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<record version="4" id="4132">
 <title>essential singularity</title>
 <name>EssentialSingularity</name>
 <created>2003-03-28 14:57:15</created>
 <modified>2003-04-03 10:59:44</modified>
 <type>Definition</type>
 <creator id="1001" name="pbruin"/>
 <author id="1001" name="pbruin"/>
 <classification>
	<category scheme="msc" code="30D30"/>
 </classification>
 <related>
	<object name="LaurentSeries"/>
	<object name="Pole"/>
	<object name="RemovableSingularity"/>
	<object name="PicardsTheorem"/>
	<object name="RiemannsRemovableSingularityTheorem"/>
 </related>
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 <content>Let $U\subset\mathbb{C}$ be a domain, $a\in U$, and let $f:U \setminus \{a\} \to \mathbb{C}$ be holomorphic.  If the Laurent series expansion of $f(z)$ around $a$ contains infinitely many terms with negative powers of $z-a$, then $a$ is said to be an \emph{essential singularity} of $f$.  Any singularity of $f$ is a removable singularity, a pole or an essential singularity.

If $a$ is an essential singularity of $f$, then the image of any punctured neighborhood of $a$ under $f$ is dense in $\mathbb{C}$ (the Casorati-Weierstrass theorem).  In fact, an even stronger statement is true: according to Picard's theorem, the image of any punctured neighborhood of $a$ is $\mathbb{C}$, with the possible exception of a single point.</content>
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