• Journal of Infrared and Millimeter Waves
  • Vol. 39, Issue 5, 576 (2020)
Min ZHONG1、* and Xian-Chun SHI2
Author Affiliations
  • 1Hezhou University, Hezhou542899, China
  • 2School of Mechanical Engineering, Anhui University of Science and Technology,Huainan232001, China
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    DOI: 10.11972/j.issn.1001-9014.2020.05.007 Cite this Article
    Min ZHONG, Xian-Chun SHI. Realization of a multiband metamaterial waveguide based on dirac semimetal in the 800~1100nm range[J]. Journal of Infrared and Millimeter Waves, 2020, 39(5): 576 Copy Citation Text show less
    (a) Schematic diagram of the proposed metal–insulator–metal waveguide. The yellow parts are Dirac semimetal layers. The green part is SU-8 layer. The blue part is SiO2. (b) The top layer of the proposed unit cell. (c) The middle layer of the proposed unit cell. (d) The bottom layer of the proposed unit cell. The thickness of SU-8 layer and SiO2 layer is set as 180nm
    Fig. 1. (a) Schematic diagram of the proposed metal–insulator–metal waveguide. The yellow parts are Dirac semimetal layers. The green part is SU-8 layer. The blue part is SiO2. (b) The top layer of the proposed unit cell. (c) The middle layer of the proposed unit cell. (d) The bottom layer of the proposed unit cell. The thickness of SU-8 layer and SiO2 layer is set as 180nm
    (a) The schematic diagram of the proposed structure. (b) Simulated and calculated transmission spectrum of the proposed structure. (c) Schematic diagram of the waveguide without metal reflector layer. (d) Simulated and calculated transmission spectrum of the waveguide without metal reflector layer
    Fig. 2. (a) The schematic diagram of the proposed structure. (b) Simulated and calculated transmission spectrum of the proposed structure. (c) Schematic diagram of the waveguide without metal reflector layer. (d) Simulated and calculated transmission spectrum of the waveguide without metal reflector layer
    (a) The magnetic field intensity distribution at resonance wavelength 842nm. (b) The magnetic field intensity distribution at resonance wavelength 921nm. (c) The magnetic field intensity distribution at resonance wavelength 900nm. (d) The magnetic field intensity distribution at resonance wavelength 950nm
    Fig. 3. (a) The magnetic field intensity distribution at resonance wavelength 842nm. (b) The magnetic field intensity distribution at resonance wavelength 921nm. (c) The magnetic field intensity distribution at resonance wavelength 900nm. (d) The magnetic field intensity distribution at resonance wavelength 950nm
    (a) The magnetic field intensity distribution at resonance wavelength 1010nm. (b) The magnetic field intensity distribution at resonance wavelength 1061nm. (c) The magnetic field intensity distribution at resonance wavelength 1040nm. (d) The magnetic field intensity distribution at resonance wavelength 1080nm
    Fig. 4. (a) The magnetic field intensity distribution at resonance wavelength 1010nm. (b) The magnetic field intensity distribution at resonance wavelength 1061nm. (c) The magnetic field intensity distribution at resonance wavelength 1040nm. (d) The magnetic field intensity distribution at resonance wavelength 1080nm
    The phase spectrum of the proposed structure
    Fig. 5. The phase spectrum of the proposed structure
    (a) The magnetic field intensity distribution of the waveguide without metal reflector layer at resonance wavelength 840nm. (b) The magnetic field intensity distribution of the waveguide without metal reflector layer at resonance wavelength 940nm. (c) The magnetic field intensity distribution of the waveguide without metal reflector layer at resonance wavelength 885nm. (d) The magnetic field intensity distribution of the waveguide without metal reflector layer at resonance wavelength 973nm
    Fig. 6. (a) The magnetic field intensity distribution of the waveguide without metal reflector layer at resonance wavelength 840nm. (b) The magnetic field intensity distribution of the waveguide without metal reflector layer at resonance wavelength 940nm. (c) The magnetic field intensity distribution of the waveguide without metal reflector layer at resonance wavelength 885nm. (d) The magnetic field intensity distribution of the waveguide without metal reflector layer at resonance wavelength 973nm
    Transmission spectrum with different Fermi energy
    Fig. 7. Transmission spectrum with different Fermi energy
    (a) Imaginary parts of the permittivity of Dirac semimetals layers. (b) Real parts of the permittivity of Dirac semimetals layers
    Fig. 8. (a) Imaginary parts of the permittivity of Dirac semimetals layers. (b) Real parts of the permittivity of Dirac semimetals layers
    ParameterPw1L1L2L3L4w2w3
    Value(nm)300301401401101508012
    Table 1. 几何参数
    Min ZHONG, Xian-Chun SHI. Realization of a multiband metamaterial waveguide based on dirac semimetal in the 800~1100nm range[J]. Journal of Infrared and Millimeter Waves, 2020, 39(5): 576
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