We show that the structure of the fluctuations close to spinodals and mean-
field critical points is qualitatively different from the structure close t
o non-mean-field critical points. This difference has important implication
s for many areas including the formation of glasses in supercooled liquids.
In particular, the divergence of the measured static structure function in
near-mean-field systems close to the glass transition is suppressed relati
ve to the mean-field prediction in systems for which a spatial symmetry is
broken.