superior performance with respect to speed and operation bandwidth than electronic based devices. [3-5] As a fundamental χ (3) process, FWM has found a wide range of applications in wavelength conversion, [6,7] optical frequency comb generation, [8,9] optical sampling, [10,11] quantum entanglement, [12,13] and many others. [14,15] Implementing nonlinear photonic devices in integrated form offers the greatest dividend in terms of compact footprint, high stability, high scalability, and mass-producibility. [1,2,16] Although silicon has been a leading platform for integrated photonic devices for many reasons, [1] including the fact that it leverages the well-developed complementary metal-oxide-semiconductor (CMOS) fabrication technologies, [17] its strong twophoton absorption (TPA) at near-infrared telecommunications wavelengths poses a fundamental limitation for devices operating in this wavelength region. Other CMOS compatible platforms such as silicon nitride (SiN) and doped silica [2,18] have a much lower TPA, although they still suffer from intrinsic limitation arising from a much lower Kerr nonlinearity. The increasing demand for high performing nonlinear integrated photonic devices has motivated the search for highly