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<record version="11" id="8928">
 <title>Bargmann-Fock space</title>
 <name>BargmannFockSpace</name>
 <created>2007-02-19 06:02:37</created>
 <modified>2007-02-21 14:45:43</modified>
 <type>Definition</type>
 <creator id="6587" name="ErlendA"/>
 <author id="6587" name="ErlendA"/>
 <classification>
	<category scheme="msc" code="43A15"/>
 </classification>
 <defines>
	<concept>Fock space</concept>
 </defines>
 <synonyms>
	<synonym concept="Bargmann-Fock space" alias="Fock space"/>
 </synonyms>
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 <content>The Bargmann-Fock space (or simply Fock space) is the Hilbert space of entire functions, $\mathcal{F}^2(\mathbb{C})$ s.t. 
$$ \int_\mathbb{C}|F(z)|^2 e^{- \pi |z|^2}dx dy&lt;\infty$$
with associated inner product
$$ \int_\mathbb{C}F(z)\overline{G(z)}e^{- \pi |z|^2}dx dy$$

where $z=x+i y$


\begin{thebibliography}{2}
\bibitem{vb} V. Bargmann, ``Remarks on a Hilbert Space of Analytic Function'' {\it Proceedings of the National Academy of Sciences of the United States of America} {\bf 48} (1962): 199 - 204
\bibitem{vbt} V. Bargmann \&amp; I. T. Todorov, ``Spaces of analytic functions on a complex cone as carriers for the symmetric tensor representations of SO(n)'' {\it Journal of Mathematical Physics} {\bf 18} 6 (1977): 1141 - 1148
\end{thebibliography}</content>
</record>
