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等离子体变色纳米腔动态光色切换

Plasmochromic Nanocavity Dynamic Light Color Switching.

作者信息

Hopmann Eric, Elezzabi Abdulhakem Y

机构信息

Ultrafast Optics and Nanophotonics Laboratory, Department of Electrical and Computer Engineering, University of Alberta, Edmonton, Alberta, T6G 2V4, Canada.

出版信息

Nano Lett. 2020 Mar 11;20(3):1876-1882. doi: 10.1021/acs.nanolett.9b05088. Epub 2020 Feb 14.

Abstract

Static plasmonic metal-insulator-nanohole (MIN) cavities have been shown to create high chromaticity spectral colors for display applications. While on-off switching of said devices has been demonstrated, introducing active control over the spectral color of a single cavity is an ongoing challenge. Electrochromic oxides such as tungsten oxide (WO) offer the possibility to tune their refractive index (2.1-1.8) and extinction (0-0.5) upon ion insertion, allowing active control over resonance conditions for MIN based devices. In combination with the dynamic change in the WO layer, the utilization of a plasmonic superstructure allows creation of well-defined spectral reflection of the nanocavity. Here, we employ inorganic, electrochromic WO as the tunable dielectric in a MIN nanocavity, resulting in a theoretically achievable resonance wavelength modulation from 601 to 505 nm, while maintaining 35% of reflectance intensity. Experimental values for the spectral modulation result in a 64 nm shift of peak wavelength with high reproducibility and fast switching speed. Remarkably, the introduced device shows electrochemical stability over 100 switching cycles while most of the intercalated charge can be regained (91.1%), leading to low power consumption (5.6 mW/cm).

摘要

静态等离子体金属-绝缘体-纳米孔(MIN)腔已被证明可为显示应用创造高色度光谱颜色。虽然上述器件的开关切换已得到证实,但对单个腔的光谱颜色进行主动控制仍是一个持续存在的挑战。诸如氧化钨(WO)之类的电致变色氧化物提供了在离子插入时调节其折射率(2.1 - 1.8)和消光(0 - 0.5)的可能性,从而能够对基于MIN的器件的共振条件进行主动控制。结合WO层中的动态变化,等离子体超结构的利用允许创建纳米腔定义明确的光谱反射。在这里,我们将无机电致变色WO用作MIN纳米腔中的可调电介质,理论上可实现共振波长从601 nm调制到505 nm,同时保持35%的反射强度。光谱调制的实验值导致峰值波长有64 nm的位移,具有高重现性和快速切换速度。值得注意的是,引入的器件在100个切换周期内显示出电化学稳定性,同时大部分插入电荷可以恢复(91.1%),从而实现低功耗(5.6 mW/cm²)。

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