I* emission. These have been extended to many systems to understand the mechanism involved in energy transfer processes. This problem has been tackled using several approaches: (a) Direct measurement of state-to-state E-v rate constants; (b) Temperature dependence of the bulk or overall quenching rate constants; (c) Isotope effects on the observed quenching rate constants; and (d) study of the quenching efficiencies of a "family" of compounds.Although the first approach is the most satisfactory and direct, only in few cases is it experimentally achievable. Few systems (HF, H 2 , and H 2 O) [5][6][7][8] have been studied directly (case a) because of the complexity added by the acceptor intramolecular energy redistribution which grows with the number of vibrational degrees of freedom. Based on the kinetic analysis of the system, state-to-state energy transfer studies are limited up to triatomic acceptor molecules.
INTRODUCTIONThe study of the electronically excited iodine atom, I ( 2 P 1/2 ) (hereafter called I*) constitutes a case example of a system which can undergo electronic to vibrational-rotational energy transfer. The I* is only about 0.92 eV above the ground state and this energy excess hardly contributes to the already low reactivity of the iodine atom in gas phase. Actually, there are few systems in which reactive quenching of I* is present (i.e., interhalogens, ozone) [1 -4].Extensive studies have been carried out measuring quenching efficiencies of several compounds on the
ABSTRACTThe deactivation of I( 2 P 1/2 ) by R-OH compounds (R ϭ H, C n H 2nϩ1 ) was studied using time-resolved atomic absorption at 206.2 nm. The second-order quenching rate constants determined for H 2 O, CH 3 OH, C 2 H 5 OH, n-C 3 H 7 OH, i-C 3 H 7 OH, n-C 4 H 9 OH, i-C 4 H 9 OH, s-C 4 H 9 OH, t-C 4 H 9 OH, are respectively, 2.4 Ϯ 0.3 ϫ 10 Ϫ12 , 5.5 Ϯ 0.8 ϫ 10 Ϫ12 , 8 Ϯ 1 ϫ 10 Ϫ12 , 10 Ϯ 1 ϫ 10 Ϫ12 , 10 Ϯ 1 ϫ 10 Ϫ12 , 11.1 Ϯ 0.9 ϫ 10 Ϫ12 , 9.8 Ϯ 0.9 ϫ 10 Ϫ12 , 7.1 Ϯ 0.7 ϫ 10 Ϫ12 , and 4.1 Ϯ 0.4ϫ 10 Ϫ12 cm 3 molec Ϫ1 s Ϫ1 at room temperature. It is believed that a quasi-resonant electronic to vibrational energy transfer mechanism accounts for most of the features of the quenching process. The influence of the alkyl group and its role in the total quenching rate is also discussed.