<oai_dc:dc xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/" xmlns:dc="http://purl.org/dc/elements/1.1/" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/ http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:title>Canonical self-affine tilings by iterated function systems</dc:title>
<dc:creator>Erin Pearse</dc:creator>
<dc:subject>28A80</dc:subject><dc:subject>28A75</dc:subject><dc:subject>52A05</dc:subject><dc:subject>52A20</dc:subject><dc:subject>52B99</dc:subject><dc:subject>52C20</dc:subject><dc:subject>52C22</dc:subject><dc:subject>26B25</dc:subject><dc:subject>49Q15</dc:subject><dc:subject>51F99</dc:subject><dc:subject>51M20</dc:subject><dc:subject>51M25</dc:subject><dc:subject>52A22</dc:subject><dc:subject>52A38</dc:subject><dc:subject>52A39</dc:subject><dc:subject>52C45</dc:subject><dc:subject>53C65</dc:subject><dc:subject>54F45</dc:subject><dc:subject>iterated function system</dc:subject><dc:subject>complex dimensions</dc:subject><dc:subject>zeta function</dc:subject><dc:subject>tube formula</dc:subject><dc:subject>fractal Steiner formula</dc:subject><dc:subject>inradius</dc:subject><dc:subject>self-affine</dc:subject><dc:subject>self-similar</dc:subject><dc:subject>tiling</dc:subject><dc:subject>curvature matrix</dc:subject><dc:subject>generating function for the geometry</dc:subject><dc:subject>distributional explicit formula</dc:subject><dc:subject>fractal string</dc:subject>
<dc:description>An iterated function system $\Phi$ consisting of contractive affine mappings has a unique attractor $F \subseteq \mathbb{R}^d$ which  is invariant under the action of the system, as was shown by  Hutchinson [J.E. Hutchinson, \textit{Fractals and self-similarity}, Indiana Univ. Math. J. \textbf{30} (1981), 713--747].  This paper shows how the action of the function system naturally  produces a tiling $\mathcal{T}$ of the convex hull of the attractor.  These tiles form a collection of sets whose geometry is typically  much simpler than that of $F$, yet retains key information about  both $F$ and $\Phi$. In particular, the tiles encode all the  scaling data of $\Phi$. We give the construction, along with some  examples and applications.  The tiling $\mathcal{T}$ is the foundation for the higher-dimensional  extension of the theory of \emph{complex dimensions} which was  developed in Lapidus-van Frankenhuijsen for the case $d=1$ (see M.L. Lapidus and M. van Frankenhuijsen, \textit{Fractal Geometry, Complex Dimensions and Zeta Functions: Geometry and Spectra of Fractal Strings}. New York: Springer-Verlag (Springer Monographs in Mathematics), 2006.)</dc:description>
<dc:publisher>Indiana University Mathematics Journal</dc:publisher>
<dc:date>2007</dc:date>
<dc:type>text</dc:type>
<dc:format>pdf</dc:format>
<dc:identifier>10.1512/iumj.2007.56.3220</dc:identifier>
<dc:source>10.1512/iumj.2007.56.3220</dc:source>
<dc:language>en</dc:language>
<dc:relation>Indiana Univ. Math. J. 56 (2007) 3151 - 3170</dc:relation>
<dc:coverage>state-of-the-art mathematics</dc:coverage>
<dc:rights>http://iumj.org/access/</dc:rights>
</oai_dc:dc>