Optimal double resonant condition in metallic core-shell nanocavity for third harmonic generation

TL;DR

This paper theoretically analyzes how to optimize third harmonic generation in metallic core-shell nanocavities by achieving double resonance conditions, significantly enhancing efficiency through mode coupling.

Contribution

It introduces a method to optimize THG efficiency in core-shell nanostructures by matching cavity modes for double resonance, with detailed theoretical and numerical analysis.

Findings

THG intensity can be enhanced up to 3 magnitudes under double resonance.

Matching two cavity modes of the same order yields optimal THG efficiency.

Changing the nonlinear susceptibility of the metal shell has minimal effect on THG efficiency.

Abstract

As the rapid development of nonlinear optics, the enhancement of optical third harmonic generation becomes a pop research realm in the fields of physics, chemistry, biology, materials science, information science and other fields. In this letter, theoretical analysis on double resonance situation in metallic core-shell nanostructure is performed in order to optimize the efficiency of third harmonic generation. As plenty of cavity modes ranging from visible area to near infrared can be excited efficiently in core-shell nanospheres, kinds of double resonant conditions can be formed by matching two different multipolar cavity modes. Numerical simulations show that the third harmonic generation (THG) intensity in the far field can be enhanced remarkably when the THG signal couples well with the high order cavity mode. More importantly, THG efficiency is optimum from the cavity on double resonant conditions coupling two modes with the same order. The THG intensity differs up to 3 magnitudes on this condition. Subsequent theoretical analysis indicates that changing third-order nonlinear susceptibility of the metal shell while keeping that of the core fixed has almost no effect on THG efficiency. This finding about optimal double resonance has an appreciable effect on optimizing THG in spherical cavity structures.