材料科学
自旋电子学
拓扑绝缘体
铁磁性
凝聚态物理
三元运算
半金属
相(物质)
锡
低能电子显微镜
拓扑(电路)
纳米技术
光电子学
带隙
电子显微镜
光学
冶金
物理
有机化学
组合数学
化学
程序设计语言
计算机科学
数学
作者
L. Gładczuk,Łukasz Gładczuk,P. Dłużewski,P. Aleshkevych,Artem Lynnyk,G. van der Laan,T. Hesjedal
标识
DOI:10.1002/admi.202201452
摘要
Abstract Topological electronic materials hold great promise for revolutionizing spintronics, owing to their topological protected, spin‐polarized conduction edge or surface state. One of the key bottlenecks for the practical use of common binary and ternary topological insulator materials is the large defect concentration that leads to a high background carrier concentration. Elemental tin in its α‐phase is a room temperature topological semimetal, which is intrinsically less prone to defect‐related shortcomings. Recently, the growth of ultrathin α‐Sn films on ferromagnetic Co surfaces has been achieved; however, thicker films are needed to reach the 3D topological Dirac semimetallic state. Here, the growth of α‐Sn films on Co at cryogenic temperatures was explored. Very low‐temperature growth holds the promise of suppressing undesired phases, alloying across the interfaces, as well as the formation of Sn pillars or hillocks. Nevertheless, the critical Sn layer thickness of ≈3 atomic layers, above which the film partially transforms into the undesired b ‐phase, remains the same as for room‐temperature growth. From ferromagnetic resonance studies, and supported by electron microscopy, it can be concluded that for cryogenic Sn layer growth, the interface between Sn and Co remains sharp and the magnetic properties of the Co layer stay intact.
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