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<record version="3" id="6077">
 <title>metric entropy</title>
 <name>MetricEntropy</name>
 <created>2004-08-05 06:47:53</created>
 <modified>2007-07-03 06:40:45</modified>
 <type>Definition</type>
 <creator id="127" name="Koro"/>
 <author id="127" name="Koro"/>
 <classification>
	<category scheme="msc" code="37A35"/>
	<category scheme="msc" code="28D20"/>
 </classification>
 <synonyms>
	<synonym concept="metric entropy" alias="entropy"/>
	<synonym concept="metric entropy" alias="measure theoretic entropy"/>
 </synonyms>
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 <content>Let $(X,\mathscr{B},\mu)$ be a probability space, and $T\colon X\to X$ a measure-preserving transformation.
The entropy of $T$ with respect to a finite measurable partition $\mathcal{P}$ is
\[h_\mu(T,\mathcal{P})=\lim_{n\to\infty}H_\mu\left(\bigvee_{k=0}^{n-1} T^{-k}\mathcal{P}\right),\]
where $H_\mu$ is the entropy of a partition and $\vee$ denotes the join of partitions.
The above limit always exists, although it can be $+\infty$.
The entropy of $T$ is then defined as
\[h_\mu(T) = \sup_{\mathcal{P}} h_\mu(T,\mathcal{P}),\]
with the supremum taken over all finite measurable partitions.
Sometimes $h_\mu(T)$ is called the metric or measure theoretic entropy of $T$, to differentiate it from topological entropy.

\textbf{Remarks.}

\begin{enumerate}
        \item There is a natural correspondence between finite measurable partitions and finite
                sub-$\sigma$-algebras of $\mathscr{B}$. Each finite sub-$\sigma$-algebra is
                generated by a unique partition, and clearly each finite partition generates a finite $\sigma$-algebra.
                Because of this, sometimes $h_\mu(T,\mathcal{P})$ is called the entropy of $T$ with respect to
                the $\sigma$-algebra $\mathscr{P}$ generated by $\mathcal{P}$, and denoted by $h_\mu(T,\mathscr{P})$.
                This simplifies the notation in some instances.
\end{enumerate}</content>
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