We study a three-dimensional conformal field theory in terms of its pa
rtition function on arbitrary curved spaces. The large N limit of the
non-linear sigma model at the non-trivial fixed point is shown to be a
n example of a conformal field theory, using zeta function regularizat
ion. We compute the critical properties of this model in various space
s of constant curvature (R(2) X S-1, S-1 X S-1 X R, S-2 X R, H-2 X R,
S-1 X S-1 X S-1 and S-2 X S-1) and we argue that what distinguishes th
e different cases is not the Riemann curvature but the conformal class
of the metric. In the case H-2 X R (constant negative curvature), the
O(N) symmetry is spontaneously broken at the critical point. In the c
ase S-2 X R (constant positive curvature) we find that the free energy
vanishes, consistent with conformal equivalence of this manifold to R
(3), although the correlation length is finite. In the zero-curvature
cases, the correlation length is finite due to finite size effects. Th
ese results describe two-dimensional quantum phase transitions or thre
e-dimensional classical ones.