具有铁磁损耗的非互易磁性光子晶体的PML-FDTD分析

Kyung‐Young Jung, B. Donderici, F. Teixeira
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引用次数: 2

摘要

非互易磁光子晶体(MPCs)是一种色散工程超材料,具有独特的特性,如电磁单向性和零群速度的冻结模式[1],[2]。非互易MPCs是由各向异性介质层(a层)和铁磁层(f层)组成的周期性结构,如图1所示。适当选择几何和张量参数的MPCs可以显示不对称色散关系ω(k),其中正向有平稳拐点(SIP),而反向无SIP[1]。由于SIP附近的群速度极低,电磁波似乎被“冻结”在正向的非互反mpc内;同时,前向传播的电磁脉冲在MPC内的振幅会急剧增长。在反向方向上,电磁波在MPCs内以普通方式传播[2]。
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PML-FDTD Analysis of Nonreciprocal Magnetic Photonic Crystals with Ferromagnetic Losses
Nonreciprocal magnetic photonic crystals (MPCs) are dispersion engineered metamaterials that exhibit unique properties such as electromagnetic unidirectionality and frozen modes with zero group velocity [1], [2]. Nonreciprocal MPCs are periodic structures composed of misaligned anisotropic dielectric layers (A-layers) and ferromagnetic layers (F-layers), as shown in Fig. 1. MPCs with a proper choice of geometry and tensor parameters can display asymmetric dispersion relation ω(k) with a stationary inflection point (SIP) in a forward direction and no SIP in a backward direction [1]. Since group velocities are extremely low near the SIP, EM waves seem to be “frozen” inside nonreciprocal MPCs in the forward direction; at the same time, forward propagating EM pulses can exhibit a dramatic growth in amplitude inside the MPC. In the backward direction, EM waves inside the MPCs propagate in an ordinary fashion [2].
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