摘要
应用密度矩阵重整化群方法,研究了存在交错离子势△时一维半满扩展Hubbard模型的相图.通过计算关联函数、结构因子、位置算符等方法,描绘了从Mott绝缘体-键有序绝缘体-Band绝缘体的特性并给出了精确的相边界.研究发现:中间的键有序绝缘体相在相图中占据了很小的一部分区域,当存在离子势△的情况下,这个区域将会有所增大;而当相互作用足够强时,这个中间相消失.给出了离子Hubbard模型(最近邻电子-电子相互作用=0)的相图.
We use a density-matrix renormalization group method to study quantitatively the phase diagram of the half-filled one-dimensional (1D) extended Hubbard model in the presence of a staggered ionic potential △. An extensive finite-size scaling analysis is carried out on the relevant structure factors and localization operator to characterize the Mott-insulator (MI)-bond-ordered insulator (BOI)-band-insulator (BI) transitions. The intermediate BOI phase occupies a small region of the phase diagram, and this region is enlarged in the presence of △. In addition, the phase diagram of ionic Hubbard (the nearest-neighbor electron-electron interaction V = 0) is also given.
出处
《物理学报》
SCIE
EI
CAS
CSCD
北大核心
2015年第10期213-218,共6页
Acta Physica Sinica
基金
国家自然科学基金(批准号:11474218)资助的课题~~
关键词
密度矩阵重整化群
HUBBARD模型
量子相变
相图
density-matrix renormalization group, Hubbard model, quantum phase transition, phasediagram