In this paper, we study adiabatic Hamiltonian systems including those
subject to small-amplitude forcing and damping. It is known that simpl
e zeroes of the adiabatic Poincare-Arnold-Melnikov function imply the
existence of primary intersection points of the stable and unstable ma
nifolds of hyperbolic orbits. Hen, we present an Nth-order Melnikov fu
nction whose simple zeroes correspond to Nth-order transverse intersec
tion points and hence to N-pulse homoclinic orbits. Using this functio
n, it can be shown that N-pulse homoclinic orbits arise in a plethora
of adiabatic models, including systems with slowly varying potentials.
The theory is illustrated on a damped Hamiltonian system with a slowl
y varying cubic potential. In addition, the Nth-order adiabatic Melnik
ov function is useful for showing the existence of multi-pulse resonan
t periodic orbits in the special class of slow, time-periodic systems.
(C) 1996 American Institute of Physics.