Photonics Research, Volume. 12, Issue 2, 218(2024)

Refractive index sensing based on a twisted nano-kirigami metasurface

Shuqi Qiao1、†, Xiaochen Zhang2、†, Qinghua Liang2, Yang Wang2, Chang-Yin Ji2, Xiaowei Li3, Lan Jiang3, Shuai Feng1, Honglian Guo1,4、*, and Jiafang Li2,5、*
Author Affiliations
  • 1School of Science, Minzu University of China, Beijing 100081, China
  • 2Key Laboratory of Advanced Optoelectronic Quantum Architecture and Measurement (Ministry of Education), Beijing Key Laboratory of Nanophotonics & Ultrafine Optoelectronic Systems, and School of Physics, Beijing Institute of Technology, Beijing 100081, China
  • 3Laser Micro/Nano Fabrication Laboratory, School of Mechanical Engineering, Beijing Institute of Technology, Beijing 100081, China
  • 4e-mail: hlguo@muc.edu.cn
  • 5e-mail: jiafangli@bit.edu.cn
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    Figures & Tables(5)
    Design of the open-loop twisted meta-molecule arrays. (a) Schematic diagram of the 2D meta-molecule with three arms which can be swung by an angle φ. (b) Top-view and side-view (insets) SEM images of the fabricated 2D and 3D meta-molecule arrays on the silica substrate (w). (c) Top-view and side-view SEM images of the fabricated free-standing 3D meta-molecule arrays without the substrate (w/o). (d) Simulated LCP and RCP transmission spectra of the two meta-molecule arrays without the silica substrate. (e) Calculated CD spectra versus the wavelength and φ. (f) Measured CD spectra of the meta-molecule arrays with and without the substrate. The lattice periods of simulated and experimental arrays are 1.2 and 1.4 μm, respectively. Scale bars: 1 μm.
    Analysis of the CD reversal. (a), (b) Top-view electric field distributions of the meta-molecule surfaces for φ=0° (at λ=1272 nm) and φ=80° (at λ=1268 nm) under the normal RCP and LCP light incidence. (c) Schematic diagram of the deformed twisted meta-molecules with φ=0°, φ=40°, and φ=80°. (d) Schematic diagram of the straight meta-molecules with φ=0°, φ=40°, and φ=80°. (e) Calculated CD spectra of straight meta-molecules in (d). Inset: top view of the meta-molecules. Here, the lattice period is 1.2 μm.
    Effect of RI of the symmetrical environmental medium on CD response. (a) CD spectra with different RIs of the environment. (b) Top-view electric field distributions of the meta-molecule surfaces for n=1.0 (at λ=1390 nm) and n=1.5 (at λ=2082 nm) under the normal RCP and LCP light incidence. (c) Simulated resonance wavelength versus the RI of the environment. (d) Simulated FoM under different RIs of the environment. Here, the lattice period is 1.4 μm.
    Effect of RIs of the unsymmetrical environmental medium on CD responses. (a) CD spectra with different nsup. (b) Top-view electric field distributions of the meta-molecule surfaces for nsup=1.0 (at λ=1730 nm) and nsup=1.5 (at λ=2070 nm) under the normal RCP and LCP light incidence. (c) Simulated resonance wavelength versus nsup. (d) Simulated FoM with different nsup. The lattice period is 1.4 μm.
    Experimental demonstrations of the RI sensing. (a) Schematic diagram of the experimental flow of RI sensing. (b), (c) Side-view SEM images of the 3D arrays after global irradiation. The lattice period is 1.4 μm. Scale bars: 2.5 μm. (d), (e) Simulated and measured CD spectra with refractive index liquids of different RIs. (f) Simulated and measured resonance wavelength versus the RI of the refractive index liquids with meta-molecules of H=250 and 400 nm, respectively. (g) Simulated CD response of meta-molecule array with different heights. The CD spectra of H=0, 250, and 400 nm are denoted by solid thick lines, solid thin lines, and dashed lines, respectively.
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    Shuqi Qiao, Xiaochen Zhang, Qinghua Liang, Yang Wang, Chang-Yin Ji, Xiaowei Li, Lan Jiang, Shuai Feng, Honglian Guo, Jiafang Li. Refractive index sensing based on a twisted nano-kirigami metasurface[J]. Photonics Research, 2024, 12(2): 218

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    Paper Information

    Category: Nanophotonics and Photonic Crystals

    Received: Oct. 12, 2023

    Accepted: Nov. 21, 2023

    Published Online: Jan. 25, 2024

    The Author Email: Honglian Guo (hlguo@muc.edu.cn), Jiafang Li (jiafangli@bit.edu.cn)

    DOI:10.1364/PRJ.507863

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