Extended Bose-Hubbard model on a honeycomb lattice

被引:34
|
作者
Gan, Jing Yu [1 ]
Wen, Yu Chuan
Ye, Jinwu
Li, Tao
Yang, Shi-Jie
Yu, Yue
机构
[1] Tsing Hua Univ, Ctr Adv Study, Beijing 100084, Peoples R China
[2] Chinese Acad Sci, Inst Theoret Phys, Beijing 100080, Peoples R China
[3] Chinese Acad Sci, Interdisciplinary Ctr Theoret Studies, Beijing 100080, Peoples R China
[4] Penn State Univ, Dept Phys, University Pk, PA 16802 USA
[5] Renmin Univ China, Dept Phys, Beijing 100872, Peoples R China
[6] Beijing Normal Univ, Dept Phys, Beijing 100875, Peoples R China
来源
PHYSICAL REVIEW B | 2007年 / 75卷 / 21期
关键词
D O I
10.1103/PhysRevB.75.214509
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
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 and the soft-core bosons. For the hard-core case, the transition between the rho=1/2 solid and the superfluid is first order, and the supersolid state is unstable toward phase separation. For the soft-core case, due to the presence of multiple occupation, a stable particle-induced supersolid (SS-p) phase emerges when 1/2 <rho < 1. The transition from the solid at rho=1/2 to the SS-p phase is second order with the superfluid density scaling as rho(s)similar to rho-1/2. The SS-p phase has the same diagonal order as the solid at rho=1/2. As the chemical potential increases further, the SS-p phase turns into a solid where two bosons occupy each site of one sublattice through a first-order transition. We also calculate the critical exponents of the transition between the rho=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, and thus the transition is also first order even at the Heisenberg point.
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页数:5
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