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Bevel-edge epitaxy of ferroelectric rhombohedral boron nitride single crystal.
Wang, Li; Qi, Jiajie; Wei, Wenya; Wu, Mengqi; Zhang, Zhibin; Li, Xiaomin; Sun, Huacong; Guo, Quanlin; Cao, Meng; Wang, Qinghe; Zhao, Chao; Sheng, Yuxuan; Liu, Zhetong; Liu, Can; Wu, Muhong; Xu, Zhi; Wang, Wenlong; Hong, Hao; Gao, Peng; Wu, Menghao; Wang, Zhu-Jun; Xu, Xiaozhi; Wang, Enge; Ding, Feng; Zheng, Xiaorui; Liu, Kaihui; Bai, Xuedong.
Affiliation
  • Wang L; Institute of Physics, Chinese Academy of Sciences, Beijing, China. liwang@iphy.ac.cn.
  • Qi J; State Key Laboratory for Mesoscopic Physics, Frontiers Science Centre for Nano-optoelectronics, School of Physics, Peking University, Beijing, China.
  • Wei W; Guangdong Provincial Key Laboratory of Quantum Engineering and Quantum Materials, School of Physics, South China Normal University, Guangzhou, China.
  • Wu M; School of Engineering, Westlake University, Hangzhou, China.
  • Zhang Z; State Key Laboratory for Mesoscopic Physics, Frontiers Science Centre for Nano-optoelectronics, School of Physics, Peking University, Beijing, China.
  • Li X; Institute of Physics, Chinese Academy of Sciences, Beijing, China.
  • Sun H; Institute of Physics, Chinese Academy of Sciences, Beijing, China.
  • Guo Q; School of Physical Sciences, University of Chinese Academy of Sciences, Beijing, China.
  • Cao M; State Key Laboratory for Mesoscopic Physics, Frontiers Science Centre for Nano-optoelectronics, School of Physics, Peking University, Beijing, China.
  • Wang Q; Institute of Physics, Chinese Academy of Sciences, Beijing, China.
  • Zhao C; State Key Laboratory for Mesoscopic Physics, Frontiers Science Centre for Nano-optoelectronics, School of Physics, Peking University, Beijing, China.
  • Sheng Y; Shenzhen Institute of Advanced Technology, Shenzhen, China.
  • Liu Z; School of Physics, Huazhong University of Science and Technology, Wuhan, China.
  • Liu C; International Centre for Quantum Materials, Collaborative Innovation Centre of Quantum Matter, Peking University, Beijing, China.
  • Wu M; Key Laboratory of Quantum State Construction and Manipulation (Ministry of Education), Department of Physics, Renmin University of China, Beijing, China.
  • Xu Z; International Centre for Quantum Materials, Collaborative Innovation Centre of Quantum Matter, Peking University, Beijing, China.
  • Wang W; Interdisciplinary Institute of Light-Element Quantum Materials and Research Centre for Light-Element Advanced Materials, Peking University, Beijing, China.
  • Hong H; Songshan Lake Materials Laboratory, Dongguan, China.
  • Gao P; Songshan Lake Materials Laboratory, Dongguan, China.
  • Wu M; Institute of Physics, Chinese Academy of Sciences, Beijing, China.
  • Wang ZJ; Songshan Lake Materials Laboratory, Dongguan, China.
  • Xu X; State Key Laboratory for Mesoscopic Physics, Frontiers Science Centre for Nano-optoelectronics, School of Physics, Peking University, Beijing, China.
  • Wang E; Interdisciplinary Institute of Light-Element Quantum Materials and Research Centre for Light-Element Advanced Materials, Peking University, Beijing, China.
  • Ding F; International Centre for Quantum Materials, Collaborative Innovation Centre of Quantum Matter, Peking University, Beijing, China.
  • Zheng X; School of Physics, Huazhong University of Science and Technology, Wuhan, China.
  • Liu K; School of Physical Science and Technology, ShanghaiTech University, Shanghai, China.
  • Bai X; Guangdong Provincial Key Laboratory of Quantum Engineering and Quantum Materials, School of Physics, South China Normal University, Guangzhou, China.
Nature ; 629(8010): 74-79, 2024 May.
Article in En | MEDLINE | ID: mdl-38693415
ABSTRACT
Within the family of two-dimensional dielectrics, rhombohedral boron nitride (rBN) is considerably promising owing to having not only the superior properties of hexagonal boron nitride1-4-including low permittivity and dissipation, strong electrical insulation, good chemical stability, high thermal conductivity and atomic flatness without dangling bonds-but also useful optical nonlinearity and interfacial ferroelectricity originating from the broken in-plane and out-of-plane centrosymmetry5-23. However, the preparation of large-sized single-crystal rBN layers remains a challenge24-26, owing to the requisite unprecedented growth controls to coordinate the lattice orientation of each layer and the sliding vector of every interface. Here we report a facile methodology using bevel-edge epitaxy to prepare centimetre-sized single-crystal rBN layers with exact interlayer ABC stacking on a vicinal nickel surface. We realized successful accurate fabrication over a single-crystal nickel substrate with bunched step edges of the terrace facet (100) at the bevel facet (110), which simultaneously guided the consistent boron-nitrogen bond orientation in each BN layer and the rhombohedral stacking of BN layers via nucleation near each bevel facet. The pure rhombohedral phase of the as-grown BN layers was verified, and consequently showed robust, homogeneous and switchable ferroelectricity with a high Curie temperature. Our work provides an effective route for accurate stacking-controlled growth of single-crystal two-dimensional layers and presents a foundation for applicable multifunctional devices based on stacked two-dimensional materials.

Full text: 1 Database: MEDLINE Language: En Year: 2024 Type: Article

Full text: 1 Database: MEDLINE Language: En Year: 2024 Type: Article