▎ 摘　　要

The interaction between graphene layers is analyzed using a local orbital occupancy approach and second-order perturbation theory. This perturbation theory yields the van der Waals forces which are calculated, within the local orbital approach, using an atom-atom interaction approximation and the local density of states of the graphene layers. Weak chemical interactions (one electron, Hartree, exchange) are calculated using an expansion in the interlayer orbital overlap. We find that the one-electron repulsion due to orthogonalization effects is much larger than the Hartree and exchange contributions. The sum of these contributions yields a net repulsive short-range energy that counteracts the attractive long-range van der Waals interaction. Our analysis of the van der Waals interaction highlights the importance of the 2s -> 3d atomic dipole transitions, which are responsible for more than half of the total van der Waals energy between two graphene layers. We obtain an interlayer equilibrium distance of 3.1-3.2 A, with a binding energy of 60-72 meV, in reasonable agreement with the experimental evidence for graphite.