Author Affiliations
1College of Information Engineering, Quzhou College of Technology, Quzhou 32400, China2Laboratory of Opto-Electronics Technology, College of Electronic Information and Control Engineering, Beijing University of Technology, Beijing 100124, Chinashow less
Fig. 1. (Color online) The proposed hybrid nanostructure to broaden graphene absorption bandwidth.
Fig. 2. (Color online) The absorption spectra of monolayer graphene in the wavelength range from 0.8 to 1.8 μm under normal incidence. Structure parameters: P = 0.7 μm, s = 0.05 μm, h = 0.02 μm, d = 0.02 μm, hs = 0.1 μm.
Fig. 3. (Color online) Distribution of magnetic field at different resonance wavelengths on the xoz plane. Structure parameters: P = 0.7 μm, s = 0.05 μm, h = 0.02 μm, d = 0.02 μm, hs = 0.1 μm.
Fig. 4. (Color online) Effect of grating width on absorption peaks. Structure parameters: P = 0.7 μm, s = 0.05 μm, h = 0.02 μm, d = 0.02 μm, hs = 0.1 μm.
Fig. 5. (Color online) Effect of SiO2 spacer thickness on absorption peaks. Structure parameters: P = 0.7 μm, s = 0.05 μm, h = 0.02 μm, hs = 0.1 μm, w1 = 0.14 μm, w2 = 0.16 μm, w3 = 0.18 μm.
Fig. 6. (Color online) Effect of grating spacing on absorption peaks. Structure parameters: P = 0.7 μm, d = 0.02 μm, h = 0.02 μm, hs = 0.1 μm, w1 = 0.14 μm, w2 = 0.16 μm, w3 = 0.18 μm.