Phase transitions of nuclear matter to the quark-gluon plasma with sub
sequent restoration of chiral symmetry have been widely discussed in t
he literature. We investigate the possibility For occurrence of dense
nuclear matter with a dibaryon Bose-Einstein condensate as an intermed
iate state below the quark-gluon phase transition. An exact analysis o
f this state of matter is presented in a one-dimensional model. The an
alysis is based on a reduction of the quantization rules For the N-bod
y problem to N coupled algebraic transcendental equations. We observe
that when the Fermi momentum approaches the resonance momentum, the on
e-particle distribution function increases near the Fermi surface. Whe
n the Fermi momentum is increased beyond the resonance momentum, the e
quation of state becomes softer. The observed behavior can be interpre
ted in terms of formation of a Bose-Einstein condensate of two-fermion
resonances (e.g., dibaryons). Ln cold nuclear matter, it should occur
at 2(m(N)+epsilon(F))greater than or equal to m(D) where m(N) and m(D
) are the nucleon and dibaryon masses and epsilon(F) is the nucleon Fe
rmi energy. (C) 1997 Academic Press.