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<record version="5" id="4013">
 <title>signed measure</title>
 <name>SignedMeasure</name>
 <created>2003-02-10 17:03:17</created>
 <modified>2005-02-25 17:55:48</modified>
 <type>Definition</type>
 <creator id="127" name="Koro"/>
 <author id="127" name="Koro"/>
 <classification>
	<category scheme="msc" code="28A12"/>
 </classification>
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 <content>A \emph{signed measure} on a measurable space $(\Omega,\mathscr{S})$ is a function $\mu:\mathscr{S}\rightarrow \mathbb{R}\cup\{+\infty\}$ which is \PMlinkname{$\sigma$-additive}{Additive} and such that $\mu(\emptyset)=0$.

\textbf{Remarks.} 
\begin{enumerate}
\item The usual (positive) measure is a particular case of signed measure, in which $|\mu| = \mu$ (see Jordan decomposition.)

\item Notice that the value $-\infty$ is not allowed. For some authors, a signed measure can only take finite values (so that $+\infty$ is not allowed either). This is sometimes useful because it turns the space of all signed measures into a normed vector space, with the natural operations, and the norm given by $\|\mu\| = |\mu|(\Omega)$.

\item An important example of signed measures arises from the usual measures in the following way: Let $(\Omega,\mathscr{S},\mu)$ be a measure space, and let $f$ be a (real valued) measurable function such that 
\[\int_{\{x\in \Omega:f(x)&lt;0\}} |f| d\mu &lt;\infty.\]
Then a signed measure is defined by
\[A\mapsto \int_A fd\mu.\]
\end{enumerate}</content>
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