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.[1] 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.
Let
(X,l{B},\mu)
T
T
l{K}\subsetl{B}
(1)l{K}\subsetTl{K}
infty | |
(2)vee | |
n=0 |
Tnl{K}=l{B}
infty | |
(3)cap | |
n=0 |
T-nl{K}=\{X,\varnothing\}
Here, the symbol
\vee
\cap
Assuming that the sigma algebra is not trivial, that is, if
l{B}\ne\{X,\varnothing\}
l{K}\neTl{K}.
All Bernoulli automorphisms are K-automorphisms, but not vice versa.
Kolmogorov automorphisms are precisely the natural extensions of exact endomorphisms,[2] i.e. mappings
T
infty | |
cap | |
n=0 |
T-nl{M}
l{M}