04.06.2015 Views

Jordan Lemma Proof - Gauge-institute.org

Jordan Lemma Proof - Gauge-institute.org

Jordan Lemma Proof - Gauge-institute.org

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

<strong>Jordan</strong> <strong>Lemma</strong> <strong>Proof</strong><br />

H. Vic Dannon<br />

In MAPLE, we confirm that<br />

and<br />

θ=<br />

∫<br />

π<br />

2<br />

θ=<br />

0<br />

θ=<br />

∫<br />

π<br />

2<br />

θ=<br />

0<br />

e<br />

e<br />

−2cosθ<br />

−2cosθ<br />

dθ<br />

dθ<br />

=<br />

=<br />

(1/2)*Pi*BesselI(0, 2)-(1/2)*Pi*StruveL(0, 2)<br />

(1/2)*Pi*BesselI(0, 2)-(1/2)*Pi*StruveL(0, 2)<br />

In the notations of Abramowitz, and Stegun<br />

BesselI(0, 2)=Modified Bessel Function I<br />

0(2)<br />

StruveL(0, 2)=Struve Function L (2) .<br />

That is, both integrals equal<br />

π<br />

( 0(2) 0(2)<br />

)<br />

2 I − L .<br />

This confirms Whittaker’s guess of equality.<br />

Nevertheless, it seems easier to complete the <strong>Jordan</strong> <strong>Lemma</strong> <strong>Proof</strong><br />

by bounding<br />

θ=<br />

∫<br />

π<br />

2<br />

θ=<br />

0<br />

e<br />

−mρcosθ<br />

0<br />

d θ, then by trying to prove the equality.<br />

4. Completed <strong>Proof</strong><br />

To complete the <strong>Jordan</strong> <strong>Lemma</strong> <strong>Proof</strong>, we need to bound<br />

ρ<br />

θ=<br />

∫<br />

π<br />

2<br />

θ=<br />

0<br />

e<br />

−ρcos<br />

θ<br />

dθ, similarly to the bounding of<br />

ρ<br />

π<br />

2<br />

θ=<br />

−ρsin<br />

θ<br />

∫ e dθ.<br />

θ=<br />

0<br />

7

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!