“…When reflections off the surfaces of the SPP are considered, the device becomes a SPP etalon that forms a new etalon geometry [28] containing a coherent superposition of OAM states with welldefined phase relationship [28,29]. In order to extend the capabilities of this photonic device as a useful tool in precision optical frequency metrology such as laser locking and stabilization systems [30][31][32][33], optical gyroscopes for rotation sensing, optical resonators [34], quantum cavity electrodynamics [35] with OAM modes, atom circuits [36,37], and other areas of device physics and metrology, it becomes important to understand transmission through the SPP etalon in different regimes, i.e., from the low-reflectivity (low-finesse) to high-reflectivity (high-finesse) regimes.…”