Stationary points on the quartet and doublet surfaces of (CH4S)+, on the triplet and singlet surfaces of (CH3S)+,
on the doublet surface of (CH2S)+, and on the singlet and triplet surfaces of (CHS)+ have been examined by
ab initio molecular orbital theory. Equilibrium and saddle point geometries have been located at second-order perturbation theory (UMP2) level using a 6-311++G(d,p) basis set. Relative energies were obtained
by means of extensive quadratic configuration interaction singles and doubles calculations with a
6-311++G(2df,2pd) basis set. On the quartet (CH4S)+ surface, an association complex stabilized by 25.2
kcal/mol with respect to CH4 and S+(4S) has been identified. Owing to its large barrier (55.5 kcal/mol) for
its dissociation, it is expected to be long-lived as assumed by Zakouril et al. (J. Phys. Chem.
1995, 99, 15890)
in their experimental work. On the (CH4S)+ doublet surface, the conventional methanethiol radical cation
(CH3SH+) is more stable than the ylide ion (CH2SH2
+) and depending upon the entrance channel, one can
expect a competitive isomerization and dissociation. Cleavage of the C−H bonds in the ylide ion involves
higher barriers compared to that in CH3SH+. Three stable isomers, viz., CH3S+, CH2SH+, and CHSH2
+, have
been located on the singlet and triplet surfaces of the (CH3S)+ system. While CH2SH+ is more stable on the
singlet surface, CH3S+ is more stable on the triplet surface. The molecular hydrogen elimination requires
higher barriers from all these isomers compared to radical dissociation. CH2S+ is predicted to be more stable
than trans-HCSH+ with a barrier of 51.9 kcal/mol for the rearrangement to the less stable isomer. A significant
barrier to 1,2 hydrogen shift isomerization is predicted on the triplet surface of the HSC+ while that on the
singlet surface is predicted to occur without activation energy. The latter signifies an unstable HSC+ minimum
on the singlet surface.