• Chinese Optics Letters
  • Vol. 20, Issue 1, 013602 (2022)
Ziyu Liu1, Limei Qi1、2、*, Feng Lan3, Chuwen Lan4、5, Jun Yang1, and Xiang Tao1
Author Affiliations
  • 1School of Electronic Engineering, Beijing University of Posts and Telecommunications, Beijing 100876, China
  • 2Collaborative Innovation Center of Light Manipulations and Applications, Shandong Normal University, Jinan 250358, China
  • 3The Yangtze Delta Region Institute (Huzhou), University of Electronic Science and Technology of China, Huzhou 313001, China
  • 4Shenzhen Research Institute, Beijing University of Posts and Telecommunications, Shenzhen 518000, China
  • 5School of Information and Communication Engineering, Beijing University of Posts and Telecommunications, Beijing 100876, China
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    DOI: 10.3788/COL202220.013602 Cite this Article Set citation alerts
    Ziyu Liu, Limei Qi, Feng Lan, Chuwen Lan, Jun Yang, Xiang Tao. A VO2 film-based multifunctional metasurface in the terahertz band[J]. Chinese Optics Letters, 2022, 20(1): 013602 Copy Citation Text show less
    (a) Sketch view and (b) unit cell of the proposed multifunctional device.
    Fig. 1. (a) Sketch view and (b) unit cell of the proposed multifunctional device.
    (a) Scheme of the dual-band EIT and linear-to-circular polarization converter. (b) Transmission curves for the metasurface with the double L (black solid), the small L (blue dotted), and the large L (red dashed) shapes when VO2 is in the insulating state. The cross symbol denotes the fitted result based on the “two-particle” model. (c) The surface current distribution at the two transmission peaks.
    Fig. 2. (a) Scheme of the dual-band EIT and linear-to-circular polarization converter. (b) Transmission curves for the metasurface with the double L (black solid), the small L (blue dotted), and the large L (red dashed) shapes when VO2 is in the insulating state. The cross symbol denotes the fitted result based on the “two-particle” model. (c) The surface current distribution at the two transmission peaks.
    (a) Reflection of Ryy and Rxy. (b) The phase and phase difference for the reflection of Ryy and Rxy. (c) The calculated ellipticity of the polarization conversion.
    Fig. 3. (a) Reflection of Ryy and Rxy. (b) The phase and phase difference for the reflection of Ryy and Rxy. (c) The calculated ellipticity of the polarization conversion.
    Sketch map of the planar-array antenna and elements of each column.
    Fig. 4. Sketch map of the planar-array antenna and elements of each column.
    (a) Transmission and (c) phase of cross polarization for VO2 in the insulating state. (b) Reflection and (d) phase of co-polarization for VO2 in the metallic state.
    Fig. 5. (a) Transmission and (c) phase of cross polarization for VO2 in the insulating state. (b) Reflection and (d) phase of co-polarization for VO2 in the metallic state.
    (a) Three- and (b) two-dimensional radiation pattern of the reflected beam. (c) Three- and (d) two-dimensional radiation pattern of the transmitted beam for VO2 in the insulating state.
    Fig. 6. (a) Three- and (b) two-dimensional radiation pattern of the reflected beam. (c) Three- and (d) two-dimensional radiation pattern of the transmitted beam for VO2 in the insulating state.
    (a) Three- and (b) two-dimensional radiation pattern of the reflected beam when VO2 is in the metallic state.
    Fig. 7. (a) Three- and (b) two-dimensional radiation pattern of the reflected beam when VO2 is in the metallic state.
    L1L2W1W2G
    125155253060
    Table 1. Parameters of EIT and Polarization Convertera
    L1L2W1W2G
    145125302515
    Table 2. Parameters of Planar-Array Antennaa
    Ziyu Liu, Limei Qi, Feng Lan, Chuwen Lan, Jun Yang, Xiang Tao. A VO2 film-based multifunctional metasurface in the terahertz band[J]. Chinese Optics Letters, 2022, 20(1): 013602
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