Journal
JOURNAL OF PHYSICAL CHEMISTRY C
Volume 124, Issue 39, Pages 21407-21417Publisher
AMER CHEMICAL SOC
DOI: 10.1021/acs.jpcc.0c05195
Keywords
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Funding
- Office of Science, Office of Basic Energy Sciences of the U.S. Department of Energy at LBNL (Berkeley, CA) [DE-AC02-05CH11231]
- Division of Chemical Sciences, Geosciences and Biosciences of the U.S. Department of Energy at LBNL (Berkeley, CA) [DE-AC02-05CH11231]
- Division of Chemical Sciences, Geosciences and Biosciences of the U.S. Department of Energy at RASEI (Boulder, CO) [DE-SC0018939]
- Office of Science, Office of Basic Energy Sciences, of the U.S. Department of Energy [DE-AC02-05CH11231]
- U.S. Department of Energy, Office of Basic Energy Sciences, Division of Materials Sciences and Engineering [DE-AC02-76SF00515]
- Office of Science, Office of Basic Energy Sciences of the U.S. Department of Energy at RASEI (Boulder, CO) [DE-SC0018939]
- U.S. Department of Energy (DOE) [DE-SC0018939] Funding Source: U.S. Department of Energy (DOE)
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Understanding the equilibrium conditions at the metal oxide/aqueous interface is a key component toward visualizing the structure of water in confined environments and differentiating the catalytic activity of transition-metal oxides. While ambient pressure X-ray photoelectron spectroscopy (AP-XPS) has been the primary technique to investigate the formation of a hydration layer on many surfaces, results over the extended relative humidity (RH) range accessible experimentally have not been compared quantitatively to theoretical predictions. With the use of first-principles theoretical methods and accumulated knowledge of AP-XPS spectral analysis, we do so here for a model surface, TiO2-terminated undoped SrTiO3(100) (STO). The measured distribution of OH and H2O coverages from vacuum up to the first hydration layer is in good agreement with a static density functional theory (DFT) configuration involving partial dissociation of H2O per Ti-atom mediated by H-bonding. Furthermore, ab initio molecular dynamics (AIMD) simulations at 300 K for select coverages (1/4, 1/2, and 1 ML) test the role of fluctuations and entropy in the competition between adsorption and dissociation with coverage. This comparison between theory and experiment for OH and H2O coverages on STO provides a foundation for a more quantitative assessment of the first hydration layer and associated competition between adsorption, dissociation, and H-bonding on transition-metal oxide surfaces.
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