The agreement between the general description of imaging with quasimon
ochromatic spatially partial coherent optical fields and the concept o
f the Schell-model beam is analysed, Radiator pairs of object Schell-m
odel beams at the entrance window of the imaging system yield interfer
ograms with different periods, visibilities and fringe orientation ont
o the entrance pupil, whose superposition determines the intensity dis
tribution there. Furthermore, the structure of the optical field in th
e entrance pupil will be modified by the properties of the imaging sys
tem through their transfer to the exit pupil, Radiator pairs in the ex
it pupil generate interferograms onto the exit window, whose superposi
tion yields the image intensity distribution, In the case of ideal ima
ging, the optical field in the exit window will also be constituted by
image Schell-model beams, which are a scaled, inverted and proportion
al version of the object Schell-model beams, and the superposed interf
erograms in the exit window will be Young's interferograms. (C) 1997 E
lsevier Science Ltd.