• Laser & Optoelectronics Progress
  • Vol. 61, Issue 17, 1723002 (2024)
Rui Xing1, Yongzhi Cheng1,3,4,**, Hui Luo1,3,4, Fu Chen1,3,4, and Xiangcheng Li2,3,4,*
Author Affiliations
  • 1School of Information Science and Engineering, Wuhan University of Science and Technology, Wuhan 430081, Hubei, China
  • 2State Key Laboratory of Refractory Materials and Metallurgy, Wuhan University of Science and Technology, Wuhan 430081, Hubei, China
  • 3Key Laboratory of High Temperature Electromagnetic Materials and Structure of MOE, Wuhan University of Science and Technology, Wuhan 430081, Hubei, China
  • 4Hubei Longzhong Laboratory, Xiangyang441000, Hubei, China
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    DOI: 10.3788/LOP232654 Cite this Article Set citation alerts
    Rui Xing, Yongzhi Cheng, Hui Luo, Fu Chen, Xiangcheng Li. Pseudo-Waveform-Selective Metasurface Absorber Based on Linear Circuits[J]. Laser & Optoelectronics Progress, 2024, 61(17): 1723002 Copy Citation Text show less
    PWSMA. (a) Array structure; (b) unit-cell structure; (c) circuit simulation configuration
    Fig. 1. PWSMA. (a) Array structure; (b) unit-cell structure; (c) circuit simulation configuration
    Electromagnetic model and equivalent circuit model. (a) Equivalent circuit model; (b) comparison of absorptance between electromagnetic model and equivalent circuit model
    Fig. 2. Electromagnetic model and equivalent circuit model. (a) Equivalent circuit model; (b) comparison of absorptance between electromagnetic model and equivalent circuit model
    Normalized energy spectra of pulse cosine waves at different pulse widths, and the resonance frequency is set to 3.3 GHz
    Fig. 3. Normalized energy spectra of pulse cosine waves at different pulse widths, and the resonance frequency is set to 3.3 GHz
    Circuit configuration of PWSMA unit-cell and absorptance comparison. (a) Circuit configuration; (b) comparison of absorptance between comparison of continuous wave and short pulse (0.5 ns)
    Fig. 4. Circuit configuration of PWSMA unit-cell and absorptance comparison. (a) Circuit configuration; (b) comparison of absorptance between comparison of continuous wave and short pulse (0.5 ns)
    Absorptance of the incident signal. (a)Absorptance of the incident signal at different pulse widths; (b) absorptance and corresponding Rozanov limit of the incident signal at different pulse widths with a resistance of 377 Ω and a resonant frequency of 3.3 GHz
    Fig. 5. Absorptance of the incident signal. (a)Absorptance of the incident signal at different pulse widths; (b) absorptance and corresponding Rozanov limit of the incident signal at different pulse widths with a resistance of 377 Ω and a resonant frequency of 3.3 GHz
    Continuous wave absorptance at a resistance of 377 Ω. (a) Continuous wave absorptance and Rozanov limit; (b) continuous wave absorptance under different resistance values
    Fig. 6. Continuous wave absorptance at a resistance of 377 Ω. (a) Continuous wave absorptance and Rozanov limit; (b) continuous wave absorptance under different resistance values
    Absorptance of PWSMA loaded with different resistance values at resonant frequency of 3.3 GHz under different incident pulse width signals
    Fig. 7. Absorptance of PWSMA loaded with different resistance values at resonant frequency of 3.3 GHz under different incident pulse width signals
    Rui Xing, Yongzhi Cheng, Hui Luo, Fu Chen, Xiangcheng Li. Pseudo-Waveform-Selective Metasurface Absorber Based on Linear Circuits[J]. Laser & Optoelectronics Progress, 2024, 61(17): 1723002
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