Hydrogen adsorption is important for understanding coverage effects for various chemical reactions and for characterizing the size of nanoparticles. Recent literature suggests that the often-assumed saturation coverage of unity may not be reasonable, at least for small nanoparticles. This includes our prior study which showed that Ir and Pt nanoparticles, which primarily bind H adsorbates in atop binding modes, can saturate at H/Msurf ratios well above 1, depending on the metal and particle size. This work examines H adsorption on small nanoparticles of Ru, Rh, Pd, and Os metals that preferentially bind H in 3-fold sites. We therefore investigate new adlayer structures to understand how undercoordinated atoms influence these H configurations. Calculations on 201-atom nanoparticles suggest H* (at low coverages) binds most favorably to undercoordinated bridge sites for all six metals of interest. As suggested by the slab model calculations, 3-fold sites are also among the most stable sites for Ru, Rh, and Pd particles, while atop sites are more stable for Os, Ir and Pt. These trends in single H* binding behavior do not significantly change with particle size. Saturation adlayers for 4d metals (Ru, Rh, and Pd) are dominated by H* bound to fcc 3-fold sites and undercoordinated bridge sites. With saturation coverages of 1.38, 1.48, and 1.28 ML respectively, Rh has the highest saturation coverage of the 4d metals, reflecting a nonmonotonic periodic trend. For the 5d metals (Os, Ir, Pt), saturated adlayers are dominated by the same undercoordinated bridge sites, but also generally favor atop-bound H* instead of 3-fold except Pt. Their saturation coverages are 1.87. 1.93, and 1.57 ML, respectively. Saturation coverage increases when moving from a 4d to a 5d metal, and the group 9 metals (Rh and Ir) exhibit the highest saturation in their respective series. Our results show that H* binding energy is largely independent of particle size for a given site type. Instead, changing the particle size primarily alters the distribution of available binding sites (corner, edge, and terrace). Therefore, the adlayer model developed for the 201-atom particle can be used to reliably estimate saturation coverages, allowing for extrapolation to both smaller and larger nanoparticles.
Waldt et al. (2026) studied this question.
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