D. Husain et al., The collisional quenching of Ca[4s4p(P-3(J))] by Ca[4s(2)(S-1(0))] following pulsed dye-laser excitation of atomic calcium, J PHOTOCH A, 136(1-2), 2000, pp. 1-5
Citations number
31
Categorie Soggetti
Physical Chemistry/Chemical Physics
Journal title
JOURNAL OF PHOTOCHEMISTRY AND PHOTOBIOLOGY A-CHEMISTRY
The collisional quenching of electronically excited calcium atoms, Ca[4s4p(
P-3(J)), 1.888 eV above the 4s(2)(S-1(0)) ground state by ground state calc
ium atoms, Ca[4s(2)(S-1(0))], has been investigated. Ca[4s4p(P-3(1))] was g
enerated by the pulsed dye-laser excitation of ground state calcium atoms a
t lambda=657.3 nm {Ca[4s4p(P-3(1))] <-- Ca[4s(2)(S-1(0))]} over a range of
elevated temperatures in the presence of excess helium buffer gas. Measurem
ents were then made of the atomic resonance fluorescence from Ca(4(3)P(1) -
-> 4(1)S(0)) after Boltzmann equilibration within Ca(4(3)P(0.1.2)). First-o
rder decay coefficients for the atomic emission profiles were quantified bo
th as a function of temperature and hence, atomic density of Ca(4(1)S(0)) a
nd of helium density itself. Consideration of the terms contributing to the
measured decay coefficients, viz. emission, diffusion, and collisional que
nching of Ca(4(3)P(J)) by Ca(4(1)S(0)) and He yields the collisional rate d
ata. The absolute second-order rate constant for quenching of Ca(P-3) by Ca
(S-1) is found to be k(Ca)=(2.4+/-0.3) x 10(-12) cm(3) per atom s(-1) (810-
997 K) marginally lower than obtained by phase angle modulation following d
ye-laser excitation for a similar temperature range. It is significantly la
rger than that obtained from earlier estimates derived from the departure o
f a T-1.5 dependence of the temperature variation of the diffusion coeffici
ent, D-12((CaP)-P-3-He), measured in the time-domain. A related analysis of
the first-order decay coefficients for Ca(43PJ) yielded the rate constant
for the collisional quenching of Ca(P-3) by He, viz. k(He)=(2.3+/-0.3)x 10(
-16) cm(3) per atom s(-1) (T=940 K). This is in agreement with the upper li
mit obtained earlier in the time-domain but significantly lower than that r
esulting from phase angle modulation measurements across a temperature rang
e in this region. (C) 2000 Elsevier Science S.A. All rights reserved.