Fig. 2 Longitudinal (local) resistance Rxx and nonlocal resistance Rnl with different terminal configurations on the six-terminal device measured without.

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Fig. 2 Longitudinal (local) resistance Rxx and nonlocal resistance Rnl with different terminal configurations on the six-terminal device measured without magnetic fields at 1.5 K. Longitudinal (local) resistance Rxx and nonlocal resistance Rnl with different terminal configurations on the six-terminal device measured without magnetic fields at 1.5 K. (A) Schematic showing the terminal number. (B) Rxx for (I: 14, V: 65); (C) Rnl for (I: 61, V: 53), (I: 61, V: 54), and (I: 61, V: 43); and (D) Rnl for (I: 62, V: 43), (I: 62, V: 53), as a function of Vg. Dotted lines show theoretical values of the resistance based on the minimal edge-state model described in the text. Both Rxx and Rnl are consistent with the theoretical value apart from fluctuations. The ratio of experimental values of Rnl(I: 61, V: 53)/Rnl(I: 61, V: 54), Rnl(I: 61, V: 53)/Rnl(I: 61, V: 43), and Rnl(I: 62, V: 53)/Rnl(I: 62, V: 43) are approximately 2. Katsuyosih Komatsu et al. Sci Adv 2018;4:eaaq0194 Copyright © 2018 The Authors, some rights reserved; exclusive licensee American Association for the Advancement of Science. No claim to original U.S. Government Works. Distributed under a Creative Commons Attribution NonCommercial License 4.0 (CC BY-NC).