Carbon bond and hydrogen bond are
common noncovalent interactions;
although recent advances on these interactions have been achieved
in both the experimental and computational aspects, little is known
about the conversion mechanism between them. Here, MP2 calculations
with aug-cc-pVDZ basis set (aug-cc-pVDZ-pp for element Sn) were used
to optimize the geometric configurations of the hydrogen-bonded complexes
MH
3
F···HCN (M = C, Si, Ge, and Sn), carbon-bonded
complexes HCN···MH
3
F (M = C, Si, Ge, and
Sn), and transition states; the conversion mechanism between these
two types of interactions has been carried out. The molecular electrostatic
potential, especially the σ-hole, is directly related to the
flatten degree of intrinsic reaction coordinate (IRC) curve. The energy
barriers from the hydrogen-bonded complexes to the carbon-bonded complexes
are 6.99, 7.73, 10.56, and 13.59 kJ·mol
–1
.
The energy barriers from the carbon-bonded complexes to the hydrogen-bonded
complexes are 4.65, 7.81, 9.10, and 13.04 kJ·mol
–1
. The breakage and formation of the bonds along the reaction paths
have been discussed by the topological analysis of electronic density.
The energy barriers are obviously related to the width of the structure
transition region (STR). For the first derivative curve of IRC energy
surface versus reaction coordinate, there is a maximum peak and a
minimum peak, reflecting the structural transition states in the ring
STRs.