It is shown that, in the paraxial approximation, the intensity distrib
ution produced throughout the space by a partially coherent field depe
nds only on certain projection integrals of the cross spectral density
. These projections, in tum, can be recovered from knowledge of the sp
atial distribution of the optical intensity. This result can enlighten
the recently evidentiated fact that two fields in different states of
coherence can give rise to the same intensity everywhere. Some exampl
es are discussed.