旋转
超导电性
联轴节(管道)
对称(几何)
共价键
材料科学
凝聚态物理
工作(物理)
拓扑(电路)
化学物理
感应耦合
手征对称性
物理
反铁磁性
纳米技术
光电子学
能量(信号处理)
机制(生物学)
分子磁体
分子对称性
磁场
对称性破坏
手性(物理)
局部对称性
磁性
作者
Tingfeng Zhang,Zhuo Xiao,Tiancheng Fang,Zhengfei Wang
出处
期刊:Nano Letters
[American Chemical Society]
日期:2026-03-31
卷期号:26 (14): 4889-4896
标识
DOI:10.1021/acs.nanolett.6c00927
摘要
The recent emergence of altermagnetism has enriched the classification of magnetic states. The symmetry constrained even-parity and odd-parity altermagnets are mainly limited to collinear and noncollinear spins in two- and three-dimensional materials. In this work, guided by the symmetry classification, we propose a general strategy for designing unconventional p-wave altermagnets in one-dimensional (1D) collinear antiferromagnets with the switchable spin-splitting under circularly polarized light, also extendable to the odd-parity altermagnets in two-dimensional (2D) collinear antiferromagnets. First-principles calculations on experimentally synthesized 1D and 2D triangulene crystals further validate our design principles, realizing the extrinsic p-wave and f-wave altermagnets. By coupling 2D altermagnetic triangulene crystals to s-wave superconductors, the high-Chern-number topological superconductivity can be achieved within spin-splitting energy windows. Our work introduces a new mechanism to engineer light-induced 1D and 2D odd-parity altermagnets and provides a molecular platform to explore the metal-free altermagnetism in π-conjugated covalent organic frameworks.
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