大学物理 ›› 2026, Vol. 45 ›› Issue (5): 105-.doi: 10.16854/j.cnki.1000-0712.250213

• 大学生园地 • 上一篇    下一篇

F型单层石墨烯纳米带阵列的可协调非对称传输

张延珊,李辉   

  1. 昆明学院 物理科学与技术学院,云南 昆明650214
  • 收稿日期:2025-04-18 修回日期:2025-09-09 出版日期:2026-07-06 发布日期:2026-08-07
  • 作者简介:张延珊(2004—),女,云南昆明人,昆明学院物理科学与技术学院2022级本科生.
  • 基金资助:
    云南省大学生创新创业项目(S202411393078);云南省教育厅科学基金项目(2022Y720; 2022Y727; 2024Y744);昆明学院科研特色团队项目(XJ20230042)资助

Asymmetric transport properties of F-type monolayer graphene array

ZHANG Yan-shan, LI Hui   

  1. School of Physical Science and Technology, Kunming University, Kunming, Yunnan 650214, China
  • Received:2025-04-18 Revised:2025-09-09 Online:2026-07-06 Published:2026-08-07

摘要: 非对称性传输(Asymmetric Transport, AT)是光的偏振态之间的转换的重要概念之一. 如何实现可调谐AT效应是构建多功能信息复用的光子集成二极管的关键技术. 然而,目前本科阶段的光学教材中对该内容介绍较少,导致学生在学习过程中较难理解和掌握. 因此,作为一个教学拓展案例,本文设计了F形单层石墨烯纳米带阵列结构,应用基于有限元法的COMSOL Multiphysics软件数值模拟了该结构的AT效应. 发现,在右旋圆偏振和左旋圆偏振光的激发下,该结构表现出Bonding和Anti-Bonding共振模式,从而引发了AT效应. 分析了F型单层石墨烯纳米带结构的臂长和石墨烯费米能级等参数对AT效应的影响. 发现,随着结构的中间臂长p增大,位于13.6 μm波长附近的共振峰会发生红移,位于波长11.4 μm附近的共振峰的位置保持不动;随着石墨烯费米能级增大,共振峰都发生了蓝移,实现了对AT信号频率的精准选择和传感. 这些结果为设计和优化用于产生及调制AT效应的石墨烯纳米结构提供了依据. 

关键词: 石墨烯, 表面等离激元, 非对称性传输

Abstract:  Asymmetric Transport (AT) is one of the key concepts in the conversion between polarization states of light. Achieving tunable AT effects is a crucial technology for constructing multifunctional information multiplexing photonic integrated diodes. However, the current undergraduate-level optics textbooks have little introduction of this content, which makes it more difficult for students to understand and master in the learning process . Therefore, as an extended teaching case, this paper designs an F-shaped monolayer graphene nanoribbon array structure and numerically simulates its AT effect using COMSOL Multiphysics software based on the Finite Element Method (FEM). It was found that under the excitation of Right Circularly Polarized (RCP) and Left Circularly Polarized (LCP) light, the structure exhibits Bonding and Anti-Bonding resonance modes, which give rise to the AT effect. The influence of parameters such as the arm length of the F-shaped monolayer graphene nanoribbon structure and the Fermi energy level of graphene on the AT effect was analyzed. It was observed that as the middle arm length p of the structure increases, the resonance peak near 13.6 μm undergoes a redshift, while the resonance peak near 11.4 μm remains stationary. Additionally, as the Fermi energy level of graphene increases, both resonance peaks exhibit a blueshift, enabling precise frequency selection and sensing of the AT signal. These results provide a basis for designing and optimizing graphene nanostructures for generating and modulating AT effects.


Key words: graphene, surface plasmon polaritons, asymmetric transmission