PHYSICAL REVIEW B 89, 199901(E) (2014) D. I. Pikulin, T. Hyart, Shuo Mi, J. Tworzydło, M. Wimmer, and C. W. J. Beenakker (Received 30 April 2014; published 7 May 2014) DOI: 10.1103/PhysRevB.89.199901 PACS number(s): 72.10.−d, 72.20.−i, 72.80.Ng, 73.21.Fg, 99.10.Cd We made a factor-of-2 error in our calculations that has the effect of doubling the scale of magnetic ﬁeld in Figs. 2–6. In particular, the magnetic ﬁeld range of Figs. 4–6 goes up to 32 T. This error has two consequences: First, the effective g factor for the data shown in Fig. 6 is g = −7.5 (instead of g = −15). Secondly, the next-to-last paragraph should read as follows: One implication of our ﬁndings (see Fig. 5) is that the weak-disorder limit is, in principle, consistent with the persistence of helical edge conduction up to 8 T perpendicular ﬁelds, reported in Ref. . However, in the presence of strong disorder the bulk conduction is expected to take over at much smaller ﬁelds. 1098-0121/2014/89(19)/199901(1) 199901-1 ©2014 American Physical Society
Physical Review B – American Physical Society (APS)
Published: May 7, 2014
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