One of the most promising, inexpensive methods for nanostructure fabrication is the nanosphere lithography (NSL). [ 1 -6 ] The simple concept of this technique is to self-assemble a layer (usually a monolayer) of polystyrene spheres (PS) on a fl at substrate. The layer of PS is subsequently used as a shadow mask for evaporation of thin fi lms, e.g., metallic thin fi lms. In the simplest version, NSL employs the self-assembly of a densely packed hexagonal lattice of PS and perpendicular substrate evaporation, which leads after PS removal to a honeycomb array of nano-quasi-triangles. [ 1 ] More complicated patterns and nanoparticle shapes can be obtained if the evaporation angle is statically or dynamically modifi ed. [ 7 ] Here, we demonstrate fabrication of nanoribbon gratings by employing NSL with a very shallow static evaporation. The PS diameter is reduced by ionic etching after the assembly and controls the grating geometry. We use this shallow angle NSL (SANSL) technique to make Au and Fe nanoribbon gratings deposited on transparent substrates.Interaction of gratings with the electromagnetic radiation has been studied extensively since 1902. [ 8 ] Classically, subwavelength metallic gratings are polarizers of the transmitted waves; a wave with electric fi eld polarized perpendicular to the grating lines passes through the grating with little back refl ection. In turn, a wave polarized parallel to the lines is strongly back refl ected. This follows from simple boundary conditions at the perfect metal surface: [ 9 ] the parallel to the metal surface component of the electric fi eld must vanish, but the perpendicular one does not. Thus, the wave polarized parallel to the grating lines cannot pass since it would have to have wavelength λ = 2 d / n (where d is the interline distance and n = 1,2,3..) in order to assure the vanishing fi eld nodes at the metal surfaces of the neighboring grating lines. This cannot happen, since in the subwavelength limit λ > > d . In the optical range, most metals (e.g., Au, Ag) cannot be considered as perfect and thus the above analysis is no longer valid. In this range, some metals can support various plasmonic oscillations, including the surface plasmon polariton (SPP). [ 11 ] The extraordinary optical transmission discovered by Ebbesen et al. [ 12 , 13 ] has been identifi ed as due to the periodicity enabled SPP.Here we study the optical transmission in the visible and infrared frequency ranges through the Au and Fe nanoribbon gratings made by SANSL. At low frequencies (large wavelength λ ) the gratings act as polarizers, as expected. For the non-plasmonic Fe ribbons, this behavior extends into the visible range. For the plasmonic Au ribbons, on the other hand, the tendency reverses in the visible range, with minimum transmission at λ = 600 nm for the perpendicular polarization. We show that this effect is due to excitation of a plasmonic dispersionless mode, with induced charges oscillating perpendicular to the wire axis in each wire.The fi rst step in the SANSL is the prepa...