The pressure-induced diatomic-to-monatomic phase transition is investigated
in a model crystal based on a Tersoff-type interatomic potential. The phas
e transition is first-order when the many-body interaction is long-ranged,
but second-order when the many-body interaction is short-ranged. The change
in the order of the phase transition is related to a crossing of the stabi
lity limits of the diatomic structure with respect to fluctuations of volum
e and with respect to fluctuations of the internal parameter. (C) 2001 Else
vier Science B.V. All rights reserved.