• Laser & Optoelectronics Progress
  • Vol. 58, Issue 21, 2116002 (2021)
Ting Zhang*, Ting Zhang*, Sen Yang, Sen Yang, XinYing Yu, XinYing Yu
Author Affiliations
  • Shanxi Vocational University of Engineering Science and Technology, Jinzhong , Shanxi 030619, China
  • show less
    DOI: 10.3788/LOP202158.2116002 Cite this Article Set citation alerts
    Ting Zhang, Ting Zhang, Sen Yang, Sen Yang, XinYing Yu, XinYing Yu. Tunable Broadband Terahertz Perfect Absorber Design Based on Vanadium Dioxide[J]. Laser & Optoelectronics Progress, 2021, 58(21): 2116002 Copy Citation Text show less
    Schematics of broadband terahertz metamaterial structure. (a) Schematic of cell array; (b) top view of cell structure
    Fig. 1. Schematics of broadband terahertz metamaterial structure. (a) Schematic of cell array; (b) top view of cell structure
    Schematics of broadband terahertz metamaterial structure. (a) Schematic of cell array; (b) top view of cell structure
    Fig. 1. Schematics of broadband terahertz metamaterial structure. (a) Schematic of cell array; (b) top view of cell structure
    Variations of absorptivity of the absorber, as well as the real and imaginary parts of permittivity of VO2 with conductivity. (a) Absorptivity; (b) real part of permittivity; (c) imaginary part of permittivity
    Fig. 2. Variations of absorptivity of the absorber, as well as the real and imaginary parts of permittivity of VO2 with conductivity. (a) Absorptivity; (b) real part of permittivity; (c) imaginary part of permittivity
    Variations of absorptivity of the absorber, as well as the real and imaginary parts of permittivity of VO2 with conductivity. (a) Absorptivity; (b) real part of permittivity; (c) imaginary part of permittivity
    Fig. 2. Variations of absorptivity of the absorber, as well as the real and imaginary parts of permittivity of VO2 with conductivity. (a) Absorptivity; (b) real part of permittivity; (c) imaginary part of permittivity
    Absorption curves of metamaterial perfect absorbers with and without VO2 under various SiO2 thicknesses
    Fig. 3. Absorption curves of metamaterial perfect absorbers with and without VO2 under various SiO2 thicknesses
    Absorption curves of metamaterial perfect absorbers with and without VO2 under various SiO2 thicknesses
    Fig. 3. Absorption curves of metamaterial perfect absorbers with and without VO2 under various SiO2 thicknesses
    Variations of real and imaginary parts of relative impedance under different VO2 conductivities. (a) Real part; (b) imaginary part
    Fig. 4. Variations of real and imaginary parts of relative impedance under different VO2 conductivities. (a) Real part; (b) imaginary part
    Variations of real and imaginary parts of relative impedance under different VO2 conductivities. (a) Real part; (b) imaginary part
    Fig. 4. Variations of real and imaginary parts of relative impedance under different VO2 conductivities. (a) Real part; (b) imaginary part
    Electric field intensity at two nearly perfect absorption peaks. (a) f1=0.82 THz; (b) f2=1.6 THz
    Fig. 5. Electric field intensity at two nearly perfect absorption peaks. (a) f1=0.82 THz; (b) f2=1.6 THz
    Electric field intensity at two nearly perfect absorption peaks. (a) f1=0.82 THz; (b) f2=1.6 THz
    Fig. 5. Electric field intensity at two nearly perfect absorption peaks. (a) f1=0.82 THz; (b) f2=1.6 THz
    Variations of absorptivity with incident angle and polarization angel. (a) Variation of absorptivity with incident angle at TE mode; (b) variation of absorptivity with incident angle at TM mode; (c) variation of absorptivity with polarization angles at TE mode
    Fig. 6. Variations of absorptivity with incident angle and polarization angel. (a) Variation of absorptivity with incident angle at TE mode; (b) variation of absorptivity with incident angle at TM mode; (c) variation of absorptivity with polarization angles at TE mode
    Variations of absorptivity with incident angle and polarization angel. (a) Variation of absorptivity with incident angle at TE mode; (b) variation of absorptivity with incident angle at TM mode; (c) variation of absorptivity with polarization angles at TE mode
    Fig. 6. Variations of absorptivity with incident angle and polarization angel. (a) Variation of absorptivity with incident angle at TE mode; (b) variation of absorptivity with incident angle at TM mode; (c) variation of absorptivity with polarization angles at TE mode
    Ting Zhang, Ting Zhang, Sen Yang, Sen Yang, XinYing Yu, XinYing Yu. Tunable Broadband Terahertz Perfect Absorber Design Based on Vanadium Dioxide[J]. Laser & Optoelectronics Progress, 2021, 58(21): 2116002
    Download Citation