Plasmonic lattice Kerker effect in ultraviolet-visible spectral range

V. Gerasimov, A. Ershov, R. G. Bikbaev, I. Rasskazov, I. L. Isaev, P. Semina, A. Kostyukov, V. Zakomirnyi, Sergey P. Polyutov, S. Karpov
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引用次数: 11

Abstract

Mostly forsaken, but revived after the emergence of all-dielectric nanophotonics, the Kerker effect can be observed in a variety of nanostructures from high-index constituents with strong electric and magnetic Mie resonances. Necessary requirement for the existence of a magnetic response limits the use of generally non-magnetic conventional plasmonic nanostructures for the Kerker effect. In spite of this, we demonstrate here for the first time the emergence of the lattice Kerker effect in regular plasmonic Al nanostructures. Collective lattice oscillations emerging from delicate interplay between Rayleigh anomalies and localized surface plasmon resonances both of electric and magnetic dipoles, and electric and magnetic quadrupoles result in suppression of the backscattering in a broad spectral range. Variation of geometrical parameters of Al arrays allows for tailoring lattice Kerker effect throughout UV and visible wavelength ranges, which is close to impossible to achieve using other plasmonic or all-dielectric materials. It is argued that our results set the ground for wide ramifications in the plasmonics and further application of the Kerker effect.
紫外-可见光谱范围内的等离子体晶格Kerker效应
Kerker效应大多被遗忘,但在全介电纳米光子学出现后复活,可以在具有强电和磁Mie共振的高指数成分的各种纳米结构中观察到。磁响应存在的必要条件限制了一般非磁性传统等离子体纳米结构用于克尔效应。尽管如此,我们在这里首次证明了晶格克尔克效应在规则等离子体Al纳米结构中的出现。瑞利异常与电偶极子和磁偶极子、电四极子和磁四极子的局部表面等离子体共振之间的微妙相互作用产生的集体晶格振荡导致了广谱范围内后向散射的抑制。Al阵列几何参数的变化允许在紫外和可见光波长范围内裁剪晶格克尔克效应,这是使用其他等离子体或全介电材料几乎不可能实现的。我们的结果为等离子体动力学的广泛分支和克尔效应的进一步应用奠定了基础。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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