This paper is concerned with the downstream evolution of a resonant tr
iad of initially non-interacting linear instability waves in a boundar
y layer with a weak adverse pressure gradient. The triad consists of a
two-dimensional fundamental mode and a pair of equal-amplitude obliqu
e modes that form a subharmonic standing wave in the spanwise directio
n. The growth rates are small and there is a well-defined common criti
cal layer for these waves. As in Goldstein & Lee (1992), the wave inte
raction takes place entirely within this critical layer and is initial
ly of the parametric-resonance type. This enhances the spatial growth
rate of the subharmonic but does not affect that of the fundamental. H
owever, in contrast to Goldstein & Lee (1992), the initial subharmonic
amplitude is assumed to be small enough so that the fundamental can b
ecome nonlinear within its own critical layer before it is affected by
the subharmonic. The subharmonic evolution is then dominated by the p
arametric-resonance effects and occurs on a much shorter streamwise sc
ale than that of the fundamental. The subharmonic amplitude continues
to increase during this parametric-resonance stage - even as the growt
h rate of the fundamental approaches zero - and the subharmonic eventu
ally becomes large enough to influence the fundamental which causes bo
th waves to evolve on the same shorter streamwise scale.