“…Optical metamaterials are composed of strongly subwavelength substructures, or “meta-atoms,” so as to realize and tune effective properties that may be less accessible or even unachievable in homogeneous materials. − Often, component materials are selected that complement or offset each other’s characteristics. For example, in multilayer metal–dielectric stacks, a real part of the effective permittivity, Re(ε eff ), of zero can be achieved at a frequency controlled by adjusting the ratio of layer thicknesses so that the negative Re(ε) of the metal is balanced by the positive Re(ε) of the dielectric. , The frequency range where Re(ε) is near zero (ENZ region) is of interest because it can give rise to strong absorption, high near-field enhancement (NFE), strong nonlinear optical response, and properties foundational for transformation optics. − More generally, two-dimensional (2-D) arrays of optical elements give rise to metasurfaces with a broad variety of effective linear and nonlinear optical properties enabling emergent applications in focusing, steering, or converting the frequency of incident light. − To make metasurfaces with components sized well below the wavelength of light and develop scalable fabrication strategies, bottom-up assembly of 2-D superlattices from colloidal nanoparticle building blocks is an appealing alternative to lithographic patterning. − A rich diversity of tunable, emergent optical properties can be envisioned when nanoparticles are assembled in dense superlattices that enable strong coupling and when the characteristics of the component building blocks, as well as their mixing ratio, can be continuously varied.…”