 Solution

An effective one-electron Hückel method operator may be writtenThe first term is one-electron kinetic energy. The effective site potentials represent attraction to the nuclei and any averaged screening implicit in the chosen parametrization. They replace the explicit many-electron interaction; they do not contain a coordinate-dependent two-electron operator $r_{12}^{-1}$.

For normalized hydrogen-centred orbitals, symmetry givesThe Hückel Coulomb parameter $\alpha$ is an on-site one-electron energy, not the electron–electron Coulomb repulsion integral. The Hückel resonance integral $\beta$ couples the sites; with the usual same-phase atomic-orbital convention it is negative and stabilizes the bonding combination. For zero overlap, the two energies are $\alpha \pm \beta$.