“…where
Under the assumption that [O 2 (0)] and [H 2 O(000)] can be taken to be time independent (i.e., that the effective vibrational temperatures are not too high), we can take α, β, γ, and δ as constants for any specific experiment, and then we solve the differential equations analytically, obtaining
where λ(fast) and λ(slow) are calculated from the two roots of the eigenvalue equation
resulting in
A similar analysis is provided by Henderson et al A more complete description would include the expected thermal equilibrium values of [O 2 (1)] and [H 2 O(010)], but the conclusions derived here about time dependence would be unchanged. The time dependencies of both [O 2 (1)] and [H 2 O(010)] are thus described by double exponentials, with an initially excited level decaying at first fast and then slow, while an initally unexcited level would rise quickly and decay slowly, as reflected in the coefficients A − D as defined by the initial excitation conditions.…”