Mc. Torquemada et al., REACTIVITY OF CO ON A TIO2(110) DEFECTIVE SURFACE STUDIED BY ELECTRON-STIMULATED DESORPTION, Surface science, 337(1-2), 1995, pp. 31-39
CO adsorption on a defective TiO2(110) surface at 150 K incorporating
about 1.7 X 10(14) cm(-2) vacancies produced by Ar+ sputtering has bee
n studied by electron stimulated desorption, ESD, and with Auger elect
ron spectroscopy, AES, as a complementary technique. When the surface
was exposed to CO up to 5 X 10(5) L the AES spectra revealed a small C
signal. From the O(KLL)/Ti(LMM) ratio increase a CO coverage of 0.06
+/- 0.01 ML was determined. In spite of this small amount of CO the ES
D technique showed dramatic changes in ion yield and energy. The chara
cteristic dominant peak at 4.0 eV and the small structure at about 7.0
eV of the ion kinetic energy distribution curve of the clean defectiv
e surface changed to a triple peak structure with maxima at 3.4, 4.3 a
nd 7.4 eV. The first is identified with the most probable kinetic ener
gy of O+ ions ejected from non-dissociated CO molecules. The 4.3 and 7
.4 eV maxima correspond to the most probable kinetic energy of O+ ions
desorbed from O in-plane and from the bridging O-ligand of the TiO2(1
10) surface, respectively. The growth of the 7.4 eV peak upon adsorpti
on is a consequence of the filling of the bridging O-ligand initial va
cancies by dissociated O from the CO molecule. The ion yield curves sh
ow, in addition to the onset at 35 eV electron energy of the clean sur
face, a threshold at about 290 eV electron energy corresponding to exc
itation of the C Is core level. The total ion yield also shows a decre
ase upon CO adsorption. The Of ion yield curves are found to be relate
d to the secondary electron yield. The chemisorption of CO is discusse
d in terms of a model where the CO is molecularly adsorbed on the Ti f
ive-fold coordination sites with a part being dissociated and leading
to O adsorbed on bridging O-ligand vacancies.