2015
DOI: 10.1103/physrevb.92.085103
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Robust local and nonlocal transport in the topological Kondo insulatorSmB6in the presence of a high magnetic field

Abstract: . (2015) Robust local and nonlocal transport in the topological Kondo insulator SmB6in the presence of a high magnetic field. Physical Review B, 92 (8). 085103. Permanent WRAP URL:http://wrap.warwick.ac.uk/87833 Copyright and reuse:The Warwick Research Archive Portal (WRAP) makes this work by researchers of the University of Warwick available open access under the following conditions. Copyright © and all moral rights to the version of the paper presented here belong to the individual author(s) and/or other co… Show more

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Cited by 13 publications
(20 citation statements)
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“…The value of l φ at 20 mK obtained from the low-field-magnetoconductance fluctuation data using Eq. (1) is ∼1400 nm, which is quite close to the value found from WAL (∼1200 nm) [19,26], showing that these are indeed UCFs. Also, the value of (δG) 2 1/2 obtained at 20 mK from the time series of resistance fluctuations (using the data presented in Fig.…”
Section: Regime I: Transport Through Only Sss (T < 3 K)supporting
confidence: 82%
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“…The value of l φ at 20 mK obtained from the low-field-magnetoconductance fluctuation data using Eq. (1) is ∼1400 nm, which is quite close to the value found from WAL (∼1200 nm) [19,26], showing that these are indeed UCFs. Also, the value of (δG) 2 1/2 obtained at 20 mK from the time series of resistance fluctuations (using the data presented in Fig.…”
Section: Regime I: Transport Through Only Sss (T < 3 K)supporting
confidence: 82%
“…The local voltage v l increased by more than four orders of magnitude as the sample was cooled down from room temperature, which attests to the high purity of the SmB 6 crystals. The nonlocal voltage appeared below ∼10 K and increased rapidly by more than six orders of magnitude before saturating below T = 3 K. We showed in a previous publication that the appearance of this nonlocal transport signal can be attributed to SSs, which creates an additional transport channel in parallel with the bulk of the sample [19]. Using the method described in Ref.…”
Section: Introductionmentioning
confidence: 88%
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“…Also, from the historical perspective of the 2D electron gas studies, dHvA quantum oscillations have been more challenging to observe than the SdH oscillations, because the total magnetic moments are very small in a typical 2D electron layer 31 . Although not a disagreement in the strict sense, it is peculiar that Shubnikov de-Haas (SdH) quantum oscillations through dc electrical transport have not been observed even up to ∼80 T, 32 although dHvA has been reported with an onset lower than 10 T. In electrical transport, weak anti-localization (WAL), which is a supporting evidence of the helical spin structure on the TI surface, has been reported [33][34][35] ; however, there is also a report that WAL may not be universal possibility because of the magnetic impurities existing on the surface 7 . As we will show in this study, there are a number of transport experiments such as Hall effect, thermal transport, etc., but these electrical transport experiments report conductivity (σ 2D ), carrier density (n 2D ) and mobility (µ 2D ) in a wide (orders of magnitude) range of different values.…”
Section: Introductionmentioning
confidence: 97%