We consider a classical spin system on the hypercubic lattice with a g
eneral interaction of the form [GRAPHICS] where s(x) epsilon{-1, +1} a
re the spin variables, beta is the inverse temperature, h is the magne
tic field, and lambda(A), are translation-invariant coupling constants
satisfying lambda(A) = 0 if diam A > 1. No symmetry relating the conf
igurations s = {s(x)} and -s = { -s(x)} is assumed. In dimension d gre
ater than or equal to 3, we construct low-temperature states which bre
ak the translation invariance of the system by introducing so called D
obrushin boundary conditions which force a horizontal interface into t
he system. In contrast to previous constructions, our methods work equ
ally well for complex interactions, and should therefore be generaliza
ble to quantum spin systems.