Figure 8

(a–d) The electric field distributions of the TJ formed by a BDS-coated dielectric cylinder at Fermi energy of \(E_{F}\) = 55 meV for source rotation angles of (b) 5°, (c) 15°, (d) 25°, and (e) 40° for the TE case. (e–h) The TM counterparts of (a–d). The dashed circles represent the boundary of the cylinder. (i, j) The emergence angle and intensity of the TJ, respectively, as a function of the uniform beam rotation angle.