Electron transfer dynamics in nanocrystalline titanium dioxide solar cells sensitized with ruthenium or osmium polypyridyl complexes

The electron transfer dynamics in solar cells that utilize sensitized nanocrystalline titanium dioxide photoelectrodes and the iodide/triiodide redox couple have been studied on a nanosecond time scale. The ruthenium and osmium bipyridyl complexes Ru(H2L')(2)(CN)(2), Os(H2L)(2)(CN)(2), Ru(H2L')(2)(NCS)(2), and Os(H2L')(2)(NCS)(2), when H2L' is 4,4'-dicarboxylic acid 2,2'-bipyridine, inject electrons into the semiconductor with a rate constant > 10(8) s(-1). The effects of excitation intensity, temperature, and applied potential on the recombination reaction were analyzed using a second-order kinetics model. The rates of charge recombination decrease with increasing driving force to the oxidized sensitizer, indicating that charge recombination occurs in the Marcus inverted region. The electronic coupling factors between the oxidized sensitizer and the injected electrons in TiO2 and the reorganization energies for the recombination reaction vary significantly for the different metal complexes. The charge recombination rates are well described by semiclassical electron transfer theory with reorganization energies of 0.55-1.18 eV. Solar cells sensitized with Ru(H2L')(2)(CN)(2), Os(H2L')(2)-(CN)(2), and Ru(H2L')(2)(NCS)(2) have favorable photoelectrochemical characteristics, and iodide is oxidized efficiently. in contrast, iodide oxidation limits the efficiency of cells based on sensitization of TiO2 with Os(H2L')(2)(NCS)(2). The observation that charge recombination occurs in the Marcus inverted region has important implications for the design of molecular sensitizers in nanocrystalline solar cells operated under our experimental conditions.