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Illustration of Faraday rotation and the unit cells of both uniform and patterned graphene layers.
Rotation angle of the transmitted plane wave versus frequency for a uniform graphene monolayer residing on SiC substrate under different magnetostatic biases, experimental (see Ref. 8) and theoretical.
(a) real part of , (b) imaginary part of , (c) real part of , and (d) imaginary part of in the anisotropic impedance matrix of a magnetically biased graphene monolayer.
Real part of the effective off-diagonal conductivity, proposed physical model versus accurate full-wave approach.
(a) Rotation angle of patterned graphene for different lattice constants and 7 T magnetic bias, with gap length fixed to one-eleventh of the lattice constant, i.e., d = L/11 and (b) Rotation angle of patterned graphene for different gap widths and 7 T magnetic bias with the lattice constant fixed to .
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