• Laser & Optoelectronics Progress
  • Vol. 62, Issue 5, 0523001 (2025)
Zherong Yu1,*, Sitong Zhou1, Gongli Xiao1, Hongyan Yang2, and Zanhui Chen1
Author Affiliations
  • 1Key Laboratory of Microelectronic Devices and Integrated Circuits, School of Information and Communication, Guilin University of Electronic Technology, Guilin 541004, Guangxi , China
  • 2School of Optoelectronic Engineering, Guilin University of Electronic Technology, Guilin 541004, Guangxi , China
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    DOI: 10.3788/LOP241414 Cite this Article Set citation alerts
    Zherong Yu, Sitong Zhou, Gongli Xiao, Hongyan Yang, Zanhui Chen. Terahertz Polarization Converter Based on Skew-Coupled Symmetric Cylinder Structure[J]. Laser & Optoelectronics Progress, 2025, 62(5): 0523001 Copy Citation Text show less
    Terahertz polarization converter based on skew-coupled symmetric cylinder structure. (a) 3D structure schematic; (b) 2D structure schematic
    Fig. 1. Terahertz polarization converter based on skew-coupled symmetric cylinder structure. (a) 3D structure schematic; (b) 2D structure schematic
    Reflectance spectra at different gold pillar structures. (a) Single gold pillar; (b) three gold pillars; (c) five gold pillars
    Fig. 2. Reflectance spectra at different gold pillar structures. (a) Single gold pillar; (b) three gold pillars; (c) five gold pillars
    Surface current distribution of the designed structure. (a) Upper pole plate; (b) lower pole plate
    Fig. 3. Surface current distribution of the designed structure. (a) Upper pole plate; (b) lower pole plate
    Reflection spectra and polarization conversion rates of different polarized waves under different long axes of gold columns. (a)‒(c) Reflection spectra at R2=8 µm, R2=12 µm, and R2=16 µm; (d)‒(f) polarization conversion rates at R2=8 µm, R2=12 µm, and R2=16 µm
    Fig. 4. Reflection spectra and polarization conversion rates of different polarized waves under different long axes of gold columns. (a)‒(c) Reflection spectra at R2=8 µm, R2=12 µm, and R2=16 µm; (d)‒(f) polarization conversion rates at R2=8 µm, R2=12 µm, and R2=16 µm
    Electric field distribution under different long axes of gold columns. (a) R2 = 8 µm; (b) R2 = 16 µm
    Fig. 5. Electric field distribution under different long axes of gold columns. (a) R2 = 8 µm; (b) R2 = 16 µm
    Circular polarization reflection spectra, scanning results distribution of R2 parameters, and corresponding polarization conversion rate under different long axes of gold columns. (a) Circularly polarized reflection spectrum at R2=16 µm; (b) distribution of scanning results for R2 parameter; (c) circularly polarized reflection spectra at R2=20 µm; (d) polarization conversion rate
    Fig. 6. Circular polarization reflection spectra, scanning results distribution of R2 parameters, and corresponding polarization conversion rate under different long axes of gold columns. (a) Circularly polarized reflection spectrum at R2=16 µm; (b) distribution of scanning results for R2 parameter; (c) circularly polarized reflection spectra at R2=20 µm; (d) polarization conversion rate
    Ref.Polarization conversion modeFunctionFrequency range /THzMaximum conversion /%
    25Linear-to-linearSingle6.68‒8.6680
    26Linear-to-circularSingle0.70‒1.4180
    27Linear-to-linearSingle1.23‒2.1278
    ProposedLinear-to-linear and linear-to-circularBi-function

    2.40‒4.90

    2.35‒5.21

    96, 92
    Table 1. Comparison of results for different structures
    Zherong Yu, Sitong Zhou, Gongli Xiao, Hongyan Yang, Zanhui Chen. Terahertz Polarization Converter Based on Skew-Coupled Symmetric Cylinder Structure[J]. Laser & Optoelectronics Progress, 2025, 62(5): 0523001
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