Fig. 1. Schematic diagram of the GH shift of the reflected beams from the G-BRC. The incident and reflected beams are schematically represented by their respective beam axes.

Fig. 2. (a) Reflectance R and (b) reflection coefficient r as functions of incident angle at different Fermi energies for the TM polarized wave. The normalized electric field profile distributions in the G-BRC (c) without and (d) with the covering of graphene.

Fig. 3. (a) Reflected phase ϕr and (b) reflected GH shift as functions of incident angle at different Fermi energies for the TM polarized wave. (c) Dependence of the reflected GH shift on the Fermi energy EF and the incident angle.

Fig. 4. Numerical simulations of the reflected beam from the G-BRC under different Fermi energies. The red and blue curves denote the incident and reflected probe beams, respectively. Other parameters are the same as in Fig. 2.

Fig. 5. Dependences of the (a) reflected phase ϕr and (b) normalized GH shift on the incident angle at different relaxation times τ of graphene.

Fig. 6. (a) Reflected GH shift as a function of incident angle and dt for the G-BRC in Fig. 1. (b) Reflected GH shift as a function of incident angle and εt for the G-BRC. Other parameters are the same as in Fig. 2.