Thickness dependence of the quantum Hall effect in films of the three-dimensional Dirac semimetal Cd3As2
Low-temperature magnetotransport studies are reported for (112)Cd3As2 films grown on (111)CdTe by molecular beam epitaxy as a function of the Cd3As2 film thickness. All films show Shubnikov-de Haas oscillations. An even-integer quantum Hall effect is observed for films thinner than 70 nm. For the th...
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2018-02-01
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Series: | APL Materials |
Online Access: | http://dx.doi.org/10.1063/1.5016866 |
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doaj-36724df146c4463db82920fbdf2ccacd2020-11-24T21:37:56ZengAIP Publishing LLCAPL Materials2166-532X2018-02-0162026105026105-610.1063/1.5016866006802APMThickness dependence of the quantum Hall effect in films of the three-dimensional Dirac semimetal Cd3As2Manik Goyal0Luca Galletti1Salva Salmani-Rezaie2Timo Schumann3David A. Kealhofer4Susanne Stemmer5Materials Department, University of California, Santa Barbara, California 93106-5050, USAMaterials Department, University of California, Santa Barbara, California 93106-5050, USAMaterials Department, University of California, Santa Barbara, California 93106-5050, USAMaterials Department, University of California, Santa Barbara, California 93106-5050, USADepartment of Physics, University of California, Santa Barbara, California 93106-9530, USAMaterials Department, University of California, Santa Barbara, California 93106-5050, USALow-temperature magnetotransport studies are reported for (112)Cd3As2 films grown on (111)CdTe by molecular beam epitaxy as a function of the Cd3As2 film thickness. All films show Shubnikov-de Haas oscillations. An even-integer quantum Hall effect is observed for films thinner than 70 nm. For the thinnest films, the bulk is gapped and transport at low temperatures occurs only via the gapless, two-dimensional states. The lowest Landau level is reached at ∼10 T, and the longitudinal resistance nearly vanishes at the plateaus in the Hall resistance. The results are discussed in the context of the current theoretical understanding of topological surface states in three-dimensional Dirac semimetals.http://dx.doi.org/10.1063/1.5016866 |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Manik Goyal Luca Galletti Salva Salmani-Rezaie Timo Schumann David A. Kealhofer Susanne Stemmer |
spellingShingle |
Manik Goyal Luca Galletti Salva Salmani-Rezaie Timo Schumann David A. Kealhofer Susanne Stemmer Thickness dependence of the quantum Hall effect in films of the three-dimensional Dirac semimetal Cd3As2 APL Materials |
author_facet |
Manik Goyal Luca Galletti Salva Salmani-Rezaie Timo Schumann David A. Kealhofer Susanne Stemmer |
author_sort |
Manik Goyal |
title |
Thickness dependence of the quantum Hall effect in films of the three-dimensional Dirac semimetal Cd3As2 |
title_short |
Thickness dependence of the quantum Hall effect in films of the three-dimensional Dirac semimetal Cd3As2 |
title_full |
Thickness dependence of the quantum Hall effect in films of the three-dimensional Dirac semimetal Cd3As2 |
title_fullStr |
Thickness dependence of the quantum Hall effect in films of the three-dimensional Dirac semimetal Cd3As2 |
title_full_unstemmed |
Thickness dependence of the quantum Hall effect in films of the three-dimensional Dirac semimetal Cd3As2 |
title_sort |
thickness dependence of the quantum hall effect in films of the three-dimensional dirac semimetal cd3as2 |
publisher |
AIP Publishing LLC |
series |
APL Materials |
issn |
2166-532X |
publishDate |
2018-02-01 |
description |
Low-temperature magnetotransport studies are reported for (112)Cd3As2 films grown on (111)CdTe by molecular beam epitaxy as a function of the Cd3As2 film thickness. All films show Shubnikov-de Haas oscillations. An even-integer quantum Hall effect is observed for films thinner than 70 nm. For the thinnest films, the bulk is gapped and transport at low temperatures occurs only via the gapless, two-dimensional states. The lowest Landau level is reached at ∼10 T, and the longitudinal resistance nearly vanishes at the plateaus in the Hall resistance. The results are discussed in the context of the current theoretical understanding of topological surface states in three-dimensional Dirac semimetals. |
url |
http://dx.doi.org/10.1063/1.5016866 |
work_keys_str_mv |
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