We present results of Monte Carlo simulations of a homopolymer with th
ree-body interactions on a lattice. At equilibrium we find three colla
psed phases with different orientational order. The first one may be d
escribed as a conventional phase with effective three-body attraction.
Two other phases are observed in the region of the phase diagram corr
esponding to three-body repulsion. The second phase is characterized b
y local orientational order within the globule. The third one possesse
s global orientational order and it appears to be analogous to nematic
phase of a liquid crystal. Kinetics of the collapse transition to the
phase III is crucially different from that of phase I and II due to f
ormation of clusters with different orientations at the intermediate s
tage. This is the origin of a metastable long-lived state in kinetics.
(C) 1996 American Institute of Physics.