the manifold advantages they have over pigmentary methods. Traditional modes of color generation are chemically unstable at high temperatures, subject to bleaching if exposed to intense UV illumination, difficult to dispose of or recycle due to toxic composition, and unsuitable for miniaturized imaging and display devices. [1] In favorable contrast to these methods, metasurfaces have shown to be more robust to chemical deterioration, [2] can deliver high spatial resolution [3] and are potentially more economical and sustainable while still rendering colors that are vibrant and aesthetically gratifying. [4,5] As synthetic composites, metasurfaces can assume a variety of configurations and consist of different combinations of materials such as metals and dielectrics in either nanostructured or thin film forms. The components are specifically selected to create a surface with desired properties. Metasurfaces can produce either transmissive or reflective colors, generated by dielectric components, [6] plasmonic metals, [7,8] or combinations of both. [9] In plasmonic metallic nanoparticles, resonant behavior occurs when incident photons excite surface plasmons at the metal-dielectric interface. This interaction leads to selective filtering of transmitted and reflected light. The strong field enhancement and subwavelength confinement characteristic of this phenomenon have led to the realization of several advancements in structural colors, [1,5] in particular with respect to the delicate balance between chromaticity and absolute reflectance across the visible. [10] In constructing metasurfaces for color generation, one prominently used geometry is the metal-insulator-metal (MIM) arrangement. In this tri-layer structure, thin metallic films make up the top and bottom layer, while a dielectric (insulator) material fills the central gap. [11][12][13][14] A simple approach is to only use multilayered thin films (1D systems) and Fabry-Pérot (FP) effects. [15] However, including lateral sub-wavelength patterns in the MIM system opens up many more possibilities to tune the structural colors by additional resonances determined by the shape and size of the individual elements. MIM structures with nanostructures on top and a very thin dielectric spacer (tens of nanometers) can exhibit so called gap surface plasmons (GSP). [16,17] The principle behind this physical phenomenon involves strong nearfield coupling between plasmon Plasmonic metasurfaces for color generation are emerging as important components for next generation display devices. Fabricating bright plasmonic colors economically and via easily scalable methods, however, remains difficult. Here, the authors demonstrate an efficient and scalable strategy based on colloidal lithography to fabricate silver-based reflective metal-insulatornanodisk plasmonic cavities that provide a cyan-magenta-yellow (CMY) color palette with high relative luminance. With the same basic structure, they exploit different mechanisms to efficiently produce a complete subtractive color palette. ...