Figure 6
From: Role of helical edge modes in the chiral quantum anomalous Hall state
Non-local resistances (R NL (↑)) for magnetization direction (↑) and (R NL (↓)) for magnetization direction (↓) in presence of both disorder as well as inelastic scattering. (a) R NL (↑) for chiral(topological) QAH edge mode with quasi-helical QSH edge modes and chiral (trivial) QAH edge mode with quasi-helical QSH edge modes for parameters R4 = 0.5, f = f0 = 0.5, (b) R NL (↑) for chiral(topological) QAH edge mode with quasi-helical QSH edge modes and chiral (trivial) QAH edge mode with quasi-helical QSH edge modes for parameters R2 = 0.5, f = f0 = 0.5. (c) R NL (↓) for chiral(trivial) QAH edge mode with quasi-helical QSH edge modes and chiral(trivial) QAH edge mode with quasi-helical QSH edge modes for parameters R4 = 0.5, f = f0 = 0.5, (d) R NL (↓) for chiral(trivial) QAH edge mode with quasi-helical QSH edge modes and chiral(trivial) QAH edge modes with quasi-helical edge modes for parameters R2 = 0.5, f = f0 = 0.5.
