I. Dance, NANOCRYSTAL [TI14C13] TO METALLOCARBOHEDRENE [TI8C13] - STRUCTURAL PRINCIPLES AND MECHANISM, Journal of the American Chemical Society, 118(11), 1996, pp. 2699-2707
Gradient-corrected density functional calculations have characterized
the geometric and electronic structures of the metal-carbon clusters [
Ti14Cr13](0,+) and [Ti8C13](0,+) and the intermediates TixC13 in the s
equence of photoextrusions of Ti atoms from [Ti14C13](+) to [Ti8C13](). Ti14C13 is a vertex-contracted ''nanocrystal'' fragment of the face
-centered cubic TiC lattice, with low-lying spin states, while Ti8C13
is a C-c-centered tetra-Ti-o-capped Ti-4(i) tetrahedron with C-2 group
s cradled in six (Ti2Ti2o)-Ti-i butterflies and has a large HOMO-LUMO
gap. This sequence of six photodissociations of Ti atoms is significan
t because it involves the transformation of a fragment of a non-molecu
lar lattice structure to a molecular cluster structure and the formati
on of six C-C bonds on the surface. The transformation is most endergo
nic in the first stage to [Ti13C13](+), and decreasingly endergonic to
[Ti12C13](+) and [Ti11C13](+). The geometry changes are concerted, wi
th each intermediate partly prepared for the next extrusion of Ti, and
the central C-c atom plays a significant role in the substantial stru
ctural rearrangements. The high symmetry (O-h) of [Ti14C13](+) is comp
letely lost at [Ti12C13](+), but there is recovery of C-3v symmetry at
the intermediate[Ti11C13](+) which already has in place the four C-c-
Ti-i bonds and the Ti-i(C-2)(3)(Ti-o)(3) face characteristic of [Ti8C1
3](+). Energy changes follow the geometry changes.