How Do You Expand a Hydrogen Atom State in an Orthonormal Basis?

carlosbgois
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Homework Statement


[/B]
Consider a hydrogen atom which, in t = 0, is in the state given by

\psi(\mathbf{r},t>0)=\frac{A}{4\pi}R_{10}(r)+\frac{cos\alpha}{4\pi}\left(\frac{z-\sqrt{2}x}{r}\right)R_{21}(r)

Expand ψ in terms of the nlm} basis of normalized eigenfunctions

\phi_{nlm}(\mathbf{r})=R_{nl}(r)Y_l^m(\theta,\phi)

Homework Equations



The result should be

A\phi_{100}(\mathbf{r})+\frac{cos\alpha}{\sqrt{3}}[\phi_{210}(\mathbf{r})+\phi_{211}(\mathbf{r})-\phi_{21,-1}(\mathbf{r})]

The Attempt at a Solution



Apart from having the supposed solution, I have no idea where to start.
Any help is appreciated.
 
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Do you understand the general principle of writing a state as a linear combination of orthonormal basis states? And how, in general, to determine the coefficients?
 
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