The 100 eV electron-induced decomposition (EID) of methanol adsorbed o
n the vacuum-annealed surface of TiO2(110) at 135 K was examined with
temperature-programmed desorption (TPD) and electron-stimulated desorp
tion (ESD). By annealing at 850 K, a TiO2(110) surface was reproducibl
y prepared with an oxygen vacancy coverage of about 0.08 ML (where 1 M
L = 5.2 x 10(14) sires cm(-2)). In the absence of electron irradiation
. CH3OH adsorbed on the vacuum-annealed surface in three main TPD stat
es: a molecular state at 295 K and two dissociative states at 350 and
480 K. The 480 K state was assigned to methoxyls at oxygen vacancy sit
es, and the 350 K state was due to methoxyls at non-vacancy sites. The
surface coverages in these states for the saturated monolayer were 0.
40 ML (295 K), 0.15 ML (350 K) and 0.08 ML (480 K). Although CH3OH dis
sociated on the surface, no irreversible decomposition was observed, a
nd CH3OH was the only desorption product in TPD. By heating a multilay
er CH3OH exposure to 197, 310 and 410 K, followed by recooling to 135
K, methanol adlayers could be prepared containing only the saturated m
onolayer, only both types of methoxyl and only the methoxyls at vacanc
ies, respectively. Given these preparation conditions, the 100 eV EID
of each methanol-related species was examined. Using CD3OD, the major
positive ESD ions detected from multilayer methanol were D+, O+/CD2+ a
nd OD+/CD3+ (the latter were mostly O+ and OD+ based on results with C
H3OH) with weaker signals from C+, CD+, CO+, DCO+ and CD2OD+. However,
the monolayer gave D+ and O+, with weak signals from OD+ and CD+. The
EID cross-section for molecularly adsorbed CH3OH (1.7 x 10(-16) cm(2)
) was only a factor of three less than the literature values for the t
otal dissociative cross-section in the gas phase suggesting that the T
iO2(110) surace had little or no influence on the dissociative ionizat
ion process. No carbon-containing surface products were detected in po
st-irradiation TPD associated with EID of molecular CH3OH, including n
o additional methoxyl formation. The initial EID cross-sections for th
e two types of methoxyls were approximately equivalent regardless of t
he surface condition, but were a factor of 5 greater in the presence o
f CH3OH (3.0-3.4 x 10(-15) cm(2)) than in its absence (5.8-6.2 x 10(-1
6) cm(2)). EID of both vacancy and non-vacancy methoxyl resulted in H2
CO products bound at the same sites, but vacancy-bound H2CO was resist
ant to further EID, whereas non-vacancy H2CO was decomposed with furth
er electron exposure. Total D+ ESD cross-sections were several orders
of magnitude lower than those measured by post-irradiation TPD, sugges
ting that the major EID channels involved ejection of neutral species.
These results demonstrated the ability of low-energy electrons to act
ive organics adsorbed on oxide surfaces with high cross-sections, and
suggest that the EID cross-sections and products for surface organics
depend on the coverage, adsorption state and adsorption site as in the
case of methanol in TiO2(110). Based on these conclusions, low-energy
electrons produced from adsorption of ionizing radiation may play a s
ignificant role in the radiocatalytic destruction of organics over oxi
de catalysts. (C) 1998 Elsevier Science B.V. All rights reserved.