“…For microwave applications, for the topological charges
, the circularly polarized waves can be used for the excitation, which exactly is what the spin–orbital conversion implies. [
17,45 ] On the other hand, for applications where the excitations are realized by guided waves [
29,31 ] (e.g., feeding networks at microwave frequencies and dielectric waveguides at optical frequencies), the first approach would need
phased wave ports, where the phases are determined by the irreps for the
group. The number of wave ports can quickly go up to
for the
(or
) group.…”