• Chinese Optics Letters
  • Vol. 17, Issue 1, 010501 (2019)
Jinhua Hu1, Jia Fu1, Xiuhong Liu2、*, Danping Ren1, Jijun Zhao1, and Yongqing Huang3、**
Author Affiliations
  • 1School of Information & Electrical Engineering, Hebei University of Engineering, Handan 056038, China
  • 2School of Mathematics & Physics, Hebei University of Engineering, Handan 056038, China
  • 3State Key Laboratory of Information Photonics and Optical Communications, Beijing University of Posts and Telecommunications, Beijing 100876, China
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    DOI: 10.3788/COL201917.010501 Cite this Article Set citation alerts
    Jinhua Hu, Jia Fu, Xiuhong Liu, Danping Ren, Jijun Zhao, Yongqing Huang. Perfect absorption in a monolayer graphene at the near-infrared using a compound waveguide grating by robust critical coupling[J]. Chinese Optics Letters, 2019, 17(1): 010501 Copy Citation Text show less
    Schematic of the graphene-based absorber. (a) Monolayer graphene covered on the top of the CWG with a DBR mirror. (b) Cross-section of the absorber for TE-polarized light at normal incidence.
    Fig. 1. Schematic of the graphene-based absorber. (a) Monolayer graphene covered on the top of the CWG with a DBR mirror. (b) Cross-section of the absorber for TE-polarized light at normal incidence.
    RCWA simulation result and theoretically calculated result of the absorption spectrum for TE polarization light at normal incidence.
    Fig. 2. RCWA simulation result and theoretically calculated result of the absorption spectrum for TE polarization light at normal incidence.
    Electric field amplitude distributions of the graphene-based absorber for TE polarization under normal incidence at the (a) on-resonant wavelength of 1550.8 nm and (b) off-resonant wavelength of 1540 nm.
    Fig. 3. Electric field amplitude distributions of the graphene-based absorber for TE polarization under normal incidence at the (a) on-resonant wavelength of 1550.8 nm and (b) off-resonant wavelength of 1540 nm.
    Absorption spectra in the structure as a function of wavelength and gap G using RCWA. The remaining parameters are set to P=710 nm, W1=200 nm, W2=150 nm, tg=220 nm, and tb=270 nm.
    Fig. 4. Absorption spectra in the structure as a function of wavelength and gap G using RCWA. The remaining parameters are set to P=710nm, W1=200nm, W2=150nm, tg=220nm, and tb=270nm.
    Absorption spectra of the structure as a function of wavelength for different grating thickness tg and slab thickness tb. P=710 nm, W1=200 nm, W2=150 nm, and G=25 nm, (a) tb=270 nm, (b) tg=220 nm.
    Fig. 5. Absorption spectra of the structure as a function of wavelength for different grating thickness tg and slab thickness tb. P=710nm, W1=200nm, W2=150nm, and G=25nm, (a) tb=270nm, (b) tg=220nm.
    G (nm)Eigenvalue NNimag/Nreal
    256.9029-0.0034i4.9254×104
    306.8774-0.0044i6.3977×104
    356.8530-0.0050i7.2702×104
    Table 1. Eigenvalues of TE Eigenmodes Corresponding to Different Gap G
    Jinhua Hu, Jia Fu, Xiuhong Liu, Danping Ren, Jijun Zhao, Yongqing Huang. Perfect absorption in a monolayer graphene at the near-infrared using a compound waveguide grating by robust critical coupling[J]. Chinese Optics Letters, 2019, 17(1): 010501
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