The kinetics of the formation of ozone was studied by using pulse radi
olysis coupled with time-resolved UV absorption at 275 nm and at T = 2
94.9 +/- 0.6 K. The rate constant for the formation of ozone (OOO)-O-1
6-O-16-O-16 in argon was determined to be k(3a) = (3.38 +/- 0.04) x 10
(-34) cm(6) molecule(-2) s(-1). The rate constants for the reactions O
-18 + (OO)-O-16-O-16 (k(3b)), O-16 + (OO)-O-16-O-18 (k(3c)), O-16 + (O
O)-O-18-O-18 (k(3d)), O-18 + (OO)-O-16-O-18 (k(3e)), and O-18 + (OO)-O
-18-O-18 (k(3f)) were studied, and the following parameters were deter
mined: (k(3b) + k(3d))/(2k(3a)) = (1.184 +/- 0.037), (k(3c) + k(3e))/(
2k(3a)) = (1.155 +/- 0.062), and k(3f)/k(3a) = (0.977 +/- 0.021). The
values for (k(3b) + k(3d))/(2k(3a)) and (k(3c) + k(3e))/(2k(3a)) obtai
ned here are equal to the values derived from the product studies and
the recently reported relative rate study but higher than the reported
values for (k(3b) + k(3d))/(2k(3a)) and (k(3c) + k(3e))/(2k(3a)) Obta
ined by using CO2 as a third body. The parameter k(3f)/k(3a) = (0.977
+/- 0.021) is lower than the value of k(3f)/k(3a) obtained by using CO
2 as a third body and the value derived from the product studies. Thes
e different values of k(3f) may be partly due to changes in third body
efficiency or due to resonance interactions between the excited ozone
molecules and the third body. The absolute measurements reported here
together with literature data suggest that the nature of the third bo
dy is an important factor in controlling the enhancements of the rate
constants for ozone formation and that asymmetry of neither ozone nor
dioxygen ensure a fast ozone formation rate.