郭锴,肖倩,马东魁
华南理工大学数学学院,广东 广州 510641
Topological pressure,introduced by Ruelle[1]and Walters[2],is a core concept in dynamical system and ergodic theory,and plays an important role in the study of thermodynamic formalism. From the viewpoint of dimension theory,Pesin and Pitskel[3-4]studied the topological pressure of non-compact subsets by using carátheory structure(C-P structure),and proposed the topological pressure of non-compact sets in dynamical systems,which is the generalization of Bowen's[5]topological entropy defined by non-compact sets. As the physical process evolves,it is natural for the evolution process to produce changes or some errors in the orbit calculation.However,a self-adaptable system should decrease errors over time. This prompted Cheng,Zhao et al[6]to study the dynamical systems under a mistake function. They defined the pressure for asymptotically sub-additive potentials under a mistake function,and proved that the topological pressure under a mistake function is equivalent to the topological pressure without mistake function by using the ergodic theory. Later,Chen et al[7]gave the concepts of topological pressure with mistake function and showed that the topological pressure under a mistake function on any subset is the same as the classical Pesin pressure of the subset in dynamical systems. This means that the topological pressure under a mistake function in the dynamical system is adaptive,which generalizes the result in the additive case in[3].
With the development of research on dynamical systems,the dynamical systems of group action has attracted people's attention. To study some questions,Xiao et al[8]gave the definitions of topological pressure and upper and lower capacity topological pressures of a free semigroup action by using C-P structure,and obtained some properties of them. Naturally,we wonder if the topological pressure of free semigroup actions has the similar result in[7]. In order to answer this question,in this paper we introduce the definitions of topological pressure of free semigroup actions under a mistake function and show the topological pressure of free semigroup actions under a mistake function is the same as the topological pressure of free semigroup actions defined by Xiao and Ma[8].
Furthermore,Gröger et al[9]showed that the entropy of the whole system with Bowen metric is equal to the entropy with mean metric. As an application,we prove that the topological pressure of free semigroup actions defined by Bowen metric coincides with the topological pressure of free semigroup actions defined by mean metric on a non-compact subset.
This paper is organized as follows. In section 1,we give some preliminaries. In section 2,we introduce two definitions of topological pressure of free semigroup actions under a mistake function and prove the main results. Finally,we give an application.
Letdenote the set of all finite words of symbols 0,1,…,m-1. For anyw∈,the length ofw,denoted by|w|,is defined the digits of symbols inw. Obviously,with respect to the law of composition is a free semigroup withmgenerators. We writew′≤wif there exists a wordsuch thatw=Forw=i1…ik∈,denotewˉ=ik…i1.
Denote by Σmthe set of all two-side infinite sequences of symbols 0,1,…,m-1,that is,
Let's recall the definition of the mistake function in[7],which is a little bit different from[6,10].
Definition 1Givenε0>0,the functiong:N ×(0,ε0]→R is called a mistake function ifg(n,ε) ≤g(n+ 1,ε) for allε∈(0,ε0]andn∈N and
For a mistake functiong,ifε>ε0,setg(n,ε) =g(n,ε0).
Let(X,d) be a compact metric space andGbe the free semigroup generated byf0,f1,…,fm-1,wherefi(0 ≤i≤m- 1) is continuous transformations fromXto itself. Givenφ0,φ1,…,φm-1∈C(X,R), denote Φ ={φ0,φ1,…,φm-1}. For simplicity of notation, we writefwinstead offi1∘fi2∘… ∘fin, wherew=i1i2…in∈Obviously,fww′=fw fw′for anyw,. Forw=i1i2…in∈,denote
Xiao and Ma[8]introduced the notion of topological pressure of free semigroup actions by C-P structure as follows:
Considering a finite open coverUofX,write | U |= max{|U|:U∈U},and let
for all U ∈GwandGwcoversZ(i.e. for any U ∈Gw,
Let
We can easily verify that the functionM(Z,α,Φ,U,N) is non-decreasing asNincreases.Therefore,the following limit exists
There is a critical value ofαat whichm(Z,α,Φ,U) jumps from ∞to 0. Denote
The topological pressure of a free semigroupGwith respect to Φ on the setZis
First,recall the definitions of the Bowen metric and(w,δ)-Bowen ball.
LetXbe a compact metric space with metricd,f0,f1,…,fm-1continuous transformations fromXto itself.Suppose that a free semigroupGwithmgeneratorsf0,f1,…,fm-1acts onX. Denote Φ ={φ0,φ1,…,φm-1},whereφ0,φ1,…,φm-1∈C(X,R). For eachw∈,a new metricdwonX(named Bowen metric)is given by
Based on the work of Climenhaga in[11],Xiao and Ma[8]defined the topological pressure of free semigroup actions by using the center of Bowen ball. Now,let us recall the definition of topological pressure of free semigroup actions by the center of Bowen ball in[8].
Let F denote the collection of Bowen ball,that is,
Givenw∈,|w|=N∈N,Z⊂Xandα∈R,define
Set
It is easy to verify that the functionM′(Z,α,Φ,δ,N) is non-decreasing asNincreases.Therefore,there exists the limit
Same as above,denote the critical value ofαby
The topological pressure of a free semigroupGwith respect to Φ on the setZis
Based on [6-7],in this section,we first give two concepts of topological pressure of free semigroup actions under a mistake function by using open covers and the center of mistake Bowen ball respectively. In addition,we show that these two concepts are equivalent to the definitions of the topological pressure of free semigroup actions introduced by Xiao and Ma[8]. Finally,we give a notion of mean metric and show that the topological pressure of free semigroup actions under a mistake function defined by Bowen metric agrees with the topological pressure of free semigroup actions defined by mean metric.
Letf0,f1,…,fm-1be the continuous transformations from compact metric space (X,d) to itself. DenoteGthe free semigroup withmgeneratorsf0,f1,…,fm-1acting onX. Givenφ0,φ1,…,φm-1∈C(X,R),denote Φ ={φ0,φ1,…,φm-1}.
Considering a finite open coverUofX. For any string U ∈Sn+1(U),let
We can easily verify that the functionM(Z,α,Φ,U,N,g) is non-decreasing asNincreases. This guarantees the existence of the following limit
There exists a critical value of the parameterα,which we will denote byPZ(G,Φ,U,g),wherem(Z,α,Φ,U,g) jumps from ∞to 0,that is,
The following theorem discusses the connection between the above definition and the topological pressure of free semigroup actions defined by using open covers.
Theorem 1For any setZ⊂X,the following limit exists and equals to the topological pressure of a free semigroup actionG,that is,
ProofWe use the analogous method as that of[3]. On the one hand,givenw=i1i2…iN∈,for any U ∈Sn+1(U),we denote the word that corresponds to U bywUsuch that,and corresponds to UgbywUgsuch thatwUg=wU,then we have
Let
and
whereG′w={Ug:U ∈,wUg=wU},γis a function such that
for allm(U) ≥N+ 1 andγ→0 as|U| →0.Moreover,we can get
which implies
Taking the limitN→∞yields
Therefore,
and as|U| →0,that is,β→0,γ→0,we obtain
By the arbitrariness ofε,we have
On the other hand,note thatwU=wUg,for any Ug∈(U),we can find
strings U ∈Sm(U) such that
whereτis the collection of such U.Using Stirling formula,there existsγ1>0 such that
for allm(U) ≥N+ 1,andγ1→0 as |U| →0. Givenw∈with |w| =N,andε>0,there is⊂S g(U)coveringZsuch that
which implies
Take the limitN→∞and we get
Therefore,
and as ||U →0,that is,β→0,γ→0,γ1→0,we obtain
Sinceε>0 is arbitrary,we have
This completes the proof.
The quantityPZ(G,Φ,g) is called the topological pressure of a free semigroupGunder a mistake functiongwith respect to Φ on the setZ.
Now,we introduce a definition of mistake Bowen ballBw(g;x,δ) for a givenw∈F+m.
Fix a numberδ>0. Givenw∈F+mand a pointx∈X,the mistake Bowen ballBw(g;x,δ) centered atxwith radiusδand length ||
w+ 1 associated to the mistake functiongis given by the following set,i.e.,
It is obvious that the(w,δ)-Bowen ball is a subset ofBw(g;x,δ).
Now,we describe another approach to redifine the topological pressure of a free semigroupGunder a mistake functiongby the center of mistake Bowen ball.Define the collection of subsets
It is easy to verify that the functionM′(Z,α,Φ,δ,N,g) is non-decreasing asNincreases. This guarantees the existence of the limit
There exists a critical value of the parameterα,which we will denote byP′Z(G,Φ,δ,g), wherem′(Z,α,Φ,δ,g) jumps from ∞to 0,namely,
The following theorem proves that the two definitions of topological pressure of free semigroup actions under a mistake function are equivalent.
Theorem 2For any setZ⊂X,the following limit exists and equals toPZ(G,Φ,g) defined by using open covers,that is,
ProofOur proof is adapted from Climenhaga's elegament argument in[11]. On the one hand,givenδ>0,let
and
Note thatm(U) =m(Ug′)=|w′ |+ 1,then
Moreover,we can get
which implies
Taking the limitN→∞yields
This implies that
Asδ→0,that is,ε(δ) →0,|U| →0,γ→0,we obtain
It follows
Hence
This implies that
Taking the limit asδ→0 gives
It is obvious thatBw(g″;x,δ) ⊂Bw(2g″;x,δ),then we obtain
which completes the proof.
Let(X,d) be a compact metric space,f0,f1,…,fm-1continuous transformations fromXto itself. Similar to the definition of mean metric in[12],for anyx,y∈X,w∈F+m,we define a mean metric-dwonXas follows:
Forx∈Xandδ>0,let
In 2015,Gröger and Jäger[9]gave a definition of topological entropy of the whole system in mean metric by using separated sets,and proved that the topological entropy defined by mean metric is equivalent to the topological entropy defined by Bowen metric. Similar to the process of defining topological pressure of a free semigroupGin Section 1,we can also use the center of(x,δ) to define topological pressure on non-compact subsetZ,denoted by(G,Φ).
Proposition 1For anyZ⊂X,we have
Now,we chooseg(n,ε) =nε. It's clear that this function satisfies the definition of the mistake function.By the following lemma and Theorem 1,it is easy to obtain the above proposition,hence we omit the proof.
Lemma 3For anyx∈X,w∈,andε>0,we have
ProofFor anyy∈X,w∈,ifdw(x,y) <ε,then(x,y) <ε,so we have
Set
whereAw={w′:w′≤w}.Since
Thus,we obtain
Theny∈Bw(g;x,).Therefore,we have