The energetics and the electronic structure of AlnC clusters (n=3, 4, 5; 11
, 12, 13) have been studied by a global optimization of their geometry with
out any symmetry constraint. The total energies of these clusters both in n
eutral and charged states are calculated using an all-electron basis and th
e generalized gradient approximation to the density functional theory. Whil
e Al4C and Al12C clusters share some characteristic features of closed shel
l structures, namely enhanced stability and low electron affinity compared
to their neighboring sizes, their ionization potentials exhibit different b
ehavior. These decrease steadily from Al3C to Al5C while that of Al12C is h
igher than its neighbors. Carbon is found to form planar structures in smal
l AlnC clusters (n=3, 4, 5) irrespective of their charge state although neu
tral Al4C possesses a nearly degenerate tetrahedral isomer lying slightly h
igher in energy from the planar configuration. The results agree well with
experimental and previous theoretical data. In larger AlnC (n=11, 12, 13) c
lusters, carbon occupies an interior site. In Al12C, carbon occupies the ce
nter of an icosahedron while it is off-centered in Al11C and Al13C. As an e
lectron is attached, the near degeneracies of the neutral Al4C is lifted wh
ereas nondegenerate isomers of neutral Al12C yield nearly degenerate anions
. Both these features produce complicated photoelectron spectra making iden
tification of their adiabatic electron affinity a difficult problem. With t
he exception of neutral Al12C, the bonding of carbon to aluminum atoms is g
overned primarily by covalent interaction. The above calculations were also
performed with a simplified basis by freezing the atomic cores of aluminum
. In most cases, this simple basis yields results in good agreement with al
l electron calculations. (C) 2001 American Institute of Physics.