How can I use Parseval's formula to solve this Fourier transform problem?

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Homework Help Overview

The discussion revolves around the application of Parseval's formula in the context of Fourier transforms, specifically to compute an integral involving a sine function and a complex denominator. Participants are exploring how to manipulate the integral using properties of Fourier transforms and inner products.

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • The original poster attempts to apply Parseval's formula to rewrite the integral and is seeking clarification on the normalization of the inner product as presented in a solution by their teacher. Some participants question the reasoning behind the specific factors introduced in the inner product.

Discussion Status

Participants are actively engaging with the mathematical details, with some providing insights into the normalization process of the inner product. There is a recognition of the correctness of the approach, and further elaboration is being requested to deepen understanding.

Contextual Notes

There is an indication that the original poster is new to the topic, which may influence their grasp of the underlying concepts and terminology related to Fourier transforms and Parseval's theorem.

rayman123
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Homework Statement



Compute the integral
[tex]\int_{-\infty}^{\infty}\frac{\sin(a\xi)}{(1+i\xi)^3\xi}d \xi[/tex]

by using Parseval's formula for Fourier transform
[tex]<\overbrace{f}^{\wedge},\overbrace{g}^{\wedge}>=2 \pi<f,g>[/tex]
where [tex]\wedge[/tex] means the Fourier transform of a function



The Attempt at a Solution





Using Parseval's formula we can rewrite the integral as

[tex]\int_{-\infty}^{\infty}\frac{\sin(a\xi)}{(1+i\xi)^3\xi}d \xi = \Bigl<\overbrace{\frac{\sin(a\xi)}{\xi}}^{\mathcal{F}},\overbrace{\frac{1}{(1+i\xi)^3}}^{\mathcal{F}}\Bigr>[/tex]

with their inversions as follows

[tex]\Bigl(\frac{\sin(a \xi)}{\xi}\Bigr)^{\wedge \wedge }=\frac{1}{2} \chi_{[-a,a]}(x)[/tex] by the table 2 in Folland p.223

and the other one
[tex]\Bigl(\frac{2}{(i \xi+1)^3}\Bigr)^{\wedge \wedge}=\frac{1}{2}x^2e^{-x}[/tex]

which I calculated myslef as follows

we let [tex]g(x)= e^{-x}[/tex] and then the Fourier transform of g(x) is [tex]\mathcal{F}[g(x)]= \frac{1}{1+i \xi}[/tex]

then using formula in Folland again table 2 [tex]\mathcal{F}[xf(x)]=i(\overbrace{f}^{\wedge})^{'})(\xi)[/tex]

and applying it to our function [tex]x^2e^{-x}[/tex]
we get
[tex]\mathcal{F}[x^2e^{-x}]=i(\overbrace{f}^{\wedge})^{''})(\xi)=\frac{2}{(1+i \xi)^3}[/tex]


Homework Statement



going back to the integral and plugging in everything in the Parseval's formula gives me smth like this

[tex]\int_{-\infty}^{\infty}\frac{\sin(a\xi)}{(1+i\xi)^3\xi}d \xi = \Bigl<\overbrace{\frac{\sin(a\xi)}{\xi}}^{\mathcal{F}},\overbrace{\frac{1}{(1+i\xi)^3}}^{\mathcal{F}}\Bigr>=2 \pi \Bigl<\frac{1}{2} \chi_{[-a,a]}, \frac{1}{2}x^2e^{-x}\Bigr>[/tex]


in the solution given by our teacher we find

[tex]\frac{1}{4}<f^{\wedge}, g^{\wedge}>= \frac{\pi}{2}<f,g>[/tex]
how did he get this [tex]\frac{1}{4}[/tex] on the left hand side and then [tex]\frac{\pi}{2}[/tex] on the right hand side??
 
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He is "norming" the inner product so that the inner product of a "basis vector" with itself is 1.
 
HallsofIvy said:
He is "norming" the inner product so that the inner product of a "basis vector" with itself is 1.

Could you elaborate it a little bit more...I am very new to this...
 
Of course it is correct, now I see it. The only thing that is done here is


[tex]\Bigl<\frac{\sin(a\xi}{\xi},\frac{1}{(1+i \xi)^3}\Bigr>=2 \pi \Bigl<\frac{1}{2}\chi_{[-a,a]}, \frac{1}{2}x^2e^{-x}\Bigr>[/tex]
so multiplying everything we simply get
[tex]*2 \pi \cdot \frac{1}{4}\int_{0}^{a}x^2e^{-x}dx[/tex] like in the solution
 

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