Author Affiliations
1School of Physics and Electronics, Hunan University, Changsha 410082, China2College of Traffic Engineering, Hunan University of Technology, Zhuzhou 412007, China3College of Electrical and Information Engineering, Hunan University, Changsha 410082, Chinashow less
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.
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.
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.
Fig. 4. (a) Frequency dispersion for TM-polarized and TE-polarized waves illuminating obliquely on the absorber and (b) the relevant maximal coherent absorption.
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.
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.
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.