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    Geometry of canonical self-similar tilings

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    We give several different geometric characterizations of the situation in which the parallel set FϵF_\epsilon of a self-similar set FF can be described by the inner ϵ\epsilon-parallel set T−ϵT_{-\epsilon} of the associated canonical tiling T\mathcal T, in the sense of \cite{SST}. For example, Fϵ=T−ϵ∪CϵF_\epsilon=T_{-\epsilon} \cup C_\epsilon if and only if the boundary of the convex hull CC of FF is a subset of FF, or if the boundary of EE, the unbounded portion of the complement of FF, is the boundary of a convex set. In the characterized situation, the tiling allows one to obtain a tube formula for FF, i.e., an expression for the volume of FϵF_\epsilon as a function of ϵ\epsilon. On the way, we clarify some geometric properties of canonical tilings. Motivated by the search for tube formulas, we give a generalization of the tiling construction which applies to all self-affine sets FF having empty interior and satisfying the open set condition. We also characterize the relation between the parallel sets of FF and these tilings.Comment: 20 pages, 6 figure

    Tube formulas and complex dimensions of self-similar tilings

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    We use the self-similar tilings constructed by the second author in "Canonical self-affine tilings by iterated function systems" to define a generating function for the geometry of a self-similar set in Euclidean space. This tubular zeta function encodes scaling and curvature properties related to the complement of the fractal set, and the associated system of mappings. This allows one to obtain the complex dimensions of the self-similar tiling as the poles of the tubular zeta function and hence develop a tube formula for self-similar tilings in \Rd\mathbb{R}^d. The resulting power series in ϵ\epsilon is a fractal extension of Steiner's classical tube formula for convex bodies K \ci \bRd. Our sum has coefficients related to the curvatures of the tiling, and contains terms for each integer i=0,1,...,d−1i=0,1,...,d-1, just as Steiner's does. However, our formula also contains terms for each complex dimension. This provides further justification for the term "complex dimension". It also extends several aspects of the theory of fractal strings to higher dimensions and sheds new light on the tube formula for fractals strings obtained in "Fractal Geometry and Complex Dimensions" by the first author and Machiel van Frankenhuijsen.Comment: 41 pages, 6 figures, incorporates referee comments and references to new result
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