“…The second approach requires breaking the spatial inversion symmetry. In this case, the transmission of nonpolarized and circularly/linearly polarized light through a device is Lorentz-reciprocal and can be realized in very diverse systems, e.g., chiral structures, 1,8,9 metallic gratings, 6,10 and dielectric-based meta-devices. 11,12 Moreover, the combination of diffraction or subwavelength gratings with one-or two-dimensional photonic crystals, 2,5,13 near-zero-index metastructures, [14][15][16][17] and hyperbolic metamaterials (HMMs) 18 can also lead to the observation of AT for linearly polarized light in the resulting hybrid structures.…”