论文标题
边界对具有不同Chern数字的双层系统轨道磁化的影响
Effects of Boundary on Orbital Magnetization for a Bilayer System with Different Chern Numbers
论文作者
论文摘要
轨道磁化(OM)的真实空间形式主义是系统的某些适当区域的局部OM的平均值。先前的研究更喜欢散装平均值(即不包括边界)。基于在半填充时具有可调节的Chern号的双层模型,我们数值研究边界对OM真实空间表达式的影响。其三个组成术语的大小收敛过程$ m _ {\ mathrm {lc}} $,$ m _ {\ mathrm {ic}} $,$ m _ {\ mathrm {bc}} $。拓扑术语$ m _ {\ mathrm {bc}} $使边界的不可忽略贡献是边缘状态的表现,尤其是在非零的Chern号码的情况下。但是,我们表明边界对$ m _ {\ mathrm {lc}} $和$ m _ {\ mathrm {ic}} $的影响完全补偿了$ m _ {\ mathrm {bc}} $。这种补偿效应得出的结论是,整个样品平均值也是热力学极限中正确的算法,其值与批量平均值和$ K $空间公式的值相同。这种澄清将有助于进一步研究轨道人,以及较高维度的轨道磁电效应。
The real space formalism of orbital magnetization (OM) is an average of the local OM over some appropriate region of the system. Previous studies prefer a bulk average (i.e., without including boundaries). Based on a bilayer model with an adjustable Chern number at half filling, we numerically investigate the effects from boundaries on the real space expressions of OM. The size convergence processes of its three constituent terms $M_{\mathrm{LC}}$, $M_{\mathrm{IC}}$, $M_{\mathrm{BC}}$ are analysed. The topological term $M_{\mathrm{BC}}$ makes a nonnegligible contribution from boundaries as a manifestation of edge states, especially in the case of nonzero Chern numbers. However, we show that the influence of the boundary on $M_{\mathrm{LC}}$ and $M_{\mathrm{IC}}$ exactly compensates that on $M_{\mathrm{BC}}$. This compensation effect leads to the conclusion that the whole sample average is also a correct algorithm in the thermodynamic limit, which gives the same value as those from the bulk average and the $k$ space formula. This clarification will be beneficial to further studies on orbitronics, as well as the orbital magnetoelectric effects in higher dimensions.