| Autor: |
McCool NS, Swierk JR; Department of Chemistry and Energy Sciences Institute, Yale University , 225 Prospect Street, P.O. Box 208107, New Haven, Connecticut 06520-8107, United States., Nemes CT; Department of Chemistry and Energy Sciences Institute, Yale University , 225 Prospect Street, P.O. Box 208107, New Haven, Connecticut 06520-8107, United States., Schmuttenmaer CA; Department of Chemistry and Energy Sciences Institute, Yale University , 225 Prospect Street, P.O. Box 208107, New Haven, Connecticut 06520-8107, United States., Mallouk TE |
| Abstrakt: |
Water-splitting dye-sensitized photoelectrochemical cells (WS-DSPECs) rely on photoinduced charge separation at a dye/semiconductor interface to supply electrons and holes for water splitting. To improve the efficiency of charge separation and reduce charge recombination in these devices, it is possible to use core/shell structures in which photoinduced electron transfer occurs stepwise through a series of progressively more positive acceptor states. Here, we use steady-state emission studies and time-resolved terahertz spectroscopy to follow the dynamics of electron injection from a photoexcited ruthenium polypyridyl dye as a function of the TiO2 shell thickness on SnO2 nanoparticles. Electron injection proceeds directly into the SnO2 core when the thickness of the TiO2 shell is less than 5 Å. For thicker shells, electrons are injected into the TiO2 shell and trapped, and are then released into the SnO2 core on a time scale of hundreds of picoseconds. As the TiO2 shell increases in thickness, the probability of electron trapping in nonmobile states within the shell increases. Conduction band electrons in the TiO2 shell and the SnO2 core can be differentiated on the basis of their mobility. These observations help explain the observation of an optimum shell thickness for core/shell water-splitting electrodes. |
