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Solid State Communications

Incommensurate domain walls in the two-dimensional Hubbard model with next-nearest-neighbor hopping

Jun Li, H. Q. Lin, Chang-De Gong

Published Jul 1, 2000• 3 citations
Publisher
DOI
10.1016/s0038-1098(00)00178-2

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The extended Bose-Hubbard model with nearest-neighbor and next-nearest-neighbor repulsive interactions on a square lattice is investigated by using the quantum Monte Carlo method. We find that for the cases of weak next-nearest-neighbor interactions and small hoppings, incommensurate solids of fractional densities varying from 1/4 to 1/2 can be stabilized in the thermodynamic limit. We further show that the continuous changes of ordering wave vectors from $(\ensuremath{\pi},\ensuremath{\pi}/2)$ $[\mathrm{or} (\ensuremath{\pi}/2,\ensuremath{\pi})]$ to $(\ensuremath{\pi},\ensuremath{\pi})$ within the incommensurate solid phase can be understood by the mechanism of domain wall formation. The related ground-state phase diagram and thermal phase transitions are also discussed.

arXiv:2012.10121•Physical review. B./Physical review. B•Mar 25, 2021•1 citation
The extended Bose-Hubbard model with nearest-neighbor and next-nearest-neighbor repulsive interactions on a square lattice is investigated by using the quantum Monte Carlo method. We find that for the cases of weak next-nearest-neighbor interactions and small hoppings, incommensurate solids of fractional densities varying from 1/4 to 1/2 can be stabilized in the thermodynamic limit. We further show that the continuous changes of ordering wave vectors from $(\ensuremath{\pi},\ensuremath{\pi}/2)$ $[\mathrm{or} (\ensuremath{\pi}/2,\ensuremath{\pi})]$ to $(\ensuremath{\pi},\ensuremath{\pi})$ within the incommensurate solid phase can be understood by the mechanism of domain wall formation. The related ground-state phase diagram and thermal phase transitions are also discussed.