We study a general field theory of a scalar held coupled to gravity through
a quadratic Gauss-Bonnet term xi(phi)R-GB(2). The coupling function has th
e form xi(phi) = phi(n), where n is a positive integer, in the absence of t
he Gauss-Bonnet term, the cosmological solutions for an empty universe and
a universe dominated by the energy-momentum tensor of a scalar field are al
ways characterized by the occurrence of a true cosmological singularity. By
employing analytical, and numerical methods, we show that, in the presence
of the quadratic Gauss-Bonnet term. for the dual case of even n, the set o
f solutions of the classical equations of motion in a curved FRW background
includes singularity-free cosmological solutions. The singular solutions a
re shown to be confined in a part of the phase space of the theory allowing
the nan-singular solutions to fill the rest of the space. We conjecture th
at the same theory with a general coupling function that satisfies certain
criteria may lead to non-singular cosmological solutions. [S0556-2821(99)01
804-4].