Growth and decay of the Pd(111)–Pd5O4 surface oxide: Pressure-dependent kinetics and structural aspects
Surface Science 600(1): 205-218
Article 2005 English
Authors
HG
Harald Gabasch
WU
W. Unterberger
KH
K. Hayek
Abstract
2 min read
Growth and decomposition of the Pd5O4 surface oxide on Pd(111) were studied at sample temperatures between 573 and 683K and O2 gas pressures between 10−7 and 6×10−5
mbar, by means of an effusive O2 beam from a capillary array doser, scanning tunnelling microscopy (STM) and thermal desorption spectrometry (TDS). Exposures beyond the p(2×2)O adlayer (saturation coverage 0.25) at 683K (near thermodynamic equilibrium with respect to Pd5O4 surface oxide formation) lead to incorporation of additional oxygen into the surface. To initiate the incorporation, a critical pressure beyond the thermodynamic stability limit of the surface oxide is required. This thermodynamic stability limit is near 8.9×10−6
mbar at 683K, in good agreement with calculations by density functional theory. A controlled kinetic study was feasible by generating nuclei by only a short O2 pressure pulse and then following further growth kinetics in the lower (10−6
mbar) pressure range.
Growth of the surface oxide layer at a lower temperature (573K) studied by STM is characterized by a high degree of heterogeneity. Among various metastable local structures, a seam of disordered oxide formed at the step edges is a common structural feature characteristic of initial oxide growth. Further oxide nucleation appears to be favoured along the interface between the p(2×2)O structure and these disordered seams. Among the intermediate phases one specifically stable phase was detected both during growth and decomposition of the Pd5O4 layer. It is hexagonal with a distance of about 0.62nm between the protrusions. Its well-ordered form is a
(
67
×
67
)
R
12.2
°
superstructure.
Isothermal decay of the Pd5O4 oxide layer at 693K involves at first a rearrangement into the
(
67
×
67
)
R
12.2
°
structure, indicating its high-temperature stability. This structure can break up into small clusters of uniform size and leaves a free metal surface area covered by a p(2×2)O adlayer. The rate of desorption increases autocatalytically with increasing phase boundary metal-oxide. We propose that at close-to-equilibrium conditions (693K) surface oxide growth and decay occur via this intermediate structure.
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