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High Chern number quantum anomalous Hall phases in graphene ribbons with Haldane orbital coupling

机译:石墨烯带中的高陈数量子异常霍尔相   Haldane轨道耦合

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摘要

We investigate possible phase transitions among the different quantumanomalous Hall (QAH) phases in a zigzag graphene ribbon under the influence ofthe exchange field. The effective tight-binding Hamiltonian for graphene ismade up of the hopping term, the Kane-Mele and Rashba spin-orbit couplings aswell as the Haldane orbital term. We find that the variation of the exchangefield results in bulk gap-closing phenomena and phase transitions occur in thegraphene system. If the Haldane orbital coupling is absent, the phasetransition between the chiral (anti-chiral) edge state $\nu=+2$ ($\nu=-2$) andthe pseudo-quantum spin Hall state ($\nu=0$) takes place. Surprisingly, whenthe Haldane orbital coupling is taken into account, an intermediate QSH phasewith two additional edge modes appears in between phases $\nu=+2$ and $\nu=-2$.This intermediate phase is therefore either the hyper-chiral edge state of highChern number $\nu=+4$ or anti-hyper-chiral edge state of $\nu=-4$ when thedirection of exchange field is reversed. We present the band structures, edgestate wave functions and current distributions of the different QAH phases inthe system. We also report the critical exchange field values for the QAH phasetransitions.
机译:我们研究了在交换场的影响下,之字形石墨烯碳带中不同量子原子霍尔(QAH)相之间可能发生的相变。石墨烯的有效紧密结合哈密顿量由跳跃项,Kane-Mele和Rashba自旋轨道耦合以及Haldane轨道项组成。我们发现交换场的变化会导致大量的缝隙闭合现象,并且在石墨烯体系中会发生相变。如果不存在Haldane轨道耦合,则手性(反手性)边缘态$ \ nu = + 2 $($ \ nu = -2 $)和伪量子自旋霍尔态($ \ nu = 0 $)之间的相变)发生。出乎意料的是,当考虑到Haldane轨道耦合时,在相位$ \ nu = + 2 $和$ \ nu = -2 $之间出现了具有两个附加边缘模式的中间QSH相,因此该中间相就是超手性边缘当交换场的方向相反时,高切尔数状态$ \ nu = + 4 $或反手征边缘状态$ \ nu = -4 $。我们介绍了系统中不同QAH相的能带结构,边缘态波函数和电流分布。我们还报告了QAH相变的临界交换场值。

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