Je. Davis et al., INTERMEDIATE STATES IN THE ADSORPTION OF MO ON IR(111) - SUBSTRATE-TEMPERATURE EFFECTS, Journal of vacuum science & technology. A. Vacuum, surfaces, and films, 14(3), 1996, pp. 1598-1603
Citations number
34
Categorie Soggetti
Physics, Applied","Materials Science, Coatings & Films
Measurements of the initial adsorption probability, S-0, of nitric oxi
de (NO) on Ir(111) as a function of incident kinetic energy, E(i), and
surface temperature, T-s, are presented. We observe a decrease in S-0
with increasing kinetic energy, E(i), from 0.052 to 1.3 eV. At low ki
netic energies, the initial molecular adsorption probability decreases
with increasing surface temperature (ranging between 77 and 300 K in
this study), while at high kinetic energies, this quantity is independ
ent of surface temperature. We propose a trapping-mediated mechanism f
or adsorption at low kinetic energies. In this low energy regime, the
surface temperature dependence reflects a kinetic competition between
desorption from a physically adsorbed state and conversion to a more s
trongly bound, molecularly chemisorbed state. At high kinetic energies
, we propose that adsorption initially occurs directly into the molecu
lar chemisorption well. Indeed, electron energy loss spectroscopy meas
urements show no evidence for direct dissociation at a low T-s and ind
icate that the surface temperature must exceed similar to 400 K for di
ssociative chemisorption to occur. The probability of dissociative che
misorption of NO on Ir(111) decreases with increasing temperature (in
the range 500-900 K in this study) at all kinetic energies investigate
d. Here, we propose a model for low kinetic energies that includes bot
h a physisorbed species and a molecularly chemisorbed species as precu
rsors to dissociation. For the high energy regime, the trapping probab
ility into the physically adsorbed state is assumed to be zero, and th
us, we model the adsorption occurring directly as a molecularly chemis
orbed intermediate with subsequent dissociation at elevated temperatur
es. The success of the model is demonstrated by the agreement of kinet
ic parameters determined separately for data employing a high kinetic
energy beam and a low energy beam. (C) 1996 American Vacuum Society.