Phase diagram of the quarter-filled extended Hubbard model on a two-leg ladder

Phase diagram of the quarter-filled extended Hubbard model on a two-leg ladder
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两腿梯上四分之一填充扩展哈伯德模型的相图

DOI:
10.1103/physrevb.63.045105
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发表时间:
2000
期刊:
影响因子:
--
通讯作者:
R. Noack
R. Noack
中科院分区:
--
文献类型:
--
作者:
M. Vojta;A. Huebsch;R. Noack

文献摘要

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利用密度矩阵重整化群方法研究了具有最近邻库仑排斥V的四分之一填充Hubbard阶梯的基态相图。基态在小V时是均匀的,在大V和不太小的就地库仑排斥U时是"棋盘“电荷有序绝缘体,并且在中等或大V和小U时是相分离的。发现均匀相和电荷有序相之间的零温转变是二级的。在均匀相和电荷有序相中,自旋能隙的存在主要取决于链间和链内跳跃的比例。在论文的第二部分,我们构造了一个有效的哈密顿量的自旋自由度的强耦合电荷有序制度,映射到一个挫折的自旋链的系统。因此,自旋能隙的打开与自发二聚化有关。
We investigate the ground-state phase diagram of the quarter-filled Hubbard ladder with nearest-neighbor Coulomb repulsion V using the Density Matrix Renormalization Group technique. The ground-state is homogeneous at small V, a ``checkerboard'' charge--ordered insulator at large V and not too small on-site Coulomb repulsion U, and is phase-separated for moderate or large V and small U. The zero-temperature transition between the homogeneous and the charge-ordered phase is found to be second order. In both the homogeneous and the charge-ordered phases the existence of a spin gap mainly depends on the ratio of interchain to intrachain hopping. In the second part of the paper, we construct an effective Hamiltonian for the spin degrees of freedom in the strong-coupling charge-ordered regime which maps the system onto a frustrated spin chain. The opening of a spin gap is thus connected with spontaneous dimerization.