• Photonics Research
  • Vol. 10, Issue 9, 2215 (2022)
Harry Miyosi Silalahi1, Wei-Fan Chiang2, Yi-Hong Shih2, Wan-Yi Wei1, Jou-Yu Su1, and Chia-Yi Huang1、*
Author Affiliations
  • 1Department of Applied Physics, Tunghai University, Taichung 40704, China
  • 2Department of Photonics, Taiwan Cheng Kung University, Tainan 70101, China
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    DOI: 10.1364/PRJ.465746 Cite this Article Set citation alerts
    Harry Miyosi Silalahi, Wei-Fan Chiang, Yi-Hong Shih, Wan-Yi Wei, Jou-Yu Su, Chia-Yi Huang. Folding metamaterials with extremely strong electromagnetic resonance[J]. Photonics Research, 2022, 10(9): 2215 Copy Citation Text show less
    (a) Design of folding metamaterial. The folding metamaterial comprises SRRs with nano-profiles. (b) Geometrical dimensions of folding and common metamaterials. (c) Illustration of biosensor based on folding metamaterial.
    Fig. 1. (a) Design of folding metamaterial. The folding metamaterial comprises SRRs with nano-profiles. (b) Geometrical dimensions of folding and common metamaterials. (c) Illustration of biosensor based on folding metamaterial.
    Scanning electron microscope images of folding metamaterial with height of 20.7 μm at (a) 45° and (b) 80° angles of incidence. Scanning electron microscope images of common metamaterial with height of 500 nm at (c) 45° and (d) 80° angles of incidence.
    Fig. 2. Scanning electron microscope images of folding metamaterial with height of 20.7 μm at (a) 45° and (b) 80° angles of incidence. Scanning electron microscope images of common metamaterial with height of 500 nm at (c) 45° and (d) 80° angles of incidence.
    (a) Experimental (solid lines) and simulated (dashed lines) spectra of folding and common metamaterials. (b) Surface current distributions of SRRs with and without nano-profiles. (c) Theoretical models of SRRs with and without nano-profiles.
    Fig. 3. (a) Experimental (solid lines) and simulated (dashed lines) spectra of folding and common metamaterials. (b) Surface current distributions of SRRs with and without nano-profiles. (c) Theoretical models of SRRs with and without nano-profiles.
    (a) Near-field distributions of SRRs with and without nano-profiles. (b) Experimental spectra of fluidic cells with folding metamaterials at various heights (h) of SRRs.
    Fig. 4. (a) Near-field distributions of SRRs with and without nano-profiles. (b) Experimental spectra of fluidic cells with folding metamaterials at various heights (h) of SRRs.
    (a) Experimental spectra of fluidic sample with folding metamaterial imbedded into air and rabbit-blood layers. The green curve is the terahertz spectrum of the rabbit-blood sample without a metamaterial. (b) Experimental spectra of fluidic sample with common metamaterial imbedded into air and rabbit-blood layers.
    Fig. 5. (a) Experimental spectra of fluidic sample with folding metamaterial imbedded into air and rabbit-blood layers. The green curve is the terahertz spectrum of the rabbit-blood sample without a metamaterial. (b) Experimental spectra of fluidic sample with common metamaterial imbedded into air and rabbit-blood layers.
    Fabrication of (a) folding and (b) common metamaterials.
    Fig. 6. Fabrication of (a) folding and (b) common metamaterials.
    Simulated spectra of the folding and solid metamaterials with a thickness of 20.7 μm. The insets present the simulated models and surface current distributions of folding and solid metamaterials.
    Fig. 7. Simulated spectra of the folding and solid metamaterials with a thickness of 20.7 μm. The insets present the simulated models and surface current distributions of folding and solid metamaterials.
    TypeResonance Frequency (THz)Resonance Transmittance (dB)Δf3dB (THz)Quality Factor
    Sim.Exp.Sim.Exp.Sim.Exp.Sim.Exp.
    Folding0.7900.776−53−490.0060.021131.737.0
    Common0.6500.654−26−250.0080.05581.311.9
    Table 1. Comparison of Simulated and Experimental Data of Folding and Common Metamaterials
    Harry Miyosi Silalahi, Wei-Fan Chiang, Yi-Hong Shih, Wan-Yi Wei, Jou-Yu Su, Chia-Yi Huang. Folding metamaterials with extremely strong electromagnetic resonance[J]. Photonics Research, 2022, 10(9): 2215
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