The adsorption and photochemistry of CD3I adsorbed on TiO2(110) at sim
ilar to 110 K has been studied by means of temperature programmed deso
rption (TPD) and x-ray photoelectron spectroscopy (XPS). Complex desor
ption behavior is observed in TPD suggesting the presence of several d
istinct coverage regimes. At submonolayer coverages there are two coex
isting phases: one dominated by adsorbate-adsorbate interaction, the o
ther dominated by adsorbate-substrate interactions. The first complete
d monolayer corresponds to (3.8+/-0.3) X 10(14) molecules cm(-2) and s
hows only one desorption peak, although this is dread and extends asym
metrically to high temperature indicative of a changing desorption act
ivation energy. With increasing coverage, a discrete, less tightly bou
nd second layer is formed which slowly rearranges to produce three-dim
ensional clusters of methyl iodide, as indicated by a sharp reduction
in the I (3d(5/2))/Ti(2p) XPS intensity ratio. There is evidence that
this rearrangement does not involve the first monolayer. Irradiation o
f 1 ML CD3I by 254 or 334 nm photons causes cleavage of the C-I bond a
nd expulsion of I and C containing species into the vacuum. There is r
etention of similar to 20% of the initial I atoms after irradiation at
254 nm. The photodissociation cross section, sigma, of adsorbed CD3 I
on TiO2(110) at 254 and 334 nm is calculated to be similar to 1.1X10(
-18) cm(2) and similar to 1.3 X 10(-20) cm(2), respectively. At 254 nm
, the adsorbate and gas phase sigma are similar suggesting cm photodis
sociation is dominated by adsorbate excitation, but at 334 nm the adso
rbate photodissociation cross section is almost an order of magnitude
larger than its gas phase counterpart. This suggests that a second pho
toexcitation mechanism may be contributing to adsorbate photodissociat
ion, possibly involving photogenerated substrate carriers.