The Extended Bose Hubbard Model on the Two Dimensional Honeycomb Lattice
arXiv:cond-mat/0701120 · doi:10.1103/PhysRevB.75.214509
Abstract
We study the extended Bose-Hubbard model on a two-dimensional honeycomb lattice by using large scale quantum Monte Carlo simulations. We present the ground state phase diagrams for both the hard-core case and the soft-core case. For the hard-core case, the transition between $Ï=1/2$ solid and the superfluid is first order and the supersolid state is unstable towards phase separation. For the soft-core case, due to the presence of the multiple occupation, a stable particle induced supersolid (SS-p) phase emerges when $1/2<Ï<1$. The transition from the solid at $Ï=1/2$ to the SS-p is second order with the superfluid density scaling as $ Ï_{s} \sim Ï-1/2 $. The SS-p has the same diagonal order as the solid at $ Ï=1/2 $. As the chemical potential increasing further, the SS-p will turn into a solid where two bosons occupying each site of a sublattice through a first order transition. We also calculate the critical exponents of the transition between $Ï=1/2$ solid and superfluid at the Heisenberg point for the hard core case. We find the dynamical critical exponent $z=0.15$, which is smaller than results obtained on smaller lattices. This indicates that $ z $ approaches zero in the thermodynamic limit, so the transition is also first order even at the Heisenberg point.
6pages, 6figures