Fig. 1. (a) Schematic diagram of the in-plane spatial and angular shifts of PSHE for LGM. (b) Configuration of glass-air interface coated with ReS₂-graphene HS. The relationships between angular shifts and deflections are Δ_±^x = z_rϕ_±^x. Θ is the rotation angle between the incident light’s polarization plane and the Re-Re chain.

Fig. 2. Differences between in-plane spatial shifts δ_±^x and angular shifts Δ_±^x of LCP and RCP components with different rotation angles Θ, incident angles θ_i, and polarization angles β at the glass-air interface coated with ReS₂-graphene HS or not, near the critical angle θ_c. (a), (b) δ₊^x−δ₋^x; (c), (d) Δ₊^x−Δ₋^x.

Fig. 3. Normalized field distribution |E_rσ|² of the reflected LCP and RCP components at the glass-air interface coated with ReS2-graphene HS for different rotation angles Θ near the critical angle θ_c, with propagation distance z_r = 250 mm, incident angle θ_i = 28.22°, and polarization angle β = 78°. The dashed lines denote the x_r = 0 and y_r = 0, and the solid lines represent the y_r = y_c (y_c is the horizontal position of the reflected beam centroid). (a)–(c) LCP and (d)–(f) RCP components.

Fig. 4. Impacts of topological charge l on the differences between in-plane spatial shifts δ_±^x and angular shifts Δ_±^x of LCP and RCP components with different incident angles θ_i and polarization angles β at the glass-air interface coated with ReS₂-graphene HS for the case of rotation angle Θ = 0°, near the critical angle θ_c. (a), (b) δ₊^x−δ₋^x; (c), (d) Δ₊^x−Δ₋^x.

Fig. 5. Anomalous enhanced in-plane spatial shifts δ_±^x and angular shifts Δ_±^x of PSHE for LGM with different rotation angles Θ, incident angles θ_i, and polarization angles β at the glass-air interface coated with ReS₂-graphene HS, far from the critical angle θ_c. (a)–(c) δ₊^x−δ₋^x; (d)–(f) Δ₊^x−Δ₋^x.

Fig. 6. (a), (c) Magnitude and (b), (d) phase of the terms k₀a, k₀b, and c in Eq. (6) with different incident angles θ_i and polarization angles β at the glass-air interface coated with ReS₂-graphene HS, for LCP component σ = 1 and rotation angle Θ = 0°.