EXTENDED HUBBARD-MODEL AT STRONG-COUPLING

The half-filled extended Hubbard model (containing nearest-neighbor interaction) is considered at strong coupling in fourth-order perturbation theory. The ground-state energies in the spin- and charge-density-wave phases and the resulting phase diagram are calculated in various dimensions: here d = 1, d = infinity, high dimensions (d much greater than 1), and d = 2,3 are discussed separately. In d = 1 it is shown that, for U greater than or similar to 6, fourth-order perturbation theory leads to excellent agreement with existing Monte Carlo data. Second-order perturbation theory alone is valid only at unrealistically large values of U and V. In d = infinity, one needs fourth-order perturbation theory to obtain any nontrivial contribution to the phase diagram at all. As a consequence the fourth-order corrections to the ground-state energy and to the phase diagram are large also in d = 2,3. The formalism used to obtain the perturbative expansion is discussed in an appendix.