Calculating the eigenvalue of orbital angular momentum

TheBlueDot
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Hello,

I'm trying to calculate the measurement of the orbital angular momentum of the state l=1 and m = -1. The operator for the angular momentum squared is
## L^2 = -\hbar (\frac{1}{sin\theta}(\frac{\partial}{\partial \theta}(sin\theta\frac{\partial}{\partial \theta})) +\frac{1}{sin\theta^2}\frac{\partial^2}{\partial\phi^2}) ##,

which expands to
## L^2 = -\hbar (\frac{1}{sin\theta}(\frac{\partial sin\theta}{\partial \theta}\frac{\partial}{\partial \theta}+sin\theta \frac{\partial^2}{\partial \theta^2}) +\frac{1}{sin\theta^2}\frac{\partial^2}{\partial\phi^2}) ##

When operate this on the wave function ##Y_{1,-1} = csin\theta e^{-i\phi}##, I got

##Y_{1,-1}*(\frac{cos^2\theta}{sin\theta} -\frac{sin^2\theta}{sin\theta}-\frac{1}{sin\theta})##,

which is zero. The answer should be ##2\hbar^2##.

If the cosine term is zero, then I'll get the right result.

Please help!

Thanks
 
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TheBlueDot said:
Hello,

I'm trying to calculate the measurement of the orbital angular momentum of the state l=1 and m = -1. The operator for the angular momentum squared is
## L^2 = -\hbar (\frac{1}{sin\theta}(\frac{\partial}{\partial \theta}(sin\theta\frac{\partial}{\partial \theta})) +\frac{1}{sin\theta^2}\frac{\partial^2}{\partial\phi^2}) ##,

which expands to
## L^2 = -\hbar (\frac{1}{sin\theta}(\frac{\partial sin\theta}{\partial \theta}\frac{\partial}{\partial \theta}+sin\theta \frac{\partial^2}{\partial \theta^2}) +\frac{1}{sin\theta^2}\frac{\partial^2}{\partial\phi^2}) ##

When operate this on the wave function ##Y_{1,-1} = csin\theta e^{-i\phi}##, I got

##Y_{1,-1}*(\frac{cos^2\theta}{sin\theta} -\frac{sin^2\theta}{sin\theta}-\frac{1}{sin\theta})##,

which is zero. The answer should be ##2\hbar^2##.

If the cosine term is zero, then I'll get the right result.

Please help!

Thanks

##\frac{cos^2(\theta)}{sin(\theta)} - \frac{sin^2(\theta)}{sin(\theta)} - \frac{1}{sin(\theta)} = \frac{1-sin^2(\theta) - sin^2(\theta) - 1}{sin(\theta)} = \frac{-2 sin^2(\theta)}{sin(\theta)} = -2 sin(\theta)##
 
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stevendaryl said:
##\frac{cos^2(\theta)}{sin(\theta)} - \frac{sin^2(\theta)}{sin(\theta)} - \frac{1}{sin(\theta)} = \frac{1-sin^2(\theta) - sin^2(\theta) - 1}{sin(\theta)} = \frac{-2 sin^2(\theta)}{sin(\theta)} = -2 sin(\theta)##
@stevendaryl,
Thanks for your response. I feel silly now. I looked at the ##sin^2(\theta) -1 ## and thought it was ##cos^2(\theta)##.
 
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It doesn't say ##\ \ \sin^2(\theta) -1\ ##, but ##\ \ - \sin^2(\theta) -1\ \ ## :rolleyes:
 

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