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<record version="3" id="5642">
 <title>Stickelberger's theorem</title>
 <name>StickelbergersTheorem</name>
 <created>2004-02-27 12:46:57</created>
 <modified>2004-03-02 17:01:56</modified>
 <type>Theorem</type>
 <creator id="2727" name="mathcam"/>
 <author id="2727" name="mathcam"/>
 <classification>
	<category scheme="msc" code="11R29"/>
 </classification>
 <defines>
	<concept>Stickelberger element</concept>
 </defines>
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 <content>\begin{Theo}[Stickelberger]
Let $L=\mathbb{Q}(\zeta_m)$ be a cyclotomic field extension of $\Q$ with Galois group $G=\{\sigma_a\}_{a\in(\Z/m\Z)^\times}$, and consider the group ring $\Q[G]$.  Define the Stickelberger element $\theta\in\Q[G]$ by
\begin{align*}
\theta=\frac{1}{m}\sum_{1\leq a\leq m, (a,m)=1}a\sigma_a^{-1},
\end{align*}
and take $\beta\in\Z[G]$ such that $\beta\theta\in\Z[G]$ as well.  Then $\beta\theta$ is an annihilator for the ideal class group of $\Q(\zeta_m)$.
\end{Theo}

Note that $\theta$ itself need not be an annihilator, just that any multiple of it in $\Z[G]$ is.

This result allows for the most basic \PMlinkescapetext{connections} between the (otherwise hard to determine) \PMlinkescapetext{structure} of a cyclotomic ideal class group and its \PMlinkescapetext{collection} of annihilators.  For an application of Stickelberger's theorem, see Herbrand's theorem.</content>
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