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Philosophical Magazine B

Hubbard model with next-nearest-neighbour interaction terms in higher dimensions: New, exactly solvable cases

Péter Gurin, Zsolt Gulácsi

Published Nov 1, 1997• 2 citations
Publisher

Abstract

The exact ground-state wavefunction and energy of an extended Hubbard model are presented containing also next-nearest-neighbour hopping, bond-charge and density interaction terms besides the nearest-neighbour and on-site contributions. Our results are valid at half-filling for a wide range of parameters, on simple hypercubic lattices in arbitrary D > I dimensions.

DOI
10.1080/01418639708241146

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arXiv:cond-mat/0003419•Journal of the Physical Society of Japan•Dec 15, 2001•10 citations
The exact ground-state wavefunction and energy of an extended Hubbard model are presented containing also next-nearest-neighbour hopping, bond-charge and density interaction terms besides the nearest-neighbour and on-site contributions. Our results are valid at half-filling for a wide range of parameters, on simple hypercubic lattices in arbitrary D > I dimensions.
Exact results related to extended Hubbard model containing couplings up to next-nearest-neighbour terms were deduced for restricted regions of parameter space in arbitrary D > 1 dimensions at half-filling and T = 0 temperature. Different types of commensurate charge-density waves and spin-density waves, a ferromagnetic domain and a phase separation region were found, the last being for the first time signalled at the level of approximation-free results in dimensions higher than one. In connection with other presented phases we extended their stability domains in comparison with previously published data. The deduced phase diagram is complete in the localized limit. The dependences on the interaction range and dimension were studied. The obtained results emphasize the importance of next-nearest neighbour terms in the development of ordered phases within the studied system.
Exact results related to extended Hubbard model containing couplings up to next-nearest-neighbour terms were deduced for restricted regions of parameter space in arbitrary D > 1 dimensions at half-filling and T = 0 temperature. Different types of commensurate charge-density waves and spin-density waves, a ferromagnetic domain and a phase separation region were found, the last being for the first time signalled at the level of approximation-free results in dimensions higher than one. In connection with other presented phases we extended their stability domains in comparison with previously published data. The deduced phase diagram is complete in the localized limit. The dependences on the interaction range and dimension were studied. The obtained results emphasize the importance of next-nearest neighbour terms in the development of ordered phases within the studied system.
We have modified an existing real space renormalization group scheme to remove some physically inconsistent features and used the rectified method to study the ground state of the one-dimensional Hubbard model with nearest-neighbour repulsion and the bond-charge interaction for half filling. For the nearest-neighbour interaction we find a phase diagram which agrees nicely with the Monte Carlo results. For the case of bond-charge interaction we have reproduced some available exact results and found some interesting information in the parameter regime where no exact solution is available.
Phase diagrams of the one-dimensional extended Hubbard model with a nearest neighbor interaction VVV and site-off-diagonal (bond-charge XXX and bond-bond WWW) interactions at half-filling are obtained numerically, using the level-crossing approach for finite-size clusters. This analysis is straightforward extension of the preceding work [cond-mat/9909277], where only the XXX term is considered as a site-off-diagonal term. Similarly to the XXX term, the WWW term enlarges bond-charge-density-wave (BCDW) and bond-spin-density-wave (BSDW) phases for W<0W<0W<0 and W>0W>0W>0 cases, respectively. In the strong-coupling region, however, the WWW term causes ferromagnetism for W>0W>0W>0, and shifts the boundary of the phase separation in the U/t≪−1U/t\ll-1U/t≪−1 region, which are different from the roles of the XXX term. In addition, we discuss a parameter region where the BSDW state is the exact ground state, and show that the exactly solvable point appears just on the phase boundary between the BSDW and the ferromagnetic phases.