M. Aschi et F. Grandinetti, Unimolecular decay of the thiomethoxy cation, CH3S+: A computational studyon the detailed mechanistic aspects, J CHEM PHYS, 111(15), 1999, pp. 6759-6768
The unimolecular decay of the triplet thiomethoxy cation CH3S+, ion 1, has
been investigated by density functional theory, ab initio, and Phase-space/
Rice Ramsperger Kassel Marcus (PST/RRKM) calculations. We have first locate
d on the singlet and triplet B3LYP/6-311+G(d,p) [C,H-3,S](+) potential ener
gy surfaces the energy minima and transition structures involved in the low
est energy decompositions of 1, including the loss of H, H-2, and S. We hav
e subsequently located the minimum energy points lying on the B3LYP/6-311+G
(d,p) hyperline of intersection between the singlet and triplet surfaces, u
sing a recently described steepest descent-based method [Theor. Chem. Acc.
99, 95 (1998)]. The total energies of all these species were refined by CCS
D(T)/cc-pVTZ single-point calculations. The obtained potential energy surfa
ce has been used to outline the full kinetic scheme for the unimolecular de
cay of ion 1. The rate constants of the various elementary steps have been
calculated by the PST and the RRKM theory. We used a nonadiabatic version o
f the latter to evaluate the rate constants of the elementary steps which i
nvolve a change in the total spin multiplicity. We found that the two kinet
ically favored decomposition channels are the loss of atomic hydrogen, with
formation of (CH2S+.)-C-2, and molecular hydrogen, with formation of (HCS)-H-1. The former process is predicted to prevail for ions 1 in the lowest
rotational states and with an internal energy content of at least 60 kcal m
ol(-1). The loss of H-2 was found to be by far the prevailing process in th
e time scale of ca. 10(-5) to ca. 10(-6) s from the formation of 1. This is
fully consistent with the experimentally observed exclusive loss of H-2 by
the CH3S+ ions which decompose in the "metastable" time window of the mass
spectrometer. The loss of H-2 from ion 1 with formation of (HCS+)-H-1 may
occur by two distinct "spin-forbidden" paths, i.e., a simple concerted 1,1
H-2 elimination or a 1,2 H shift followed by a 1,2 H-2 elimination from the
singlet mercaptomethyl ion 2. In the metastable time window, these two mec
hanisms may occur alternatively, depending on the degree of rotational exci
tation of 1. (C) 1999 American Institute of Physics. [S0021-9606(99)30237-3
].