双通道磁光光子晶体波导中的可控功率传输

Peide He, S. Xie, Jiawei Liu, W. Liang
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摘要

通过引入两层普通氧化铝(Al2O3)光子晶体作为耦合层,研究了双通道磁光光子晶体波导中拓扑光子态的耦合效应。有趣的是,对于两通道宽度相同的结构,由于拓扑光子态的耦合效应,电磁波单向向右侧传播,并在波导内呈现波状路径。这种独特的特性提供了一种有效的方法,通过在波导的不同长度处终止结构,在两个右输出之间达到所需的功率比。此外,可以方便地利用外加磁场调节功率比。对于具有不同通道宽度的非对称波导,在带隙中存在两种非对称的单向拓扑光子态(即类奇模式和类偶模式)。本征场分析表明,类奇模的电场在较低的通道中更强,而类偶模的电场则相反。当类旧模式向右传播时,两个通道中的电磁波通过耦合层相互耦合,然后上层通道的功率逐渐向下层通道转移,最终下层输出的透光率几乎达到100%。然而,类偶模态的情况则完全相反。这些结果在信号传输、光调制和拓扑器件设计等许多应用领域具有很大的前景。
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Controllable power transfer in a double-channel magneto-optical photonic crystal waveguide
We have studied the coupling effect of topological photonic states in a double-channel magneto-optical photonic crystal waveguide by introducing a two-layer ordinary alumina (Al2O3) photonic crystal as the coupling layer. Interestingly, for the structure with the same widths of the two channels, the electromagnetic wave propagates one-way to the right side and exhibits wave-like path within the waveguide due to the coupling effect of topological photonic states. This unique property provides an effective way to achieve desired power ratio between two right outputs by terminating the structure at different length of waveguide. Moreover, the power ratio can be tuned by the external magnetic field conveniently. As for an asymmetric waveguide with different channel widths, there exist two asymmetric one-way topological photonic states (i.e., the odd-like and even-like modes) in the bandgap. The eigenfield analyses show that the electric field of odd-like mode is stronger in the lower channel, while that of even-like mode is contrary. As the old-like mode propagates rightwards, electromagnetic waves in the two channels couple with each other via the coupling layer, then the power in the upper channel gradually transfers to the lower channel, and finally reach almost 100% transmittance in the lower output. However, the case for the even-like mode is totally contrary. These results hold great promise for many application fields such as signal transmission, optical modulation, and the design of topological devices.
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