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<record version="3" id="7941">
 <title>Cameron-Martin space</title>
 <name>CameronMartinSpace</name>
 <created>2006-05-31 02:51:36</created>
 <modified>2006-05-31 03:04:23</modified>
 <type>Definition</type>
 <creator id="4974" name="neldredge"/>
 <author id="4974" name="neldredge"/>
 <classification>
	<category scheme="msc" code="60H99"/>
 </classification>
 <defines>
	<concept>Cameron-Martin space</concept>
 </defines>
 <related>
	<object name="WienerMeasure"/>
 </related>
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 <content>\begin{definition}
Let $W(\mathbb{R}^d)$ be Wiener space.  The \emph{Cameron-Martin space} $H(\mathbb{R}^d)$ is the subspace of $W(\mathbb{R}^d)$ consisting of all paths $\omega$ such that $\omega$ is absolutely continuous and $\int_0^\infty |\omega'(s)|^2\,ds &lt; \infty$.  (Note that if $\omega$ is absolutely continuous, then it is almost everywhere differentiable, so the integral makes sense.)
\end{definition}

This can be thought of as the set of paths with ``finite energy.''

Note that $H(\mathbb{R}^d)$ has Wiener measure $0$, since sample paths of Brownian motion are nowhere differentiable, whereas a path from $H(\mathbb{R}^d)$ is almost everywhere differentiable.
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