Quantum Yield and Mechanism
of Singlet Oxygen Generation via UV Photoexcitation of O<sub>2</sub>–O<sub>2</sub> and N<sub>2</sub>–O<sub>2</sub> Encounter
Complexes
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Abstract
The mechanism and spectral dependence of the quantum
yield of singlet oxygen O<sub>2</sub>(a <sup>1</sup>Δ<sub>g</sub>) photogenerated by UV radiation in gaseous oxygen at elevated pressure
(32–130 bar) have been experimentally investigated within the
238–285 nm spectral region overlapping the range of the Wulf
bands in the absorption spectrum of oxygen. The dominant channel of
singlet oxygen generation with measured quantum yield up to about
2 is attributed to the one-quantum absorption by the encounter complexes
O<sub>2</sub>–O<sub>2</sub>. This absorption gives rise to
oxygen in the Herzberg III state O<sub>2</sub>(A′ <sup>3</sup>Δ<sub>u</sub>), which is assumed to be responsible for singlet
oxygen production in the relaxation process O<sub>2</sub>(A′ <sup>3</sup>Δ<sub>u</sub>, υ) + O<sub>2</sub>(X <sup>3</sup>Σ<sub>g</sub><sup>–</sup>) → O<sub>2</sub>({a <sup>1</sup>Δ<sub>g</sub>}, {b <sup>1</sup>Σ<sub>g</sub><sup>+</sup>}) + O<sub>2</sub>({a <sup>1</sup>Δ<sub>g</sub>, υ =
0}, {b <sup>1</sup>Σ<sub>g</sub><sup>+</sup>, υ = 0}) with further collisional relaxation
of b to a state. This mechanism is deduced from the analysis of the
avoiding crossing locations on the potential energy surface of colliding
O<sub>2</sub>–O<sub>2</sub> pair. The observed drop of the
O<sub>2</sub>(a <sup>1</sup>Δ<sub>g</sub>) yield near spectral
threshold for O<sub>2</sub> dissociation is explained by the competition
between above relaxation and reaction giving rise to O<sub>3</sub> + O (O + O + O<sub>2</sub>) supposed in literature. The quantum
yield of O<sub>2</sub>(a <sup>1</sup>Δ<sub>g</sub>) formation
from encounter complex N<sub>2</sub>–O<sub>2</sub> measured
at λ = 266 nm was found to be the same as that for O<sub>2</sub>–O<sub>2</sub>