2(Γ)H^2(Γ), and for every point zz in $\bd$, f(z)f(z) admits a boundary integral represented by an associated measure μμ, with integration over $\suppμ$ placed as a Cantor subset on the circle $\bt := \{bd}(\bd)$. We study families of pairs: measures μμ and sets ΓΓ of lacunary form, admitting lacunary Fourier series in L2(μ)L^2(μ); i.e., configurations ΓΓ arranged with a geometric progression of empty spacing, or missing parts, gaps. Given ΓΓ, we find corresponding generalized Szeg\" o kernels GΓG_Γ, and we compare them to the classical Szeg\" o kernel for $\bd$. Rather than the more traditional approach of starting with μμ, and then asking for possibilities for sets ΓΓ, such that we get Fourier series representations, we turn the problem upside down; now starting instead with a countably infinite discrete subset ΓΓ, and, within a new duality framework, we study the possibilities for choices of measures μμ.

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