20. Recurrence and Unique Ergodicity

20. Recurrence and Unique Ergodicity

MATH41112/61112 Ergodic Theory Lecture 20 20. Recurrence and Unique Ergodicity x20.1 Poincar´e's Recurrence Theorem We now go back to the general setting of a measure-preserving transforma- tion of a probability space (X; B; µ). The following is the most basic result about the distribution of orbits. Theorem 20.1 (Poincar´e's Recurrence Theorem) Let T : X ! X be a measure-preserving transformation of (X; B; µ) and let n 1 A 2 B have µ(A) > 0. Then for µ-a.e. x 2 A, the orbit fT xgn=0 returns to A infinitely often. Proof. Let E = fx 2 A j T nx 2 A for infinitely many ng; then we have to show that µ(AnE) = 0. If we write F = fx 2 A j T nx 62 A 8n ≥ 1g then we have the identity 1 − A n E = (T kF \ A): =0 k[ Thus we have the estimate 1 − µ(AnE) = µ (T kF \ A) k=0 ! [1 − ≤ µ T kF k=0 ! 1 [ − ≤ µ(T kF ): =0 Xk Since µ(T −kF ) = µ(F ) 8k ≥ 0 (because the measure is preserved), it suffices to show that µ(F ) = 0. First suppose that n > m and that T −mF \ T −nF 6= ;. If y lies in this intersection then T my 2 F and T n−m(T my) = T ny 2 F ⊂ A, which contradicts the definition of F . Thus T −mF and T −nF are disjoint. 1 MATH41112/61112 Ergodic Theory Lecture 20 −k 1 Since fT F gn=0 is a disjoint family, we have 1 1 − − µ(T kF ) = µ T kF ≤ µ(X) = 1: =0 =0 ! Xk k[ Since the terms in the summation have the constant value µ(F ), we must have µ(F ) = 0. 2 Exercise 20.1 Construct an example to show that Poincar´e's recurrence theorem does not hold on infinite measure spaces. (Recall that a measure space (X; B; µ) is infinite if µ(X) = 1.) x20.2 Unique Ergodicity We finish this section by looking at the case where T : X ! X has a unique invariant probability measure. Definition. Let (X; B) be a measurable space and let T : X ! X be a measurable transformation. If there is a unique T -invariant probability measure then we say that T is uniquely ergodic. Remark. You might wonder why we don't just call such T `uniquely in- variant'. Recall from Lecture 19 that the extremal points of M(X; T ) are precisely the ergodic measures. If M(X; T ) consists of just one measure then that measure is extremal, and so must be ergodic. Unique ergodicity (for continuous maps) implies the following strong convergence result. Theorem 20.2 Let X be a compact metric space and let T : X ! X be a continuous transformation. The following are equivalent: (i) T is uniquely ergodic; (ii) for each f 2 C(X) there exists a constant c(f) such that n−1 1 f(T jx) ! c(f); n j=0 X uniformly for x 2 X, as n ! 1. Proof. (ii) ) (i): Suppose that µ, ν are T -invariant probability measures; we shall show that µ = ν. 2 MATH41112/61112 Ergodic Theory Lecture 20 Integrating the expression in (ii), we obtain n−1 1 f dµ = lim f ◦ T j dµ n!1 n j=0 Z X Z n−1 1 = lim f ◦ T j dµ n!1 n j=0 Z X = c(f) dµ = c(f); Z and, by the same argument f dν = c(f): Z Therefore f dµ = f dν 8f 2 C(X) Z Z and so µ = ν (by the Riesz Representation Theorem). (i) ) (ii): Let M(X; T ) = fµg. If (ii) is true, then, by the Dominated Convergence Theorem, we must necessarily have c(f) = f dµ. Suppose that (ii) is false. Then we can find f 2 C(X) and sequences n 2 N and R k xk 2 X such that nk−1 1 j lim f(T xk) 6= f dµ. k!1 n k j=0 X Z For each k ≥ 1, define a measure νk 2 M(X) by nk−1 1 j ν = T∗ δxk ; k n k j=0 X so that nk−1 1 f dν = f(T jx ): k n k k j=0 Z X ∗ By the proof of Theorem 13.1, νk has a subsequence which converges weak to a measure ν 2 M(X; T ). In particular, we have f dν = lim f dνk 6= f dµ. k!1 Z Z Z Therefore, ν 6= µ, contradicting unique ergodicity. 2 3 MATH41112/61112 Ergodic Theory Lecture 20 x20.3 Example: The Irrational Rotation Let X = R=Z, T : X ! X : x 7! x + α mod 1, α irrational. Then T is uniquely ergodic (and µ = Lebesgue measure is the unique invariant prob- ability measure). Proof. Let m be an arbitrary T -invariant probability measure; we shall show that m = µ. 2πikx Write ek(x) = e . Then ek(x) dm = ek(T x) dm Z Z = ek(x + α) dm Z 2πikα = e ek(x) dm: Z Since α is irrational, if k 6= 0 then e2πikα 6= 1 and so ek dm = 0: (20.1) Z 1 Let f 2 C(X) have Fourier series k=−∞ akek, so that a0 = f dµ. For n ≥ 1, we let σn denote the average of the first n partial sums. Then σn ! f P R uniformly as n ! 1. Hence lim σn dm = f dm: n!1 Z Z However using (20.1), we may calculate that σn dm = a0 = f dµ. Z Z Thus we have that f dm = f dµ, for every f 2 C(X), and so m = µ. 2 R R 4.

View Full Text

Details

  • File Type
    pdf
  • Upload Time
    -
  • Content Languages
    English
  • Upload User
    Anonymous/Not logged-in
  • File Pages
    4 Page
  • File Size
    -

Download

Channel Download Status
Express Download Enable

Copyright

We respect the copyrights and intellectual property rights of all users. All uploaded documents are either original works of the uploader or authorized works of the rightful owners.

  • Not to be reproduced or distributed without explicit permission.
  • Not used for commercial purposes outside of approved use cases.
  • Not used to infringe on the rights of the original creators.
  • If you believe any content infringes your copyright, please contact us immediately.

Support

For help with questions, suggestions, or problems, please contact us