Wang Ning, Zeisberger Matthias, Huebner Uwe, Giannini Vincenzo, Schmidt Markus A
Leibniz Institute of Photonic Technology, Albert-Einstein-Str. 9, 07745, Jena, Germany.
The Blackett Laboratory, Department of Physics, Imperial College London, London, SW7 2AZ, UK.
Sci Rep. 2019 Feb 27;9(1):2873. doi: 10.1038/s41598-019-39779-x.
Due to unique properties and great design flexibilities, Fano resonances represent one of the most promising optical features mediated by metallic nanostructures, while the excitation of some Fano modes is impossible due to symmetry reasons. The aim of this work is to show that dense lattice arrangements can have a profound impact on the optical properties of nanostructures and, in particular, can enable the excitation of otherwise dark modes. Here, we demonstrate this concept using the example of rectangular arrays of symmetric trimers packed so densely that the coupling between neighbouring unit cells imposes a symmetry break, enabling the excitation of magnetic Fano resonances. We found that in experiments as well as in simulations, electric and magnetic Fano resonances can be simultaneously formed in cases where the inter-trimer distances are sufficiently small. By analysing the transition from an isolated trimer mode into a regime of strong near-field coupling, we show that by modifying the rectangular unit cell lengths due to the symmetry mismatch between lattice and trimer, two types of Fano resonances can be found, especially magnetic Fano resonances with loop-type magnetic field distributions within the centre of each trimer, which can be either enhanced or suppressed. In addition, the influence of the refractive index environment was measured, showing sensitivity values of approximately 300 nm/RIU. Our work provides fundamental insights into the interaction of the lattice and nanostructure response and paves the way towards the observation of novel optical excitations.
由于具有独特的性质和极大的设计灵活性,法诺共振是金属纳米结构介导的最有前途的光学特性之一,然而由于对称性原因,某些法诺模式无法被激发。这项工作的目的是表明密集晶格排列会对纳米结构的光学性质产生深远影响,特别是能够激发原本暗的模式。在这里,我们以紧密排列的对称三聚体矩形阵列为例来证明这一概念,相邻晶胞之间的耦合导致对称性破缺,从而能够激发磁法诺共振。我们发现,在实验和模拟中,当三聚体间距离足够小时,电法诺共振和磁法诺共振能够同时形成。通过分析从孤立三聚体模式到强近场耦合状态的转变,我们表明,由于晶格和三聚体之间的对称性不匹配而改变矩形晶胞长度时,可以发现两种类型的法诺共振,特别是在每个三聚体中心具有环形磁场分布的磁法诺共振,其可以增强或抑制。此外,还测量了折射率环境的影响,显示出约300 nm/RIU的灵敏度值。我们的工作为晶格与纳米结构响应之间的相互作用提供了基本见解,并为观察新型光学激发铺平了道路。