KINETIC INVESTIGATION OF THE TIME-RESOLVED ATOMIC FLUORESCENCE SR(5 P-3(1)-]5 S-1(0)) AND MOLECULAR CHEMILUMINESCENCE SRCL(A (2)PI, B (2)SIGMA-]X (3)SIGMA+ FOLLOWING THE PULSED DYE-LASER GENERATION OF SR(5 P-3(J)) IN THE PRESENCE OF CH3CL AND CF3CL()
Mns. Rayo et al., KINETIC INVESTIGATION OF THE TIME-RESOLVED ATOMIC FLUORESCENCE SR(5 P-3(1)-]5 S-1(0)) AND MOLECULAR CHEMILUMINESCENCE SRCL(A (2)PI, B (2)SIGMA-]X (3)SIGMA+ FOLLOWING THE PULSED DYE-LASER GENERATION OF SR(5 P-3(J)) IN THE PRESENCE OF CH3CL AND CF3CL(), Journal of the Chemical Society. Faraday transactions, 89(11), 1993, pp. 1645-1651
Citations number
53
Categorie Soggetti
Chemistry Physical","Physics, Atomic, Molecular & Chemical
A kinetic study of the vibronic energy distribution in SrCl following
the collision of the optically metastable, electronically excited stro
ntium atom, Sr[(5s)1(5p)1, 3P(J)], 1.807 eV above its (5s)2, 1S(o) ele
ctronic ground state, in the presence of CH3Cl and CF3Cl is presented.
This is investigated in the time-resolved mode following the generati
on of the excited atom by pulsed dye-laser excitation at elevated temp
erature from ground-state strontium vapour in the presence of reactant
s and an excess of helium buffer gas in a slow-flow system, kineticall
y equivalent to a static system. The decay of Sr(5 3P(J)) is monitored
by time-resolved atomic fluorescence at the resonance wavelength [lam
bda = 689.3 nm, Sr(5 P-3(1)) --> Sr(5 1S(o)) + h(nu)], following rapid
Boltzmann equilibrium within the 5 3P(J) spin-orbit manifold using bo
xcar integration. Electronically excited SrCl in the A 2PI1/2,3/2 and
B 2SIGMA+ states, respectively 1.855 eV (179.0 kJ mol-1) and 1.948 eV
(188.0 kJ mol-1) above the X 2SIGMA+ ground state, was also monitored
by time-resolved molecular chemiluminescence of the A, B-X systems und
er identical conditions to those employed for characterising the decay
profiles of Sr(5 3P(J)). Both atomic and molecular chemiluminescence
emissions showed exponential decay profiles, characterised by first-or
der decay coefficients which were found to be equal under the same exp
erimental conditions within experimental error. SrCl(A 2PI) and SrCl(B
2SIGMA+) are thus shown to arise from direct production on the collis
ion of Sr(5 3p(J)) with CH3Cl and CF3Cl where these processes are ener
getically favourable. These results from measurements in the time-doma
in are considered with analogous data for Ca(4 3P(J)) Collisions invol
ving F, Cl, Br and I atom abstraction reactions and with chemiluminesc
ence from SrCl(A, B-X) systems in the single-collision condition follo
wing the reaction of Sr(5 3p(J)) with various Cl-containing molecules.