Cascaded optical nonlinearities in dielectric metasurfaces

TL;DR

This paper demonstrates the existence of cascaded second-order nonlinearities in dielectric metasurfaces, showing that multi-step frequency mixing can produce signals comparable to direct third harmonic generation, with surface nonlinearities playing a key role.

Contribution

It provides the first analysis confirming cascaded second-order nonlinearities in dielectric metasurfaces, expanding the understanding of nonlinear optical processes at the nanoscale.

Findings

Cascaded second-order nonlinearities are experimentally confirmed.

Third wave mixing signals can rival direct third harmonic generation.

Surface nonlinearities dominate the cascaded nonlinear processes.

Abstract

Since the discovery of the laser, optical parametric nonlinearities have been at the core of efficient light conversion sources. Typically, thick transparent crystals or quasi-phase matched waveguides, are utilized in conjunction with phase-matching techniques to select a single parametric process. In recent years, due to the rapid developments in artificially structured materials, optical frequency mixing has been achieved at the nanoscale in subwavelength resonators arrayed as metasurfaces. Phase matching becomes relaxed for these wavelength-scale structures, and all allowed nonlinear processes can, in principle, occur on an equal footing. This could promote harmonic generation via a cascaded (consisting of several frequency mixing steps) process. However, so far, all reported work on dielectric metasurfaces have assumed frequency mixing from a direct (single step) nonlinear process. In this work, we prove the existence of cascaded second-order optical nonlinearities by analyzing the second and third wave mixing from a highly nonlinear metasurface in conjunction with polarization selection rules and crystal symmetries. We find that the third wave mixing signal from a cascaded process can be of comparable strength to that from conventional third harmonic generation, and that surface nonlinearities are the dominant mechanism that contributes to cascaded second order nonlinearities