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Abstract
The deterministic creation and modification of domain walls in ferroelectric films have attracted broad interest due to their unprecedented potential as the active element in non-volatile memory, logic computation and energy-harvesting technologies. However, the correlation between charged and antiphase states, and their hybridization into a single domain wall still remain elusive. Here we demonstrate the facile fabrication of antiphase boundaries in BiFeO3 thin films using a He-ion implantation process. Cross-sectional electron microscopy, spectroscopy and piezoresponse force measurement reveal the creation of a continuous in-plane charged antiphase boundaries around the implanted depth and a variety of atomic bonding configurations at the antiphase interface, showing the atomically sharp 180° polarization reversal across the boundary. Therefore, this work not only inspires a domain-wall fabrication strategy using He-ion implantation, which is compatible with the wafer-scale patterning, but also provides atomic-scale structural insights for its future utilization in domain-wall nanoelectronics.
The correlation between charged and antiphase states in BiFeO3 remain elusive. Here, the authors report a fabrication of in-plane charged antiphase boundaries in BiFeO3 thin films, revealing the atomic bonding configurations and atomically sharp 180° polarization reversal of such boundaries.
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1 South China Normal University, Guangdong Provincial Key Laboratory of Optical Information Materials and Technology, and Institute for Advanced Materials, South China Academy of Advanced Optoelectronics, Guangzhou, China (GRID:grid.263785.d) (ISNI:0000 0004 0368 7397); Nanyang Technological University, Division of Physics and Applied Physics, School of Physical and Mathematical Sciences, Singapore, Singapore (GRID:grid.59025.3b) (ISNI:0000 0001 2224 0361)
2 South China Normal University, Guangdong Provincial Key Laboratory of Optical Information Materials and Technology, and Institute for Advanced Materials, South China Academy of Advanced Optoelectronics, Guangzhou, China (GRID:grid.263785.d) (ISNI:0000 0004 0368 7397)
3 Southern University of Science and Technology, Department of Physics, Shenzhen, China (GRID:grid.263817.9) (ISNI:0000 0004 1773 1790)
4 Institute of Ion Beam Physics and Materials Research, Helmholtz-Zentrum Dresden-Rossendorf, Dresden, Germany (GRID:grid.40602.30) (ISNI:0000 0001 2158 0612); Guangdong Mechanical and Electrical Polytechnic, School of Electronics & Communication, Guangzhou, China (GRID:grid.40602.30)
5 Peking University, State Key Laboratory of Nuclear Physics and Technology, School of Physics, Beijing, China (GRID:grid.11135.37) (ISNI:0000 0001 2256 9319)
6 Institute of Ion Beam Physics and Materials Research, Helmholtz-Zentrum Dresden-Rossendorf, Dresden, Germany (GRID:grid.40602.30) (ISNI:0000 0001 2158 0612)
7 Chinese Academy of Sciences, Institute of High Energy Physics, Beijing, China (GRID:grid.9227.e) (ISNI:0000000119573309)
8 Nanyang Technological University, Division of Physics and Applied Physics, School of Physical and Mathematical Sciences, Singapore, Singapore (GRID:grid.59025.3b) (ISNI:0000 0001 2224 0361)
9 South China Normal University, Guangdong Provincial Key Laboratory of Optical Information Materials and Technology, and Institute for Advanced Materials, South China Academy of Advanced Optoelectronics, Guangzhou, China (GRID:grid.263785.d) (ISNI:0000 0004 0368 7397); Nanjing University, Laboratory of Solid State Microstructures and Innovation Center of Advanced Microstructures, Nanjing, China (GRID:grid.41156.37) (ISNI:0000 0001 2314 964X)
10 The Hong Kong Polytechnic University, Department of Applied Physics, Research Institute for Smart Energy, Hong Kong, China (GRID:grid.16890.36) (ISNI:0000 0004 1764 6123)