  We consider an O(N) version of a massive, interacting, chiral supersymmetry
model solved exactly in the large N limit. We demonstrate that the system
approaches a stable attractor at high energy densities, corresponding to a
non-perturbative state for which the relevant field quanta are massless. The
state is one of spontaneously broken O(N), which, due to the influence of
supersymmetry, does not become restored at high energies. Introducing soft
supersymmetry breaking to the Lagrangian results in scalar masses at the soft
breaking scale m_s independent of the mass scale of supersymmetry mu, with even
smaller masses for the fermions.
