Crush1986
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- 10
Homework Statement
Determine the spherical harmonics and the eigenvalues of \vec{\hat{L}}^2 by solving the eigenvalue equation \vec{\hat{L}}^2 |\lambda, m \rangle in position space,
[\frac{1}{sin \theta} \frac{\partial}{\partial \theta} ( sin \theta \frac{\partial}{\partial \theta} ) + \frac{1}{sin^2 \theta} \frac{\partial^2}{\partial \phi^2}] \Theta_{\lambda,m}(\theta) e^{im\phi}
restrict your attention to the m = 0 case. Rewrite the equation in terms of u = cos \theta and show that it becomes
(1-u^2) \frac{d^2 \Theta_{\lambda, 0}}{du^2}-2u \frac{d \Theta_{\lambda,m}}{du} + \lambda \Theta_{\lambda,0} = 0
Homework Equations
distributing the \frac{\partial}{\partial \theta} and recognizing that the double phi derivative turns to zero I am working with the equation -[cot \theta \frac{\partial}{\partial \theta} + \frac{\partial^2}{\partial \theta^2}] \Theta_{\lambda,0} = \lambda \Theta_{\lambda,0}
so, using u = cos \theta I get that du = -sin \theta d \theta, which in turn gives me that \frac{d}{d \theta} = - sin \theta \frac{d}{du}
So I'm pretty sure I'm messing up when I am substituting in for \frac{d^2}{d^2 \theta} = -sin \theta \frac{d}{du} (-sin \theta \frac{d}{du})
I'm then saying -sin \theta = \frac{du}{d \theta} then using the chain rule I get \frac{d^2}{d^2 \theta} = -sin [ \frac {d}{d \theta} \frac{d}{du} + \frac{du}{d \theta} \frac {d^2}{du^2}] = -sin \theta [-sin \theta \frac{d^2}{du^2}-sin \theta \frac{d^2}{du^2}] = 2 sin^2 \theta \frac{d^2}{du^2}<br />
The Attempt at a Solution
I'd appreciate any help. When i put this all together I'm getting
2(1-u^2)\frac{d^2 \Theta_{\lambda,0}}{du^2} - u \frac{d \Theta_{\lambda,0}}{du} + \lambda \Theta_{\lambda,0}=0
I'm pretty sure it's just me doing something stupid while trying to find what the second derivative with respect to theta equals after the change of variable.
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