Definition of the Subject
Our main goal in this article is to consider when two measure preserving transformations are in some sense different presentations of the same underlying object. To make this precise we say two measure preserving maps \( { (\mathbf{X},T) } \) and \( { (\mathbf{Y},S) } \) are isomorphic if there exists a measurable map \( { \phi \colon X \to Y } \) such that
- (1)
ϕ is measure preserving,
- (2)
ϕ is invertible almost everywhere and
- (3)
\( { \phi(T(x))=S(\phi(x)) } \) for almost every x.
The main goal of the subject is to construct a collection of invariants of a transformation such that a necessary condition for two transformations to be isomorphic is that the invariant be the same for both transformations. Another goal of the subject is to solve the much more difficult problem of constructing invariants such that the invariants being the same for two transformations is a sufficient condition for the transformation to be isomorphic. Finally we apply these...
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Abbreviations
- Almost everywhere:
-
A property is said to hold almost everywhere (a.e.) if the set on which the property does not hold has measure 0.
- Bernoulli shift:
-
A Bernoulli shift is a stochastic process such that all outputs of the process are independent.
- Conditional measure:
-
For any measure space \( { (X,\mathcal{B},\mu) } \) and σ‑algebra \( { \mathcal{C} \subset \mathcal{B} } \) the conditional measure is a \( { \mathcal{C} } \)‐measurable function g such that \( { \mu(C)=\int_C g \, \mathrm{d}\mu } \) for all \( { C \in \mathcal{C} } \).
- Coupling of two measure spaces:
-
A coupling of two measure spaces \( { (X,\mu,\mathcal{B}) } \) and \( { (Y,\nu,\mathcal{C}) } \) is a measure γ on \( { X \times Y } \) such that \( { \gamma(B \times Y) = \mu(B) } \) for all \( { B \in \mathcal{B} } \) and \( { \gamma(X \times C) = \nu(C) } \) for all \( { C \in \mathcal{C} } \).
- Ergodic measure preserving transformation:
-
A measure preserving transformation is ergodic if the only invariant sets \( { (\mu(A \triangle T^{-1}(A)) = 0) } \) have measure 0 or 1.
- Ergodic theorem:
-
The pointwise ergodic theorem says that for any measure preserving transformation \( { (X,\mathcal{B},\mu) } \) and T and any L 1 function f the time average
$$ \lim_{n \to \infty} \frac{1}{n} \, \sum_{i=1}^{n}f(T^{i}(x)) $$converges a.e. If the transformation is ergodic then the limit is the space average, \( { \int f \, \mathrm{d}\mu } \) a.e.
- Geodesic:
-
A geodesic on a Riemannian manifold is a distance minimizing path between points.
- Horocycle:
-
A horocycle is a circle in the hyperbolic disk which intersects the boundary of the disk in exactly one point.
- Invariant measure:
-
Likewise a measure μ is said to be invariant with respect to \( { (\mathbf{X},T) } \) provided that \( { \mu(T^{-1}(A))=\mu(A) } \) for all measurable \( { A \in \mathcal{B} } \).
- Joining of two measure preserving transformations:
-
A joining of two measure preserving transformations \( { (\mathbf{X},T) } \) and \( { (\mathbf{Y},S) } \) is a coupling of X and Y which is invariant under \( { T \times S } \).
- Markov shift:
-
A Markov shift is a stochastic process such that the conditional distribution of the future outputs (\( { \{x_n\}_{n \mathchar"313E 0} } \)) of the process conditioned on the last output (x 0) is the same as the distribution conditioned on all of the past outputs of the process (\( { \{x_n\}_{n\leq 0} } \)).
- Measure preserving transformation:
-
A measure preserving transformation consists of a probability space \( { (\mathbf{X},T) } \) and a measurable function \( { T \colon X \to X } \) such that \( { \mu(T^{-1}(A))=\mu(A) } \) for all \( { A \in \mathcal{B} } \).
- Measure theoretic entropy:
-
A numerical invariant of measure preserving transformations that measures the growth in complexity of measurable partitions refined under the iteration of the transformation.
- Probability space:
-
A probability space \( { \mathbf{X}=(X,\mu,\mathcal{B}) } \) is a measure space such that \( { \mu(B)=1 } \).
- Rational function, rational map:
-
A rational function \( { f(z)=g(z)/h(z) } \) is the quotient of two polynomials. The degree of f(z) is the maximum of the degrees of g(z) and h(z). The corresponding rational maps \( { T_f \colon z \to f(z) } \) on the Riemann sphere ℂ are a main object of study in complex dynamics.
- Stochastic process:
-
A stochastic process is a sequence of measurable functions \( { \{x_n\}_{n \in \mathbb{Z}} } \) (or outputs) defined on the same measure space, X. We refer to the value of the functions as outputs.
Bibliography
Ashley J, Marcus B, Tuncel S (1997) The classification of one-sided Markov chains. Ergod Theory Dynam Syst 17(2):269–295
Birkhoff GD (1931) Proof of the ergodic theorem. Proc Natl Acad Sci USA 17:656–660
Breiman L (1957) The individual ergodic theorem of information theory. Ann Math Statist 28:809–811
Den Hollander F, Steif J (1997) Mixing E properties of the generalized \( { T,T^{-1} } \)-process. J Anal Math 72:165–202
Einsiedler M, Lindenstrauss E (2003) Rigidity properties of \( { \mathbb{Z}^d } \)-actions on tori and solenoids. Electron Res Announc Amer Math Soc 9:99–110
Einsiedler M, Katok A, Lindenstrauss E (2006) Invariant measures and the set of exceptions to Littlewood's conjecture. Ann Math (2) 164(2):513–560
Feldman J (1976) New K‑automorphisms and a problem of Kakutani. Isr J Math 24(1):16–38
Freire A, Lopes A, Mañé R (1983) An invariant measure for rational maps. Bol Soc Brasil Mat 14(1):45–62
Friedman NA, Ornstein DS (1970) On isomorphism of weak Bernoulli transformations. Adv Math 5:365–394
Furstenberg H (1967) Disjointness in ergodic theory, minimal sets, and a problem in Diophantine approximation. Math Syst Theory 1:1–49
Gallavotti G, Ornstein DS (1974) Billiards and Bernoulli schemes. Comm Math Phys 38:83–101
Gromov M (2003) On the entropy of holomorphic maps. Enseign Math (2) 49(3–4):217–235
Halmos PR (1950) Measure theory. D Van Nostrand, New York
Harvey N, Peres Y. An invariant of finitary codes with finite expected square root coding length. Ergod Theory Dynam Syst, to appear
Heicklen D (1998) Bernoullis are standard when entropy is not an obstruction. Isr J Math 107:141–155
Heicklen D, Hoffman C (2002) Rational maps are d‑adic Bernoulli. Ann Math (2) 156(1):103–114
Hoffman C (1999) A K counterexample machine. Trans Amer Math Soc 351(10):4263–4280
Hoffman C (1999) A Markov random field which is K but not Bernoulli. Isr J Math 112:249–269
Hoffman C (2004) An endomorphism whose square is Bernoulli. Ergod Theory Dynam Syst 24(2):477–494
Hoffman C (2003) The scenery factor of the \( { [T,T^{-1}] } \) transformation is not loosely Bernoulli. Proc Amer Math Soc 131(12):3731–3735
Hoffman C, Rudolph D (2002) Uniform endomorphisms which are isomorphic to a Bernoulli shift. Ann Math (2) 156(1):79–101
Hopf E (1971) Ergodic theory and the geodesic flow on surfaces of constant negative curvature. Bull Amer Math Soc 77:863–877
Jong P (2003) On the isomorphism problem of p‑endomorphisms. Ph D thesis, University of Toronto
Kalikow SA (1982) \( { T,T^{-1} } \) transformation is not loosely Bernoulli. Ann Math (2) 115(2):393–409
Kammeyer JW, Rudolph DJ (2002) Restricted orbit equivalence for actions of discrete amenable groups. Cambridge tracts in mathematics, vol 146. Cambridge University Press, Cambridge
Katok AB (1975) Time change, monotone equivalence, and standard dynamical systems. Dokl Akad Nauk SSSR 223(4):789–792; in Russian
Katok A (1980) Smooth non‐Bernoulli K‑automorphisms. Invent Math 61(3):291–299
Katok A, Spatzier RJ (1996) Invariant measures for higher‐rank hyperbolic abelian actions. Ergod Theory Dynam Syst 16(4):751–778
Katznelson Y (1971) Ergodic automorphisms of T n are Bernoulli shifts. Isr J Math 10:186–195
Keane M, Smorodinsky M (1979) Bernoulli schemes of the same entropy are finitarily isomorphic. Ann Math (2) 109(2):397–406
Kolmogorov AN (1958) A new metric invariant of transient dynamical systems and automorphisms in Lebesgue spaces. Dokl Akad Nauk SSSR (NS) 119:861–864; in Russian
Kolmogorov AN (1959) Entropy per unit time as a metric invariant of automorphisms. Dokl Akad Nauk SSSR 124:754–755; in Russian
Krieger W (1970) On entropy and generators of measure‐preserving transformations. Trans Amer Math Soc 149:453–464
Ledrappier F (1978) Un champ markovien peut être d'entropie nulle et mélangeant. CR Acad Sci Paris Sér A–B 287(7):A561–A563; in French
Lindenstrauss E (2001) Pointwise theorems for amenable groups. Invent Math 146(2):259–295
Lyons R (1988) On measures simultaneously 2- and 3‑invariant. Isr J Math 61(2):219–224
Mañé R (1983) On the uniqueness of the maximizing measure for rational maps. Bol Soc Brasil Mat 14(1):27–43
Mañé R (1985) On the Bernoulli property for rational maps. Ergod Theory Dynam Syst 5(1):71–88
Meilijson I (1974) Mixing properties of a class of skew‐products. Isr J Math 19:266–270
Meshalkin LD (1959) A case of isomorphism of Bernoulli schemes. Dokl Akad Nauk SSSR 128:41–44; in Russian
Nevo A (1994) Pointwise ergodic theorems for radial averages on simple Lie groups. I. Duke Math J 76(1):113–140
Nevo A, Stein EM (1994) A generalization of Birkhoff's pointwise ergodic theorem. Acta Math 173(1):135–154
Ornstein DS (1973) A K automorphism with no square root and Pinsker's conjecture. Adv Math 10:89–102
Ornstein D (1970) Factors of Bernoulli shifts are Bernoulli shifts. Adv Math 5:349–364
Ornstein D (1970) Two Bernoulli shifts with infinite entropy are isomorphic. Adv Math 5:339–348
Ornstein D (1970) Bernoulli shifts with the same entropy are isomorphic. Adv Math 4:337–352
Ornstein DS (1973) An example of a Kolmogorov automorphism that is not a Bernoulli shift. Adv Math 10:49–62
Ornstein DS (1973) A mixing transformation for which Pinsker's conjecture fails. Adv Math 10:103–123
Ornstein DS, Rudolph DJ, Weiss B (1982) Equivalence of measure preserving transformations. Mem Amer Math Soc 37(262). American Mathematical Society
Ornstein DS, Shields PC (1973) An uncountable family of K‑automorphisms. Adv Math 10:63–88
Ornstein D, Weiss B (1983) The Shannon–McMillan–Breiman theorem for a class of amenable groups. Isr J Math 44(1):53–60
Ornstein DS, Weiss B (1973) Geodesic flows are Bernoullian. Isr J Math 14:184–198
Ornstein DS, Weiss B (1974) Finitely determined implies very weak Bernoulli. Isr J Math 17:94–104
Ornstein DS, Weiss B (1987) Entropy and isomorphism theorems for actions of amenable groups. J Anal Math 48:1–141
Parry W (1981) Topics in ergodic theory. Cambridge tracts in mathematics, vol 75. Cambridge University Press, Cambridge
Parry W (1969) Entropy and generators in ergodic theory. WA Benjamin, New York
Petersen K (1989) Ergodic theory. Cambridge studies in advanced mathematics, vol 2. Cambridge University Press, Cambridge
Pinsker MS (1960) Dynamical systems with completely positive or zero entropy. Dokl Akad Nauk SSSR 133:1025–1026; in Russian
Ratner M (1978) Horocycle flows are loosely Bernoulli. Isr J Math 31(2):122–132
Ratner M (1982) Rigidity of horocycle flows. Ann Math (2) 115(3):597–614
Ratner M (1983) Horocycle flows, joinings and rigidity of products. Ann Math (2) 118(2):277–313
Ratner M (1991) On Raghunathan's measure conjecture. Ann Math (2) 134(3):545–607
Halmos PR (1960) Lectures on ergodic theory. Chelsea Publishing, New York
Rudolph DJ (1985) Restricted orbit equivalence. Mem Amer Math Soc 54(323). American Mathematical Society
Rudolph DJ (1979) An example of a measure preserving map with minimal self‐joinings, and applications. J Anal Math 35:97–122
Rudolph DJ (1976) Two nonisomorphic K‑automorphisms with isomorphic squares. Isr J Math 23(3–4):274–287
Rudolph DJ (1983) An isomorphism theory for Bernoulli free Z‐skew‐compact group actions. Adv Math 47(3):241–257
Rudolph DJ (1988) Asymptotically Brownian skew products give non‐loosely Bernoulli K‑automorphisms. Invent Math 91(1):105–128
Rudolph DJ (1990) \( { \times 2 } \) and \( { \times 3 } \) invariant measures and entropy. Ergod Theory Dynam Syst 10(2):395–406
Schmidt K (1984) Invariants for finitary isomorphisms with finite expected code lengths. Invent Math 76(1):33–40
Shields P (1973) The theory of Bernoulli shifts. Chicago lectures in mathematics. University of Chicago Press, Chicago
Sinaĭ JG (1962) A weak isomorphism of transformations with invariant measure. Dokl Akad Nauk SSSR 147:797–800; in Russian
Sinaĭ J (1959) On the concept of entropy for a dynamic system. Dokl Akad Nauk SSSR 124:768–771; in Russian
Thouvenot J-P (1975) Quelques propriétés des systèmes dynamiques qui se décomposent en un produit de deux systèmes dont l'un est un schéma de Bernoulli. Conference on ergodic theory and topological dynamics, Kibbutz, Lavi, 1974. Isr J Math 21(2–3):177–207; in French
Thouvenot J-P (1975) Une classe de systèmes pour lesquels la conjecture de Pinsker est vraie. Conference on ergodic theory and topological dynamics, Kibbutz Lavi, 1974. Isr J Math 21(2–3):208–214; in French
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Hoffman, C. (2009). Isomorphism Theory in ErgodicTheory . In: Meyers, R. (eds) Encyclopedia of Complexity and Systems Science. Springer, New York, NY. https://doi.org/10.1007/978-0-387-30440-3_297
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