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Wandering set : ウィキペディア英語版
Wandering set
In those branches of mathematics called dynamical systems and ergodic theory, the concept of a wandering set formalizes a certain idea of movement and mixing in such systems. When a dynamical system has a wandering set of non-zero measure, then the system is a dissipative system. This is very much the opposite of a conservative system, for which the ideas of the Poincaré recurrence theorem apply. 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.\,
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.

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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