• Laser & Optoelectronics Progress
  • Vol. 59, Issue 17, 1716003 (2022)
Nanning Yi, Rong Zong, and Rongrong Qian*
Author Affiliations
  • School of Information, Yunnan University, Kunming 650500, Yunnan , China
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    DOI: 10.3788/LOP202259.1716003 Cite this Article Set citation alerts
    Nanning Yi, Rong Zong, Rongrong Qian. Broadband Switchable Bifunction Terahertz Polarization Converter Based on Dirac Semimetal[J]. Laser & Optoelectronics Progress, 2022, 59(17): 1716003 Copy Citation Text show less
    Structure of the switchable bifunction polarization converter. (a) Perspective view; (b) top view; (c) side view of the unit cell
    Fig. 1. Structure of the switchable bifunction polarization converter. (a) Perspective view; (b) top view; (c) side view of the unit cell
    Dielectric constants of BDS at different Fermi energy levels. (a) Real part; (b) imaginary part
    Fig. 2. Dielectric constants of BDS at different Fermi energy levels. (a) Real part; (b) imaginary part
    Simulation results when BDS are used as QWP. (a) Reflection coefficient of co-polarization and cross-polarization; (b) phase and phase difference corresponding to reflection coefficient; (c) decomposition diagram of incident wave vector; (d) phase and phase corresponding to reflection coefficient in u-v coordinate system; (e) ellipticity
    Fig. 3. Simulation results when BDS are used as QWP. (a) Reflection coefficient of co-polarization and cross-polarization; (b) phase and phase difference corresponding to reflection coefficient; (c) decomposition diagram of incident wave vector; (d) phase and phase corresponding to reflection coefficient in u-v coordinate system; (e) ellipticity
    Simulation results when BDS are used as HWP. (a) Reflection coefficient and PCR; (b) phase and phase difference corresponding to reflection coefficient in u-v coordinate system
    Fig. 4. Simulation results when BDS are used as HWP. (a) Reflection coefficient and PCR; (b) phase and phase difference corresponding to reflection coefficient in u-v coordinate system
    Current distribution of top resonator and gold film when metasurface are used as QWP. (a) 2.048 THz; (b) 2.693 THz; (c) 3.344 THz
    Fig. 5. Current distribution of top resonator and gold film when metasurface are used as QWP. (a) 2.048 THz; (b) 2.693 THz; (c) 3.344 THz
    Current distribution of top resonator and gold film when metasurface are used as HWP. (a) 2.770 THz; (b) 3.495 THz
    Fig. 6. Current distribution of top resonator and gold film when metasurface are used as HWP. (a) 2.770 THz; (b) 3.495 THz
    Performance of metasurface at different Fermi energy levels. (a) QWP; (b) HWP
    Fig. 7. Performance of metasurface at different Fermi energy levels. (a) QWP; (b) HWP
    Spectra of the metasurface. (a) Spectra in TE mode when metasurface acts as QWP; (b) spectra in TM mode when metasurface acts as QWP; (c) spectra in TE mode when metasurface acts as HWP; (d) spectra in TM mode when metasurface acts as HWP
    Fig. 8. Spectra of the metasurface. (a) Spectra in TE mode when metasurface acts as QWP; (b) spectra in TM mode when metasurface acts as QWP; (c) spectra in TE mode when metasurface acts as HWP; (d) spectra in TM mode when metasurface acts as HWP
    Nanning Yi, Rong Zong, Rongrong Qian. Broadband Switchable Bifunction Terahertz Polarization Converter Based on Dirac Semimetal[J]. Laser & Optoelectronics Progress, 2022, 59(17): 1716003
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