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利用时间非福斯特超材料结构来捕获和放大电磁波。

Holding and amplifying electromagnetic waves with temporal non-foster metastructures.

作者信息

Pacheco-Peña Victor, Kiasat Yasaman, Solís Diego M, Edwards Brian, Engheta Nader

机构信息

School of Mathematics, Statistics and Physics, Newcastle University, Newcastle Upon Tyne, United Kingdom.

Department of Electrical and Systems Engineering, University of Pennsylvania, Philadelphia, PA, USA.

出版信息

Nat Commun. 2025 Mar 20;16(1):2757. doi: 10.1038/s41467-025-57739-0.

Abstract

We introduce a mechanism that can both hold and amplify electromagnetic waves by rapidly changing the permittivity of the medium during the wave travel from a positive to a dispersionless (i.e. non-Foster) negative value and then back again. The underlying physics behind this phenomenon is theoretically explored by considering plane wave and Gaussian pulse propagation in an unbounded medium. Interestingly, we show that a rapid positive-to-negative temporal change of ε(t) causes the propagation of the wave to stop (observed by a frozen phase in time) while the amplitude of the frozen field exponentially grows. Stepping the permittivity back to the original (or a new) positive value will cause the wave to thaw and resume propagation with the original (or the new) frequency, respectively. We numerically study the case of dipole radiation in such time-varying non-Foster structures. As a possible implementation, we propose a parallel plate waveguide platform loaded with time-dependent media emulating parallel lumped non-Foster negative capacitors. Such non-Foster time-varying structures may open new venues in controlling and manipulating wave-matter interaction.

摘要

我们介绍了一种机制,该机制可以在电磁波传播过程中,通过在波从正值快速变化到无色散(即非福斯特)负值然后再变回正值的过程中快速改变介质的介电常数,来捕获并放大电磁波。通过考虑平面波和高斯脉冲在无界介质中的传播,从理论上探究了这一现象背后的物理原理。有趣的是,我们发现ε(t)从正到负的快速时间变化会导致波的传播停止(通过时间上的冻结相位观察到),而冻结场的幅度呈指数增长。将介电常数变回原始(或新的)正值会使波解冻,并分别以原始(或新的)频率恢复传播。我们对这种时变非福斯特结构中的偶极辐射情况进行了数值研究。作为一种可能的实现方式,我们提出了一种加载有随时间变化介质的平行板波导平台,该介质模拟平行集总非福斯特负电容。这种非福斯特时变结构可能会为控制和操纵波与物质的相互作用开辟新途径。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a7d5/11926376/bd2a2f6e1483/41467_2025_57739_Fig1_HTML.jpg

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