Normalization of the Fourier transform

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SUMMARY

The forum discussion centers on the normalization of the Fourier transform of a wave function defined as $$\Phi(p) = \frac{N}{(1+\frac{a_0^2p^2}{\hbar^2})^2}$$. Participants clarify the process of calculating the normalization constant \(N\) through the integral $$\int d^3\vec{p}|\Phi(p)|^2=1$$. The discussion emphasizes the use of spherical coordinates for the triple integral, highlighting the correct angular variables, where $$\sin(\theta)$$ is used instead of $$\sin(\phi)$$. The distinction between mathematical and physical conventions for angular variables is also addressed.

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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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