4.8 Article

Plasmonic Nanocrystal Arrays on Photonic Crystals with Tailored Optical Resonances

Journal

ACS APPLIED MATERIALS & INTERFACES
Volume 12, Issue 33, Pages 37657-37669

Publisher

AMER CHEMICAL SOC
DOI: 10.1021/acsami.0c05596

Keywords

plasmonic-photonic microsphere; photonic stop band; slow light effect; localized surface plasmon resonance; surface-enhanced Raman spectroscopy

Funding

  1. National Key Research & Development Program of China [2016YFB0401502]
  2. Special Fund Project of Science and Technology Application in Guangdong [2017B020240002]
  3. Science and Technology Program of Guangzhou [2019050001]
  4. Pioneers in Healthcare voucher (project Ischemia on chip) of the University of Twente
  5. MST
  6. ZGT in the Netherlands
  7. Oversea study of Guangzhou Elite Project support in China
  8. NWA Startup Quantum NanoKeys grant [40017607]
  9. Alexander von Humboldt Foundation
  10. German Science Foundation [EXC-2082/1-390761711]

Ask authors/readers for more resources

Hierarchical plasmonic-photonic microspheres (PPMs) with high controllability in their structures and optical properties have been explored toward surface-enhanced Raman spectroscopy. The PPMs consist of gold nanocrystal (AuNC) arrays (3rd-tier) anchored on a hexagonal nanopattern (2nd-tier) assembled from silica nanoparticles (SiO(2)NPs) where the uniform microsphere backbone is termed the 1st-tier. The PPMs sustain both photonic stop band (PSB) properties, resulting from periodic SiO2NP arrangements of the 2nd-tier, and a surface plasmon resonance (SPR), resulting from AuNC arrays of the 3rd-tier. Thanks to the synergistic effects of the photonic crystal (PC) structure and the AuNC array, the electromagnetic (EM) field in such a multiscale composite structure can tremendously be enhanced at certain wavelengths. These effects are demonstrated by experimentally evaluating the Raman enhancement of benzenethiol (BT) as a probe molecule and are confirmed via numerical simulations. We achieve a maximum SERS enhancement factor of up to similar to 10(8) when the resonances are tailored to coincide with the excitation wavelength by suitable structural modifications.

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