Sj. Garrett et al., PHOTOCHEMISTRY OF ADSORBED MOLECULES .18. PHOTODISSOCIATION AND EXCHANGE-REACTION IN CH3BR MGO(001) AT 193 NM/, The Journal of chemical physics, 106(18), 1997, pp. 7847-7855
Methyl photofragments from the 193 nm photodissociation of CH3Br adsor
bed on MgO(001) were studied by angularly resolved time-of-flight mass
spectrometry. The translational energy distributions of the photofrag
ments showed evidence of three pathways for the release of CH3. The pa
thways were termed ''direct'' [DIR], ''indirect(1)'' [IND(1)], and ''i
ndirect(2)'' [IND(2)]. The DIR methyl translational energy distributio
n, P(E-T') peaked at 2.3 eV, with a full width at half-maximum (FWHM)
of 0.65 eV, corresponding roughly to that reported for gas phase CH3 (
peak=2.5 eV, FWHM=0.5 eV). The P(E-T') of the DIR pathway was consiste
nt with CH3 escaping directly from the topmost molecular layer without
collisions. For these DIR methyls, as previously demonstrated, the an
gular distribution reflected the prior Br-C bond direction. In the hig
her coverage range, 1.5-10 monolayers (ML) angular distributions, P(Th
eta'), for the DIR methyls peaked at 22 degrees to the normal with FWH
M of 20 degrees. At low coverage, 0.75 ML, the DIR peak shifted to sim
ilar to 40 degrees with doubled FWHM. The IND(1) methyls, despite the
loss of 1.2 eV in a strong inelastic encounter, exhibited the same ang
ular distributions and FWHM as the DIR component: 22 degrees peak, 20
degrees FWHM at high coverage; 40 degrees peak, 40 degrees FWHM at low
coverage. The mechanism attributed to IND(1), which accounts for the
retention of direction of methyl with concurrent substantial energy lo
ss, is one proposed in a prior theoretical study [Barclay et al., J. P
hys. Chem. 97, 12541 (1993)]: an exchange reaction favored by the adso
rbate geometry; in the present case CH3+BrCH3'-->CH3Br+CH3'. The secon
d indirect channel, IND(2), exhibited broader translational energy dis
tribution than DIR or IND(1) peaked at 0.6 eV lower energy than IND(1)
, and a broad angular distribution (cos(2) Theta') peaked at the norma
l, characteristic of strongly inelastic encounters in which memory of
the initial CH3 recoil direction is lost. (C) 1997 American Institute
of Physics.