Nonwandering Point

In dynamical systems and ergodic theory, the concept of a wandering set formalizes a certain idea of movement and mixing. When a dynamical system has a wandering set of non-zero measure, then the system is a dissipative system. This is the opposite of a conservative system, to which the Poincaré recurrence theorem applies. Intuitively, the connection between wandering sets and dissipation is easily understood: if a portion of the phase space "wanders away" during normal time-evolution of the system, and is never visited again, then the system is dissipative. The language of wandering sets can be used to give a precise, mathematical definition to the concept of a dissipative system. The notion of wandering sets in phase space was introduced by Birkhoff in 1927.

Wandering points

A common, discrete-time definition of wandering sets starts with a map $f:X\to X$ of a topological space ''X''. A point $x\in X$ is said to be a wandering point if there is a neighbourhood ''U'' of ''x'' and a positive integer ''N'' such that for all $n>N$, the iterated map is non-intersecting:

:$f^n(U) \cap U = \varnothing.$

A handier definition requires only that the intersection have measure zero. To be precise, the definition requires that ''X'' be a measure space, i.e. part of a triple $(X,\Sigma,\mu)$ of Borel sets $\Sigma$ and a measure $\mu$ such that

:$\mu\left(f^n(U) \cap U \right) = 0,$

for all $n>N$. Similarly, a continuous-time system will have a map $\varphi_t:X\to X$ defining the time evolution or flow of the system, with the time-evolution operator $\varphi$ being a one-parameter continuous abelian group action on ''X'':

:$\varphi_ = \varphi_t \circ \varphi_s.$

In such a case, a wandering point $x\in X$ will have a neighbourhood ''U'' of ''x'' and a time ''T'' such that for all times $t>T$, the time-evolved map is of measure zero:

:$\mu\left(\varphi_t(U) \cap U \right) = 0.$

These simpler definitions may be fully generalized to the group action of a topological group. Let $\Omega=(X,\Sigma,\mu)$ be a measure space, that is, a set with a measure defined on its Borel subsets. Let $\Gamma$ be a group acting on that set. Given a point $x \in \Omega$, the set

:$\$

is called the trajectory or orbit of the point ''x''.

An element $x \in \Omega$ is called a wandering point if there exists a neighborhood ''U'' of ''x'' and a neighborhood ''V'' of the identity in $\Gamma$ such that
:$\mu\left(\gamma \cdot U \cap U\right)=0$

for all $\gamma \in \Gamma-V$.

Non-wandering points

A non-wandering point is the opposite. In the discrete case, $x\in X$ is non-wandering if, for every open set ''U'' containing ''x'' and every ''N'' > 0, there is some ''n'' > ''N'' such that

:$\mu\left(f^n(U)\cap U \right) > 0.$

Similar definitions follow for the continuous-time and discrete and continuous group actions.

Wandering sets and dissipative systems

A wandering set is a collection of wandering points. More precisely, a subset ''W'' of $\Omega$ is a wandering set under the action of a discrete group $\Gamma$ if ''W'' is measurable and if, for any $\gamma \in \Gamma - \$ the intersection

:$\gamma W \cap W$

is a set of measure zero.

The concept of a wandering set is in a sense dual to the ideas expressed in the Poincaré recurrence theorem. If there exists a wandering set of positive measure, then the action of $\Gamma$ is said to be ', and the dynamical system $(\Omega, \Gamma)$ is said to be a dissipative system. If there is no such wandering set, the action is said to be ', and the system is a conservative system. For example, any system for which the Poincaré recurrence theorem holds cannot have, by definition, a wandering set of positive measure; and is thus an example of a conservative system.

Define the trajectory of a wandering set ''W'' as

:$W^* = \bigcup_ \;\; \gamma W.$

The action of $\Gamma$ is said to be ' if there exists a wandering set ''W'' of positive measure, such that the orbit $W^*$ is almost-everywhere equal to $\Omega$, that is, if

:$\Omega - W^*$

is a set of measure zero.

The Hopf decomposition states that every measure space with a non-singular transformation can be decomposed into an invariant conservative set and an invariant wandering set.

See also

* No wandering domain theorem

References

*
* Alexandre I. Danilenko and Cesar E. Silva (8 April 2009).
Ergodic theory: Nonsingular transformations
'; Se
Arxiv arXiv:0803.2424

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{{DEFAULTSORT:Wandering Set
Ergodic theory
Limit sets
Dynamical systems