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Heterostructured ferromagnet–topological insulator with dual-phase magnetic properties

The introduction of ferromagnetism at the surface of a topological insulator (TI) produces fascinating spin-charge phenomena. It has been assumed that these fascinating effects are associated with a homogeneous ferromagnetic (FM) layer possessing a single type of magnetic phase. However, we obtained...

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Detalles Bibliográficos
Autores principales: Chang, Shu-Jui, Chuang, Pei-Yu, Chong, Cheong-Wei, Chen, Yu-Jung, Andrew Huang, Jung-Chun, Chen, Po-Wen, Tseng, Yuan-Chieh
Formato: Online Artículo Texto
Lenguaje:English
Publicado: The Royal Society of Chemistry 2018
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9078499/
https://www.ncbi.nlm.nih.gov/pubmed/35539151
http://dx.doi.org/10.1039/c8ra00068a
Descripción
Sumario:The introduction of ferromagnetism at the surface of a topological insulator (TI) produces fascinating spin-charge phenomena. It has been assumed that these fascinating effects are associated with a homogeneous ferromagnetic (FM) layer possessing a single type of magnetic phase. However, we obtained phase separation within the FM layer of a Ni(80)Fe(20)/Bi(2)Se(3) heterostructure. This phase separation was caused by the diffusion of Ni into Bi(2)Se(3), forming a ternary magnetic phase of Ni:Bi(2)Se(3). The inward diffusion of Ni led to the formation of an FeSe phase outward, transforming the original Ni(80)Fe(20)/Bi(2)Se(3) into a sandwich structure comprising FeSe/Ni:Bi(2)Se(3)/Bi(2)Se(3) with dual-phase magnetic characteristics similar to that driven by the proximity effect. Such a phenomenon might have been overlooked in previous studies with a strong focus on the proximity effect. X-ray magnetic spectroscopy revealed that FeSe and Ni:Bi(2)Se(3) possess horizontal and perpendicular magnetic anisotropy, respectively. The overall magnetic order of the heterostructure can be easily tuned by adjusting the thickness of the Bi(2)Se(3) as it compromises the magnetic orders of the two magnetic phases. This discovery is essential to the quantification of spin-charge phenomena in similar material combinations where the FM layer is composed of multiple elements.