“…A LG beam propagating along the z-axis with orbital angular momentum l and polarization e α can be written in terms of a slowly varying envelope u l,p (r, φ, z) of the electric field as E α,l,p (r, t) = u l,p (r, φ, z) e i(kz−kz 0 −ωt) e α + c.c., (1) with field amplitude mode LG l p (r) ≡ u l,p (r) [2][3][4],…”