Two solid structures, a bcc orientationally disordered phase and a strained
monoclinic orientationally ordered phase, may coexist for clusters of octa
hedral molecules. However, this coexistence is more difficult to observe in
computer simulations of SF6 clusters than of TeF6 clusters although the SF
6 and TeF6 molecules have the same symmetry. This study finds why this diff
erence occurs. On the potential surface of the (SF6)(89) cluster the relati
ve energies of most of the linked minima differ only slightly, and the barr
iers between them are low. An exception is the global minimum, correspondin
g to a completely orientationally ordered phase. At relevant temperatures,
the fraction of the available phase space of the (SF6)(89) cluster correspo
nding to a partially ordered structure is smaller than it is for the (TeF6)
(89) cluster. In simulations, the latter readily exhibits coexistence of th
e ordered and disordered forms due to better separation of the higher-energ
y local minima and the larger available phase space volume. (C) 2001 Americ
an Institute of Physics.