Figure 5
From: Metamaterial Perfect Absorber Analyzed by a Meta-cavity Model Consisting of Multilayer Metasurfaces

Reflection, Ex field and current distributions for lowest three orders FP modes. (a) Simulated reflection spectra for actual MPA structures with the spacer thickness of \({t}_{s1}=0.09\,\mu m\) (1st order: black), \({t}_{s2}={t}_{s1}+{\lambda }_{s}/2=2.06\,\mu m\) (2nd order: red) and \({t}_{s3}={t}_{s1}+{\lambda }_{s}=4.03\,\mu m\) (3rd order: blue). (b) The corresponding reflection spectra for three-layer thin film model with spacer thickness \({t}_{s1}=0.09\,\mu m\), \({t}_{s2}=2.06\,\mu m\) and \({t}_{s3}=4.03\,\mu m\). Top views of current density on the cross-wire and MPG for (c) 1st order, (d) 2nd order and (e) 3rd order MPA. Insets placed on the right side of (c)–(e) show the x-component of electric field \(({E}_{x})\) along z-direction (propagation direction). Current density on the meta-film representing cross-wire and the MGP for (f) 1st order, (g) 2nd order and (h) 3rd order. Insets on the right side of (f)–(h) display \({E}_{x}\) along z-direction for the three-layer thin film structures.