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Kolmogorov automorphism

Measure preserving automorphism


Measure preserving automorphism

In mathematics, a Kolmogorov automorphism, K-automorphism, K-shift or K-system is an invertible, measure-preserving automorphism defined on a standard probability space that obeys Kolmogorov's zero–one law. All Bernoulli automorphisms are K-automorphisms (one says they have the K-property), but not vice versa. Many ergodic dynamical systems have been shown to have the K-property, although more recent research has shown that many of these are in fact Bernoulli automorphisms.

Although the definition of the K-property seems reasonably general, it stands in sharp distinction to the Bernoulli automorphism. In particular, the Ornstein isomorphism theorem does not apply to K-systems, and so the entropy is not sufficient to classify such systems – there exist uncountably many non-isomorphic K-systems with the same entropy. In essence, the collection of K-systems is large, messy and uncategorized; whereas the B-automorphisms are 'completely' described by Ornstein theory.

Formal definition

Let (X, \mathcal{B}, \mu) be a standard probability space, and let T be an invertible, measure-preserving transformation. Then T is called a K-automorphism, K-transform or K-shift, if there exists a sub-sigma algebra \mathcal{K}\subset\mathcal{B} such that the following three properties hold:

:\mbox{(1) }\mathcal{K}\subset T\mathcal{K}

:\mbox{(2) }\bigvee_{n=0}^\infty T^n \mathcal{K}=\mathcal{B}

:\mbox{(3) }\bigcap_{n=0}^\infty T^{-n} \mathcal{K} = {X,\varnothing}

Here, the symbol \vee is the join of sigma algebras, while \cap is set intersection. The equality should be understood as holding almost everywhere, that is, differing at most on a set of measure zero.

Properties

Assuming that the sigma algebra is not trivial, that is, if \mathcal{B}\ne{X,\varnothing}, then \mathcal{K}\ne T\mathcal{K}. It follows that K-automorphisms are strong mixing.

All Bernoulli automorphisms are K-automorphisms, but not vice versa.

Kolmogorov automorphisms are precisely the natural extensions of exact endomorphisms, i.e. mappings T for which \bigcap_{n=0}^\infty T^{-n} \mathcal{M} consists of measure-zero sets or their complements, where \mathcal{M} is the sigma-algebra of measureable sets,.

References

References

  1. Peter Walters, ''An Introduction to Ergodic Theory'', (1982) Springer-Verlag {{isbn. 0-387-90599-5
  2. V. A. Rohlin, ''Exact endomorphisms of Lebesgue spaces'', Amer. Math. Soc. Transl., Series 2, 39 (1964), 1-36.
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