2008, Vol.11, No.2, pp.269-273
We consider the Hamiltonian system derived from spatially
homogenious solutions of the Landau-Lifshitz-Gilbert equation for
the macroscopic magnetization of the ferromagnetic system without
damping. The static field also breaks the plane symmetry
Sz-Sz. We find the continued periodic orbits from
the unperturbed integrable part to the perturbed system, with the
help of first order perturbation theory. By transforming the one
degree of freedom time dependent system into a two degree of
freedom system and with the help of second order perturbation
theory we predict the continuation of extra periodic orbits. We
also find the stability of the continued periodic orbits of the
first order perturbation theory. We finally find the value of the
perturbative parameter where the main resonances overlap end
therefore global chaos appears.
Key words:
macroscopic magnetization, hamiltonian systems,
continuation of periodic orbits, overlapping of resonances
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