• Aucun résultat trouvé

Limit theory for some positive stationary processes with infinite mean

N/A
N/A
Protected

Academic year: 2022

Partager "Limit theory for some positive stationary processes with infinite mean"

Copied!
29
0
0

Texte intégral

(1)

www.imstat.org/aihp 2014, Vol. 50, No. 1, 256–284

DOI:10.1214/12-AIHP513

© Association des Publications de l’Institut Henri Poincaré, 2014

Limit theory for some positive stationary processes with infinite mean

Jon Aaronson

a,1

and Roland Zweimüller

b

aSchool of Math. Sciences, Tel Aviv University, 69978 Tel Aviv, Israel. E-mail:[email protected] bFaculty of Mathematics, University of Vienna, 1090 Vienna, Austria. E-mail:[email protected]

Received 20 September 2011; revised 16 June 2012; accepted 4 July 2012

Abstract. We prove stable limit theorems and one-sided laws of the iterated logarithm for a class of positive, mixing, stationary, stochastic processes which contains those obtained from nonintegrable observables over certain piecewise expanding maps. This is done by extending Darling–Kac theory to a suitable family of infinite measure preserving transformations.

Résumé. Nous prouvons des théorèmes limites et des lois du logarithme itéré unilatérales pour une classe de processus stochas- tiques positifs, mélangeants et stationnaires. Cette classe contient en particulier les processus obtenus par des observables noninté- grables de certaines applications dilatantes. Ceci est obtenu en généralisant la théorie de Darling–Kac à une famille appropriée de transformations préservant la mesure.

MSC:Primary 60Fxx; secondary 37A40; 60G10

Keywords:Infinite invariant measure; Transfer operator; Infinite ergodic theory; Darling–Kac theorem; Pointwise dual ergodic; Mixing coefficient; Stable limit; One-sided law of iterated logarithm

Overview

We prove limit theorems for positive, stationary, processes with infinite mean satisfying mixing conditions which occur naturally in certain dynamical systems:stable limit theoremsfor certainϑμ-mixing processes andone-sided laws of the iterated logarithmfor certainψ-mixing processes (definitions below).

The method of proof is byinversionwhich is done by first building aKakutani towerover the generating probability preserving transformation, using the time zero observation as height function.

The mixing properties of the stationary process ensure that the resulting infinite measure preserving transformation isweakly pointwise dual ergodic, which allows us to develop a generalizedDarling–Kac theoryfor ergodic sums of this system. The results for the original stochastic process then follow by a standard inversion argument.

We illustrate both the finite-measure and the infinite-measure results by applying them to certain one-dimensional dynamical systems.

1Partially supported by Israel Science Foundation Grant No. 1114/08.

(2)

1. Definitions and preliminaries Stationary processes

We are going to consider partial sums of ergodicR+-valued stationary processesn)n0 withEn)= ∞. Such a process can always be represented asξn=ϕSn, whereS is a measure preserving transformation on a probability space(Ω,A, P ), andϕ:Ω→R+is measurable withE(ϕ)= ∞(and w.l.o.g.A=σ{ϕSn:n≥0}). Due to nonin- tegrability, it will suffice to restrict attention to theN-valued case, as by the ergodic theorem the partial sums of the fractional parts are asymptotically negligible compared to the partial sums of the process. Henceforth,ϕ:Ω→N, and we letα=αϕ= {[ϕ=l]:l∈N}. This gives aprobability preserving fibred system(Ω,A, P , S, α)in the sense of the following definition.

Nonsingular transformations and fibred systems

A measurable mapSon aσ-finite space(Ω,A, m)is callednonsingularifmS1m. Itstransfer operator(with respect tom) is the positive linear mapS:L1(m)L1(m)defined by

A

Sfdm=

S1A

fdm

fL1(m), AA .

Afibred or piecewise invertible systemis a quintuple(Ω,A, m, S, α) whereS is a nonsingular transformation on (Ω,A, m), andαAis a countable, unilateral generator so that the restrictionS:aSais invertible, nonsingular on eachaα. In this case, for everyk≥1,(Ω,A, m, Sk, αk)is a fibred system, whereαk:=k1

j=0Sjα.

The transfer operator of(Ω,A, m, S, α)can be represented as Sf =

aα

1Sava(fva),

whereva:Saadenotes the inverse ofS:aSa, andva :=dmdmva.

If m actually is an S-invariant probability measure, the system is called probability preserving, and we write P :=m.

Mixing

LetP(Ω,A)denote the collection of probability measures on(Ω,A), and callμP(Ω,A)equivalenttoP,μP, ifμP μ. Various mixing conditions for a probability preserving fibred system(Ω,A, P , S, α)are defined in terms of the asymptotics of certainmixing coefficients, all defined forn≥1 (and only using pairs of sets for which the denominator is nonzero). The system is called

ϑμ-mixing(for someμP(Ω,A)withμP) ifϑμ(n)→0, where ϑμ(n):=sup

|P (AS(n+k)B)P (A)P (B)|

μ(B) : k≥1, A∈σ (αk), BA ;

ψ-mixingifψ(n)→1, where ψ(n):=sup

P (AS(n+k)B)

P (A)P (B) : k≥1, A∈σ (αk), BA ;

ψ-mixingifψ (n)→0, where ψ (n):=sup

|P (AS(n+k)B)P (A)P (B)|

P (A)P (B) : k≥1, A∈σ (αk), BA ; andcontinued fraction mixingif, in addition toψ-mixing,ψ (1) <∞.

(3)

Remark 1. (a)The notion ofϑμ-mixing generalizes that of reverseφ-mixingwhich requires thatφ(n)→0,where φ(n):=sup

|P (AS(n+k)B)P (A)P (B)|

P (B) : k≥1, A∈σ (αk), BA , so thatϑP(n)=φ(n)for alln.

(b)As shown in [11],ψ(1) <implies ψ-mixing.Elementary computation shows that φ(n)ψ(n)−1, henceψ-mixing entails reverseφ-mixing,that is,ϑP-mixing.

(c)It is immediate thatψ-mixing impliesψ-mixing.Moreover,note thatψ(1)≤1+ψ (1).In view of(a),ψ (1) <

also impliesψ-mixing.

(d)For examples withψ(1) <which are notψ-mixing,see chapter5in[12].

(e)In Section 7below,we consider a class of interval maps(weakly mixing Rychlik-maps)for whichϑμ(n)→ 0 exponentially fast(as shown in [8]).We prove that,under some natural extra assumptions,ψ(1) <implies continued fraction mixing in this setup.

Strong distributional convergence and limit laws

For(X,B, m)aσ-finite measure space,Fn:X→ [0,∞]measurable, andY a random variable taking values in[0,∞], we say that(Fn)converges strongly in distribution toY, written

Fn−→d

n→∞Y,

if it converges in law with respect to all absolutely continuous probabilities, that is, if for all continuous (hence bounded)g:[0,∞] →Rand allPP(X,B)withP m,

X

g(Fn)dP −→

n→∞E g(Y )

.

Forγ ∈ [0,1]we letYγ ≥0 denote a random variable which has the normalized Mittag-Leffler distribution of orderγ, that is,E(Yγp)=p!(1((1++pγ )γ ))p forp≥0. EvidentlyY1≡1, andY0has exponential distribution. Also,Y1/2is the absolute value of a centered Gaussian random variable.

Forγ(0,1], the variableZγ :=Y1/γ then has apositiveγ-stable distributionwithE(et Zγ)=exp(−(1+ γ )tγ)fort >0.

2. Results on stationary processes

Recall that a functiona:(L,)(0,)isregularly varying of indexρ∈Rif it is measurable anda(ct )/a(t )cρ ast→ ∞for allc >0. In caseρ >0, such ana has anasymptotically inverse functionb (uniquely determined up to asymptotic equivalence), meaning thata(b(t ))b(a(t))t ast→ ∞, andbis regularly varying of index 1/ρ.

These concepts are extended to sequences(a(n))by interpreting them as functions onR+ viat−→a(t)(which we shall do without further mention).

In the statements below,(Ω,A, P , S, α)is a probability preserving fibred system, andϕ:Ω→Nisα-measurable.

We let ϕn:=

n1

k=0

ϕSk, n≥0,

denote the partial sums of the stationary processn)n0=Sn)n0, and define aϕ(n):=

n

k=1

P

[ϕkn]

, n≥0.

(4)

In order to establish our results, we will need to assume that the growth of aϕ(n) is adapted to the decay of the mixing coefficients of the process. The main condition is as follows although we will use a stronger version (2.6) in Theorem2.3.

Definition of adaptedness

Letτ (n)↓0. We will say that the sequence(a(n))n∈Nin(0,)isadapted to(τ (n))n∈Nif nτ (δa(n))

a(n) −→

n→∞0 for allδ >0. (2.1)

Observe that in this case any sequence asymptotically equivalent to(a(n))is adapted, too. Note also that if(a(n))is regularly varying with positive index, then it is adapted to(τ (n))as soon as (2.1) holds for oneδ >0.

Our first result is a distributional limit theorem. In the barely infinite measure case (γ =1) it comes with an associated a.e. result. For γ(0,1), corresponding statements will be established under stronger assumptions in Theorem2.3below.

Theorem 2.1. Suppose that(Ω,A, P , S, α)is aϑμ-mixing probability preserving fibred system,and thatϕ:Ω→N isα-measurable.

(a) (Stable limit theorem)Let(a(n))=(aϕ(n))beγ-regularly varying for someγ(0,1],and assume that it is adapted to(ϑμ(n)).Then,

ϕn b(n)

−→d

n→∞Zγ, (2.2)

wherebis asymptotically inverse toa,b(a(n))a(b(n))n.

(b) (One-sided law of the iterated logarithm forγ =1)If,in addition,γ =1andb(n/log logn)log lognb(n), then

lim

n→∞

ϕn

b(n)=1 a.s. (2.3)

Remark 2. (a)The conclusion of Theorem2.1(a) was established for certain φ-mixing processes in([17], Corol- lary5.10)and for continued fraction mixing processes in[13] (see also[3]).

(b)A functional version of (a)is also valid,and can be proved using a straightforward,appropriate adaptation of[9].

(c)An analogue of Theorem2.1(b)forψ-mixing processes was established in[4].

The results mentioned in Remark2(a) also compute theaϕ(n)from the marginal distributions, for which additional

“close correlation” assumptions such asψ(1) <∞are required. We now show how to determine the asymptotics of aϕ(n)from the marginal distributions under the weaker close correlation condition (2.4) (but we still use the stronger ψ(1) <∞in Theorem2.3below).

Theorem 2.2 (Identifying the normalization). Let (Ω,A, P , S, α)be a ϑμ-mixing probability preserving fibred system.Assume thatϕ:Ω→Nisα-measurable,and that there exists someΦL1(P )+such that

S(ϕn)≤En)Φn≥1. (2.4)

Assume that(a(n))˜ is regularly varying with indexγ(0,1],and adapted to(ϑμ(n)),then En)

n→∞

n

(2γ )(1+γ )a(n)˜ (2.5)

implies

aϕ(n)

n→∞a(n).˜

(5)

Finally, replacing adaptedness (2.1) to μ(n)) by the stronger assumption (2.6) involving a(a(n)) below, we establish the following pointwise result.

Theorem 2.3 (The one-sided law of the iterated logarithm). Suppose that(Ω,A, P , S, α)is aψ-mixing proba- bility preserving fibred system withψ(1) <∞,and thatϕ:Ω→Nisα-measurable.

If(a(n))=(aϕ(n))isγ-regularly varying for someγ(0,1)with asymptotic inverseb(n),and if P(δa(a(n)))

a(n) −→

n→∞0 for someδ >0, (2.6)

then,lettingCγ :=Kγ1/γ withKγ:=γγ(1(1+γ )γ )1γ,we have lim

n→∞

ϕn

b(n/log log(n))log log(n)=Cγ a.s. (2.7)

Moreover,if(τ (n))is any sequence in(0,)withτ (n)andτ (n)/n↓,letκτ be the unique number in[0,∞]such that

n1eκτ (n)/nconverges forκ > κτ and diverges forκ < κτ.Then lim

n→∞

ϕn

b(n/κτ (n))κτ (n)Cγ a.s.ifκ∈ [κτ,), (2.8)

and lim

n→∞

ϕn

b(n/κτ (n))κτ (n)Cγ a.s.ifκ(0, κτ]. (2.9)

Remark 3. (a)The conclusion of Theorem2.3was established for iid processes in[21],and forψ-mixing processes in [5].Our proof of Theorem2.3is by establishing the conditions needed for the methods of[5].Therefore the functional version also follows as in[6].

(b)Recall thatϑP(n)=φ(n),see Remark1(a).

Inversion:Kakutani towers and return time processes

Our results will be established using the well-known technique of “inverting” corresponding results for infinite mea- sure preserving transformations, the connection being established via the following concept. Given a probability pre- serving transformation(Ω,A, P , S)and a measurable functionϕ:Ω→N, theKakutani towerof(Ω,A, P , S, ϕ)is the object(X,B, m, T )with(X,B, m)theσ-finite space defined by

X:=

n1[ϕn] × {n},

B:= {

n1Bn× {n}: BnA∩ [ϕn] ∀n≥1},

m(A× {n}):=P (A),

andT:XXis the map given by

T (x, n):=

(x, n+1), ϕ(x) > n, (Sx,1), ϕ(x)=n.

It follows that(X,B, m, T )is a conservative, measure preserving transformation which is ergodic iff(Ω,A, P , S)is ergodic.

This “tower building process” is reversible. Given a conservative ergodic σ-finite measure preserving system (X,B, m, T ), we define thereturn time process of T onΩF:= {BB: 0< m(B) <∞}as theN-valued sta- tionary processΩTΩn)n0on(Ω,BΩ, mΩ, ), where

ϕ(x)=ϕΩ(x):=min{n≥1:TnxΩ},

TΩ(x):=Tϕ(x)(x), and

mΩ(A):=m(AΩ)/m(Ω).

(6)

It follows that the Kakutani tower of(Ω,BΩ, mΩ, TΩ, ϕΩ)is a factor of(X,B, m, T )wherem=m(Ω)1 m(and an isomorph in caseT is invertible).

Now setϕj:=j1

i=0ϕΩTΩi, which is the time of thenth return toΩ. It is straightforward to check that these are dual to theoccupation timesofΩ,Sn(1Ω):=n1

k=01ΩTkin that

Sn(1Ω)j iff ϕjn. (2.10)

This entails, via routine arguments, that various properties of j)j1are equivalent to corresponding properties of (Sn(1Ω))n1. Specifically, suppose thata(n)isγ-regularly varying withγ(0,1], and letbbe asymptotically inverse toa. Then, forY a[0,∞]-valued random variable,

1

a(n)Sn(1Ω)−→d m(Ω)Y iff ϕn b(n)

−→d

1 m(Ω)Y

1/γ

, (2.11)

and

nlim→∞

1

a(n)Sn(1Ω)a.e.=m(Ω) iff lim

n→∞

ϕn b(n)

a.e.= 1

m(Ω) 1/γ

. (2.12)

3. Weak pointwise dual ergodic measure preserving transformations

In this section, we consider the properties of infinite ergodic systems to be used in the proofs of the above results.

Weak pointwise dual ergodicity

LetT be a conservative, ergodic, measure preserving transformation (not necessarily invertible) on theσ-finite space (X,B, m), andT:L1(m)L1(m)its transfer operator, which naturally extends to all nonnegative measurable func- tions. Invariance ofmmeans thatT1X=1X, and sinceT is conservative ergodic, any measurableg:X→ [0,∞) which is subinvariant,T gg, is, in fact, constant. Hurewicz’s ratio ergodic theorem (Theorem 2.2.1 of [1]), guaran- tees that

n1

k=0Tkf n1

k=0Tkg −→

n→∞

m(f )

m(g) a.e. onX (3.1)

for allf, gL1+(m):= {fL1(m): f ≥0 andm(f ) >0}. (Due to conservativity,n1

k=0Tkf → ∞a.e. for such f.)

Throughout, convergence in measure, −→m , for our σ-finite measure m, is understood to mean convergence in measure,−→, for every finiteν νm(or, equivalently, for allν=mAwithAF).

The conservative ergodic measure preserving transformation T on the σ-finite space (X,B, m) will be called weakly pointwise dual ergodicif there exist constantsa(n) >0, n≥1,such that

1 a(n)

n1

k=0

Tkf −→m

n→∞

X

fdm forfL1+(m), (3.2)

and

nlim→∞

1 a(n)

n1

k=0

Tkf =

X

fdm a.e. onXforfL1+(m). (3.3)

This generalizes the notion ofpointwise dual ergodicity(cf. Section 3.7 of [1], or [2]), which requiresa(n) >0 such that

1 a(n)

n1

k=0

Tkf −→

n→∞

X

fdm a.e. onXforfL1+(m). (3.4)

(7)

In either case the return sequence (a(n))n1, which is determined up to asymptotic equivalence and satisfies a(n+1)∼a(n)→ ∞, can (and will) be taken nondecreasing. It is usually denoted(an(T ))n1.

Remark 4. No invertibleconservative ergodic measure preserving transformation(X,B, m, T )withm(X)= ∞is pointwise dual ergodic. (Since in this caseT f =fT1,so that(3.4)would give a pointwise ergodic theorem with normalizing constantsa(n)forT1,which is impossible,see Section2.4of[1].)However,invertible systems can still be weakly pointwise dual ergodic.

Example 1. For a concrete example,letT:(0,1)→(0,1)be given byT x:=1xx forx < 12 andT x:=2x−1for x >12,which is conservative ergodic with invariant measuremhaving density 1x,and definea(n):=n/logn.By the Darling–Kac theorem for pointwise dual ergodic transformations, (see[2,14],Section3.7of[1],or[24]),

1 a(n)

n1

k=0

fTk −→m

n→∞

X

fdm forfL1+(m), and according to Proposition2of[4],

nlim→∞

1 a(n)

n1

k=0

fTk=

X

fdm a.e.onXforfL1+(m).

These carry over to the natural extensionT ofT:This is immediate for functions of the formf=fπ,withπ denoting the factor map.Then use the ratio ergodic theorem to pass to generalfL1+(m).Therefore,the invertible conservative ergodic measure preserving transformationT1,with transfer operatorffTis weakly pointwise dual ergodic,and hence so isT,withan(T)an(T1)a(n).

Conditions of this flavour can be exploited most efficiently if one succeeds in identifying special sets on which there is additional control on the convergence. Recall (cf. [1,19]) thatAF= {BB: 0< m(B) <∞}is called a uniform set(forfL1+(m)) if there area(n) >0, such that

ess sup

A

1 a(n)

n1

k=0

Tkfm(f ) −→

n→∞0, and, more specifically, aDarling–Kac setif

ess sup

A

1 a(n)

n1

k=0

Tk1Am(A) −→

n→∞0.

We now defineAFto be alimited setif there exist constantsa(n) >0 such that 1

a(n)

n1

k=0

Tk1A mA

n−→→∞m(A), (3.5)

and

ess sup

A

1 a(n)

n1

k=0

Tk1A−→

n→∞m(A). (3.6)

Due to (3.1) the asymptotics of(a(n))does not depend onf orA. It is not hard to see that defining aA(n):=

n1

k=0

m(ATkA)

m(A)2 forAF,

(8)

we have a(n)

n→∞aA(n) in (3.5) and (3.6) for every limited setA. (3.7)

The existence of uniform sets is equivalent to pointwise dual ergodicity, anda(n)an(T )in this case. (But we do not know if every pointwise dual ergodic transformation has a Darling–Kac set.) Similarly,weak pointwise dual ergodicity is equivalent to the existence of limited sets, as we have

Proposition 3.1 (Limited sets and weak pointwise dual ergodicity from local behaviour). LetT be a conservative ergodic measure preserving transformation on theσ-finite space(X,B, m).

(a)Suppose there areAF,fL1+(m),and constantsa(n) >0,n≥1,such that 1

a(n)

n1

k=0

Tkf −→mA

n→∞

X

fdm, (3.8)

and

nlim→∞

1 a(n)

n1

k=0

Tkf =

X

fdm a.e.onA. (3.9)

Then,for everyη >0,T possesses a limited setAFAwith return sequence(a(n))n1andm(A)m(A)η.

(b)IfT has a limited set,then it is weakly pointwise dual ergodic.

Proof. (a) LetB0:=A. By Hurewicz’s ratio ergodic theorem we may assume w.l.o.g. thatf =1B0, and given any setBjFAwithm(Bj) > m(A)η, we also havea(n)1n1

k=0Tk1Bjm(Bj)a.e. onA. Egorov’s theorem then provides us with someBj+1FBj such thatm(Bj+1) > m(A)η, and

1 a(n)

n1

k=0

Tk1Bj −→

n→∞m(Bj) uniformly onBj+1.

Using this to inductively define a decreasing sequence(Bj)j0inF, we obtain a setA:=

j0Bj withm(A)m(A)η. Givenε >0 choosej withm(Bj) < m(A)+ε/2. Then, fornnj(ε),

ess sup

A

1 a(n)

n1

k=0

Tk1A≤ess sup

Bj+1

1 a(n)

n1

k=0

Tk1Bj < m(Bj)+ε 2.

This gives the required control from above. Since, by (3.1), (3.8) also holds withf =1A, we see thatAis indeed a limited set.

(b) Now start from the assumption thatT has a limited setA. Due to Hurewicz’s theorem, weak pointwise dual ergodicity follows as soon as we check the defining conditions (3.2) and (3.3) forf=1A, i.e. we have to prove

fn:= 1 a(n)

n1

k=0

Tk1A

−→m

n→∞m(A), (3.10)

and

f¯:= lim

n→∞

1 a(n)

n1

k=0

Tk1A=m(A) a.e. onX. (3.11)

(9)

LettingAn:=A∩ [ϕA> n],n≥0, we have, by routine arguments,

n0

Tn1An=1X, (3.12)

and decomposing, for anyn≥0, A according to the time of the last return before time n, A=Ann1

k=0AT(nk)(Ak)(disjoint), we find that forN≥0,

N

n=0

Tn1A=

N1

k=0

Tk

1Ak Nk

j=0

Tj1A

+

N

n=0

Tn1An. (3.13)

SinceAis a limited set, there is someM(0,)such that 1

a(n)

n1

k=0

Tk1AM onAforn≥1. (3.14)

With (3.14) and (3.12) providing bounds for the sums in (3.13), we get 1

a(N )

N1

n=0

Tn1AM·1X forN≥1, (3.15)

whereM:=M+1/a(1)∈(0,). Consequently,f¯≤M·1X. Now observe that|T f nfn| ≤2/a(n)→0. Com- bined with a variant of Fatou’s lemma forT, Lemma3.1below, this yields

Tf¯≥ lim

n→∞T f n= ¯f a.e. onX.

Henceg:=M·1X− ¯f≥0 is subinvariant,T gg. AsT is conservative ergodic, this implies thatgis constant a.e., and hence so isf¯. In view of (3.5), this yields (3.11).

To finally prove convergence in measure onX, it suffices to check it on each of the setsTlA,l≥0, since these coverX. But for eachl,

TlA

1 a(n)

n1

k=0

Tk1A

dm=aA(n+l)aA(l)

a(n) m(A)−→

n→∞m(A).

Together with (3.15) and (3.11) this entailsa(n)1n1 k=0Tk1A

mT−l A

−→m(A), and hence (3.10).

The preceding proof made use of

Lemma 3.1. LetT be measure preserving on theσ-finite space (X,A, m),with transfer operatorT,and letM(0,).

(a)Ifg, gk:X→ [0, M]are measurable withgkgk+1ga.e.,then

T gkT g a.e.onX. (3.16)

(b)Iffn:X→ [0, M]are measurable functions,then T (lim

n→∞fn)≥ lim

n→∞T f n a.e.onX. (3.17)

Proof. (a) By positivity of T, we haveT MT g 1T g 2≥ · · · ≥T g a.e., whileT M=M by invariance ofm.

Now take anyAA,m(A) <∞, then 1T1Agk−→1T1AginL1(m). Due toL1-continuity ofT, this entails 1AT g k=T (1 T1Agk)−→T (1 T1Ag)=1AT g inL1(m),

and sinceAwas arbitrary, the latter implies (3.16).

(10)

(b) Letgk:=supnkfnfk, andg:=limn→∞fn, theng, gk satisfy the assumptions of (a). Hence,T g kT g a.e. By positivity, however, we haveT gkT f k a.e. for allk≥1. Together, these observations give (3.17).

The notion of return sequences has originally been introduced in the context of rationally ergodic transformations (cf. Section 3.3 of [1]). The present use of the term is justified by

Proposition 3.2 (Weak pointwise dual ergodicity implies rational ergodicity). LetT be a weakly pointwise dual ergodic measure preserving transformation on theσ-finite space(X,B, m).Then every limited setAsatisfies a Rényi inequality,meaning that there is someM=M(A)(0,)such that

A

Sn(1A)2

dm≤M

A

Sn(1A)dm 2

forn≥1.

In particular,T is rationally ergodic with(an(T ))n1a return sequence in the sense of[1].

Proof. Same as the proof of Proposition 3.7.1 in [1], using (3.7) and the existence of limited sets established above.

(Weak)pointwise dual ergodicity and special sets for Kakutani towers

We are going to show that Kakutani towers aboveϑμ-mixing systems satisfying our adaptedness conditions are weakly pointwise dual ergodic. Moreover, in the presence of regular variation,ϑμ-mixing with sufficiently fast rate implies pointwise dual ergodicity.

Note first that if(X,B, m, T )is a conservative ergodic measure preserving transformation andΩB, m(Ω)=1, has return timeϕ=ϕΩ, andϕj:=j1

i=0ϕTΩi , then, in view of (2.11), aΩ(n)

n

k=1

m

ΩTkΩ

= n

j=1

m

Ω∩ [ϕjn]

=aϕ(n). (3.18)

Via (3.7) this links(aϕ(n))to the asymptotic type of a weakly pointwise dual ergodic system.

Theorem 3.1 ((Weak) pointwise dual ergodicity viaϑμ-mixing return processes). Let(X,B, m, T )be a conser- vative ergodic measure preserving transformation on a σ-finite space,and suppose thatΩB, m(Ω)=1,has a countable partitionαBΩ such thatϕ=ϕΩ isα-measurable and that(Ω,BΩ, P , TΩ, α)isϑμ-mixing for someμequivalent toP :=mΩ.

(a)If(a(n)):=(aΩ(n))is adapted to(ϑμ(n)),thenT is weakly pointwise dual ergodic withan(T )a(n).In addition,ε >0 ∃Nεs.t.nNε,

1 a(n)

n

k=1

Tk1Ω−1≤ε

1+dμ dP

a.e.onΩ. (3.19)

In particular,ifdP<∞,thenΩis a limited set.

(b)If(a(n))n1isγ-regularly varying for someγ(0,1]and ϑμ(n)=O

1 nr

for somer > 1 γ −1,

then(a(n))is adapted to(ϑμ(n)),andT is pointwise dual ergodic withan(T )a(n).

(c)If(a(n))n1isγ-regularly varying for someγ(0,1],andψ(1) <∞,and μ(δa(a(n)))

a(n) −→

n→∞0 for allδ >0, (3.20)

(11)

then(a(n))is adapted to(ϑμ(n)),andT is pointwise dual ergodic withan(T )a(n).Moreover,∀ε >0 ∃Nε such thatnNε

1 a(n)

n

k=1

Tk1Ω−1 ≤ε

1+dμ

dP

a.e.onΩ. (3.21)

In particular,ifdP<∞,thenΩ is a Darling–Kac set.

Proof. We write(Ω,A, P , S, α):=(Ω,BΩ, mΩ, TΩ, α). Note first that by definition ofϑμ, we have forj, p≥1 andAαj,

B

Sj+p1AdP ≤

B

P (A)+ϑμ(p)dμ dP

dP for arbitraryBA, and hence

Sj+p1AP (A)+ϑμ(p)

dP a.e. onΩ. (3.22)

We claim that forn, p≥1, Tn:=

n

k=1

Tk1Ωp+a(n)+μ(p)

dP a.e. onΩ. (3.23)

To see this, observe thatTk1Ω=

j1Sj1[ϕj=k]a.e. onΩ, and hence

Tn= n

j=1

Sj1[ϕjn]

n+p

j=1

Sj1[ϕjn]

p+ n

j=1

Sj+p1[ϕj+pn]p+ n

j=1

Sj+p1[ϕjn]

p+ n

j=1

P

[ϕjn]

+ϑμ(p)dμ dP

=p+a(n)+μ(p)

dP a.e. onΩ, since[ϕjn] ∈αj.

Proof of (a): To establish (3.19), we letp=pn,ε:= εa(n)forε >0. By adaptedness we can chooseNε such thatμ(pn,ε) < εa(n)whenevernNε. Then by (3.23),

Tna(n)

1+ε

1+dμ dP

a.e. onΩfornNε, (3.24)

as required.

To prove weak pointwise dual ergodicity, we will use part (a) of Proposition3.1. WriteRn:=Tn/a(n)and observe first that by (3.19),

nlim→∞Rn≤1 a.e. onΩ. (3.25)

In fact, (3.19) shows that for anyM >0, the estimate (3.25) holds uniformly onΩ∩ [dPM]. Consequently, P

Rn≥1+ε

n−→→∞0 for everyε>0. (3.26)

(12)

To obtain the analogous statement for convergence from below, we observe that fort(0,1), Rn≤1+ε

1+dμ

dP

a.e. onΩP

[Rnt]

≤ 2ε

1+εt, (3.27)

since (Edenoting expectation with respect toP) 1=E(Rn)=E(Rn1[Rn>t])+E(Rn1[Rnt])

(1+ε)P

[Rn> t] +εμ

[Rn> t] +t P

[Rnt]

≤1+2ε−(1+εt )P

[Rnt] .

Now fixε(0,1)and takeNε as in (3.24). Fort:=1−√

ε(0,1), observation (3.27) then yields P

[Rn≤1−√ ε]

≤2√

ε fornNε. This readily implies

P

Rn≤1−ε

n−→→∞0 for everyε>0,

which, together with (3.26), gives (3.8). Combined with (3.25) the latter yields (3.9). (There is some subsequence nk ∞such thatRnk→1 a.e. forP.)

Proof of (b): Computation of the indices of regular variation shows that the assumptions of (b) entail adaptedness.

As in part (a) this implies (3.25).

To check pointwise dual ergodicity, it remains to show that lim

n→∞Rn≥1 a.e. onΩ. (3.28)

(Proposition 3.7.5 of [1] ensures that a.e. convergence on someAFsuffices.) To this end, choosec≥1 such that ϑμ(n)c/nr for alln≥1. There exists >0 andN0so that

a(n) > n1/(r+1)+2sn > N0. Choosingp=n1/(r+1)in (3.23) we have

Rn= Tn

a(n) ≤1+ 1 n2s

1+dμ

dP

onΩnN0. Due to (3.27), we then see that fort(0,1),

qt(n):=P

[Rnt]

≤2c ns ·

1−t+ c ns

1

≤ 2c

(1t )ns fornN0. Since, for alltandλ >1,

n1qtn) <∞, the Borel–Cantelli Lemma now implies lim

n→∞Rλn≥1 a.s. onΩfor allλ >1. (3.29)

To finally prove convergence (3.28) of the full sequence, fix any λ >1 and choose integers κn(λ) ∞ so that λκn(λ)nλκn(λ)+1. Then regular variation of(a(n))n1yields

Tn

a(n)Tλκn(λ)

a(λκn(λ)+1)

n→∞

1 λγ

Tλκn(λ)

a(λκn(λ)) a.e. onΩ.

In view of (3.29), we thus have limn→∞Rnλγ a.s. onΩfor allλ >1, and (3.28) follows.

(13)

Proof of(c): Note first that adaptedness, and hence (3.19) holds. Thus, to prove (3.21), it suffices to check that for nNε,

1 a(n)

n

k=1

Tk1Ω≥1−ε

1+dμ dP

a.e. onΩ. (3.30)

We show first that∀p, q, n∈Nwithnq, Tna(n)pμ(p)

dP −ψ(1)2 P

[ϕp> q]

a(n)+q

(3.31) a.e. onΩ. To see this, observe that

Tn = n

j=1

Sj1[ϕjn]n

j=1

Sj+p1[ϕj+pn]p

= n

j=1

Sj+p1[ϕjn]n

j=1

Sj+p1[ϕjn<ϕj+p]p

=:Σ1Σ2p.

Now, because[ϕjn] ∈αj, we have Σ1

n

j=1

P

[ϕjn]

ϑμ(p)dμ dP

=a(n)μ(p)dμ dP. On the other hand,

Σ2ψ(1) n

j=1

P

[ϕjn < ϕj+p]

=ψ(1) n

j=1

n

=j

P

ϕj=, ϕpSj> n

ψ(1)2 n

j=1

n

=j

P

[ϕj=] P

[ϕp> n]

=ψ(1)2

Σ2+Σ2 with

Σ2 :=

n

j=1 nq

=j

P

[ϕj=] P

[ϕp> n]

P

[ϕp> q]n

j=1 nq

=j

P

[ϕj=]

P

[ϕp> q]n

j=1

P

[ϕjn]

=P

[ϕp> q] a(n);

Références

Documents relatifs

Equation (2.3) of Proposition 2.7 is also used in the proof of Theo- rem 2.8 in order to “transfer” the study of M(X)-pointwise integrals to B b (X)- pointwise integrals; since

In paper [1] that measure is constructed for the periodic problem for a nonlinear Klein-Gordon equation and in paper [2] a similar.. construction is made for a certain

Two main ingredients for proving the ergodicity of µ s are: the mutual singularity between all measures µ s ’s (derived from the strong law of large numbers) and an a priori

In Section 3 the Weyl and Anti-Wick calculus are introduced in a projective way after recalling accurately (most of all the scaling) of finite dimensional semiclassical calculus.

For many chaotic systems it has been proved that the central limit theorem holds for H¨older continuous functions.. If the action of K is H¨older continuous, then the central

Using the work of Olshanski and Vershik [6] and Rabaoui [10], [11], we give a sufficient condition, called “radial boundedness” of a matrix, for weak pre- compactness of its family

The distinguishing feature is that the rate of the external input is determined by an independent continuous-time Markov chain J (·) (commonly referred to as the background

Surprisingly, ID-disjointness mixed with the theory of Gaussian dynamical systems allows us to derive a new result on spectral theory of infinite ergodic measure preserving