Why must q be an integer in the azimuthal wavefunction?

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I have a question that I'm struggling with a bit.

The azimuthal part of the wavefunction of a particle is

[tex]\Psi(\phi) = Ae^{-iq\phi}[/tex] where [tex]\phi[/tex] is the azimuthal angle. Show that q must be an integer. By normalising the wavefunction, find the value of A. What is the value of L_z for this particle?

Ok, I know that [tex]\Psi(\phi) = \Psi(\phi + 2\pi)[/tex] because [tex]\phi[/tex] and [tex]\phi + 2\pi[/tex] are the same angle.

So, [tex]Ae^{-iq\phi} = Ae^{-iq(\phi + 2\pi)}[/tex]

and [tex]Ae^{-iq\phi} = Ae^{-iq\phi}e^{-iq2\pi}[/tex]

[tex]\Rightarrow e^{-iq2\pi} = 1[/tex]

How does this imply that q is an integer? This was the way it was done in lectures, but we were just told that this shows q is an integer. I thought it was something to do with [tex]e^{ix} = \cos x + i\sin x[/tex], but I'm not sure.

For the normalising bit, I know I need to use [tex]\int \Psi^* \Psi d\phi = 1[/tex] but I'm not sure about the limits. This is what I've done:

[tex]\int \Psi^* \Psi d\phi = 1[/tex]

[tex]\int_{0}^{2\pi} Ae^{iq\phi}Ae^{-iq\phi} = 1[/tex]

[tex]A^2 \int_{0}^{2\pi} d\phi = 1[/tex]

So [tex]A = \sqrt{ \frac{1}{2\pi} }[/tex]

Is this correct? As for the angular momentum component, I'm working on it.

Thanks.
 
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Sure,that's the Condon-Shortley convention.Actually the wave function is a phase factor;so other one would be superfluous.

[tex]e^{-iq2\pi}=\cos\left(-q2\pi\right)+i\sin\left(-q2\pi\right)=1[/tex]

So when is the cosine =1 ...?(Don't worry,the sine in those points is automatically 0)

Daniel.
 
That's where I was getting confused. How do you know sine is 0 there? I know [tex]\sin n\pi = 0[/tex] where n is an integer, but if you don't know n is an integer in the first place, how can you assume that those sine terms are 0?
 
If the cosine is "+1" (as it should be),then automatically the sine is 0,because we know that

[tex]\sin^2 x+\cos^2 x=1 \, \ x\in\mathbb{R}[/tex]

Daniel.

P.S.As i said,don't worry about the sine.
 
Here's another way to look at it: [itex]q[/itex] must satisfy both of the following conditions:

[tex]\cos (-q2 \pi) = 1[/tex]

[tex]\sin(-q2 \pi) = 0[/tex]

If we start with the first condition, that eliminates all values of [itex]q[/itex] except the + and - integers, and zero. These remaining values of [itex]q[/itex] all satisfy the second condition, so we're done.

Alternatively, we can start with the second condition. In this case, we eliminate all values of [itex]q[/itex] except the + and - integers and half-integers, and zero. Now we apply the first condition to those remaining values, which eliminates the half-integers, and gives us the same final result as before.