<?xml version="1.0" encoding="UTF-8"?>

<record version="7" id="3997">
 <title>absolutely continuous</title>
 <name>AbsolutelyContinuous</name>
 <created>2003-02-08 14:29:56</created>
 <modified>2008-12-02 23:23:03</modified>
 <type>Definition</type>
 <creator id="127" name="Koro"/>
 <author id="127" name="Koro"/>
 <classification>
	<category scheme="msc" code="28A12"/>
 </classification>
 <defines>
	<concept>absolute continuity</concept>
 </defines>
 <related>
	<object name="RadonNikodymTheorem"/>
	<object name="AbsolutelyContinuousFunction2"/>
 </related>
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%\usepackage{psfrag}
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%\usepackage{graphicx}
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 <content>Let $\mu$ and $\nu$ be signed measures or complex measures on the same measurable space
$(\Omega, \mathscr{S})$. We say that $\nu$ is \emph{absolutely continuous}
with respect to $\mu$ if, for each $A\in \mathscr{S}$ such that $|\mu|(A)=0$,
it holds that $\nu(A)=0$. This is usually denoted by $\nu \ll \mu$.

\textbf{Remarks.}

If $\mu$ and $\nu$ are signed measures and $(\nu^+, \nu^-)$ is the Jordan decomposition of $\nu$, the following \PMlinkescapetext{propositions} are equivalent:
\begin{enumerate}
\item $\nu\ll\mu$;
\item $\nu^+\ll\mu$ and $\nu^-\ll\mu$;
\item $|\nu|\ll|\mu|$.
\end{enumerate}

If $\nu$ is a finite signed or complex measure and $\nu\ll\mu$, the following useful property holds: for each $\varepsilon&gt;0$, there is a $\delta&gt;0$ such that 
$|\nu|(E)&lt;\varepsilon$ whenever $|\mu|(E)&lt;\delta$.</content>
</record>
