R. J. Rollason and J. M. C. Plane
The reactions between Fe+(a6D) and O3, O2 and N2 have been studied by the pulsed four-photon dissociation at 248 nm of ferrocene vapour in He bath gas, followed by time-resolved laser-induced fluorescence spectroscopy at 260.0 nm [Fe+(z6D9/2o–a6D9/2)]. This yielded: k(Fe++O3→FeO++O2, 200–383 K)=(7.07±2.30)×10-10 exp[-(1.08±0.12) kJ mol-1/RT] cm3 molecule-1 s-1; k(Fe++O2+He→FeO2++He, 194–479 K)=(4.17±0.23)×10-30 (T/300 K)-1.86±0.15 cm6 molecule-2 s-1; and k(Fe++N2+He→FeN2++He, 196–482 K)=(1.96±0.05)×10-30 (T/300 K)-1.52±0.08 cm6 molecule-2 s-1, where the quoted uncertainties are a combination of the 1σ standard errors in the kinetic data and the systematic experimental errors. k(Fe++O3) is shown to be a factor of 2–3 slower than predicted by ion–polar molecule capture theory, with a small positive, rather than slightly negative, temperature dependence. The results for the recombination reactions are interpreted by combining abinitio quantum calculations on FeN2+ and FeO2+ with a semi-empirical formalism for ion–molecule association. Finally, the role of the reactions in the conversion of Fe+ to atomic Fe in the upper atmosphere is considered.