Homoclinic connection

{{ safesubst:#invoke:Unsubst||$N=Unreferenced |date=__DATE__ |$B= {{#invoke:Message box|ambox}} }} In dynamical systems, a branch of mathematics, a structure formed from the stable manifold and unstable manifold of a fixed point.

File:Connections.png
Homoclinic, Heteroclinic Connections and Intersections.

Definition for maps

Let ${\displaystyle f:M\to M}$ be a map defined on a manifold ${\displaystyle M}$, with a fixed point ${\displaystyle p}$. Let ${\displaystyle W^{s}(f,p)}$ and ${\displaystyle W^{u}(f,p)}$ be the stable manifold and the unstable manifold of the fixed point ${\displaystyle P}$, respectively. Let ${\displaystyle V}$ be an connected invariant manifold such that

${\displaystyle V\subseteq W^{s}(f,p)\cup W^{u}(f,p)}$

Then ${\displaystyle V}$ is called a homoclinic connection.

Heteroclinic connection

It is a similar notion, but it refers to two fixed points, ${\displaystyle p}$ and ${\displaystyle q}$. The condition satisfied by ${\displaystyle V}$ is replaced with:

${\displaystyle V\subseteq W^{s}(f,p)\cup W^{u}(f,q)}$

This notion is not symmetric with respect to ${\displaystyle p}$ and ${\displaystyle q}$.

Homoclinic and heteroclinic intersections

When the invariant manifolds ${\displaystyle W^{s}(f,p)}$ and ${\displaystyle W^{u}(f,q)}$, possibly with ${\displaystyle p=q}$, intersect but there is no homoclinic/heteroclinic connection, a different structure is formed by the two manifolds, sometimes referred to as the homoclinic/heteroclinic tangle. The figure has a conceptual drawing illustrating their complicated structure. The theoretical result supporting the drawing is the lambda-lemma. Homoclinic tangles are always accompanied by a Smale horseshoe.

Definition for continuous flows

For continuous flows, the definition is essentially the same.

2. Historically, the first case considered was that of a continuous flow on the plane, induced by an ordinary differential equation. In this case, a homoclinic connection is a single trajectory that converges to the fixed point ${\displaystyle p}$ both forwards and backwards in time. A pendulum in the absence of friction is an example of a mechanical system that does have a homoclinic connection. When the pendulum is released from the top position (the point of highest potential energy), with infinitesimally small velocity, the pendulum will return to the same position. Upon return, it will have exactly the same velocity. The time it will take to return will increase to ${\displaystyle \infty }$ as the initial velocity goes to zero. One of the demonstrations in the pendulum article exhibits this behavior.