Normalization of the Fourier transform

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Homework Help Overview

The problem involves the normalization of the Fourier transform of a wave function in three dimensions, specifically focusing on determining the normalization constant \( N \) given the expression for the Fourier transform and the requirement that the integral of its squared magnitude equals one.

Discussion Character

  • Exploratory, Assumption checking, Conceptual clarification

Approaches and Questions Raised

  • Participants discuss converting the three-dimensional integral into spherical coordinates, questioning the validity of the coordinate transformation and the corresponding limits of integration.

Discussion Status

The discussion is ongoing with participants exploring the use of spherical coordinates for the momentum vector \( \vec{p} \). There is some clarification regarding the notation for angles and the correct limits of integration, with participants acknowledging differing conventions between mathematics and physics.

Contextual Notes

There is a noted confusion regarding the angular variables used in spherical coordinates, particularly the roles of \( \theta \) and \( \phi \), and their respective ranges in the context of the integral.

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Homework Statement


The Fourier transfrom of the wave function is given by
$$\Phi(p) = \frac{N}{(1+\frac{a_0^2p^2}{\hbar^2})^2}$$
where ##p:=|\vec{p}|## in 3 dimensions.
Find N, choosing N to be a positive real number.

Homework Equations


$$\int d^3\vec{p}|\Phi(p)|^2=1$$
, over all p in the 3 dimensions.

The Attempt at a Solution


First finding the complex conjugate,
$$\Phi^*(p) = \frac{N}{(1+\frac{a_0^2 p^2}{\hbar^2})^2}$$
So,
$$|\Phi(p)|^2 = \frac{N^2}{(1+\frac{a_0^2 p^2}{\hbar^2})^4}$$
So,
$$\frac{1}{N^2} = \int d^3 \vec{p}\frac{1}{(1+\frac{a_0^2 p^2}{\hbar^2})^4}$$

How would I change ##d^3\vec{p}## to be a triple integral, one of which is over dp?
 
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By using spherical coordinates for ##\vec{p}## ...
 
eys_physics said:
By using spherical coordinates for ##\vec{p}## ...
I thought of using spherical coordinates for p, but would they be the same as for x.
So would it be that the integral, ignoring the function of integration, becomes?
$$\int d^3\vec{p}= \int_{0}^{\pi}\int_{0}^{2\pi}\int_{0}^{\infty}p^2sin(\phi)dpd\theta d\phi$$?

If the above is true, why can the same be written for p as was for x.
 
It doesn't matter if you have ##p## or ##x##. You can write write any three-dimensional vector ##\vec{a}## as
$$\vec{a}=a_x e_x + a_y e_y + a_z e_z$$,
where ##e_x##, ##e_y## and ##e_z## are the cartesian basis vectors.
You can then transform to spherical coordinates, i.e. instead writing ##\vec{a}## in terms of ##e_r##, ##e_\theta## and ##e_\phi## . It is not important what ##\vec{a}## represent.

In your formula it should be ##\sin\theta## instead of ##\sin\phi##.
 
eys_physics said:
It doesn't matter if you have ##p## or ##x##. You can write write any three-dimensional vector ##\vec{a}## as
$$\vec{a}=a_x e_x + a_y e_y + a_z e_z$$,
where ##e_x##, ##e_y## and ##e_z## are the cartesian basis vectors.
You can then transform to spherical coordinates, i.e. instead writing ##\vec{a}## in terms of ##e_r##, ##e_\theta## and ##e_\phi## . It is not important what ##\vec{a}## represent.

In your formula it should be ##\sin\theta## instead of ##\sin\phi##.
Why would you use ##sin(\theta)##?
Using ##sin(\theta)##,
$$\int_{0}^{2\pi}sin(\theta)d\theta = [-cos(\theta)]_0^{2\pi} = -1-(-1) = 0$$
Also, http://mathworld.wolfram.com/SphericalCoordinates.html. ##sin(\phi)## is used where ##\phi## ranges from 0 to ##\pi##, which is what I have in my integral.
 
Yes, you are correct. I thought the range for ##\phi## was ##[0,2\pi]## and ##[0,\pi]## for ##\theta##.
 
eys_physics said:
Yes, you are correct. I thought the range for ##\phi## was ##[0,2\pi]## and ##[0,\pi]## for ##\theta##.
The OP is using the mathematics convention. Physicists typically use ##\theta## to be the polar angle and ##\phi## for the azimuthal angle.
 

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