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CuWO4 is an n-type oxide semiconductor with a bandgap of 2.2 eV which exhibits great potential for photoelectrochemical (PEC) conversion of solar energy into chemical fuels. However, the photocurrent achieved so far is limited to ∼0.3 mA cm−2 at +1.23 V vs. reversible hydrogen electrode (RHE). Possible limiting factors include slow surface reaction kinetics, poor charge carrier mobility and/or presence of surface defect states. A detailed understanding of the fundamental electronic structure and its correlation with PEC activity is of significant importance for devising strategies for further improvements. In this work, we have synthesized CuWO4 thin films showing a record photocurrent density of 0.50 mA cm−2 at +1.23 V vs. RHE. Importantly, we have used a synergistic combination of photoemission spectroscopy, X-ray absorption spectroscopy and density functional theory (DFT) to unravel the electronic structure of CuWO4. Our results show that the valence band (VB) consists of strongly hybridized states of O 2p6 and Cu 3d9, while the bottom of the conduction band (CB) is primarily composed of unoccupied Cu 3d states. The localized nature of the Cu 3d state leads to the low charge carrier mobility and the localization of the photo-excited electrons to the CB. The combined experimental and theoretical results also indicate that CuWO4 is better described as having a direct but d–d forbidden optical bandgap, leading to a low absorption coefficient for visible light. Furthermore, the implication of the electronic structure on its PEC characteristics and strategies for further improvements by adding Co3O4 as a co-catalyst or surface layer to increase the interfacial band bending to facilitate photo-carriers transport, are discussed. [ABSTRACT FROM AUTHOR]

The electronic structure of IrO2 has been investigated using hard x-ray photoelectron spectroscopy and density-functional theory. Excellent agreement is observed between theory and experiment. We show that the electronic structure of IrO2 involves crystal field splitting of the iridium 5d orbitals in a distorted octahedral field. The behavior of IrO2 closely follows the theoretical predictions of Goodenough for conductive rutile-structured oxides [J. B. Goodenough, J. Solid State Chem. 3, 490 (1971).