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	<title>Peano-Russell notation - Revision history</title>
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	<updated>2026-07-10T17:39:44Z</updated>
	<subtitle>Revision history for this page on the wiki</subtitle>
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		<title>en&gt;Jan Schreiber: /* External links */ Link to SEP</title>
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		<updated>2014-11-23T11:50:43Z</updated>

		<summary type="html">&lt;p&gt;&lt;span class=&quot;autocomment&quot;&gt;External links: &lt;/span&gt; Link to SEP&lt;/p&gt;
&lt;a href=&quot;https://en.formulasearchengine.com/w/index.php?title=Peano-Russell_notation&amp;amp;diff=255064&amp;amp;oldid=17551&quot;&gt;Show changes&lt;/a&gt;</summary>
		<author><name>en&gt;Jan Schreiber</name></author>
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	<entry>
		<id>https://en.formulasearchengine.com/w/index.php?title=Peano-Russell_notation&amp;diff=17551&amp;oldid=prev</id>
		<title>24.44.161.44: Changed the dots so that they are different, per Russel&#039;s original notation</title>
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		<updated>2011-06-09T00:06:10Z</updated>

		<summary type="html">&lt;p&gt;Changed the dots so that they are different, per Russel&amp;#039;s original notation&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;&lt;br /&gt;
Siegel disc is a connected [[Classification of Fatou components|component in the Fatou set]] where the dynamics is analytically [[Topological_conjugation|conjugated]] to an [[irrational rotation]].&lt;br /&gt;
&lt;br /&gt;
==Description==&lt;br /&gt;
Given a [[holomorphic]] [[endomorphism]] &amp;lt;math&amp;gt;f:S\to S&amp;lt;/math&amp;gt; on a [[Riemann surface]] &amp;lt;math&amp;gt;S&amp;lt;/math&amp;gt; we consider the [[dynamical system]] generated by the [[Iterated function|iterates]] of &amp;lt;math&amp;gt;f&amp;lt;/math&amp;gt; denoted by &amp;lt;math&amp;gt;f^n=f\circ\stackrel{\left(n\right)}{\cdots}\circ f&amp;lt;/math&amp;gt;. We then call the [[Orbit_(dynamics)|orbit]] &amp;lt;math&amp;gt;\mathcal{O}^+(z_0)&amp;lt;/math&amp;gt; of &amp;lt;math&amp;gt;z_0&amp;lt;/math&amp;gt; as the set of forward iterates of &amp;lt;math&amp;gt;z_0&amp;lt;/math&amp;gt;. We are interested in the asymptotic behavior of the orbits in &amp;lt;math&amp;gt;S&amp;lt;/math&amp;gt; (which will usually be &amp;lt;math&amp;gt;\mathbb{C}&amp;lt;/math&amp;gt;, the [[complex plane]] or &amp;lt;math&amp;gt;\mathbb{\hat C}=\mathbb{C}\cup\{\infty\}&amp;lt;/math&amp;gt;, the [[Riemann sphere]]), and we call &amp;lt;math&amp;gt;S&amp;lt;/math&amp;gt; the [[phase plane]] or &amp;#039;&amp;#039;dynamical plane&amp;#039;&amp;#039;. &lt;br /&gt;
&lt;br /&gt;
One possible asymptotic behavior for a point &amp;lt;math&amp;gt;z_0&amp;lt;/math&amp;gt; is to be a [[fixed point (mathematics)|fixed point]], or in general a &amp;#039;&amp;#039;periodic point&amp;#039;&amp;#039;. In this last case &amp;lt;math&amp;gt;f^p(z_0)=z_0&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt;p&amp;lt;/math&amp;gt; is the [[Orbit_(dynamics)|period]] and &amp;lt;math&amp;gt;p=1&amp;lt;/math&amp;gt; means &amp;lt;math&amp;gt;z_0&amp;lt;/math&amp;gt; is a fixed point. We can then define the &amp;#039;&amp;#039;multiplier&amp;#039;&amp;#039; of the orbit as &amp;lt;math&amp;gt;\rho=(f^p)&amp;#039;(z_0)&amp;lt;/math&amp;gt; and this enables us to classify periodic orbits as &amp;#039;&amp;#039;attracting&amp;#039;&amp;#039; if &amp;lt;math&amp;gt;|\rho|&amp;lt;1&amp;lt;/math&amp;gt; &amp;#039;&amp;#039;superattracting&amp;#039;&amp;#039; if &amp;lt;math&amp;gt;|\rho|=0&amp;lt;/math&amp;gt;), &amp;#039;&amp;#039;repelling&amp;#039;&amp;#039; if &amp;lt;math&amp;gt;|\rho|&amp;gt;1&amp;lt;/math&amp;gt; and indifferent if &amp;lt;math&amp;gt;\rho=1&amp;lt;/math&amp;gt;. Indifferent periodic orbits split in &amp;#039;&amp;#039;rationally indifferent&amp;#039;&amp;#039; and &amp;#039;&amp;#039;irrationally indifferent&amp;#039;&amp;#039;, depending on whether &amp;lt;math&amp;gt;\rho^n=1&amp;lt;/math&amp;gt; for some &amp;lt;math&amp;gt;n\in\mathbb{Z}&amp;lt;/math&amp;gt; or &amp;lt;math&amp;gt;\rho^n\neq1&amp;lt;/math&amp;gt; for all &amp;lt;math&amp;gt;n\in\mathbb{Z}&amp;lt;/math&amp;gt;, respectively.&lt;br /&gt;
&lt;br /&gt;
&amp;#039;&amp;#039;&amp;#039;Siegel discs&amp;#039;&amp;#039;&amp;#039; are one of the possible cases of connected components in the Fatou set (the complementary set of the [[Julia set]]), according to [[Classification of Fatou components]], and can occur around irrationally indifferent periodic points. The Fatou set is, roughly, the set of points where the iterates behave similarly to their neighbours (they form a [[normal family]]). &amp;#039;&amp;#039;&amp;#039;Siegel discs&amp;#039;&amp;#039;&amp;#039; correspond to points where the dynamics of &amp;lt;math&amp;gt;f&amp;lt;/math&amp;gt; is analytically &lt;br /&gt;
[[Topological_conjugation|conjugated]] to an irrational rotation of the complex disc.&lt;br /&gt;
&lt;br /&gt;
==Name==&lt;br /&gt;
The disk is named in honor of [[Carl Ludwig Siegel]].&lt;br /&gt;
==Gallery==&lt;br /&gt;
&amp;lt;gallery widths=&amp;quot;300px&amp;quot; heights=&amp;quot;300px&amp;quot; perrow=3&amp;gt;&lt;br /&gt;
Image:SiegelDisk.jpg |Siegel disc for a polynomial-like mapping&lt;br /&gt;
Image:FigureJuliaSetForPolynomialLike.jpg|Julia set for &amp;lt;math&amp;gt;B(z)=\lambda a(e^{z/a}(z+1-a)+a-1)&amp;lt;/math&amp;gt;, where &amp;lt;math&amp;gt;a=15-15i&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;\lambda&amp;lt;/math&amp;gt; is the [[golden ratio]]. Orbits of some points inside the &amp;#039;&amp;#039;&amp;#039;Siegel disc&amp;#039;&amp;#039;&amp;#039; emphasized&lt;br /&gt;
Image:UnboundedSiegeldisk.jpg|Julia set for &amp;lt;math&amp;gt;B(z)=\lambda a(e^{z/a}(z+1-a)+a-1)&amp;lt;/math&amp;gt;, where &amp;lt;math&amp;gt;a=-0.33258+0.10324i&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;\lambda&amp;lt;/math&amp;gt; is the [[golden ratio]]. Orbits of some points inside the &amp;#039;&amp;#039;&amp;#039;Siegel disc&amp;#039;&amp;#039;&amp;#039; emphasized. The Siegel disc is either unbounded or its boundary is an indecomposable continuum.&amp;lt;ref&amp;gt;Rubén Berenguel and Núria Fagella &amp;#039;&amp;#039;An entire transcendental family with a persistent Siegel disc, 2009 preprint: [http://arxiv.org/abs/0907.0116 arXiV:0907.0116]&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
File:Golden Mean Quadratic Siegel Disc Speed.png | Filled Julia set for &amp;lt;math&amp;gt;f_c(z) = z*z + c&amp;lt;/math&amp;gt; for [[Golden ratio|Golden Mean]] rotation number with interior colored propotional to the average discrete velocity on the orbit = abs( z_(n+1) - z_n ). Note that there is only one Siegel disc and many preimages of the orbits within the Siegel disk&lt;br /&gt;
File:Golden Mean Quadratic Siegel Disc.png|Filled Julia set for &amp;lt;math&amp;gt;f_c(z) = z*z + c&amp;lt;/math&amp;gt; for [[Golden ratio|Golden Mean]] rotation number with Siegel disc and some orbits inside&lt;br /&gt;
File:Siegel quadratic 3,2,1000,1... ,.png|Julia set of quadratic polynomial with Siegel disk for rotation number [3,2,1000,1...]&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Formal definition==&lt;br /&gt;
Let &amp;lt;math&amp;gt;f:S\to S&amp;lt;/math&amp;gt; be a [[holomorphic]] [[endomorphism]] where &amp;lt;math&amp;gt;S&amp;lt;/math&amp;gt; is a [[Riemann surface]], and let U be a [[connected component (analysis)| connected component]] of the Fatou set &amp;lt;math&amp;gt;\mathcal{F}(f)&amp;lt;/math&amp;gt;. We say U is a Siegel disc of f around the point z_0 if there exists an analytic homeomorphism &amp;lt;math&amp;gt;\phi:U\to\mathbb{D}&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt;\mathbb{D}&amp;lt;/math&amp;gt; is the unit disc and such that &amp;lt;math&amp;gt;\phi(f^n(\phi^{-1}(z)))=e^{2\pi i\alpha}z&amp;lt;/math&amp;gt; for some &amp;lt;math&amp;gt;\alpha\in\mathbb{R}\backslash\mathbb{Q}&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;\phi(z_0)=0&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[[Carl Ludwig Siegel|Siegel&amp;#039;s]] theorem proves the existence of &amp;#039;&amp;#039;&amp;#039;Siegel discs&amp;#039;&amp;#039;&amp;#039; for [[Irrational Number|irrational numbers]] satisfying a &amp;#039;&amp;#039;strong irrationality condition&amp;#039;&amp;#039; (a [[Diophantine condition]]), thus solving an open problem since Fatou conjectured his theorem on the [[Classification of Fatou components]].&amp;lt;ref&amp;gt;[[Lennart Carleson]] and Theodore W. Gamelin, &amp;#039;&amp;#039;Complex Dynamics&amp;#039;&amp;#039;, Springer 1993&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Later [[A. D. Brjuno]] improved this condition on the irrationality, enlarging it to the [[Brjuno number]]s.&amp;lt;ref name=&amp;quot;MilnorComplexDynamics&amp;quot;&amp;gt;[[John W. Milnor]], &amp;#039;&amp;#039;Dynamics in One Complex Variable&amp;#039;&amp;#039; (Third Edition), Annals of Mathematics Studies 160, Princeton University Press 2006 (First appeared in 1990 as a [http://www.math.sunysb.edu/preprints.html Stony Brook IMS Preprint], available as [http://www.arxiv.org/abs/math.DS/9201272 arXiV:math.DS/9201272].)&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
This is part of the result from the [[Classification of Fatou components]].&lt;br /&gt;
&lt;br /&gt;
==See also==&lt;br /&gt;
* [[Herman ring]]&lt;br /&gt;
{{wikibooks|Fractals/Iterations in the complex plane/siegel}}&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
{{reflist}}&lt;br /&gt;
* [http://www.scholarpedia.org/article/Siegel_disks Siegel disks ar Scholarpedia]&lt;br /&gt;
&lt;br /&gt;
[[Category:Fractals]]&lt;br /&gt;
[[Category:Limit sets]]&lt;br /&gt;
[[Category:Complex dynamics]]&lt;/div&gt;</summary>
		<author><name>24.44.161.44</name></author>
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