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. 2016 May 5;6:25442. doi: 10.1038/srep25442

Figure 3.

Figure 3

Iso-frequency contour plot of the GhHC (a) at wavenumber 1600 cm−1 where hBN behaves as a Type-II hyperbolic material (b) at wavenumber 800 cm−1 where hBN acts as a Type-I hyperbolic material; thickness of graphene and hBN in the unit cell, d1 = 1 nm and d2 = 100 nm respectively, the chemical potential of graphene, μc = 0.5 eV. (c,d) are the zoomed-in view of the specific zone covered by the dashed lines in Fig. 3(a,b), respectively. The shaded regions indicate the bandgap in k-space where no propagating wave is allowed. (e) Iso-frequency contour plot of a graphene-dielectric multilayer hyperbolic metamaterial; thickness of graphene and dielectric in the unit cell, d1 = 1 nm and d2 = 100 nm respectively, permittivity of the dielectric εd = 2.2, the chemical potential of graphene, μc = 1 eV.