Review Article

Applications of Hyperbolic Metamaterial Substrates

Figure 3

(a) Dispersion of the dielectric constants in a practical multilayer semiconductor realization of the HMM. Note the broadband region in which type I HMM response is achieved. (b) Exact numerical calculation (neglecting loss) in the multilayer structure showing the Bloch high- mode and coupled surface plasmons at the interfaces. (c) Evanescent wave incident on an effective medium slab couples to the high- mode and is transmitted. In contrast, the evanescent wave decays away in vacuum.
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