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I wish to solve an eigenvalue problem:

$$\nabla^{2}f=Ef $$

If I assume spherical symmetry $f(r,\theta,\phi)=f(r)$, I can reduce the problem to 1D:

$$(\frac{2}{r}\frac{d}{dr}+\frac{d^{2}}{dr^{2}})f=Ef$$

My boundary conditions are $f(r=0)=0$ and $f(r=L)=0$, where $L$ is the size of the discrete grid.

I am attempting to solve this problem using a orthogonal basis set expansion, but the issue I am experiencing is the divergence of $r$ at $r=0$. Is there a better method for solving this type of problem? How can I accommodate the singularity?

nicoguaro
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