  Gibbs' phase rule states that two-phase coexistence of a single-component
system, characterized by an n-dimensional parameter-space, may occur in an
n-1-dimensional region. For example, the two equilibrium phases of the Ising
model coexist on a line in the temperature-magnetic-field phase diagram.
Nonequilibrium systems may violate this rule and several models, where phase
coexistence occurs over a finite (n-dimensional) region of the parameter space,
have been reported. The first example of this behaviour was found in Toom's
model [Toom,Geoff,GG], that exhibits generic bistability, i.e. two-phase
coexistence over a finite region of its two-dimensional parameter space (see
Section 1). In addition to its interest as a genuine nonequilibrium property,
generic multistability, defined as a generalization of bistability, is both of
practical and theoretical relevance. In particular, it has been used recently
to argue that some complex structures appearing in nature could be truly stable
rather than metastable (with important applications in theoretical biology),
and as the theoretical basis for an error-correction method in computer science
(see [GG,Gacs] for an illuminating and pedagogical discussion of these ideas).
