“…One solution for this is to use nondivergent OVs, called high-order Bessel–Gauss beams, which exhibit annihilation reconstruction properties and stability in atmospheric turbulences [ 5 , 8 ]. One can generate diffraction-free OVs with axicons [ 10 , 11 , 12 , 13 , 14 ], either by loading a high-order phase hologram on a spatial light modulator [ 15 , 16 , 17 ], amplitude binary masks [ 15 ], or shaping a Laguerre–Gauss beam with a refractive axicon—a doublet of a real spiral phase plate and a zero-order refractive axicon (with continuous profile) [ 18 ], Pancharatnam–Berry phase elements [ 18 ], a digital micromirrors device [ 19 ], circular Dammann gratings [ 20 ], Mach–Zehnder interferometer [ 21 ], cylindrical waveguides [ 22 ], conformal transformation elements (for OAM detection) [ 23 , 24 , 25 ], or metasurfaces [ 26 , 27 ].…”