Proving the Integral of a Limit of a Function

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psid
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Homework Statement



How does one prove that [tex]\int^\infty_{-\infty}\lim_{\epsilon \rightarrow 0}(1/\pi)\frac{\epsilon g(x)}{(x-a)^{2}+\epsilon^{2}}dx=g(a)[/tex]?
 
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psid said:

Homework Statement



How does one prove that [tex]\int^\infty_{-\infty}\lim_{\epsilon \rightarrow 0}(1/\pi)\frac{\epsilon g(x)}{(x-a)^{2}+\epsilon^{2}}dx=g(a)[/tex]?

One doesn't, since the result isn't true. The limit has to be outside the integral sign.

Mathematical Physics by Butkov has a nice proof on pages 238-239. The idea is, for positive [itex]\epsilon[/itex] to write

[tex]\lim_{\epsilon \rightarrow 0} \int_{-\infty}^\infty = \lim_{\epsilon \rightarrow 0} \int_{-\infty}^{a-\epsilon} + lim_{\epsilon \rightarrow 0} \int_{a-\epsilon}^{a+\epsilon} + lim_{\epsilon \rightarrow 0} \int_{a+\epsilon}^{\infty},[/tex]

and then to assume [itex]g[/itex] is bounded to show that the first and last terms go to zero.

For [itex]\epsilon[/itex] small and [itex]g[/itex] continuous, [itex]g(x)[/itex] is approximately equal to the constant value [itex]g(a)[/itex] over the middle interval, so pull this outside of the middle integral, or, more rigorously, use the mean value theorem for integrals.
 
Thanks, got it right now. The limit was indeed before the integral sign.