• Photonics Research
  • Vol. 13, Issue 4, 1010 (2025)
Qianwen Jia1, Junhong Deng2, Anwen Jiang1, Guoxia Yang1..., Fengzhao Cao1, Min Ni1, Jiayi Zhang1, Yihe Li1, Haojie Li1,3, Dahe Liu1, Guixin Li4 and Jinwei Shi1,*|Show fewer author(s)
Author Affiliations
  • 1Applied Optics Beijing Area Major Laboratory and Key Laboratory of Multiscale Spin Physics, Ministry of Education, School of Physics and Astronomy, Beijing Normal University, Beijing 100875, China
  • 2Shenzhen Institute for Quantum Science and Engineering, Southern University of Science and Technology, Shenzhen 518055, China
  • 3School of Physics and Optoelectronic Engineering, Shandong University of Technology, Zibo 255000, China
  • 4Department of Materials Science and Engineering, Southern University of Science and Technology, Shenzhen 518055, China
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    DOI: 10.1364/PRJ.553211 Cite this Article Set citation alerts
    Qianwen Jia, Junhong Deng, Anwen Jiang, Guoxia Yang, Fengzhao Cao, Min Ni, Jiayi Zhang, Yihe Li, Haojie Li, Dahe Liu, Guixin Li, Jinwei Shi, "Reusable high-Q plasmonic metasurface," Photonics Res. 13, 1010 (2025) Copy Citation Text show less

    Abstract

    Metallic nanostructures supporting surface plasmons are crucial for various ultrathin photonic devices. However, these applications are often limited by inherent metallic losses. Significant efforts have been made to achieve high quality-factor (Q-factor) resonances in plasmonic metasurfaces, particularly through surface lattice resonances (SLRs) and bound states in the continuum (BICs). Despite these advances, a direct comparison between these two mechanisms remains unexplored. Here, we report a reusable plasmonic metasurface that supports multiple high-Q resonances by leveraging hybrid plasmonic–photonic modes. By systematically tuning the lattice constant and dielectric cladding thickness, we achieve substantial Q-factor enhancements of both SLRs and BICs in a monolithic device with a small footprint of 200μm×200μm by using an incoherent light source. A direct comparison between these two resonances is also discussed. This high-Q performance holds significant promise for applications in sensing, lasing, and nonlinear and quantum optics, paving the way for the development of next-generation nanophotonic devices.
    H=[ELSPRiγ1gstrgstrgstrERA1iγ2gbgiγ2γ3gstrgbgiγ2γ3ERA1iγ3],

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    Ea=E2gbg,

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    Eb=E1+E2+gbgi(2γ2+γ1)[E2E1+gbgi(2γ2γ1)]2+8gstr22,

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    Ec=E1+E2+gbgi(2γ2+γ1)+[E2E1+gbgi(2γ2γ1)]2+8gstr22.

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    ωRA=±cnRA(k±2πPy),

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    ωWGM=cnWGM(mπLcav)2+(k±2πPy)2,

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    Qianwen Jia, Junhong Deng, Anwen Jiang, Guoxia Yang, Fengzhao Cao, Min Ni, Jiayi Zhang, Yihe Li, Haojie Li, Dahe Liu, Guixin Li, Jinwei Shi, "Reusable high-Q plasmonic metasurface," Photonics Res. 13, 1010 (2025)
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