• Chinese Journal of Lasers
  • Vol. 50, Issue 6, 0613001 (2023)
Yuting Chen1, Wenrui Xue1、*, Jing Zhang1, Haotian Fan1, and Changyong Li2、3
Author Affiliations
  • 1College of Physics and Electronic Engineering, Shanxi University, Taiyuan 030006, Shanxi , China
  • 2State Key Laboratory of Quantum Optics and Quantum Optics Devices, Institute of Laser Spectroscopy, Shanxi University, Taiyuan 030006, Shanxi , China
  • 3Collaborative Innovation Center of Extreme Optics, Shanxi University, Taiyuan 030006, Shanxi , China
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    DOI: 10.3788/CJL220767 Cite this Article Set citation alerts
    Yuting Chen, Wenrui Xue, Jing Zhang, Haotian Fan, Changyong Li. Infrared Ultra-Wide-Band Absorber Based on VO2, NaF, and TiO2[J]. Chinese Journal of Lasers, 2023, 50(6): 0613001 Copy Citation Text show less
    Schematic of unit structure of infrared ultra-wideband absorber
    Fig. 1. Schematic of unit structure of infrared ultra-wideband absorber
    Dielectric permittivity versus wavelength for TiO2, NaF and VO2. (a) TiO2; (b) NaF; (c) real part of dielectric permittivity of VO2; (d) imaginary part of dielectric permittivity of VO2
    Fig. 2. Dielectric permittivity versus wavelength for TiO2, NaF and VO2. (a) TiO2; (b) NaF; (c) real part of dielectric permittivity of VO2; (d) imaginary part of dielectric permittivity of VO2
    Polarization sensitivity of absorber. (a) Absorptivity versus wavelength for TE wave and TM wave at zero-degree incidence; (b) absorptivity as a function of azimuth angle and wavelength
    Fig. 3. Polarization sensitivity of absorber. (a) Absorptivity versus wavelength for TE wave and TM wave at zero-degree incidence; (b) absorptivity as a function of azimuth angle and wavelength
    Absorptivity as a function of incident angle and wavelength. (a) TM wave; (b) TE wave
    Fig. 4. Absorptivity as a function of incident angle and wavelength. (a) TM wave; (b) TE wave
    Normalized electric and magnetic field profiles in x-y and x-z planes at three absorption peaks p1, p2 and p3 when TE and TM waves are vertically incident. (a) Electric field of TE wave in x-y plane; (b) magnetic field of TE wave in x-y plane; (c) electric and magnetic fields of TE wave in x-z plane; (d) electric field of TM wave in x-y plane; (e) magnetic field of TM wave in x-y plane; (f) electric and magnetic fields of TM wave in x-z plane
    Fig. 5. Normalized electric and magnetic field profiles in x-y and x-z planes at three absorption peaks p1, p2 and p3 when TE and TM waves are vertically incident. (a) Electric field of TE wave in x-y plane; (b) magnetic field of TE wave in x-y plane; (c) electric and magnetic fields of TE wave in x-z plane; (d) electric field of TM wave in x-y plane; (e) magnetic field of TM wave in x-y plane; (f) electric and magnetic fields of TM wave in x-z plane
    Relative impedance of absorber versus wavelength
    Fig. 6. Relative impedance of absorber versus wavelength
    Absorptivity curves and corresponding magnetic field distributions under different structural parameters
    Fig. 7. Absorptivity curves and corresponding magnetic field distributions under different structural parameters
    Effect of conductivity of VO2 on absorption spectrum
    Fig. 8. Effect of conductivity of VO2 on absorption spectrum
    Comparison of absorption effects with and without pattern in TiO2 layer when TE wave is incident
    Fig. 9. Comparison of absorption effects with and without pattern in TiO2 layer when TE wave is incident
    ReferenceAbsorption bandwidthMaximum absorptivity /%Relative bandwidth /%Average absorptivity /%

    Dielectric

    material

    77-14 μm99.357.393.8Ti-Si
    157.5-13.25 μm98.65994Ti-Si
    338-14 μm99.06490Ti-Ge
    348-14 μm99.410094.5Ti-Ge-Si3N4
    350.4-0.7 μm99.554.595.7Au-SiO2
    367-14 μm99.066.791.0Ti-GaAs
    This work12-50 μm99.612496.4TiO2-NaF-VO2-SiO2
    Table 1. Comparison of infrared absorber performances
    Yuting Chen, Wenrui Xue, Jing Zhang, Haotian Fan, Changyong Li. Infrared Ultra-Wide-Band Absorber Based on VO2, NaF, and TiO2[J]. Chinese Journal of Lasers, 2023, 50(6): 0613001
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