Photocurrent Enhancement of Graphene Photodetectors by Photon Tunneling of Light into Surface Plasmons

TL;DR

This study demonstrates that surface plasmon resonances excited by photon tunneling significantly enhance photocurrent in graphene photodetectors, with potential applications in sensing and optical detection.

Contribution

We show that photon tunneling-induced surface plasmon resonances can amplify photocurrent in graphene detectors, revealing wavelength and polarization dependencies and enabling new device architectures.

Findings

Surface plasmon resonances enhance photocurrent significantly.

Shorter wavelengths produce higher photocurrent due to increased damping.

Photocurrent polarity switches across the gap as the light spot moves.

Abstract

We demonstrate that surface plasmon resonances excited by photon tunneling through an adjacent dielectric medium enhance photocurrent detected by a graphene photodetector. The device is created by overlaying a graphene sheet over an etched gap in a gold film deposited on glass. The detected photocurrents are compared for five different excitation wavelengths, ranging from nm to nm. The photocurrent excited with incident p-polarized light (the case for resonant surface plasmon excitation) is significantly amplified in comparison with that for s-polarized light (without surface plasmon resonances). We observe that the photocurrent is greater for shorter wavelengths (for both s and p-polarizations) due to the increased photothermal current resulting from higher damping of surface plasmons at shorter wavelength excitation. Position-dependent Raman spectroscopic analysis of the optically-excited graphene photodetector indicates the presence of charge carriers near the metallic edge. In addition, we show that the polarity of photocurrent switches across the gap as the incident light spot moves across the gap. Graphene-based photodetectors offer a simple architecture which can be fabricated on dielectric waveguides to exploit the plasmonic photocurrent enhancement of the evanescent field for detection. Applications for these devices include photo-detection, optical sensing and direct plasmonic detection.