Also, Coulomb assume point charges. This means well localized. But within an atom, that picture fails.
you can just think of the terms of the Hamiltonian in position space as H(x,y,z) such that H(x,y,z)|ψ|^2 d^3x is the average energy in a box of volume d^3x located at (x,y,z)
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Well, in this sense, the Hamiltonian in QM only has a meaning within a distribution.
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that's right, at least in position space
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