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非对称环境下,MIM纳米光栅在正入射时观测到的极窄等离子体表面晶格共振的理论研究。

Theoretical study of extremely narrow plasmonic surface lattice resonances observed by MIM nanogratings under normal incidence in asymmetric environments.

作者信息

Yang Xiuhua, Xia Dunzhu, Li Jinhui

机构信息

Key Laboratory of Micro-Inertial Instrument and Advanced Navigation Technology, Ministry of Education, School of Instrument Science and Engineering, Southeast University, Nanjing 210096, People's Republic of China.

出版信息

Nanotechnology. 2022 Aug 17;33(44). doi: 10.1088/1361-6528/ac84e0.

Abstract

Nanoarray structures can support plasmonic surface lattice resonances (SLRs) with extremely narrow linewidths and huge electric field enhancement features, which are attractive applications in nanolasers, biochemical sensors, and nonlinear optics. However, current nanoarray structures located in an asymmetric dielectric environment with a refractive index contrast of 1.00/1.52 of the superstrate/substrate excite much poorer SLRs under normal incidence, which largely limits their application range. In this work, we report extremely narrow SLRs supported by one-dimensional metal-insulator-metal nanograting in asymmetric dielectric environments. The simulation results show that an SLRs with linewidth of 3.26 nm and quality factor of 233.2 can be excited under normal incidence. This high-quality SLRs is attributed to the interference formation between the out-of-plane dipole resonance mode and the out-of-plane quadrupole resonance mode. We also show that the resonance wavelength and quality factor can be tuned by changing the structure geometry and period, and we calculate the normal incidence SLRs quality factor to be up to 248 in 1.33/1.52 and 250 in 1.45/1.52. We expect the SLRs of this work to find potential applications in asymmetric dielectric environments.

摘要

纳米阵列结构能够支持具有极窄线宽和巨大电场增强特性的表面等离激元晶格共振(SLR),这在纳米激光器、生化传感器和非线性光学等领域具有诱人的应用前景。然而,当前位于上层/下层折射率对比度为1.00/1.52的非对称介电环境中的纳米阵列结构,在正入射下激发的表面等离激元晶格共振效果较差,这在很大程度上限制了它们的应用范围。在这项工作中,我们报道了在非对称介电环境中由一维金属-绝缘体-金属纳米光栅所支持的极窄表面等离激元晶格共振。模拟结果表明,在正入射下能够激发线宽为3.26纳米、品质因数为233.2的表面等离激元晶格共振。这种高质量的表面等离激元晶格共振归因于面外偶极子共振模式与面外四极子共振模式之间的干涉形成。我们还表明,共振波长和品质因数可以通过改变结构几何形状和周期来调节,并且我们计算出在1.33/1.52的情况下正入射表面等离激元晶格共振品质因数高达248,在1.45/1.52的情况下为250。我们期望这项工作中的表面等离激元晶格共振能够在非对称介电环境中找到潜在应用。

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