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利用超表面的时间不连续性控制表面波。

Controlling surface waves with temporal discontinuities of metasurfaces.

作者信息

Wang Xuchen, Mirmoosa Mohammad S, Tretyakov Sergei A

机构信息

Institute of Nanotechnology, Karlsruhe Institute of Technology, Karlsruhe, Germany.

Department of Electronics and Nanoengineering, Aalto University, Espoo, Finland.

出版信息

Nanophotonics. 2023 Jan 24;12(14):2813-2822. doi: 10.1515/nanoph-2022-0685. eCollection 2023 Jul.

Abstract

Static reactive metasurfaces allow excitation and propagation of surface waves. In this paper, we theoretically elucidate how surface-wave propagation along a reactive boundary is affected by temporal discontinuities of effective parameters characterizing the boundary. First, we show that by switching the value of the surface reactance, the velocity of surface waves is fully controlled, and the power of reflected and transmitted surface waves can be amplified. Second, we indicate that when a boundary supporting waves with transverse-electric polarization is switched to the one allowing only transverse-magnetic polarization, the propagating surface wave is "frozen" and converted to a static magnetic-field distribution. Moreover, efficiently, these fields can be "melted", restoring propagating surface waves when the boundary is switched back to the initial state. Finally, we demonstrate that temporal jumps of the boundary reactance couple free-space propagating waves to the surface wave, in an analogy to a spatial prism. All these intriguing phenomena enabled by temporal discontinuities of effective properties of reactive metasurfaces open up interesting possibilities for the generation and control of surface waves.

摘要

静态反应性超表面允许表面波的激发和传播。在本文中,我们从理论上阐明了沿反应性边界的表面波传播是如何受到表征该边界的有效参数的时间不连续性影响的。首先,我们表明,通过切换表面电抗的值,可以完全控制表面波的速度,并且可以放大反射和透射表面波的功率。其次,我们指出,当支持横向电偏振波的边界切换到仅允许横向磁偏振的边界时,传播的表面波会“冻结”并转换为静态磁场分布。此外,有效地,当边界切换回初始状态时,这些场可以“融化”,恢复传播的表面波。最后,我们证明,边界电抗的时间跃变将自由空间传播波耦合到表面波,这类似于空间棱镜。反应性超表面有效特性的时间不连续性所带来的所有这些有趣现象,为表面波的产生和控制开辟了有趣的可能性。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6bd7/11501961/d322c849835f/j_nanoph-2022-0685_fig_001.jpg

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