Internal energy selection in vacuum ultraviolet photoionization of ethanol and ethanol dimers

Abstract

Internal energy selected ethanol monomer and ethanol dimer ions were prepared by threshold photoionization of a supersonic molecular beam seeded with ethanol. The dissociative photoionization processes of the monomer, the lowest-energy CH3-loss channel of the dimer, and the fragmentation of larger clusters were found to be disjunct from the ionization onset to about 12 eV, which made it possible to determine the 0 K appearance energy of C-C bond breaking in the H-donor unit of the ethanol dimer cation as 9.719 ± 0.004 eV. This reaction energy is used together with ab initio calculations in a thermochemical cycle to determine the binding energy change from the neutral ethanol dimer to a protonated ethanol-formaldehyde adduct. The cycle also shows general agreement between experiment, theory, and previously published enthalpies of formation. The role of the initial ionization site, or rather the initial photoion state, is also discussed based on the dimer breakdown diagram and excited state calculations. There is no evidence for isolated state behavior, and the ethanol dimer dissociative photoionization processes appear to be governed by statistical theory and the ground electronic state of the ion. In the monomer breakdown diagram, the smoothly changing branching ratio between H and CH3 loss is at odds with rate theory predictions, and shows that none of the currently employed few-parameter rate models, appropriate for experimental rate curve fitting, yields a correct description for this process in the experimental energy range.

Dissociative Photoionization of Dimethyl Carbonate: The More It Is Cut, the Bigger the Fragment Ion

“…Furthermore, the fragmentation of the unseen intermediate ethanol cation at m/z = 46 may also contribute to the m/z = 31 signal by methyl loss at higher energies. 73 3.5. Thermochemical Calculations.…”

“…This is probably due to the fact that CH 2 OH + is also a minor dissociation product of ethylene glycol cation, a channel unaccounted for in the statistical model and in competition with m / z = 33 formation. Furthermore, the fragmentation of the unseen intermediate ethanol cation at m / z = 46 may also contribute to the m / z = 31 signal by methyl loss at higher energies …”