Transactions of the Faraday Society · 1968 · 38 citations · 0 references
Natural SciencesChemistryPhysicsChemical KineticsPhysical ChemistrySpectroscopyAtomic ExcitationOptical SpectroscopyPhotochemical KineticsPhotochemistryExothermic TransitionsIodine ChemistryKinetic SpectroscopyPhotochemical Reaction KineticsPhotodissociation KineticsPhotolysisQuenching ProcessesRate Constants
ion of an iodine atom from an alkyl iodide by an electronically excited iodine atom, I(52P½), is an exothermic process and thus may compete with collisional quenching at room temperature. I(52P½), generated by the flash photolysis of CF3I, has been monitored by kinetic spectroscopy in absorption in the ultra-violet in the presence of seven alkyl iodides. The overall second-order rate constants for the removal of I(52P½) at ∼300°K were 1.7 × 10–12, 1.9 × 10–13, 2.0 × 10–13, 2.0 × 10–13, 2.9 × 10–13, 2.9 × 10–13 and 3.8 × 10–13 cm3 molecule–1 sec–1 for CH3I, C2H5I, n-C3H7I, i-C3H7I, n-C4H9I, i-C4H9I and t-C4H9I, respectively. Absorption spectroscopy in the vacuum ultra-violet following the flash photolysis of CH3I itself, at low pressure, demonstrates that spin orbit relaxation dominates I atom abstraction, and it is proposed that electronic deactivation is the main process for all the iodides studied. For normal and isopropyl iodides, a difference in laser action from I(52P1/2) may be attributed to the relative yields of the atoms in the 2P½ and 2P states on photodissociation rather than to any difference in the rates of electronic quenching of the excited atom by the iodides.