Abstract
We study Hamiltonian systems with two degrees of freedom near an equilibrium point, when the linearized system is not semisimple. The invariants of the adjoint linear system determine the normal form of the full Hamiltonian system. For work on stability or bifurcation the problem is typically reduced to a semisimple (diagonalizable) case. Here we study the nilpotent cases directly by looking at the Poisson algebra generated by the polynomials of the linear system and its adjoint.
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Notes
It would also be possible to use \(\mathbf{H}=a(xX+yY)+\delta xY\) with \(a>0\) and \(\delta=\pm 1\), so that only positive times have to be taken into account.
Indeed, for a differential equation of the form \(\dot{z}=\nabla L\times\nabla H\) both \(L\) and \(H\) are integrals since \(\dot{L}=\nabla L\cdot\dot{z}=\nabla L\cdot\nabla H\times\nabla L=0\) (the triple product with two common terms is zero). Similarly for \(H\).
Another possibility is to use \(\mathbb{H}=a(xY-Xy)+\frac{\delta}{2}(x^{2}+y^{2})\) with \(a>0,\delta=\pm 1\) so that only positive time has to be considered.
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MSC2010
34C40, 37C80, 37J15, 70H85
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Meyer, K.R., Schmidt, D.S. Normal Forms for Hamiltonian Systems in Some Nilpotent Cases. Regul. Chaot. Dyn. 27, 538–560 (2022). https://doi.org/10.1134/S1560354722050033
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DOI: https://doi.org/10.1134/S1560354722050033