Hydrogen activation by rhodium under the cover of a copper oxide thin film

• Dilute amounts of Rh dopants under a Cu 2 O thin film model system accelerate the reduction of the oxide by H 2 . • A complete Cu 2 O layer covering all the Rh atoms is reduced by H 2 more rapidly than a defective layer with exposed Rh sites. • Exposed Rh atoms on the defective oxide surface are easily poisoned by background CO. • Rh atoms alloyed into the Cu(111) surface under the oxide are resistant to CO poisoning. • These Rh atoms under the oxide are active for catalyzing H 2 dissociation at ambient pressure conditions. The activation of reactants by catalytically active metal sites at metal-oxide interfaces is important for understanding the effect of metal-support interactions on nanoparticle catalysts and for tuning activity and selectivity. Using a combined experimental and theoretical approach, we studied the activation of H 2 and the effect of CO poisoning on isolated Rh atoms completely or partially covered by a copper oxide (Cu 2 O) thin film . Temperature-programmed desorption (TPD) experiments conducted in ultra-high vacuum (UHV) show that neither a partially nor a fully oxidized Cu 2 O layer grown on a Rh/Cu(111) single-atom alloy can activate hydrogen in UHV. However, in situ ambient pressure X-ray photoelectron spectroscopy (AP-XPS) experiments performed at elevated H 2 pressures reveal that Rh significantly accelerates the reduction of these Cu 2 O thin films by hydrogen. Remarkably, the fastest reduction rate is observed for the fully oxidized sample with all Rh sites covered by Cu 2 O. Both TPD and AP-XPS data demonstrate that these covered Rh sites are inaccessible to CO, indicating that Rh under Cu 2 O is active for H 2 dissociation but cannot be poisoned by CO. In contrast, an incomplete oxide film leaves some of the Rh sites exposed and accessible to CO, and hence prone to CO poisoning. Density functional theory calculations demonstrate that unlike many reactions in which hydrogen activation is rate limiting, the rate-determining step in the dissociation of H 2 on thin-film Cu 2 O with Rh underneath is the adsorption of H 2 on the buried Rh site, and once adsorbed, the dissociation of H 2 is barrierless. These calculations also explain why H 2 can only be activated at higher pressures. Together, these results highlight how different the reactivity of atomically dispersed Rh in Cu can be depending on its accessibility through the oxide layer, providing a way to engineer Rh sites that are active for hydrogen activation but resilient to CO poisoning.

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Publication Details

Journal
Journal of Catalysis
Published
2024-09-28
DOI
https://doi.org/10.1016/j.jcat.2024.115779
Citations
1
Primary Topic
Catalytic Processes in Materials Science
Type
article
Field-Weighted Citation Impact
0.12

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article

Hydrogen activation by rhodium under the cover of a copper oxide thin film

Hojoon Lim, Volkan Çınar, Iradwikanari Waluyo, Jean‐Sabin McEwen et al.
1 citations
Journal of Catalysis
Catalytic Processes in Materials Science
0.12
article

Hydrogen activation by rhodium under the cover of a copper oxide thin film

Hojoon Lim, Volkan Çınar, Iradwikanari Waluyo, Jean‐Sabin McEwen, E. Charles H. Sykes, Eva Peurrung, Maggie Rickman, Adrian P. Hunt, Grace Miller
article en
1 citations

Abstract

• Dilute amounts of Rh dopants under a Cu 2 O thin film model system accelerate the reduction of the oxide by H 2 . • A complete Cu 2 O layer covering all the Rh atoms is reduced by H 2 more rapidly than a defective layer with exposed Rh sites. • Exposed Rh atoms on the defective oxide surface are easily poisoned by background CO. • Rh atoms alloyed into the Cu(111) surface under the oxide are resistant to CO poisoning. • These Rh atoms under the oxide are active for catalyzing H 2 dissociation at ambient pressure conditions. The activation of reactants by catalytically active metal sites at metal-oxide interfaces is important for understanding the effect of metal-support interactions on nanoparticle catalysts and for tuning activity and selectivity. Using a combined experimental and theoretical approach, we studied the activation of H 2 and the effect of CO poisoning on isolated Rh atoms completely or partially covered by a copper oxide (Cu 2 O) thin film . Temperature-programmed desorption (TPD) experiments conducted in ultra-high vacuum (UHV) show that neither a partially nor a fully oxidized Cu 2 O layer grown on a Rh/Cu(111) single-atom alloy can activate hydrogen in UHV. However, in situ ambient pressure X-ray photoelectron spectroscopy (AP-XPS) experiments performed at elevated H 2 pressures reveal that Rh significantly accelerates the reduction of these Cu 2 O thin films by hydrogen. Remarkably, the fastest reduction rate is observed for the fully oxidized sample with all Rh sites covered by Cu 2 O. Both TPD and AP-XPS data demonstrate that these covered Rh sites are inaccessible to CO, indicating that Rh under Cu 2 O is active for H 2 dissociation but cannot be poisoned by CO. In contrast, an incomplete oxide film leaves some of the Rh sites exposed and accessible to CO, and hence prone to CO poisoning. Density functional theory calculations demonstrate that unlike many reactions in which hydrogen activation is rate limiting, the rate-determining step in the dissociation of H 2 on thin-film Cu 2 O with Rh underneath is the adsorption of H 2 on the buried Rh site, and once adsorbed, the dissociation of H 2 is barrierless. These calculations also explain why H 2 can only be activated at higher pressures. Together, these results highlight how different the reactivity of atomically dispersed Rh in Cu can be depending on its accessibility through the oxide layer, providing a way to engineer Rh sites that are active for hydrogen activation but resilient to CO poisoning.

Journal of CatalysisVol. 440
Tufts University (US), Pacific Northwest National Laboratory (US), Brookhaven National Laboratory (US), National Synchrotron Light Source II, Washington State University (US)
National Science Foundation, U.S. Department of Energy, Battelle, Washington State University, Office of Science, Basic Energy Sciences, Brookhaven National Laboratory
Openalex Percentile: Top 59%
Catalytic Processes in Materials Science
0.12
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