Solving the classical problem of hydrogen hamiltonian eigenvalues one obtain energies (in atomic units) E_n=-0.5, -0.125... etc

These energies depend only on principal quantum number. How one can obtain orbital splitting in the electromegnetic field by means of numerically searching for eigenvalues of the hamiltonian with matrix elements < n L | H | n1 L1 >?

When I use only < n 0 | H | n1 0 > elements of free hamiltonian, I obtain E_n=-0.5, -0.125... etc (as expected).

If I use the whole matrix < n L | H | n1 L1 >, how can I obtain the correct energy levels in the case of atomic hamiltonian and in the case of the atom in the electromagnetic field by means of hamiltonian diagonalization?

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