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<record version="4" id="6552">
 <title>Barb\u{a}lat's lemma</title>
 <name>BarbualatsLemma</name>
 <created>2004-12-10 12:26:52</created>
 <modified>2005-04-09 15:00:55</modified>
 <type>Theorem</type>
 <creator id="4157" name="jirka"/>
 <author id="4157" name="jirka"/>
 <classification>
	<category scheme="msc" code="26A06"/>
 </classification>
 <synonyms>
	<synonym concept="Barb\u{a}lat's lemma" alias="Barbalat's lemma"/>
 </synonyms>
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 <content>\begin{lemma}[Barb\u{a}lat]
Let $f \colon (0,\infty) \to {\mathbb{R}}$ be Riemann integrable and uniformly continuous then
\begin{equation*}
\lim_{t \to \infty} f(t) = 0 .
\end{equation*}
\end{lemma}

Note that if $f$ is non-negative, then Riemann integrability is the same as being $L^1$ in the sense of Lebesgue, but if $f$ oscillates then the Lebesgue integral may not exist.

Further note that the uniform continuity is required to prevent sharp ``spikes'' that might prevent the limit from existing.  For example suppose we add a spike of height 1 and area $2^{-n}$ at every integer.  Then the function is continuous and $L^1$ (and thus Riemann integrable), but
$f(t)$ would not have a limit at infinity.

\begin{thebibliography}{9}
\bibitem{LoRy}
Hartmut Logemann, Eugene P.\@ Ryan.
\PMlinkescapetext{Asymptotic behaviour of nonlinear systems}.
\emph{The American Mathematical Monthly}, 111(10):864--889,
2004.
\end{thebibliography}</content>
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