When two waves propagating in a one-dimensional medium are locked together
as a composite wave, a natural question arises as to whether the new wave i
s stable. An interesting and novel instability mechanism is exposed here in
which a cascade of eigenvalues accumulates at a distinguished point in the
unstable half plane. The underlying assumption is that the transition betw
een the two waves occurs at an unstable, homogeneous steady state of the pa
rtial differential equations. This causes the individual waves to have an u
nstable continuous spectrum, but the instability of the full wave cannot be
predicted from the configuration of these spectra alone. (C) 2000 Elsevier
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