Quantum anomalous Hall effect in real materials
Zhang Jiayong1, Zhao Bao1, Zhou Tong1, Yang Zhongqin1, 2, †,
       

(a) The calculated Berry curvature (red) for the whole valence bands. The black curves and green dots denote the band structures obtained from the DFT calculations and the TB model, respectively. (b) The calculated edge density of states for the armchair edge of the semi-infinite system. (c) and (d) The same as panels (a) and (b) except that the distance (vdW gap) between graphene and the Cr2Ge2Te6 sheet is reduced by 0.3 Å (d = 3.26 Å). (e) The induced exchange splitting (M) in the graphene layer as a function of dd0, where d is the vdW distance between graphene and the Cr2Ge2Te6 sheet and d0 is the corresponding optimized vdW distance (d0 = 3.56 Å). (f) The SOC induced band gap Eg as a function of dd0. Reprinted with permission from Ref. [18]. Copyright 2015 by the American Physical Society.