Figure 1: Quantum anomalous Hall effect in the six QL (Cr0.12Bi0.26Sb0.62)2Te3 film. | Nature Communications

Figure 1: Quantum anomalous Hall effect in the six QL (Cr0.12Bi0.26Sb0.62)2Te3 film.

From: Metal-to-insulator switching in quantum anomalous Hall states

Figure 1

(a) Schematic representation of the mm-sized Hall bar structure and four-point Hall measurements based on the MBE-grown magnetic TI thin film. (b) Quantum anomalous Hall results at T=0.26 K. The Hall resistances are quantized to be±h/e2 where the signs are determined by the chirality of the edge conduction. (c) Temperature-dependent magneto-resistance results (from 0.02 to 13 K). At the coercive field, the peak of Rxx quickly diverges at lower temperatures. (d)Temperature-dependent Rxx_PEAK and Ryx extracted from (b,c). The anomalous Hall resistance Ryx becomes quantized up to 0.3 K, and the giant Rxx_PEAK resolved at 0.02 K is 400 kΩ, the largest value obtained among all reported QAHE systems.

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