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强耦合辐射纳米棒小系统的点偶极近似

Point-dipole approximation for small systems of strongly coupled radiating nanorods.

作者信息

Watson Derek W, Jenkins Stewart D, Fedotov Vassili A, Ruostekoski Janne

机构信息

Mathematical Sciences and Centre for Photonic Metamaterials, University of Southampton, Southampton, SO17 1BJ, United Kingdom.

Optoelectronics Research Centre and Centre for Photonic Metamaterials, University of Southampton, Southampton, SO17 1BJ, United Kingdom.

出版信息

Sci Rep. 2019 Apr 5;9(1):5707. doi: 10.1038/s41598-019-41327-6.

DOI:10.1038/s41598-019-41327-6
PMID:30952960
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC6450961/
Abstract

Systems of closely-spaced resonators can be strongly coupled by interactions mediated by scattered electromagnetic fields. In large systems the resulting response has been shown to be more sensitive to these collective interactions than to the detailed structure of individual resonators. Attempts to describe such systems have resulted in point-dipole approximations to resonators that are computationally efficient for large resonator ensembles. Here we provide a detailed study for the validity of point dipole approximations in small systems of strongly coupled plasmonic nanorods, including the cases of both super-radiant and subradiant excitations, where the characteristics of the excitation depends on the spatial separation between the nanorods. We show that over an appreciable range of rod lengths centered on 210 nm, when the relative separation kl in terms of the resonance wave number of light k satisfies [Formula: see text], the point electric dipole model becomes accurate. However, when the resonators are closer, the finite-size and geometry of the resonators modifies the excitation modes, in particular the cooperative mode line shifts of the point dipole approximation begin to rapidly diverge at small separations. We also construct simplified effective models by describing a pair of nanorods as a single effective metamolecule.

摘要

间距紧密的谐振器系统可通过散射电磁场介导的相互作用实现强耦合。在大型系统中,已证明由此产生的响应对这些集体相互作用比对单个谐振器的详细结构更为敏感。描述此类系统的尝试导致了对谐振器的点偶极近似,这对于大型谐振器集合在计算上是高效的。在此,我们详细研究了强耦合等离子体纳米棒小系统中点偶极近似的有效性,包括超辐射和亚辐射激发的情况,其中激发特性取决于纳米棒之间的空间间距。我们表明,在以210 nm为中心的相当长的棒长度范围内,当以光的共振波数k表示的相对间距kl满足[公式:见正文]时,点电偶极模型变得准确。然而,当谐振器靠得更近时,谐振器的有限尺寸和几何形状会改变激发模式,特别是在小间距下,点偶极近似的协同模式线移开始迅速发散。我们还通过将一对纳米棒描述为单个有效超分子来构建简化的有效模型。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b987/6450961/004250b11c23/41598_2019_41327_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b987/6450961/b5d64dfaa650/41598_2019_41327_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b987/6450961/004250b11c23/41598_2019_41327_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b987/6450961/b5d64dfaa650/41598_2019_41327_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b987/6450961/004250b11c23/41598_2019_41327_Fig5_HTML.jpg

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