When illuminated with visible light, nanostructured noble metals exhibit a strong
plasmon resonance at wavelength, p, that has been shown to be sensitive to its size,
structure, the dielectric properties of the surrounding medium, and charge density. The
tunability of the plasmon resonance has allowed metal nanosystems to be fabricated with
resonances matching the solar spectrum for us in plasmon promoted catalysis, plasmonic
photovoltaics, and surface-enhanced raman spectroscopy. Here we use UV-Visible spectroscopy
to track the shifts of the plasmon resonances from an array of gold nanoparticles
buried under metal oxide layers of varying thickness when in contact with one of two bulk
metals: aluminum or silver. By assuming the array of gold nanoparticles and metal-oxide
layers to be an optically homogenous lm of core-shell particles on a substrate, we developed
a Maxwell-Garnett effective medium approximation to extract reliable optical
parameters for the gold nanoparticles, yielding their charge state before and after contact
with the bulk metal.
Based on the optical parameters extracted from our model, we nd the magnitude of
charge transfer from the bulk metal to the gold nanoparticle is independent of the work
function of the bulk metal. Furthermore, when gold is used as the bulk layer in contact
with the gold nanoparticles, we measured an appreciable amount of charge transfer to the
gold nanoparticles, failing to support the well-established model for electrostatic contact
electrication. Instead, we attribute the charge transfer to the so called plasmoelectric
effect, an optically induced charge transfer mechanism, in which the gold nanoparticle
modifes its charge density to allow its resonant wavelength to match that of the incident
light. We show, however, that in our devices the Schottky barriers between the metals
and the metal oxide layers create a rectication effect that favors electron transfer from
the bulk metal to the nanoparticles over the reverse effect.