4.8 Article

Intramolecular and Lateral Intermolecular Hole Transfer at the Sensitized TiO2 Interface

Journal

JOURNAL OF THE AMERICAN CHEMICAL SOCIETY
Volume 136, Issue 3, Pages 1034-1046

Publisher

AMER CHEMICAL SOC
DOI: 10.1021/ja410647c

Keywords

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Funding

  1. Division of Chemical Sciences, Office of Basic Energy Sciences, Office of Energy Research, U.S. Department of Energy [DE-FG02-96ER14662]
  2. Canadian Natural Science and Engineering Research Council
  3. Canadian Foundation for Innovation
  4. Alberta Ingenuity
  5. Canada School of Energy and Environment (CSEE)
  6. U.S. Department of Energy (DOE) [DE-FG02-96ER14662] Funding Source: U.S. Department of Energy (DOE)

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Characterization of the redox properties of TiO2 interfaces sensitized to visible light by a series of cyclometalated ruthenium polypyridyl compounds containing both a terpyridyl ligand with three carboxylic acid/carboxylate or methyl ester groups for surface binding and a tridentate cyclometalated ligand with a conjugated triarylamine (NAr3) donor group is described. Spectroelectrochemical studies revealed non-Nernstian behavior with nonideality factors of 1.37 +/- 0.08 for the Ru-III/II couple and 1.15 +/- 0.09 for the NAr3 center dot+/0 couple. Pulsed light excitation of the sensitized thin films resulted in rapid excited-state injection (k(inj) > 10(8) s(-1)) and in some cases hole transfer to NAr3 [TiO2(e(-))/Ru-III-NAr3 -> TiO2(e(-))/Ru-II-NAr3 center dot+]. The rate constants for charge recombination [TiO2(e(-))/Ru-III-NAr3 -> TiO2/Ru-II-NAr3 or TiO2(e(-))/Ru-II-NAr3 center dot+ -> TiO2/Ru-II-NAr3] were insensitive to the identity of the cyclometalated compound, while the open-circuit photovoltage was significantly larger for the compound with the highest quantum yield for hole transfer, behavior attributed to a larger dipole moment change (Delta mu = 7.7 D). Visible-light excitation under conditions where the Ru-III centers were oxidized resulted in injection into TiO2 [TiO2/Ru-III-NAr3 + h nu -> TiO2(e(-))/Ru-III-NAr3 center dot+] followed by rapid back interfacial electron transfer to another oxidized compound that had not undergone excited-state injection [TiO2(e(-))/Ru-III-NAr3 -> TiO2/Ru-II-NAr3]. The net effect was the photogeneration of equal numbers of fully reduced and fully oxidized compounds. Lateral intermolecular hole hopping (TiO2/Ru-II-NAr3 + TiO2/Ru-III-NAr3 center dot+ -> 2TiO(2)/Ru-III-NAr3) was observed spectroscopically and was modeled by Monte Carlo simulations that revealed an effective hole hopping rate of (130 ns)(-1).

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