Definition of the Subject
An abstract measurable dynamical system consists of a set X (phase space) with a transformation\( { T \colon X \to X } \) (evolution law ortime) and a finite or σ‑finite measure μ on X that specifies a class ofnegligible subsets. Nonsingular ergodic theory studies systems where Trespects μ in a weak sense:the transformation preserves only the class of negligible subsets but it may not preserve μ. This survey is about dynamics and invariants ofnonsingular systems. Such systems model ‘non‐equilibrium’ situations in which events that are impossible at some time remain impossibleat any other time. Of course, the first question that arises is whether it is possible to find an equivalent invariant measure, i. e. pass toa hidden equilibrium without changing the negligible subsets? It turns out that there exist systems which do not admit an equivalent invariant finiteor even σ‑finite measure. They are of our primary interest here. In a way (Baire category) most of...
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- 1.
This abbreviates ‘infinite tensor product of factors of type I’ (came from the theory of von Neumann algebras).
Abbreviations
- Nonsingular dynamical system:
-
Let \( { (X, \mathcal{B}, \mu) } \) be a standard Borel space equipped with a σ‑finite measure. A Borel map \( { T \colon X \to X } \) is a nonsingular transformation of X if for any \( { N \in \mathcal{B} } \), \( { \mu(T^{-1} N) = 0 } \) if and only if \( { \mu(N) = 0 } \). In this case the measure μ is called quasi‐invariant for T; and the quadruple \( { (X, \mathcal{B}, \mu, T) } \) is called a nonsingular dynamical system. If \( { \mu(A) = \mu(T^{-1}A) } \) for all \( { A \in \mathcal{B} } \) then μ is said to be invariant under T or, equivalently, T is measure‐preserving.
- Conservativeness:
-
T is conservative if for all sets A of positive measure there exists an integer \( { n \mathchar"313E 0 } \) such that \( { \mu(A \cap T^{-n} A) \mathchar"313E 0 } \).
- Ergodicity:
-
T is ergodic if every measurable subset A of X that is invariant under T (i. e., \( { T^{-1}A = A } \)) is either μ-null or μ‑conull. Equivalently, every Borel function \( { f \colon X \to \mathbb{R} } \) such that \( { f \circ T = f } \) is constant a. e.
- Types II, \( { \mathrm{II}_1 } \), \( { \mathrm{II}_\infty } \) and III:
-
Suppose that μ is non‐atomic and T ergodic (and hence conservative). If there exists a σ‑finite measure ν on \( { \mathcal{B} } \) which is equivalent to μ and invariant under T then T is said to be of type II. It is easy to see that ν is unique up to scaling. If ν is finite then T is of type II 1. If ν is infinite then T is of type \( { \mathrm{II}_\infty } \). If T is not of type II then T is said to be of type III.
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Danilenko, A.I., Silva, C.E. (2009). Ergodic Theory : Non-singular Transformations . In: Meyers, R. (eds) Encyclopedia of Complexity and Systems Science. Springer, New York, NY. https://doi.org/10.1007/978-0-387-30440-3_183
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