Hénon–Heiles system
The Hénon-Heiles system is a nonlinear mathematical model that describes the motion of a particle in a two-dimensional potential. It was introduced in 1964 by astronomers Michel Hénon and Carl Heiles to study the dynamics of stars in a galaxy. Still, it has become an example in the study of nonlinear dynamical systems, Hamiltonian chaos, and celestial mechanics.
While at Princeton University in 1962, Michel Hénon and Carl Heiles worked on the non-linear motion of a star around a galactic center with the motion restricted to a plane. In 1964, they published an article titled "The applicability of the third integral of motion: Some numerical experiments". Their original idea was to find a third integral of motion in a galactic dynamics. For this purpose, they considered a simplified two-dimensional, nonlinear, rotational symmetric potential and found that the third integral existed only for a limited number of initial conditions.
In the modern perspective, the initial conditions that do not have the third integral of motion are called chaotic orbits.
Introduction
The Hénon–Heiles potential can be expressed asThe Hénon–Heiles Hamiltonian can be written as
The Hénon–Heiles system is defined by the following four equations:
In the classical chaos community, the value of the parameter is usually taken as unity.
Since HHS is specified in, we need a Hamiltonian with 2 degrees of freedom to model it.
It can be solved for some cases using Painlevé analysis.
Quantum Hénon–Heiles Hamiltonian
In the quantum case, the Hénon–Heiles Hamiltonian can be written as a two-dimensional Schrödinger equation.The corresponding two-dimensional Schrödinger equation is given by