We study a globally coupled version of the complex Ginzburg-Landau equ
ation (GC-CGLE) which consists of a large number N of identical two-di
mensional oscillators coupled through their mean amplitude, Depending
on parameter values, different dynamical regimes are attained. We focu
s particularly on an interesting regime where the individual oscillato
rs follow erratic motion but in a sufficiently coherent way so that th
e average motion does not vanish when N becomes large and is also chao
tic. A simple description of this state is proposed by considering the
motion of a single forced two-dimensional system which has both a lim
it cycle and a fixed point as stable attractors. Determining which of
these two deterministic attractors is selected by a weak noise and how
this depends on the parameter of the reduced system allows us to dete
rmine self-consistently the average amplitude and dominant frequency o
f the collective behaviour of the full system. Finally, we show that a
dding a small noise to the GC-CGLE transforms the chaotic collective b
ehaviour into a purely periodic one.