Engineering covalently bonded 2D layered materials by self-intercalation

范德瓦尔斯力 插层(化学) 双层 材料科学 空位缺陷 化学计量学 共价键 结晶学 过渡金属 铁磁性 化学物理 化学 纳米技术 分子 无机化学 凝聚态物理 物理化学 物理 有机化学 催化作用 冶金 生物化学
作者
Xiaoxu Zhao,Peng Song,Chengcai Wang,Anders C. Riis-Jensen,Wei Fu,Ya Deng,Dongyang Wan,Lixing Kang,Shoucong Ning,Jiadong Dan,T. Venkatesan,Zheng Liu,Wu Zhou,Kristian S. Thygesen,Xin Luo,Stephen J. Pennycook,Kian Ping Loh
出处
期刊:Nature [Nature Portfolio]
卷期号:581 (7807): 171-177 被引量:254
标识
DOI:10.1038/s41586-020-2241-9
摘要

Two-dimensional (2D) materials1–5 offer a unique platform from which to explore the physics of topology and many-body phenomena. New properties can be generated by filling the van der Waals gap of 2D materials with intercalants6,7; however, post-growth intercalation has usually been limited to alkali metals8–10. Here we show that the self-intercalation of native atoms11,12 into bilayer transition metal dichalcogenides during growth generates a class of ultrathin, covalently bonded materials, which we name ic-2D. The stoichiometry of these materials is defined by periodic occupancy patterns of the octahedral vacancy sites in the van der Waals gap, and their properties can be tuned by varying the coverage and the spatial arrangement of the filled sites7,13. By performing growth under high metal chemical potential14,15 we can access a range of tantalum-intercalated TaS(Se)y, including 25% Ta-intercalated Ta9S16, 33.3% Ta-intercalated Ta7S12, 50% Ta-intercalated Ta10S16, 66.7% Ta-intercalated Ta8Se12 (which forms a Kagome lattice) and 100% Ta-intercalated Ta9Se12. Ferromagnetic order was detected in some of these intercalated phases. We also demonstrate that self-intercalated V11S16, In11Se16 and FexTey can be grown under metal-rich conditions. Our work establishes self-intercalation as an approach through which to grow a new class of 2D materials with stoichiometry- or composition-dependent properties. The intercalation of native atoms into bilayer transition metal dichalcogenides during growth generates ultrathin, covalently bonded materials into which ferromagnetic ordering can be introduced.
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