<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>The escape trichotomy for singularly perturbed rational maps</dc:title>
<dc:creator>Robert Devaney</dc:creator><dc:creator>Daniel Look</dc:creator><dc:creator>David Uminsky</dc:creator>
<dc:subject>37F10</dc:subject><dc:subject>37F45</dc:subject><dc:subject>Julia set</dc:subject><dc:subject>rational map</dc:subject><dc:subject>escape trichotomy</dc:subject><dc:subject>McMullen Domain</dc:subject><dc:subject>Sierpinski curve</dc:subject>
<dc:description>In this paper we consider the dynamical behavior of the family of complex rational maps given by $F_{\lambda}(z) = z^n + \frac{\lambda}{z^d}$ where $n \geq 2$, $d \geq 1$.  Despite the high degree of these maps, there is only one free critical orbit up to symmetry.  Also, the point at $\infty$ is always a superattracting fixed point.  Our goal is to consider what happens when the free critical orbit tends to $\infty$.  We show that there are three very different types of Julia sets that occur in this case.  Suppose the free critical orbit enters the immediate basin of attraction of $\infty$ at iteration $j$.  Then we show: (1) If $j = 1$, the Julia set is a Cantor set; (2) If $j = 2$, the Julia set is a Cantor set of simple closed curves; (3) If $j &gt; 2$, the Julia set is a Sierpinski curve.</dc:description>
<dc:publisher>Indiana University Mathematics Journal</dc:publisher>
<dc:date>2005</dc:date>
<dc:type>text</dc:type>
<dc:format>pdf</dc:format>
<dc:identifier>10.1512/iumj.2005.54.2615</dc:identifier>
<dc:source>10.1512/iumj.2005.54.2615</dc:source>
<dc:language>en</dc:language>
<dc:relation>Indiana Univ. Math. J. 54 (2005) 1621 - 1634</dc:relation>
<dc:coverage>state-of-the-art mathematics</dc:coverage>
<dc:rights>http://iumj.org/access/</dc:rights>
</oai_dc:dc>