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Phase-Changing in Graphite Assisted by Interface Charge Injection.
Pan, Fei; Ni, Kun; Ma, Yue; Wu, Hongjian; Tang, Xiaoyu; Xiong, Juan; Yang, Yaping; Ye, Chuanren; Yuan, Hong; Lin, Miao-Ling; Dai, Jiayu; Zhu, Mengjian; Tan, Ping-Heng; Zhu, Yanwu; Novoselov, Kostya S.
Affiliation
  • Pan F; Hefei National Research Center for Physical Sciences at the Microscale, & CAS Key Laboratory of Materials for Energy Conversion & Department of Materials Science and Engineering, University of Science and Technology of China, 96 Jin Zhai Road, Hefei, Anhui 230026, P. R. China.
  • Ni K; Hefei National Research Center for Physical Sciences at the Microscale, & CAS Key Laboratory of Materials for Energy Conversion & Department of Materials Science and Engineering, University of Science and Technology of China, 96 Jin Zhai Road, Hefei, Anhui 230026, P. R. China.
  • Ma Y; State Key Laboratory of Solidification Processing, & Center for Nano Energy Materials, & School of Materials Science and Engineering, Northwestern Polytechnical University & Shaanxi Joint Laboratory of Graphene (NPU), Xi' an, Shaanxi 710072, P. R. China.
  • Wu H; Department of Physics, National University of Defense Technology, Changsha, Hunan 410073, P. R. China.
  • Tang X; State Key Laboratory of Solidification Processing, & Center for Nano Energy Materials, & School of Materials Science and Engineering, Northwestern Polytechnical University & Shaanxi Joint Laboratory of Graphene (NPU), Xi' an, Shaanxi 710072, P. R. China.
  • Xiong J; Hefei National Research Center for Physical Sciences at the Microscale, & CAS Key Laboratory of Materials for Energy Conversion & Department of Materials Science and Engineering, University of Science and Technology of China, 96 Jin Zhai Road, Hefei, Anhui 230026, P. R. China.
  • Yang Y; Science and Technology on Advanced Ceramic Fibers and Composites Laboratory, College of Aerospace Science and Engineering, National University of Defense Technology, Changsha, Hunan 410073, P. R. China.
  • Ye C; Hefei National Research Center for Physical Sciences at the Microscale, & CAS Key Laboratory of Materials for Energy Conversion & Department of Materials Science and Engineering, University of Science and Technology of China, 96 Jin Zhai Road, Hefei, Anhui 230026, P. R. China.
  • Yuan H; Hefei National Research Center for Physical Sciences at the Microscale, & CAS Key Laboratory of Materials for Energy Conversion & Department of Materials Science and Engineering, University of Science and Technology of China, 96 Jin Zhai Road, Hefei, Anhui 230026, P. R. China.
  • Lin ML; State Key Laboratory of Superlattices and Microstructures, Institute of Semiconductors, Chinese Academy of Sciences, Beijing 100083, P. R. China.
  • Dai J; Department of Physics, National University of Defense Technology, Changsha, Hunan 410073, P. R. China.
  • Zhu M; College of Advanced Interdisciplinary Studies, National University of Defense Technology, Changsha, Hunan 410073, P. R. China.
  • Tan PH; State Key Laboratory of Superlattices and Microstructures, Institute of Semiconductors, Chinese Academy of Sciences, Beijing 100083, P. R. China.
  • Zhu Y; Hefei National Research Center for Physical Sciences at the Microscale, & CAS Key Laboratory of Materials for Energy Conversion & Department of Materials Science and Engineering, University of Science and Technology of China, 96 Jin Zhai Road, Hefei, Anhui 230026, P. R. China.
  • Novoselov KS; National Graphene Institute, University of Manchester, Oxford Road, Manchester, M13 9PL, United Kingdom.
Nano Lett ; 21(13): 5648-5654, 2021 Jul 14.
Article in En | MEDLINE | ID: mdl-34165978
ABSTRACT
Among many phase-changing materials, graphite is probably the most studied and interesting the rhombohedral (3R) and hexagonal (2H) phases exhibit dramatically different electronic properties. However, up to now the only way to promote 3R to 2H phase transition is through exposure to elevated temperatures (above 1000 °C); thus, it is not feasible for modern technology. In this work, we demonstrate that 3R to 2H phase transition can be promoted by changing the charged state of 3D graphite, which promotes the repulsion between the layers and significantly reduces the energy barrier between the 3R and 2H phases. In particular, we show that charge transfer from lithium nitride (α-Li3N) to graphite can lower the transition temperature down to 350 °C. The proposed interlayer slipping model potentially offers the control over topological states at the interfaces between different phases, making this system even more attractive for future electronic applications.
Key words

Full text: 1 Collection: 01-internacional Database: MEDLINE Language: En Journal: Nano Lett Year: 2021 Document type: Article

Full text: 1 Collection: 01-internacional Database: MEDLINE Language: En Journal: Nano Lett Year: 2021 Document type: Article