The coherent three-wave interaction, with linear growth in the higher
frequency wave and damping in the two other waves, is reconsidered; fo
r equal dampings, the resulting three-dimensional (3-D) flow of a rela
tive phase and just two amplitudes behaved chaotically, no matter how
small the growth of the unstable wave. The general case of different d
ampings is studied here to test whether, and how, that hard scenario f
or chaos is preserved in passing from 3-D to four-dimensional flows. I
t is found that the wave with higher damping is partially slaved to th
e other damped wave; this retains a feature of the original problem (a
n invariant surface that meets an unstable fixed point, at zero growth
rate) that gave rise to the chaotic attractor and determined its stru
cture, and suggests that the sudden transition to chaos should appear
in more complex wave interactions. (C) 1998 American Institute of Phys
ics.