Basically, stand-alone QEs (i.e., in a homogeneous environment) exhibit several shortcomings that make their use in quantum systems and networks very problematic. The main QE challenging properties include their low spontaneous emission (SE) rates (due to limited transition dipole magnitudes), broad emission spectrum (due to phonon-mediated decoherence), and emission in practically all directions (due to its electric dipole nature). [6,7] In general, there are two different routes for shaping single-photon emission. One can conveniently make use of common optical components, including polarizers, waveplates, mirrors, and phase modulators, to change the polarization, direction, and wave front of single-photon emission. This classical (farfield) approach has been widely used for molding classical light, while being known for requiring bulky optical setups. Alternatively, one can use recently developed near-field coupling approaches that are based on utilizing either individual nanostructures or extended surface nanoarrays (metasurfaces). Placing QEs in a suitably nanostructured environment opens several avenues for single-photon generation