The Hénon-Heiles system is a Hamiltonian system with two degrees of freedom and Hamiltonian function
Its Hamilton's equations give and . Its potential energy combines an isotropic quadratic minimum with a cubic interaction.
The potential energy in the Hénon-Heiles system has the following expression in polar coordinates:
so it is invariant under rotation through . Solving gives a strict local minimum at the origin and three saddle points, at and . All three saddle points have value . Their common level set factors exactly:
Thus this level set is the union of the three lines and . They bound an equilateral triangle containing the local minimum. The Hessian matrix is the identity at the origin; at each of the other three stationary points it has eigenvalues and . For energies , the central accessible region is bounded; above that value the three saddle passages allow paths from the centre to arbitrarily large radius. This follows directly from the radial potential: in each direction with , its radial maximum occurs at , with value .
The autonomous planar system , preserves . Its origin is a center equilibrium and are saddle equilibria. The level is : its two inner arcs are heteroclinic orbits enclosing periodic motion, while its outer branches connect saddles to escaping trajectories. Since on escaping levels, infinity is reached in finite time. Adding to gives , so positive produces outward crossing of central levels and breaks the equal-energy heteroclinic connections.

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A Hamiltonian system is a mathematical formulation of classical mechanics that describes the evolution of a physical system in terms of its momenta and positions. It is based on Hamiltonian mechanics, which is an alternative to the more common Lagrangian mechanics.