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Intramolecular and Lateral Intermolecular Hole Transfer at the Sensitized TiO2 Interface

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...

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Bibliographic Details
Published in:Journal of the American Chemical Society 2014-01, Vol.136 (3), p.1034-1046
Main Authors: Hu, Ke, Robson, Kiyoshi C. D, Beauvilliers, Evan E, Schott, Eduardo, Zarate, Ximena, Arratia-Perez, Ramiro, Berlinguette, Curtis P, Meyer, Gerald J
Format: Article
Language:English
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Summary: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 RuIII/II couple and 1.15 ± 0.09 for the NAr3 •+/0 couple. Pulsed light excitation of the sensitized thin films resulted in rapid excited-state injection (k inj > 108 s–1) and in some cases hole transfer to NAr3 [TiO2(e–)/RuIII–NAr3 → TiO2(e–)/RuII–NAr3 •+]. The rate constants for charge recombination [TiO2(e–)/RuIII–NAr3 → TiO2/RuII–NAr3 or TiO2(e–)/RuII–NAr3 •+ → TiO2/RuII–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 (Δμ = 7.7 D). Visible-light excitation under conditions where the RuIII centers were oxidized resulted in injection into TiO2 [TiO2/RuIII–NAr3 + hν → TiO2(e–)/RuIII–NAr3 •+] followed by rapid back interfacial electron transfer to another oxidized compound that had not undergone excited-state injection [TiO2(e–)/RuIII–NAr3 → TiO2/RuII–NAr3]. The net effect was the photogeneration of equal numbers of fully reduced and fully oxidized compounds. Lateral intermolecular hole hopping (TiO2/RuII–NAr3 + TiO2/RuIII–NAr3 •+ → 2TiO2/RuIII–NAr3) was observed spectroscopically and was modeled by Monte Carlo simulations that revealed an effective hole hopping rate of (130 ns)−1.
ISSN:0002-7863
1520-5126
DOI:10.1021/ja410647c