“…2, both co-and cross-polarized components of the far-field are symmetrical to the direction θ = θ m = 0 • . Here θ m is the main beam direction and its definition is the same as in [28,44] (i.e., the beam due to the co-polarized component of the electric field only, and for x -directed dipole in the ϕ = 90 • plane this implies E ϕ component). Since the axes of the four constitutive tensors c (i) (c = ε, µ, ξ, η) in case (a) are chosen to be in the same direction (…”