Conspectus
Plasmonic nanostructures have garnered widescale
scientific interest
because of their strong light–matter interactions and the tunability
of their absorption across the solar spectrum. At the heart of their
superlative interaction with light is the resonant excitation of a
collective oscillation of electrons in the nanostructure by the incident
electromagnetic field. These resonant oscillations are known as localized
surface plasmon resonances (LSPRs). In recent years, the community
has uncovered intriguing photochemical attributes of noble metal nanostructures
arising from their LSPRs. Chemical reactions that are otherwise unfavorable
or sluggish in the dark are induced on the nanostructure surface upon
photoexcitation of LSPRs. This phenomenon has led to the birth of
plasmonic catalysis. The rates of a variety of kinetically challenging
reactions are enhanced by plasmon-excited nanostructures. While the
potential utility for solar energy harvesting and chemical production
is clear, there is a natural curiosity about the precise origin(s)
of plasmonic catalysis. One explanation is that the reactions are
facilitated by the action of the intensely concentrated and confined
electric fields generated on the nanostructure upon LSPR excitation.
Another mechanism of activation involves hot carriers transiently
produced in the metal nanostructure by damping of LSPRs.
In
this Account, we visit a phenomenon that has received less attention
but has a key role to play in plasmonic catalysis and chemistry. Under
common chemical scenarios, plasmonic excitation induces a potential
or a voltage on a nanoparticle. This photopotential modifies the energetics
of a chemical reaction on noble metal nanoparticles. In a range of
cases studied by our laboratory and others, light-induced potentials
underlie the plasmonic enhancement of reaction kinetics. The photopotential
model does not replace other known mechanisms, but it complements
them. There are multiple ways in which an electrostatic photopotential
is produced by LSPR excitation, such as optical rectification, but
one that is most relevant in chemical media is asymmetric charge transfer
to solution-phase acceptors. Electrons and holes produced in a nanostructure
by damping of LSPRs are not removed at the same rate. As a result,
the slower carrier accumulates on the nanostructure, and a steady-state
charge is built up on the nanostructure, leading to a photopotential.
Potentials of up to a few hundred millivolts have been measured by
our laboratory and others. A photocharged nanoparticle is a source
of carriers of a higher potential than an uncharged one. As a result,
redox chemical reactions on noble metal nanoparticles exhibit lower
activation barriers under photoexcitation. In electrochemical reactions
on noble metal nanoparticles, the photopotential supplements the applied
potential. In a diverse set of reactions, the photopotential model
explains the photoenhancement of rates as well as the trends as a
function of light intensity and photon energy. With further g...