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结构化理想导电表面上的类表面等离激元模式

Surface plasmon-like modes on structured perfectly conducting surfaces.

作者信息

Lan Yung-Chiang, Chern Ruey-Lin

出版信息

Opt Express. 2006 Nov 13;14(23):11339-47. doi: 10.1364/oe.14.011339.

Abstract

Surface plasmon-like (SPL) modes are the electromagnetic surface eigenmodes supported by the structured perfectly conducting surfaces. The standard eigenvalue-solving method is adopted to solve these SPL modes. The field patterns of the SPL modes in the square holes for in-plane wavevectors k(x) = 2pi / 2d and k(x) = 2pi /d are TE(10)-like and TE(11), respectively. However, the field patterns can no longer be identified as any particular waveguide mode for other in-plane wavevectors. The dispersion relations of the SPL modes are obtained numerically. The change in mode character with wavevector prevents the dispersion relation from being derived by assuming only the fundamental mode in the holes. On a thin perfect conductor perforated with structures, the SPL mode splits into a high-frequency anti-symmetric mode and a low-frequency symmetric mode, which is caused by the mutual interaction of the electromagnetic evanescent fields on both sides.

摘要

类表面等离子体(SPL)模式是由结构化的理想导电表面所支持的电磁表面本征模式。采用标准的特征值求解方法来求解这些SPL模式。对于面内波矢k(x) = 2π / 2d和面内波矢k(x) = 2π /d,方孔中SPL模式的场分布分别类似于TE(10)和TE(11)。然而,对于其他面内波矢,场分布不能再被识别为任何特定的波导模式。通过数值方法获得了SPL模式的色散关系。模式特性随波矢的变化使得无法仅通过假设孔中的基模来推导出色散关系。在穿孔有结构的薄理想导体上,SPL模式分裂为高频反对称模式和低频对称模式,这是由两侧电磁倏逝场的相互作用引起的。

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