• Chinese Optics Letters
  • Vol. 19, Issue 8, 081601 (2021)
Jipeng Wu1、2, Jie Tang1, Rongzhou Zeng2, Xiaoyu Dai3, and Yuanjiang Xiang1、*
Author Affiliations
  • 1School of Physics and Electronics, Hunan University, Changsha 410082, China
  • 2College of Traffic Engineering, Hunan University of Technology, Zhuzhou 412007, China
  • 3College of Electrical and Information Engineering, Hunan University, Changsha 410082, China
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    DOI: 10.3788/COL202119.081601 Cite this Article Set citation alerts
    Jipeng Wu, Jie Tang, Rongzhou Zeng, Xiaoyu Dai, Yuanjiang Xiang. Tunable coherent perfect absorption in three-dimensional Dirac semimetal films[J]. Chinese Optics Letters, 2021, 19(8): 081601 Copy Citation Text show less
    Two coherent beams illuminate on the Dirac semimetal film, I+ and I− represent the coherent input beams, O+ and O− correspond to the output lights, the incident angle of the coherent input light is θ, and the thickness of the BDS film is d.
    Fig. 1. Two coherent beams illuminate on the Dirac semimetal film, I+ and I represent the coherent input beams, O+ and O correspond to the output lights, the incident angle of the coherent input light is θ, and the thickness of the BDS film is d.
    (a) Spectra of transmission, reflection, and absorption for Dirac semimetal film illuminated normally by a single TM-polarized beam. (b) The corresponding phase difference of reflection and transmission coefficients.
    Fig. 2. (a) Spectra of transmission, reflection, and absorption for Dirac semimetal film illuminated normally by a single TM-polarized beam. (b) The corresponding phase difference of reflection and transmission coefficients.
    (a) Coherent absorption as a function of frequency and phase difference of the two input beams, and the maximal coherent absorption appears at the frequency of 43.89 THz with zero phase difference. (b) The coherent absorption with the change of phase difference at the frequency of 43.89 THz.
    Fig. 3. (a) Coherent absorption as a function of frequency and phase difference of the two input beams, and the maximal coherent absorption appears at the frequency of 43.89 THz with zero phase difference. (b) The coherent absorption with the change of phase difference at the frequency of 43.89 THz.
    (a) Frequency dispersion for TM-polarized and TE-polarized waves illuminating obliquely on the absorber and (b) the relevant maximal coherent absorption.
    Fig. 4. (a) Frequency dispersion for TM-polarized and TE-polarized waves illuminating obliquely on the absorber and (b) the relevant maximal coherent absorption.
    Regulation of coherent absorption via changing the thickness of BDS thin film for the parameters EF = 0.15 eV, g = 40, Δϕ2 = 0, and θ = 0.
    Fig. 5. Regulation of coherent absorption via changing the thickness of BDS thin film for the parameters EF = 0.15 eV, g = 40, Δϕ2 = 0, and θ = 0.
    Manipulation of coherent absorption by changing the Fermi energy EF, for the parameters g = 40, d = 3.1 µm, Δϕ2 = 0, and θ = 0.
    Fig. 6. Manipulation of coherent absorption by changing the Fermi energy EF, for the parameters g = 40, d = 3.1 µm, Δϕ2 = 0, and θ = 0.
    Coherent absorption spectrum as a function of frequency for different degeneracy factors g, in which g = 40, εb = 1 corresponds to AlCuFe quasi-crystals, g = 24, εb = 6.2 corresponds to Eu2IrO7, and g = 4, εb = 12 corresponds to Na3Bi.
    Fig. 7. Coherent absorption spectrum as a function of frequency for different degeneracy factors g, in which g = 40, εb = 1 corresponds to AlCuFe quasi-crystals, g = 24, εb = 6.2 corresponds to Eu2IrO7, and g = 4, εb = 12 corresponds to Na3Bi.
    Jipeng Wu, Jie Tang, Rongzhou Zeng, Xiaoyu Dai, Yuanjiang Xiang. Tunable coherent perfect absorption in three-dimensional Dirac semimetal films[J]. Chinese Optics Letters, 2021, 19(8): 081601
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