Stand-alone memory chips incorporating chalcogenide phase change materials (PCMs) such as Ge 2 Sb 2 Te 5 (GST) have been available commercially for several years. These devices exploit the resistivity difference between the amorphous and crystalline phases to encode data. Operation is robust and reliable, in part because switching the phase of a very small volume of PCM material, less than 0.001 μm 3 , leads to a very large change in device resistance. [1] Recently, researchers have explored the use of PCMs incorporated into photonic devices to create reconfigurable nonvolatile elements for applications such as o ptical switching, [2] erasable photonics, [3] tunable filters, [4] active metasurfaces, [5] and neuromorphic computing. [6] PCM-enabled nonvolatile photonic devices have been demonstrated in which the PCM is deposited on one or more segments of a ring resonator, [7] Mach-Zender interferometer, [8] or waveguide directional coupler. [9] A difference in optical path length is generated by setting the PCM into an amorphous (low index) or crystalline (high index) state, and light is thereby directed to one or the other output port. The state of the PCM is set using a resistive heater element: a short, high-temperature pulse amorphizes the PCM,