Abstract

AbstractWe prove the existence and multiplicity of subharmonic solutions for Hamiltonian systems obtained as perturbations ofNplanar uncoupled systems which, e.g., model some type of asymmetric oscillators. The nonlinearities are assumed to satisfy Landesman–Lazer conditions at the zero eigenvalue, and to have some kind of sublinear behavior at infinity. The proof is carried out by the use of a generalized version of the Poincaré–Birkhoff Theorem. Different situations, including Lotka–Volterra systems, or systems with singularities, are also illustrated.

Highlights

  • Introduction and main resultWe are interested in finding periodic solutions of a nonautonomous Hamiltonian system in R2N

  • We prove the existence and multiplicity of subharmonic solutions for Hamiltonian systems obtained as perturbations of N planar uncoupled systems which, e.g., model some type of asymmetric oscillators

  • In assumption (A2) we have the well-known Landesman–Lazer conditions: they will force the large-amplitude solutions of the uncoupled planar systems to rotate around the origin

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Summary

Introduction and main result

We are interested in finding periodic solutions of a nonautonomous Hamiltonian system in R2N. In assumption (A2) we have the well-known Landesman–Lazer conditions: they will force the large-amplitude solutions of the uncoupled planar systems to rotate around the origin. This property, which might have an independent interest, has already been exploited in [3, 4, 9, 23], and is stated in Lemma 2.5 below. We will find a T-periodic solution of (1.1) with ε = 0, which will be used in a change of variables, in order to have the origin as a constant solution This will enable us to compute the rotation number on each planar subsystem, so to apply a generalized version of the Poincaré–Birkhoff Theorem recently obtained in [14]. We have proved that system (2.2) has a T-periodic solution

A change of variables
The rotational lemma
End of the proof
Proof of the corollaries and final remarks
Full Text
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