4.8 Article

Fourier-Engineered Plasmonic Lattice Resonances

期刊

ACS NANO
卷 16, 期 4, 页码 5696-5703

出版社

AMER CHEMICAL SOC
DOI: 10.1021/acsnano.1c10710

关键词

plasmonics; metasurfaces; lattice resonances; nanoparticle arrays; nanophotonics

资金

  1. Canada First Research Excellence Fund
  2. Canada Research Chairs program
  3. China Scholarship Council
  4. Academy of Finland [320165]
  5. Alexander von Humboldt Foundation through the Feodor Lynen Return Research Fellowship
  6. Natural Sciences and Engineering Research Council of Canada (NSERC) [RGPIN/2017-06880, RGPIN/2020-03989, 950-231657, STPGP/521619-2018]

向作者/读者索取更多资源

This study introduces the concept of Fourier lattice resonances (FLRs) and achieves complete control over the transmission spectrum of a metasurface by flexibly placing resonances. Based on standard lithographic fabrication methods, metasurfaces suitable for various optical cavity applications can be designed and manufactured.
Resonances in optical systems are useful for many applications, such as frequency comb generation, optical filtering, and biosensing. However, many of these applications are difiicult to implement in optical metasurfaces because traditional approaches for designing multiresonant nanostructures require significant computational and fabrication efforts. To address this challenge, we introduce the concept of Fourier lattice resonances (FLRs) in which multiple desired resonances can be chosen a priori and used to dictate the metasurface design. Because each resonance is supported by a distinct surface lattice mode, each can have a high quality factor. Here, we experimentally demonstrate several metasurfaces with flexibly placed resonances (e.g., at 1310 and 1550 nm) and Q-factors as high as 800 in a plasmonic platform. This flexible procedure requires only the computation of a single Fourier transform for its design, and is based on standard lithographic fabrication methods, allowing one to design and fabricate a metasurface to fit any specific, optical-cavity-based application. This work represents a step toward the complete control over the transmission spectrum of a metasurface.

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