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Resonant Transparency and Non-Trivial Non-Radiating Excitations in Toroidal Metamaterials

机译:环形超材料的共振透明性和非传递性非辐射激发

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摘要

Engaging strongly resonant interactions allows dramatic enhancement of functionalities of many electromagnetic devices. However, resonances can be dampened by Joule and radiation losses. While in many cases Joule losses may be minimized by the choice of constituting materials, controlling radiation losses is often a bigger problem. Recent solutions include the use of coupled radiant and sub-radiant modes yielding narrow asymmetric Fano resonances in a wide range of systems, from defect states in photonic crystals and optical waveguides with mesoscopic ring resonators to nanoscale plasmonic and metamaterial systems exhibiting interference effects akin to electromagnetically-induced transparency. Here we demonstrate theoretically and confirm experimentally a new mechanism of resonant electromagnetic transparency, which yields very narrow isolated symmetric Lorentzian transmission lines in toroidal metamaterials. It exploits the long sought non-trivial non-radiating charge-current excitation based on interfering electric and toroidal dipoles that was first proposed by Afanasiev and Stepanovsky in [J. Phys. A Math. Gen. 28, 4565 (1995)].
机译:进行强共振相互作用可以大大增强许多电磁设备的功能。但是,焦耳和辐射损耗会抑制共振。尽管在许多情况下,通过选择构成材料可以使焦耳损耗最小化,但控制辐射损耗通常是一个更大的问题。最近的解决方案包括使用耦合辐射模式和次辐射模式在各种系统中产生狭窄的不对称Fano共振,从光子晶体的缺陷状态和具有介观环形共振器的光波导到表现出类似于电磁干扰效应的纳米级等离子和超材料系统引起的透明度。在这里,我们从理论上论证并通过实验证实了一种新的共振电磁透明机制,该机制在环形超材料中产生了非常窄的孤立的对称洛伦兹传输线。它利用了长期以来寻求的基于干扰电偶极和环形偶极子的非平凡非辐射电荷电流激励,该激励最初是由Afanasiev和Stepanovsky在[J.物理数学。 Gen.28,4565(1995)]。

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