I. Introduction
The field of nanophotonics has grown significantly in recent years due to developments in both nanofabrication and device design and optimization. Perhaps the most exciting nanophotonic devices are those based on optical metasurfaces [1]. These so-called “metadevices” are often realized through the patterning of unintuitive freeform structures which have been engineered to achieve a desired functionality over a specified frequency band and angular field of view of interest. Metasurfaces work by introducing engineered phase discontinuities on a surface which lets designers exploit the generalized form of Snell's law to achieve tailored reflection and transmission behaviors not possible with conventional optical components [2] including non-mechanical reconfigurability [3]. These phase discontinuities are often realized through the patterning of constituent unit cells (i.e., “meta-atoms”) which have been designed to produce a desired dispersion-engineered phase profile. However, the performance potential of the metasurface is ultimately determined by the behaviors of its individual meta-atoms.