Influence of plasmon resonances and symmetry effects on second harmonic generation in WS2-plasmonic hybrid metasurfaces

TL;DR

This study explores how plasmonic resonances and symmetry influence second harmonic generation in WS2-plasmonic hybrid metasurfaces, revealing polarization-dependent effects and significant SHG enhancement for potential future applications.

Contribution

It demonstrates the impact of plasmonic dipole resonances and lattice symmetry on SHG in WS2 hybrid metasurfaces, including polarization control and signal enhancement.

Findings

SHG polarization dependency is influenced by lattice structure and orientation.

Hybrid metasurfaces can generate SHG in otherwise forbidden polarization states.

SHG signal is enhanced by over 40 times in certain channels.

Abstract

The nonlinear process of second harmonic generation (SHG) in monolayer (1L) transition metal dichalcogenides (TMD), like $WS_2$, strongly depends on the polarization state of the excitation light. Combining plasmonic nanostructures with $1L-WS_2$ by transferring it onto a plasmonic nanoantenna array, a hybrid metasurface is realized impacting the polarization dependency of its SHG. Here, we investigate how plasmonic dipole resonances affect the process of SHG in plasmonic-TMD hybrid metasurfaces by nonlinear spectroscopy. We show, that the polarization dependency is affected by the lattice structure of plasmonic nanoantenna arrays as well as by the relative orientation between the $1L-WS_2$ and the individual plasmonic nanoantennas. In addition, such hybrid metasurfaces show SHG in polarization states, where SHG is usually forbidden for either $1L-WS_2$ or plasmonic nanoantennas. By comparing the SHG in these channels with the SHG generated by the hybrid metasurface components, we detect an enhancement of the SHG signal by a factor of more than 40. Meanwhile, an attenuation of the SHG signal in usually allowed polarization states is observed. Our study provides valuable insight into hybrid systems where symmetries strongly affecting the SHG and open up the possibility for tailoring the SHG in $1L-WS_2$ for future applications.