has led to significant works on antireflecting coatings [1] or enhanced absorption in thin film photovoltaics. [2] The second is surface plasmon polariton (SPP). SPP describes both an excitation of surface charges and the propagation of an EM field confined at a metal-dielectric interface. This feature can be tuned either by designing an appropriate stack of refractive indices above the metal surface, or by structuring it to produce a grating whose periodicity will control which wavevectors are able to propagate at the interface. Both of these methods were successfully implemented for surface enhanced Raman spectroscopy [3] or increased absorption in organic solar cells. [4] However, one of the drawbacks of surface modification is the cost that comes from the use of processes such as e-beam lithography or milling, or the low yield obtained by certain specific structures with nanometric gaps between metal tips. [5] More recently, a hybrid concept has arisen. Instead of using the LSP coming from nanoparticles embedded into a bulk, or the SPP that appears on a textured metal surface, colloidal nanoparticles are directly deposited upon a metal film. Because they are synthetized and kept in liquid phase, these nanoparticles need to be individually protected by a thin (a few nanometers) shell of surfactant -often polymers, such as polyvinylpyrrolidone (PVP) -to prevent aggregation. Once deposited on a film, this dielectric shell acts as a spacer that creates a metalinsulator-metal (MIM) nanocavity between the particle and the substrate. This design has been shown to couple gap plasmon modes at frequencies related to the width of the particle, the thickness of the gap, and the material used. [6,7] This bottom-up method has two main advantages: i) it is a low-cost technique compared with other e-beam lithography or milling processes and ii) it can create nanometric gaps that are very challenging to design at comparable yield with other approaches. Despite these advantages, it is still difficult to control the thickness of the dielectric spacer with a high degree of accuracy. Indeed, the thickness of the gap is only tuned by washing the colloidal nanoparticles to reduce the amount of PVP that covers them, up to the approximate desired thickness. Since a nanometric difference in cavity thickness results in a resonance shift of about a hundred nanometers, it is crucial to improve control on the cavity geometry if we aim to address specific spectral ranges. In the case of PVP-spaced nanopatch antennas there is furthermore a limit to gaps thicker than 3 nm because of the residual Nanopatch antennas based on the assembly of nanocubes are an appealing way to easily produce structures that feature very thin gaps between metals at a very low cost compared with other surface modification techniques. If these coatings are very good absorbers in the visible and near-infrared range, they can also be of interest for reaching light confinement regimes where nonlocality arises strongly, or for designing molecular electronics junctions e...