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	<entry>
		<id>https://en.formulasearchengine.com/index.php?title=Koebe_quarter_theorem&amp;diff=21987</id>
		<title>Koebe quarter theorem</title>
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		<updated>2013-07-14T09:57:29Z</updated>

		<summary type="html">&lt;p&gt;134.130.180.133: &lt;/p&gt;
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{{Portal:Algebra/box-header|Selected Article|Portal:Algebra/Selected article/1}}&amp;lt;/noinclude&amp;gt;&lt;br /&gt;
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| [[Image:Mona Lisa with eigenvector.png|none|175px]]&lt;br /&gt;
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| width=180 style=&amp;quot;font-size: 85%; text-align: center; &amp;quot; |In this [[shear (mathematics)|shear]] transformation of the [[Mona Lisa]], the central vertical axis (red vector) is unchanged, but the diagonal vector (blue) has changed direction. Hence the red vector is said to be an &#039;&#039;&#039;eigenvector&#039;&#039;&#039; of this particular transformation and the blue vector is not. &lt;br /&gt;
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In [[mathematics]], an  &#039;&#039;&#039;eigenvector&#039;&#039;&#039; of a [[linear transformation|transformation]] is a [[vector space|vector]] which that transformation simply multiplies by a constant factor, called the &#039;&#039;&#039;eigenvalue&#039;&#039;&#039; of that vector. Often, a transformation is completely described by its eigenvalues and eigenvectors. The &#039;&#039;&#039;eigenspace&#039;&#039;&#039; for a factor is the [[set (mathematics)|set]] of eigenvectors with that factor as eigenvalue. &lt;br /&gt;
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In the specific case of [[linear algebra]], the &#039;&#039;eigenvalue problem&#039;&#039; is this: given an &#039;&#039;n&#039;&#039; by &#039;&#039;n&#039;&#039; matrix &#039;&#039;A&#039;&#039;,what nonzero vectors &#039;&#039;x&#039;&#039; in &amp;lt;math&amp;gt;R^n&amp;lt;/math&amp;gt; exist, such that &#039;&#039;Ax&#039;&#039; is a scalar multiple of &#039;&#039;x&#039;&#039;? &lt;br /&gt;
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The scalar multiple is denoted by the Greek letter &#039;&#039;&amp;amp;lambda;&#039;&#039; and is called an &#039;&#039;eigenvalue&#039;&#039; of the matrix A, while &#039;&#039;x&#039;&#039; is called the &#039;&#039;eigenvector&#039;&#039; of &#039;&#039;A&#039;&#039; corresponding to &#039;&#039;&amp;amp;lambda;&#039;&#039;. These concepts play a major role in several branches of both [[pure mathematics|pure]] and [[applied mathematics]] &amp;amp;mdash; appearing prominently in [[linear algebra]], [[functional analysis]], and to a lesser extent in [[nonlinear]] situations. &lt;br /&gt;
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It is common to prefix any natural name for the vector with &#039;&#039;eigen&#039;&#039; instead of saying &#039;&#039;eigenvector&#039;&#039;.  For example, &#039;&#039;eigenfunction&#039;&#039; if the eigenvector is a [[function (mathematics)|function]], &#039;&#039;eigenmode&#039;&#039; if the eigenvector is a [[harmonic mode]], &#039;&#039;eigenstate&#039;&#039; if the eigenvector is a [[quantum state]], and so on.  Similarly for the eigenvalue, e.g. &#039;&#039;eigenfrequency&#039;&#039; if the eigenvalue is (or determines) a [[frequency]].&lt;br /&gt;
{| width=&amp;quot;100%&amp;quot; border=&amp;quot;0&amp;quot; style=&amp;quot;padding: 0; margin:0; background:transparent;&amp;quot;&lt;br /&gt;
|align=left|&#039;&#039;&#039;[[Portal:Algebra/Selected article|...Archive]]&#039;&#039;&#039;&lt;br /&gt;
|align=center| &amp;lt;small&amp;gt;Image credit: [[User:Voyajer]]&amp;lt;/small&amp;gt;&lt;br /&gt;
|align=right|&#039;&#039;&#039;[[Eigenvalue, eigenvector and eigenspace|Read more...]]&#039;&#039;&#039;&lt;br /&gt;
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&amp;lt;noinclude&amp;gt;{{Portal:Algebra/box-footer-empty}}&amp;lt;/div&amp;gt;&amp;lt;/noinclude&amp;gt;&lt;/div&gt;</summary>
		<author><name>134.130.180.133</name></author>
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