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Abstract
Utilizing plasmon-generated hot carriers to drive chemical reactions has currently become an active area of research in solar photocatalysis at the nanoscale. However, the mechanism underlying exact transfer and the generation dynamics of hot carriers, and the strategies used to further improve the quantum efficiency of the photocatalytic reaction still deserve a further look. In this work, we perform a nonadiabatic excited-state dynamics study to depict the correlation between the reaction rate of plasmon-driven water splitting (PDWS) and the sizes of gold particles, the incident light frequency and intensity, and the near-field's spatial distribution. Four model systems, \ce{H2O} and \ce{Au20}@\ce{H2O} separately interacting with the laser field and the near field generated by the Au nanoparticle (NP) with a few nanometers in size, have been investigated. Our simulated results clearly unveil the mechanism of PDWS and hot-electron injection in a Schottky-free junction: the electrons populated on the antibonding orbitals of \ce{H2O} are mandatory to drive the \ce{OH} bond breaking and the strong orbital hybridization between \ce{Au20} and \ce{H2O} creates the condition for direct electron injection. We further find that the linear dependence of the reaction rate and the field amplitude only holds at a relatively weak field and it breaks down when the second {\ce{OH}} bond begins to dissociate and field-induced water fragmenting at a very intensive field, and that with the guarantee of electron injection, the water splitting rate increases with the increase of NP's size. This study will be helpful for further improving the efficiency of the photochemical reactions involving the plasmon-generated hot carriers and expanding the applications of hot carriers in varieties of chemical
reactions.
Supplementary materials
Title
Understanding the Mechanism of Plasmon-Driven Water Splitting: Hot Electron Injection and Near Field Enhancement Effect
Description
The materials in SI include the DOS of isolated \ce{H2O} molecule, the evolution of \ce{OH} bond when an isolated \ce{H2O} molecule interacts with the laser field, the time evolution of \ce{OH} bonds in \ce{Au20}@\ce{H2O} system under the laser field with $E_{max}=$\SI[per-mode=symbol]{1.60}{\volt\per\angstrom} and $E_{max}=$\SI[per-mode=symbol]{1.70}{\volt\per\angstrom}), the absorption spectra of \ce{Au20}@\ce{H2O} vary with the intensity of incident field, the absorption spectra of \ce{Au} tetrahedrons with L=\SI{2.88}{\nm}, \SI{4.32}{\nm}, and \SI{5.76}{\nm} calculated by FDTD, the contour plot of near fields, the time evolution of the forces acted on \ce{H2O} molecule in the XZ plane under a uniform field and the real near field, respectively.
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