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<record version="1" id="5912">
 <title>proof of Poincar\'e lemma</title>
 <name>ProofOfPoincareLemma</name>
 <created>2004-06-12 14:49:14</created>
 <modified>2004-06-12 14:49:14</modified>
 <type>Proof</type>
<parent id="5509">Poincar\'e lemma</parent>
 <selfproof>0</selfproof>
 <creator id="1001" name="pbruin"/>
 <author id="1001" name="pbruin"/>
 <classification>
	<category scheme="msc" code="53-00"/>
	<category scheme="msc" code="55N05"/>
 </classification>
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 <content>Let $X$ be a smooth manifold, and let $\omega$ be a closed differential form of degree $k&gt;0$ on $X$.  For any $x\in X$, there exists a contractible neighbourhood $U\subset X$ of $x$ (i.e. $U$ is homotopy equivalent to a single point), with inclusion map
$$\iota\colon U\hookrightarrow X.$$
To construct such a neighbourhood, take for example an open ball in a coordinate chart around $x$.  Because of the homotopy invariance of de Rham cohomology, the $k$th de Rham cohomology group ${\rm H}^k(U)$ is isomorphic to that of a point; in particular,
$$
{\rm H}^k(U)=0\quad\hbox{for all $k&gt;0$}.
$$
Since $d(\iota^*\omega)=\iota^*(d\omega)=0$, this implies that there exists a $(k-1)$-form $\eta$ on $U$ such that $d\eta=\iota^*\omega$.  In the case where $X$ is a contractible manifold, such an $\eta$ exists globally since we can choose $U=X$ above.</content>
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