Ab initio calculations of closo-alane and gallane A(6)H(6)(2-) and A(12)H(12)(2-) anions and Al12H12L salts with L = Li+, Na+, Be2+, Mg2+, Al+, Al3+ and H+ cations coordinated inside and outside the icosahedral Al-12 cluster
Op. Charkin et al., Ab initio calculations of closo-alane and gallane A(6)H(6)(2-) and A(12)H(12)(2-) anions and Al12H12L salts with L = Li+, Na+, Be2+, Mg2+, Al+, Al3+ and H+ cations coordinated inside and outside the icosahedral Al-12 cluster, RUSS J IN C, 45(10), 2000, pp. 1539-1551
Ab initio calculations of geometrical, vibrational, magnetic, and energetic
parameters of closo-alane and gallane Al6H62-, Ga6H62-, Al12H122-, and Ga1
2H122- dianions and Al6H6L and Al12H12L salts with light alkali-metal and a
lkaline-earth cations or proton (L = Li+, Na+, Be2+, Mg2+, Al+, Al3+, H+) w
ere performed at the Hartree-Fock (HF) level of theory and within the frame
work of the density functional theory (B3LYP) with 6-31G" and 6-311+G"" bas
is sets. It was found that the A112H12 a"d Gal2H12 structures with close R(
AlAl) and R(GaGa) distances. The most favorable structures of Al12H12L (and
, probably, of Ga12H12L) salts are tridentate isomers C-3v(t) with the L ca
tion coordinated to the center of one of the 20 equivalent faces (Al-3). Th
e potential-energy barrier (bidentate structure C-2v(b)) between the C-3v(t
) structures is small and, similarly to borane analogues, alane salts shoul
d be nonrigid from the standpoint of migration of the outer cation around t
he icosahedral [Al-12] cluster from one face to another over the adjacent e
dge. As in the case of closo-boranes, the symmetrical Ih structure with the
cation at the center of the Al-12 icosahedron is untypical for Al12H12L mo
lecules (lies very high and possessed six or more imaginary frequencies) wi
th hard bases L = H+, Be2+, and Al3+, which disturb the system of bonding M
Os of the cluster core. In contrast to boranes, the endohedral structure of
salts with softer bases Na+, Li+, and Mg2+ corresponds to a local minimum,
which is 59, 24, and 41 kcal/mol less stable than the C-3v(t) structure, r
espectively, and possesses relatively high frequencies of bending vibration
s. This intermediate is stabilized kinetically and can exist. The differenc
es in vibrational spectra and in NMR chemical shifts of I-h and C-3v(t) iso
mers are considered, along with the possibility of their identification by
IR and NMR spectroscopy.