Fig. 3 Supercurrents in various conductance plateau regions.

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Fig. 3 Supercurrents in various conductance plateau regions. Supercurrents in various conductance plateau regions. (A) Differential resistance R against I in the conductance plateau regions of (2,0), (0,2), and (2,2). Isw in the (2,2) region is much larger than the sum of the Isw values in the (2,0) and (0,2) regions. (B) R against I in the conductance plateau regions of (4,0), (0,4), and (4,4). The sum of the Isw value in the (4,4) region is much larger than the sum of the Isw values in the (4,0) and (0,4) regions. (C) Isw(m, n) against G(m, n) in the conductance plateau regions (m, n) = (2,2), (2,4), (4,2), (2,6), (6,2), and (4,4), respectively, and the sum of Isw(m, 0) and Isw(0, n) against the sum of G(0, n) and G(m, 0) in the conductance plateau regions (0, n) = (0,2) and (0,4) and (m, 0) = (2,0) and (4,0). The bars indicate variations of Isw and G in the measurement performed at various points of the respective plateaus. Isw(m, n) is significantly larger than Isw(n, 0) + Isw(0, m) because of the CPS contribution to the DNW. Kento Ueda et al. Sci Adv 2019;5:eaaw2194 Copyright © 2019 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).