Math 2.0

Dynamical systems and ergodic theory Ergodic theory Theorem

Ornstein isomorphism theorem

Builds on Bernoulli schemeKolmogorov–Sinai entropyMeasure-preserving transformationKolmogorov automorphism

Statement

Let p=(p1,…,pk)p = (p_1, \dots, p_k) and q=(q1,…,ql)q = (q_1, \dots, q_l) be probability vectors, and let B(p)B(p) and B(q)B(q) be the two-sided Bernoulli schemes they define. Two invertible measure-preserving transformations TT on (X,μ)(X, \mu) and SS on (Y,ν)(Y, \nu) are isomorphic if the following holds. There are sets X0⊆XX_0 \subseteq X, Y0⊆YY_0 \subseteq Y of full measure and a measurable bijection φ ⁣:X0→Y0\varphi \colon X_0 \to Y_0 with measurable inverse. It satisfies ν(φ(A))=μ(A)\nu(\varphi(A)) = \mu(A) for measurable A⊆X0A \subseteq X_0, and φ∘T=S∘φ\varphi \circ T = S \circ \varphi on X0X_0. Then B(p)B(p) and B(q)B(q) are isomorphic if and only if they have the same Kolmogorov–Sinai entropy, that is, −∑i=1kpilog⁡pi=−∑j=1lqjlog⁡qj.-\sum_{i=1}^{k} p_i \log p_i = -\sum_{j=1}^{l} q_j \log q_j.

Remarks

The direction "isomorphic implies equal entropy" is due to Kolmogorov, who introduced entropy as an isomorphism invariant in 1958. The converse is Ornstein's theorem of 1970. Its proof builds the isomorphism as a limit of better and better finite codes, using the finitely determined property, which every Bernoulli scheme has. Example: B(1/4,1/4,1/4,1/4)B(1/4, 1/4, 1/4, 1/4) and B(1/2,1/8,1/8,1/8,1/8)B(1/2, 1/8, 1/8, 1/8, 1/8) both have entropy log⁡4\log 4, so they are isomorphic, although their alphabets have different sizes. Meshalkin had found an explicit isomorphism in this case before Ornstein's theorem. On the other hand B(1/2,1/2)B(1/2, 1/2) and B(1/3,1/3,1/3)B(1/3, 1/3, 1/3) have entropies log⁡2≠log⁡3\log 2 \ne \log 3, so they are not isomorphic, even though they are spectrally isomorphic. Ornstein's theory extends the theorem to Bernoulli schemes on countable alphabets and to Bernoulli flows.

Going deeper

For a student

Before Ornstein, it was not known whether entropy was the only obstruction. The theorem makes entropy a complete invariant for Bernoulli schemes. Ornstein's methods then showed that many smooth systems are isomorphic to Bernoulli schemes. Examples are ergodic toral automorphisms and geodesic flows on surfaces of negative curvature. Every Bernoulli scheme is a Kolmogorov automorphism, but Ornstein also constructed K-automorphisms that are not isomorphic to any Bernoulli scheme. Compare with Sinai's factor theorem, which gives Bernoulli factors of every system of positive entropy.

Reading path

To understand this page from the ground up, read these 8 pages in order. The foundations come first.

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Each page uses the pages above it. The colour of the bar on a box shows how strong the evidence is, and the box also gives it as text. The list has the same pages.
  • no evidence level
  1. Bernoulli process concept
  2. Infinite product measure concept
  3. Kolmogorov automorphism concept
  4. Kolmogorov–Sinai entropy concept
  5. Measure-preserving transformation concept
  6. Mixing concept
  7. Bernoulli scheme example
  8. Ornstein isomorphism theorem statement

Further reading

  1. Web https://en.wikipedia.org/wiki/Ornstein_isomorphism_theorem
About this page
Tag8H4GF58E9M
URIm2://8H4GF58E9M
Kindstatement, theorem
WritingW0 stub
MSC37A35, 28D20
StatusThis copy of the site has no build data. Run m2 status 8H4GF58E9M.
AboutBernoulli scheme, Kolmogorov–Sinai entropy
UsesBernoulli scheme, Kolmogorov–Sinai entropy, Measure-preserving transformation, Kolmogorov automorphism
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