Hidden toric symmetry and structural stability of singularities in integrable systems

Abstract

The goal of the paper is to develop a systematic approach to the study of (perhaps degenerate) singularities of integrable systems and their structural stability. As the main tool, we use "hidden" system-preserving torus actions near singular orbits. We give sufficient conditions for the existence of such actions and show that they are persistent under integrable perturbations. We find toric symmetries for several infinite series of singularities and prove, as an application, structural stability of Kalashnikov's parabolic orbits with resonances in the real-analytic case. We also classify all Hamiltonian $k$-torus actions near a singular orbit on a symplectic manifold $M^{2n}$ (or on its complexification) and prove that the normal forms of these actions are persistent under small perturbations. As a by-product, we prove an equivariant version of the Vey theorem (1978) about local symplectic normal form of nondegenerate singularities.

arXiv comment69 pages, 2 tables, 1 figure

References in corpus (6)

• Torus Actions and Integrable Systems
• Symplectic invariants for parabolic orbits and cusp singularities of integrable systems with two degrees of freedom
• Classification of Hamiltonian torus actions with two dimensional quotients
• The Liouville-type theorem for integrable Hamiltonian systems with incomplete flows
• Existence of a smooth Hamiltonian circle action near parabolic orbits
• (Vanishing) Twist in the Saddle-Centre and Period-Doubling Bifurcation

Cited by in corpus (6)

• Existence of a smooth Hamiltonian circle action near parabolic orbits
• Structurally stable non-degenerate singularities of integrable systems
• Bifurcations of magnetic geodesic flows on surfaces of revolution
• Symplectic classification for universal unfoldings of $A_n$ singularities in integrable systems
• Parabolicity of degenerate singularities of axisymmetric Zhukovsky case
• $C^{\infty }$ symplectic invariants of parabolic orbits and flaps in integrable Hamiltonian systems