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<record version="2" id="2848">
 <title>construction of Dirac delta function</title>
 <name>ConstructionOfDiracDeltaFunction</name>
 <created>2002-04-19 01:04:11</created>
 <modified>2002-04-21 17:44:42</modified>
 <type>Derivation</type>
<parent id="1491">Dirac delta function</parent>
 <creator id="24" name="djao"/>
 <author id="24" name="djao"/>
 <classification>
	<category scheme="msc" code="34L40"/>
	<category scheme="msc" code="26E35"/>
 </classification>
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 <content>The Dirac delta function is notorious in mathematical circles for having no actual \PMlinkescapetext{realization} as a function. However, a little known secret is that in the domain of nonstandard analysis, the Dirac delta function admits a completely legitimate construction as an actual function. We give this construction here.

Choose any positive infinitesimal $\varepsilon$ and define the hyperreal valued function $\delta:\,^*\R \longrightarrow\,^*\R$ by
$$
\delta(x) :=
\begin{cases}
1/\varepsilon &amp; -\varepsilon/2 &lt; x &lt; \varepsilon/2, \\
0 &amp; \text{otherwise.}
\end{cases}
$$
We verify that the above function satisfies the required properties of the Dirac delta function. By definition, $\delta(x) = 0$ for all nonzero real numbers $x$. Moreover,
$$
\int_{-\infty}^\infty \delta(x)\ dx = \int_{-\varepsilon/2}^{\varepsilon/2} \frac{1}{\varepsilon} \ dx = 1,
$$
so the integral property is satisfied. Finally, for any {\em continuous} real function $f: \R \longrightarrow \R$, choose an infinitesimal $z &gt; 0$ such that $|f(x) - f(0)| &lt; z$ for all $|x| &lt; \varepsilon/2$; then
$$
\varepsilon \cdot \frac{f(0) - z}{\varepsilon} &lt; \int_{-\infty}^\infty \delta(x) f(x)\ dx &lt; \varepsilon \cdot \frac{f(0) + z}{\varepsilon}
$$
which implies that $\int_{-\infty}^\infty \delta(x) f(x)\ dx$ is within an infinitesimal of $f(0)$, and thus has real part equal to $f(0)$.</content>
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