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<record version="1" id="10242">
 <title>failure of Hartogs' theorem in one dimension</title>
 <name>FailureOfHartogsTheoremInOneDimension</name>
 <created>2008-02-06 12:48:59</created>
 <modified>2008-02-06 12:48:59</modified>
 <type>Example</type>
<parent id="3892">Hartogs' theorem</parent>
 <creator id="4157" name="jirka"/>
 <author id="4157" name="jirka"/>
 <classification>
	<category scheme="msc" code="32H02"/>
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 <content>It is instructive to see an example where Hartogs' theorem fails in one dimension.
Take $U = {\mathbb C}$ and let $K = \{0\}.$
The function $\frac{1}{z}$ is holomorphic in $U \setminus K,$ but cannot be extended to $U.$

To understand the example and failure of the theorem it is important to understand \PMlinkname{the proof}{ProofOfHartogsTheorem}.  In the proof, the way we construct an extension is that we start with a function holomorphic in $U \setminus K,$
modify it in a neighbourhood of $K$ to be zero, hence extending as a smooth function through $K.$  Then we solve the
\PMlinkname{$\bar{\partial}$ operator}{BarPartialOperator} inhomogeneous equation $\bar{\partial}\psi = g$ to ``correct'' our extension to be holomorphic.
The key point is that $g$ has compact support allowing us to solve the equation and find a $\psi$
with compact support.  This fails in dimension 1.  While we always get a solution $\psi,$ the solution can never have compact support.  Hence, if we tried the proof with $\frac{1}{z},$ the new function we obtain in the proof does not agree with $\frac{1}{z}$ on any open set and hence is not an extension.</content>
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