Figure 9
(a–d) The electric field distributions of the TJ formed by a BDS-coated dielectric cube with R = 300 μm and dDS = 1.5 μm at Fermi energy of \(E_{F}\) = 55 meV for source rotation angles of (a) 5°, (b) 10°, (c) 20°, and (d) 35° for the TE case. (e–h) The TM counterparts of (a-d). The dashed squares represent the boundary of the cube. (i, j) The output angle and intensity of the TJ, respectively, as a function of the uniform beam rotation angle.
