Two-dimensional extended Hubbard model at half-filling

We consider the extended Hubbard model on a two-dimensional square lattice at half-filling. The model is investigated using the strong coupling diagram technique. We sum infinite series of ladder diagrams allowing for full-scale charge and spin fluctuations and the actual short-range antiferromagnetic order for nonzero temperatures. In agreement with earlier results, we find the first-order phase transition in the charge subsystem occurring at v = v ( c ) greater than or similar to U/4 with v and U the intersite and on-site Coulomb repulsion constants. The transition reveals itself in an abrupt sign change of a sharp maximum in the zero-frequency charge susceptibility at the corner of the Brillouin. States arising at the transition have alternating deviations of electron occupations from the mean value on neighboring sites. Due to fluctuations, these alternating occupation deviations have short-range order. For the considered parameters, such behavior is found for U less than or similar to 5t with t the hopping constant. For the insulating case U greater than or similar to 6t, in which the transition is not observed, we find a continuous growth of the Mott gap with v. The evolution of the electron density of states with increasing v is also considered.

Automated summary

In this study, the extended Hubbard model on a two-dimensional square lattice at half-filling is investigated using the strong coupling diagram technique. The first-order phase transition in the charge subsystem is found to occur at v = v(c) greater than or similar to U/4. The transition is characterized by an abrupt sign change in the zero-frequency charge susceptibility at the corner of the Brillouin zone. The alternating deviations of electron occupations from the mean value on neighboring sites have short-range order due to fluctuations.