The structure of mixed H2O–OH monolayer films on Ru(0001)
Author(s) -
M. Tatarkhanov,
Э. В. Фомин,
Miquel Salmerón,
Klas Andersson,
Hirohito Ogasawara,
Lars G. M. Pettersson,
Anders Nilsson,
J. I. Cerdá
Publication year - 2008
Publication title -
the journal of chemical physics
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.071
H-Index - 357
eISSN - 1089-7690
pISSN - 0021-9606
DOI - 10.1063/1.2988903
Subject(s) - scanning tunneling microscope , x ray absorption spectroscopy , crystallography , x ray photoelectron spectroscopy , monolayer , chemistry , molecule , substrate (aquarium) , density functional theory , metastability , materials science , absorption spectroscopy , nanotechnology , computational chemistry , nuclear magnetic resonance , biochemistry , physics , oceanography , organic chemistry , quantum mechanics , geology
Scanning tunneling microscopy (STM) and x-ray absorption spectroscopy (XAS) have been used to study the structures produced by water on Ru(0001) at temperatures above 140 K. 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{sub 2}O-OH structures. XPS and XAS revealed the presence of hydroxyl groups with their O-H bond essentially parallel to the surface. STM images show that the mixed H{sub 2}O-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 H{sub 2}O-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 stripe geometry. The optimized geometry was then utilized to calculate STM images for comparison with the experiment
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