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Proximity Effect induced transport Properties between MBE grown (Bi(1−x)Sb(x))(2)Se(3) Topological Insulators and Magnetic Insulator CoFe(2)O(4)

In this study, we investigate the proximity effect in topological insulator (TI) and magnetic insulator bilayer system. (Bi(1−x)Sb(x))(2)Se(3)/CoFe(2)O(4) (CFO) heterostructure was fabricated using molecular beam epitaxy and pulsed laser deposition system respectively. As revealed from the magnetore...

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Autores principales: Huang, Shun-Yu, Chong, Cheong-Wei, Tung, Yi, Chen, Tzu-Chin, Wu, Ki-Chi, Lee, Min-Kai, Huang, Jung-Chun-Andrew, Li, Z., Qiu, H.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group UK 2017
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5445069/
https://www.ncbi.nlm.nih.gov/pubmed/28546637
http://dx.doi.org/10.1038/s41598-017-02662-8
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author Huang, Shun-Yu
Chong, Cheong-Wei
Tung, Yi
Chen, Tzu-Chin
Wu, Ki-Chi
Lee, Min-Kai
Huang, Jung-Chun-Andrew
Li, Z.
Qiu, H.
author_facet Huang, Shun-Yu
Chong, Cheong-Wei
Tung, Yi
Chen, Tzu-Chin
Wu, Ki-Chi
Lee, Min-Kai
Huang, Jung-Chun-Andrew
Li, Z.
Qiu, H.
author_sort Huang, Shun-Yu
collection PubMed
description In this study, we investigate the proximity effect in topological insulator (TI) and magnetic insulator bilayer system. (Bi(1−x)Sb(x))(2)Se(3)/CoFe(2)O(4) (CFO) heterostructure was fabricated using molecular beam epitaxy and pulsed laser deposition system respectively. As revealed from the magnetoresistance measurement, the weak anti-localization (WAL) is strongly suppressed by proximity effect in (Bi(1−x)Sb(x))(2)Se(3)/CFO interface. Modified Hikama-Larkin-Nagaoka equation was used to fit the WAL results so that the size of surface state gap can be extracted successfully. The temperature-dependent resistance of the heterostructures at small and large perpendicular magnetic fields were also measured and analyzed. The results indicate that the surface band gap can be induced in TI and continuously enlarged up to 9 T, indicating the gradual alignment of the magnetic moment in CFO under perpendicular magnetic field. The approaches and results accommodated in this work show that CFO can effectively magnetize (Bi(1−x)Sb(x))(2)Se(3) and the heterostructures are promising for TI-based spintronic device applications.
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spelling pubmed-54450692017-05-26 Proximity Effect induced transport Properties between MBE grown (Bi(1−x)Sb(x))(2)Se(3) Topological Insulators and Magnetic Insulator CoFe(2)O(4) Huang, Shun-Yu Chong, Cheong-Wei Tung, Yi Chen, Tzu-Chin Wu, Ki-Chi Lee, Min-Kai Huang, Jung-Chun-Andrew Li, Z. Qiu, H. Sci Rep Article In this study, we investigate the proximity effect in topological insulator (TI) and magnetic insulator bilayer system. (Bi(1−x)Sb(x))(2)Se(3)/CoFe(2)O(4) (CFO) heterostructure was fabricated using molecular beam epitaxy and pulsed laser deposition system respectively. As revealed from the magnetoresistance measurement, the weak anti-localization (WAL) is strongly suppressed by proximity effect in (Bi(1−x)Sb(x))(2)Se(3)/CFO interface. Modified Hikama-Larkin-Nagaoka equation was used to fit the WAL results so that the size of surface state gap can be extracted successfully. The temperature-dependent resistance of the heterostructures at small and large perpendicular magnetic fields were also measured and analyzed. The results indicate that the surface band gap can be induced in TI and continuously enlarged up to 9 T, indicating the gradual alignment of the magnetic moment in CFO under perpendicular magnetic field. The approaches and results accommodated in this work show that CFO can effectively magnetize (Bi(1−x)Sb(x))(2)Se(3) and the heterostructures are promising for TI-based spintronic device applications. Nature Publishing Group UK 2017-05-25 /pmc/articles/PMC5445069/ /pubmed/28546637 http://dx.doi.org/10.1038/s41598-017-02662-8 Text en © The Author(s) 2017 Open Access This article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made. The images or other third party material in this article are included in the article’s Creative Commons license, unless indicated otherwise in a credit line to the material. If material is not included in the article’s Creative Commons license and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this license, visit http://creativecommons.org/licenses/by/4.0/.
spellingShingle Article
Huang, Shun-Yu
Chong, Cheong-Wei
Tung, Yi
Chen, Tzu-Chin
Wu, Ki-Chi
Lee, Min-Kai
Huang, Jung-Chun-Andrew
Li, Z.
Qiu, H.
Proximity Effect induced transport Properties between MBE grown (Bi(1−x)Sb(x))(2)Se(3) Topological Insulators and Magnetic Insulator CoFe(2)O(4)
title Proximity Effect induced transport Properties between MBE grown (Bi(1−x)Sb(x))(2)Se(3) Topological Insulators and Magnetic Insulator CoFe(2)O(4)
title_full Proximity Effect induced transport Properties between MBE grown (Bi(1−x)Sb(x))(2)Se(3) Topological Insulators and Magnetic Insulator CoFe(2)O(4)
title_fullStr Proximity Effect induced transport Properties between MBE grown (Bi(1−x)Sb(x))(2)Se(3) Topological Insulators and Magnetic Insulator CoFe(2)O(4)
title_full_unstemmed Proximity Effect induced transport Properties between MBE grown (Bi(1−x)Sb(x))(2)Se(3) Topological Insulators and Magnetic Insulator CoFe(2)O(4)
title_short Proximity Effect induced transport Properties between MBE grown (Bi(1−x)Sb(x))(2)Se(3) Topological Insulators and Magnetic Insulator CoFe(2)O(4)
title_sort proximity effect induced transport properties between mbe grown (bi(1−x)sb(x))(2)se(3) topological insulators and magnetic insulator cofe(2)o(4)
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5445069/
https://www.ncbi.nlm.nih.gov/pubmed/28546637
http://dx.doi.org/10.1038/s41598-017-02662-8
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