Tao Xiang, Qi Limei, Hu Haifeng, Fu Tao, Uqaili Junaid Ahmed
Opt Express. 2021 Jul 5;29(14):21044-21055. doi: 10.1364/OE.421367.
The reported dual-band asymmetric transmission is usually an effect of mutual polarization conversion, where one polarized wave is converted to its cross-polarization in the first band while the other polarized wave is converted to its cross-polarization in the second band. In this work, we experimentally demonstrate a dual-band asymmetric transmission effect only for one-polarized linear wave in the terahertz band. It is measured that the cross-polarization transmission coefficient T reaches two peaks of 0.715 and 0.548 at the frequency of 0.74 THz and 1.22 THz, respectively. While the transmission coefficient T is lower than 0.2 in the wide-band from 0.5 THz to 1.5 THz. Firstly, the multiple interference model is used to discuss the physical mechanism of the dual-band asymmetric transmission. However, the second band of the calculated spectrum is offset due to the strong near field coupling between the two metal layers. The coupled-mode theory is then introduced and the fitting result of the coupled-mode theory is in good agreement with that of the experiment in the two bands. This research would provide new theoretical instructions in designing and analyzing multiband asymmetric transmission in the terahertz, microwave or the optical bands.
报道的双频段非对称传输通常是相互极化转换的结果,其中一个极化波在第一频段转换为其交叉极化,而另一个极化波在第二频段转换为其交叉极化。在这项工作中,我们通过实验证明了太赫兹频段中仅针对单极化线性波的双频段非对称传输效应。测量发现,交叉极化传输系数T在0.74太赫兹和1.22太赫兹频率处分别达到0.715和0.548两个峰值。而在从0.5太赫兹到1.5太赫兹的宽带内,传输系数T低于0.2。首先,使用多重干涉模型来讨论双频段非对称传输的物理机制。然而,由于两个金属层之间强烈的近场耦合,计算光谱的第二频段发生了偏移。随后引入了耦合模理论,耦合模理论的拟合结果与两个频段的实验结果吻合良好。这项研究将为太赫兹、微波或光学频段的多频段非对称传输的设计和分析提供新的理论指导。