Nature Communications (Nov 2020)
Designer spin order in diradical nanographenes
- Yuqiang Zheng,
- Can Li,
- Chengyang Xu,
- Doreen Beyer,
- Xinlei Yue,
- Yan Zhao,
- Guanyong Wang,
- Dandan Guan,
- Yaoyi Li,
- Hao Zheng,
- Canhua Liu,
- Junzhi Liu,
- Xiaoqun Wang,
- Weidong Luo,
- Xinliang Feng,
- Shiyong Wang,
- Jinfeng Jia
Affiliations
- Yuqiang Zheng
- Key Laboratory of Artificial Structures and Quantum Control (Ministry of Education), Shenyang National Laboratory for Materials Science, School of Physics and Astronomy, Shanghai Jiao Tong University
- Can Li
- Key Laboratory of Artificial Structures and Quantum Control (Ministry of Education), Shenyang National Laboratory for Materials Science, School of Physics and Astronomy, Shanghai Jiao Tong University
- Chengyang Xu
- Key Laboratory of Artificial Structures and Quantum Control (Ministry of Education), Shenyang National Laboratory for Materials Science, School of Physics and Astronomy, Shanghai Jiao Tong University
- Doreen Beyer
- Center for Advancing Electronics Dresden and Department of Chemistry and Food Chemistry, Technische Universität Dresden
- Xinlei Yue
- Key Laboratory of Artificial Structures and Quantum Control (Ministry of Education), Shenyang National Laboratory for Materials Science, School of Physics and Astronomy, Shanghai Jiao Tong University
- Yan Zhao
- Key Laboratory of Artificial Structures and Quantum Control (Ministry of Education), Shenyang National Laboratory for Materials Science, School of Physics and Astronomy, Shanghai Jiao Tong University
- Guanyong Wang
- Key Laboratory of Artificial Structures and Quantum Control (Ministry of Education), Shenyang National Laboratory for Materials Science, School of Physics and Astronomy, Shanghai Jiao Tong University
- Dandan Guan
- Key Laboratory of Artificial Structures and Quantum Control (Ministry of Education), Shenyang National Laboratory for Materials Science, School of Physics and Astronomy, Shanghai Jiao Tong University
- Yaoyi Li
- Key Laboratory of Artificial Structures and Quantum Control (Ministry of Education), Shenyang National Laboratory for Materials Science, School of Physics and Astronomy, Shanghai Jiao Tong University
- Hao Zheng
- Key Laboratory of Artificial Structures and Quantum Control (Ministry of Education), Shenyang National Laboratory for Materials Science, School of Physics and Astronomy, Shanghai Jiao Tong University
- Canhua Liu
- Key Laboratory of Artificial Structures and Quantum Control (Ministry of Education), Shenyang National Laboratory for Materials Science, School of Physics and Astronomy, Shanghai Jiao Tong University
- Junzhi Liu
- Department of Chemistry and State Key Laboratory of Synthetic Chemistry, The University of Hong Kong
- Xiaoqun Wang
- Key Laboratory of Artificial Structures and Quantum Control (Ministry of Education), Shenyang National Laboratory for Materials Science, School of Physics and Astronomy, Shanghai Jiao Tong University
- Weidong Luo
- Key Laboratory of Artificial Structures and Quantum Control (Ministry of Education), Shenyang National Laboratory for Materials Science, School of Physics and Astronomy, Shanghai Jiao Tong University
- Xinliang Feng
- Center for Advancing Electronics Dresden and Department of Chemistry and Food Chemistry, Technische Universität Dresden
- Shiyong Wang
- Key Laboratory of Artificial Structures and Quantum Control (Ministry of Education), Shenyang National Laboratory for Materials Science, School of Physics and Astronomy, Shanghai Jiao Tong University
- Jinfeng Jia
- Key Laboratory of Artificial Structures and Quantum Control (Ministry of Education), Shenyang National Laboratory for Materials Science, School of Physics and Astronomy, Shanghai Jiao Tong University
- DOI
- https://doi.org/10.1038/s41467-020-19834-2
- Journal volume & issue
-
Vol. 11,
no. 1
pp. 1 – 7
Abstract
The ability to control magnetic coupling in graphene nanomaterials remains elusive. Here, the authors report an approach of engineering magnetic ground states in open-shell bipartite/nonbipartite nanographenes where the magnetic coupling sign between two spins are controlled via breaking bipartite lattice symmetry.
