Controlling field asymmetry in nanoscale gaps for second harmonic generation

TL;DR

This paper demonstrates precise control over the field asymmetry in nanoscale gaps of plasmonic antennas, significantly enhancing second harmonic generation through geometrical asymmetry introduced via helium ion beam milling.

Contribution

It introduces a novel method to systematically control field asymmetry in nanoscale gaps, enhancing nonlinear optical responses in plasmonic antennas.

Findings

Increased second harmonic radiation with greater asymmetry.

Nearly complete suppression of SHG in symmetric dimers.

Detailed understanding of SHG mechanisms at the nanoscale.

Abstract

Plasmonic dimer antennas create strong field enhancement by squeezing light into a nanoscale gap. These optical hotspots are highly attractive for boosting nonlinear processes, such as harmonic generation, photoelectron emission, and ultrafast electron transport. Alongside large field enhancement, such phenomena often require control over the field asymmetry in the hotspot, which is challenging considering the nanometer length scales. Here, by means of strongly enhanced second harmonic generation, we demonstrate unprecedented control over the field distribution in a hotspot by systematically introducing geometrical asymmetry to the antenna gap. We use focused helium ion beam milling of mono-crystalline gold to realize asymmetric-gap dimer antennas in which an ultra-sharp tip with 3 nm apex radius faces a flat counterpart, conserving the bonding antenna mode and the concomitant field enhancement at the fundamental frequency. By decreasing the tip opening angle, we are able to systematically increase both field enhancement and asymmetry, thus enhancing second harmonic radiation to the far-field, which is nearly completely suppressed for equivalent symmetric dimer antennas. Combining these findings with second harmonic radiation patterns as well as quantitative nonlinear simulations, we further obtain remarkably detailed insights into the mechanism of second harmonic generation at the nanoscale. Our results open new opportunities for the realization of novel nonlinear nanoscale systems, where the control over local field asymmetry in combination with large field enhancement is essential to create nonreciprocal functionalities.