English

Degenerate bifurcation points of periodic solutions of autonomous Hamiltonian systems

Classical Analysis and ODEs 2007-05-23 v1

Abstract

We study connected branches of non-constant {2π2\pi-pe}riodic solutions of the Hamilton equation \begin{displaymath} \dot{x}(t)=\lambda J\nabla H(x(t)), \end{displaymath} where λ\halfline,\lambda\in\halfline, HC2(Rn×Rn,R)H\in C^2(\R^n\times\R^n,\R) and 2H(x0)=[A00B] \displaystyle \nabla^2H(x_0)= [ \begin{array}{cc} A&0 0&B \end{array} ] for x0H1(0).x_0\in\nabla H^{-1}(0). The Hessian 2H(x0)\nabla^2H(x_0) can be singular. We formulate sufficient conditions for the existence of such branches bifurcating from given (x0,λ0).(x_0,\lambda_0). As a consequence we prove theorems concerning the existence of connected branches of arbitrary periodic nonstationary trajectories of the Hamiltonian system x˙(t)=JH(x(t))\dot{x}(t)=J\nabla H(x(t)) emanating from x0.x_0. We describe also minimal periods of trajectories near x0.x_0.

Keywords

Cite

@article{arxiv.math/0604288,
  title  = {Degenerate bifurcation points of periodic solutions of autonomous Hamiltonian systems},
  author = {W. Radzki and S. Rybicki},
  journal= {arXiv preprint arXiv:math/0604288},
  year   = {2007}
}

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18 pages