Emerging Anomalous Hall Effect in (111)‐Oriented Artificial Iridate Honeycomb Lattices

Abstract Complex Ir oxides provide a promising platform for investigating cooperativity and competition between Mott physics and spin‐orbit coupling in condensed matter physics. These materials have the potential to reveal intriguing phases, such as topological phases and the Kitaev spin liquid state, an exactly solvable S = 1/2 spin model describing Ir 4+ ions on a 2D honeycomb lattice. However, experimental confirmation of such phases in iridate films has been hindered by the difficulty of preparing (111)‐oriented samples of the perovskite phase. Herein, by constructing SrIrO 3 /SrTiO 3 superlattices on SrTiO 3 (111) substrates, (111)‐oriented perovskite phase SrIrO 3 films are achieved with the unprecedentedly large thickness of 6 unit cells. Electrical and magnetic characterizations reveal that these films exhibit anomalous Hall insulating behavior, significant charge fluctuations, and long‐range antiferromagnetic order. Moreover, these properties can be tuned by varying the thickness of the SrIrO₃ layer. These emergent phenomena underscore the complex interactions among spin‐orbit coupling, electron–electron correlations, and crystal structure in (111)‐oriented artificial iridate honeycomb lattices. Further, spin fractionalization and topological quantum spin liquid may be achieved by tuning the spin–orbit coupling and crystal field intensity from interface engineering.

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Publication Details

Journal
Advanced Functional Materials
Published
2024-11-05
DOI
https://doi.org/10.1002/adfm.202414425
Citations
1
Primary Topic
Advanced Condensed Matter Physics
Type
article
Field-Weighted Citation Impact
0.31

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article

Emerging Anomalous Hall Effect in (111)‐Oriented Artificial Iridate Honeycomb Lattices

Zhan Yang, Yuhao Hong, Zhaoliang Liao, Lei Wang et al.
1 citations
Advanced Functional Materials
Advanced Condensed Matter Physics
0.31
article

Emerging Anomalous Hall Effect in (111)‐Oriented Artificial Iridate Honeycomb Lattices

Zhan Yang, Yuhao Hong, Zhaoliang Liao, Lei Wang, Yulin Gan, Wen Xiao, Qinghua Zhang, Meilin Liu, Kai Chen, Zhixiong Deng, Junhua Liu, Shilin Hu, Xiaofei Gao, Ziyue Shen, Runze Yao
article en
1 citations

Abstract

Abstract Complex Ir oxides provide a promising platform for investigating cooperativity and competition between Mott physics and spin‐orbit coupling in condensed matter physics. These materials have the potential to reveal intriguing phases, such as topological phases and the Kitaev spin liquid state, an exactly solvable S = 1/2 spin model describing Ir 4+ ions on a 2D honeycomb lattice. However, experimental confirmation of such phases in iridate films has been hindered by the difficulty of preparing (111)‐oriented samples of the perovskite phase. Herein, by constructing SrIrO 3 /SrTiO 3 superlattices on SrTiO 3 (111) substrates, (111)‐oriented perovskite phase SrIrO 3 films are achieved with the unprecedentedly large thickness of 6 unit cells. Electrical and magnetic characterizations reveal that these films exhibit anomalous Hall insulating behavior, significant charge fluctuations, and long‐range antiferromagnetic order. Moreover, these properties can be tuned by varying the thickness of the SrIrO₃ layer. These emergent phenomena underscore the complex interactions among spin‐orbit coupling, electron–electron correlations, and crystal structure in (111)‐oriented artificial iridate honeycomb lattices. Further, spin fractionalization and topological quantum spin liquid may be achieved by tuning the spin–orbit coupling and crystal field intensity from interface engineering.

Advanced Functional MaterialsVol. 35(5)
University of Science and Technology of China (CN), Chinese Academy of Sciences (CN), Zhengzhou University (CN), National Synchrotron Radiation Laboratory (CN), Institute of Physics (CN)
National Natural Science Foundation of China, Ministry of Science and Technology of the People's Republic of China, Fundamental Research Funds for the Central Universities
Openalex Percentile: Top 42%
Advanced Condensed Matter Physics
0.31
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