超导电性
亚稳态
八面体
结晶学
材料科学
Crystal(编程语言)
晶体结构
相(物质)
单晶
衍射
凝聚态物理
相变
化学
物理
光学
有机化学
程序设计语言
计算机科学
作者
Yuqiang Fang,Jie Pan,Jianqiao He,Ruichun Luo,Dong Wang,Xiangli Che,Kejun Bu,Wei Zhao,Pan Liu,Gang Mu,Hui Zhang,Tianquan Lin,Fuqiang Huang
标识
DOI:10.1002/ange.201710512
摘要
Abstract 2H MoS 2 has been intensively studied because of its layer‐dependent electronic structures and novel physical properties. Though the metastable 1T MoS 2 with a [MoS 6 ] octahedron was observed over the microscopic area, the true crystal structure of 1T phase has not been strictly determined. Moreover, the true physical properties have not been demonstrated from experiments owing to the challenge for the preparation of pure 1T MoS 2 crystals. 1T MoS 2 single crystals were successfully synthesized and the crystal structure of 1T MoS 2 re‐determined from single‐crystal X‐ray diffraction. 1T MoS 2 crystallizes in the space group P m1 with a cell of a=b=3.190(3) Å and c=5.945(6) Å. The individual MoS 2 layer consists of MoS 6 octahedra sharing edges with each other. More surprisingly, the bulk 1T MoS 2 crystals undergo a superconducting transition of T c =4 K, which is the first observation of superconductivity in pure 1T MoS 2 phase.
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