ARE HETEROCYCLIC 2-PI-ELECTRON AROMATIC SYSTEMS HC-GA(H)-CH, M[HGA-C(H)-GAH], [HGA-C(H)-GAH](-), HSI-GA(H)-SIH, M[HGA-SI(H)-GAH] (M = LI, NA, AND K), AND [HGA-SI(H)-GAH](-) STABLE
Ym. Xie et al., ARE HETEROCYCLIC 2-PI-ELECTRON AROMATIC SYSTEMS HC-GA(H)-CH, M[HGA-C(H)-GAH], [HGA-C(H)-GAH](-), HSI-GA(H)-SIH, M[HGA-SI(H)-GAH] (M = LI, NA, AND K), AND [HGA-SI(H)-GAH](-) STABLE, Organometallics, 17(1), 1998, pp. 114-122
Ab initio and density functional (BHLYP, B3LYP, and BP86) quantum mech
anical methods were applied to predict the structures, properties, and
stabilities of HC-Ga(H)-CH, M[H-Ga-C(H)-GaH], [HGa-C(H)-GaH](-), HSi-
Ga(H)-SiH, M[HGa-Si(H)-GaH], and [HGa-Si(H)-GaH](-)(M = Li, Na, K) thr
ee-membered ring systems. These structures derive from the previously
theoretically and experimentally characterized parent homonuclear cycl
ogallenes M-2(GaH)(3). Basis sets of triple-zeta plus double polarizat
ion augmented with diffuse functions (TZ2P + diffuse) quality were emp
loyed at self-consistent field (SCF) and density functional levels of
theory. Equilibrium geometries, harmonic vibrational frequencies, and
chemical shifts are reported to facilitate experimental verification o
f the computed structures. All title compounds are minima and their ge
ometries as well as their properties compare well with the cyclogallen
e three-membered ring compounds M-2(GaH)(3). Singly charged [HGa- Si(H
)-GaH](-) and even neutral HSi-Ga(H)-SiH may well be feasible experime
ntal targets. The large negative nucleus independent chemical shifts (
NICS), used as a criterion for aromatic cyclic delocalization, suggest
that all title compounds are aromatic.