Nature of water and hydrogen reactions on transition metal surfaces studied by scanning tunneling microscopy

Scanning Tunneling Microscopy (STM) has already been established as a tool for the investigation of simple reaction mechanisms. In this work I present results of two parallel studies using STM: first, hydrogen on Ru(0001) surface and second, water on Ru(0001) and Pd(111). In both studies initial stages of adsorption up to saturation monolayer coverage were investigated by variable temperature scanning tunneling microscopy (VT STM).;The first step of the hydrogen adsorption study was the identification and characterization of the various coverage structures on clean Ru(0001). Hydrogen was found to adsorb dissociatively forming ( 3×3 )R30°, 3 domains of (2×1), (2×2)-3H and (1×1) for increasing coverages of Θ=0.3 ML, 0.5 ML, 0.75 ML and 0.1 ML respectively. Some of these structures were observed to coexist at intermediate coverage values. In addition effects of impurities such as oxygen and carbon on hydrogen adsorption has been discussed.;Next, near saturation coverage the interesting mechanism of how H 2 dissociates and binds to the surface of Ru(0001) has been observed. We found that the H2 dissociation takes place only on Ru sites where the metal atom is not bound to any H atom. Such active sites are formed when at least 3 H-vacancies aggregate by thermal diffusion. Sites formed by single H-vacancies (i.e. unoccupied Ru sites) or pairs of adjoining vacancies were found to be unreactive toward H2. H-vacancies were observed as single entities diffusing on the surface at 50 K and able to form transient triangular shaped aggregations where H2 molecules dissociated. It was found that the diffusion and aggregation of the H-vacancies is essential in creation of active sites where dissociative adsorption of hydrogen occurs.;The first step of water studies was the initial stages of growth of water on the hexagonal surfaces of Pd(111) and Ru(0001) in the temperature range between 40 K and 130 K. In addition, DFT calculations and STM image simulations were used to validate the models. Below 130 K water dissociation does not occur at any appreciable rate and only molecular films are formed. At these temperatures the kinetics of water growth leads to structures where the molecules bind to the metal substrate through the O-lone pair while making 3 H-bonds with neighboring molecules and form clusters of hexagonal units with a honeycomb structure. This bonding geometry imposes limitations to the size of the clusters, with unsaturated H-bonds confined to the cluster periphery. It is found that growth proceeds by attachement of water molecules to the edge of the clusters by H-bonds. These molecules bind only weakly to the metal substrate and can hop around the edges. Comparison of DFT and STM image calculations with experiments shows that on Pd the edge-attached molecules form two different structures, a metastable one where the molecule is elevated by 2.7 Å with respect to the cluster molecules, and another where they are elevated by only 0.4 Å. On Ru only the less elevated (0.4 Å higher) edge-attached molecules are observed.;In next final step, water structures on Ru(0001) were studied at temperatures above 140K. STM findings were backed by x-ray absorption spectroscopy. Additional DFT calculations and STM simulations provided validation of proposed models. It was found that while undissociated water layers are metastable below 140 K, heating above this temperature produces drastic transformations whereby a fraction of the water molecules partially dissociate and form mixed H 2O-OH structures. XPS and XAS revealed the presence of hydroxyl groups with their O-H bond essentiallymostly parallel to the surface. STM images show that the mixed H2O-OH structures consist of long narrow stripes aligned with the three crystallographic directions perpendicular to the close-packed atomic rows of the Ru(0001) substrate. The internal structure of the stripes is a honeycomb network of H-bonded water and hydroxyl species. We found that the metastable low temperature molecular phase can also be converted to a mixed H2O-OH phase through excitation by the tunneling electrons when their energy is 0.5 eV or higher above the Fermi level. Structural models based on the STM images were used for Density Functional Theory optimizations of the stripes geometry. The optimized geometry was then utilized to calculate STM images for comparison with the experiment.