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Electronic Structure and Interface Energetics of CuBi(2)O(4) Photoelectrodes

[Image: see text] CuBi(2)O(4) exhibits significant potential for the photoelectrochemical (PEC) conversion of solar energy into chemical fuels, owing to its extended visible-light absorption and positive flat band potential vs the reversible hydrogen electrode. A detailed understanding of the fundam...

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Detalles Bibliográficos
Autores principales: Oropeza, Freddy E., Dzade, Nelson Y., Pons-Martí, Amalia, Yang, Zhenni, Zhang, Kelvin H. L., de Leeuw, Nora H., Hensen, Emiel J. M., Hofmann, Jan P.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Chemical Society 2020
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7659311/
https://www.ncbi.nlm.nih.gov/pubmed/33193938
http://dx.doi.org/10.1021/acs.jpcc.0c08455
Descripción
Sumario:[Image: see text] CuBi(2)O(4) exhibits significant potential for the photoelectrochemical (PEC) conversion of solar energy into chemical fuels, owing to its extended visible-light absorption and positive flat band potential vs the reversible hydrogen electrode. A detailed understanding of the fundamental electronic structure and its correlation with PEC activity is of significant importance to address limiting factors, such as poor charge carrier mobility and stability under PEC conditions. In this study, the electronic structure of CuBi(2)O(4) has been studied by a combination of hard X-ray photoemission spectroscopy, resonant photoemission spectroscopy, and X-ray absorption spectroscopy (XAS) and compared with density functional theory (DFT) calculations. The photoemission study indicates that there is a strong Bi 6s–O 2p hybrid electronic state at 2.3 eV below the Fermi level, whereas the valence band maximum (VBM) has a predominant Cu 3d–O 2p hybrid character. XAS at the O K-edge supported by DFT calculations provides a good description of the conduction band, indicating that the conduction band minimum is composed of unoccupied Cu 3d–O 2p states. The combined experimental and theoretical results suggest that the low charge carrier mobility for CuBi(2)O(4) derives from an intrinsic charge localization at the VBM. Also, the low-energy visible-light absorption in CuBi(2)O(4) may result from a direct but forbidden Cu d–d electronic transition, leading to a low absorption coefficient. Additionally, the ionization potential of CuBi(2)O(4) is higher than that of the related binary oxide CuO or that of NiO, which is commonly used as a hole transport/extraction layer in photoelectrodes. This work provides a solid electronic basis for topical materials science approaches to increase the charge transport and improve the photoelectrochemical properties of CuBi(2)O(4)-based photoelectrodes.