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DIMENSIONS IN INFINITE ITERATED FUNCTION SYSTEMS CONSISTING OF BI-LIPSCHITZ MAPPING

CHIH-YUNG CHU#AND SZE-MAN NGAI*

Abstract. We study infinite iterated functions systems (IIFSs) consisting of bi-Lipschitz mappings instead of conformal contractions, focusing on IFSs that do not satisfy the open set condition. By assuming the logarithmic distortion property and some cardinality growth condition, we obtain a formula for the Hausdorff, box, and packing dimensions of the limit set in terms of certain topological pressure. By assuming, in addition, the weak separation condition, we show that these dimensions are equal to the growth dimension of the limit set.

1. Introduction

The study of infinite iterated function systems form an important branch of the theory of IFSs. Mauldin and Urbanski [10] showed that fractal phenomena not exhibited by finite IFSs can appear in IIFSs, such as the existence of dimensionless limit sets, and that the box and packing dimensions are strictly greater than the Hausdorff dimension. They also showed that IIFSs can be used to study complex continued fractions. Fernau [7] showed that IIFSs have stronger descriptive power than finite ones; in fact, any closed set in a separable metric space is the attractor of some IIFS, while there exists a closed and bounded subset of a complete metric space that is the attractor of an IIFS but not of a finite IFS.

The open set condition (OSC) is assumed in [10]. Dimensions of IIFSs consisting of conformal contractions, but not satisfying (OSC), are studied [11] by Tong and the second author. The conformality condition is relaxed in [3], but the IFSs studied are finite.

The main purpose of this paper is to weaken all three assumptions, namely, (OSC), finiteness of the IFS, and conformality. We assume, as in [3], that the IFS maps are bi- Lipschitz essential contractions. By assuming an IIFS satisfies the logarithmic distortion property and a cardinality growth condition (CGC) (see definitions in Section 2), we obtain a formula for the Hausdorff, box, and packing dimensions of the limit set, extending a theorem in [3].

2010Mathematics Subject Classification. Primary: 28A80, 28A78.

Key words and phrases. Fractal, infinite iterated function system, Hausdorff dimension.

The first author is supported in part by a Shaanxi Natural Science Foundation of China (Grant No.

2017JM1018), a State Foundation for Studying Abroad (CSC Scholarship No. 201706305020). The second author is supported in part by the National Natural Science Foundation of China, grant 11771136, and Construct Program of the Key Discipline in Hunan Province.

*Corresponding author. #The first author also publishes under the name Zhiyong Zhu.

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For FIFSs of contractive similitudes satisfying (WSC), Zerner proved in [12] that if the attractorK is not contained in a hyperplane, then the Hausdorff dimension ofK is equal to the growth dimension of the IFS. This result is extended by Deng and Ngai [2] to conformal FIFSs and by Ngai and Tong [11] to IIFSs of contractive similitudes. In this paper, we generalize this result to IFSs of essential contractions (see Theorem 2.18).

This paper is organized as follows. In Section 2, we first introduce some basic definitions, preliminary results, and assumptions, and then state the main results of this paper. In Section 3, we study the logarithmic distortion property (LDP) and a variant called the logarithmic* distortion property (L*DP). We also study two topological pressure functions.

Sections 4 is devoted to the proof of the main theorems on dimension formula. In Section 5, we study the growth dimension and prove that, under suitable assumptions, it equals the other dimensions. Finally in Section 6, we illustrate our main theorems by a number examples.

2. Preliminaries and Statements of Main Results

In this section we first introduce some basic definitions and notation. Then we state the main theorems in the paper.

Definition 2.1. LetXbe a non-empty compact subset ofRd, equipped with the Euclidean metric, and let I be a countable set with at least two elements, Si :X → X, i ∈I, be a countable family of mappings. If there exists a metricρonXthat is topologically equivalent to the Euclidean metric and a constantη ∈(0,1) such that

ρ(Si(x), Si(y))≤ηρ(x, y) for all i∈I and x, y∈X, (2.1) then we call{Si}i∈Ianiterated function system (IFS) of essential contractions with respect to ρ. We say that {Si}i∈I is an infinite iterated function system (IIFS) of essential con- tractions ifI is countably infinite, and a finite iterated function system (FIFS) of essential contractions ifI is finite.

Let

I0: ={∅}, Ik:={(i1, . . . , ik) :i1, . . . , ik∈I} fork≥1, I: =

[

k=0

Ik, I:={(i1, i2, . . .) :ij ∈I for all j≥1}.

We call I the space of finite words with alphabets i ∈ I, and I the coding space. For i= (i1, . . . , ik)∈Ik, we denote by |i|=kthelength ofi and writeSi:=Si1 ◦ · · · ◦Sik(S is defined to be the identity). We often denote i= (i1, . . . , ik) simply by i =i1. . . ik and let i−m :=i1. . . ik−m be the word obtained fromiby deleting its lastm(1≤m≤k) alphabets.

Ifi∈IS

I andn≥1 does not exceed the length ofi, we denote byi|n the wordi1· · ·in

consisting of the firstn alphabets ofi.

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Since ρ is topologically equivalent to the Euclidean metric, (X, ρ) is a compact metric space in Rd and {Si}i∈I is a family of contraction mapping on (X, ρ). For E ⊂ Rd, we denote the diameter of E by diam(E) = supx,y∈Eρ(x, y). For each i =i1i2· · · ∈ I, the compact sets Si|n(X), n≥1, are decreasing and their diameters converge to zero. In fact, by (2.1),

diam(Si|n(X))≤ηndiam(X). (2.2)

This implies that the set

π(i) =

\

n=1

Si|n(X)

is a singleton and therefore this formula defines a map π:I→X, called thecoding map, which, in view of (2.2), is continuous. Following [10] and [7], we define the limit set and attractor of an IFS as follows.

Definition 2.2. Let{Si}i∈I be an IFS described as above. Define thelimit set as K := [

i∈I

\

n=1

Si|n(X).

IfK is closed, it is called the attractor (orfixed point) of the IFS.

The limit setKis a Souslin set and is hence measurable with respect to Hausdorff measure (see, [4]). K is independent of the metric ρ. Moreover, K is the attractor if and only if it satisfiesK =S

i∈ISi(K). Since Sj(π(i)) =π(ji) for any j∈I andi∈I, we have K =π(I) =π

[

j∈I

[

i∈I

ji

= [

j∈I

[

i∈I

π(ji) = [

j∈I

[

i∈I

Sj(π(i))

=[

j∈I

Sj [

i∈I

π(i)

= [

j∈I

Sj(π(I)) = [

j∈I

Sj(K).

Thus the limit setK satisfies

K=[

i∈I

Si(K).

Notice that ifI is finite, thenK is compact. Unlike FIFSs,K is not necessarily compact if I is countably infinite. Also, ifKis not compact, it is not necessarily the unique non-empty bounded subset of Rd satisfying K =S

i∈ISi(K) (see, e.g., [11, Example 2.2]). It follows from Banach’s fixed point theorem and uniform contractivity that {Si}i∈I has a unique fixed point K, and if U ⊂ X is a nonempty invariant set (i.e., S

i∈ISi(U) ⊂ U), then K ⊂K⊂U. It is well known that ifI is finite, then

K =

\

n=1

[

i∈In

Si(X), (2.3)

and thus K is a Borel set. When I is countably infinite, Mauldin and Urba´nski in [10]

showed that (2.3) also holds under the assumption that the system{Si :i∈I}ispointwise finite (meaning that each element ofXbelongs to at most finitely many elements ofSi(X)).

In this case,K is anFσδ and is thus a Borel set. As pointed out in [10],K may even have a

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much more complicated descriptive set-theoretic structure when the system is not assumed to be pointwise finite. In this paper, we will consider such IFSs of essential contractions.

Let|·|denote the Euclidean metric. We write ri:= inf

x6=y∈X

|Si(x)−Si(y)|

|x−y| , Ri := sup

x6=y∈X

|Si(x)−Si(y)|

|x−y| , i∈I, (2.4) r := inf

i∈Iri, R := sup

i∈I

Ri, (2.5)

We also write rϕ :=ri and Rϕ:=Ri ifϕ=Si for somei∈I. Since for any i,j∈I,

|Sij(x)−Sij(y)|

|x−y| = |Sij(x)−Sij(y)|

|Sj(x)−Sj(y)| ·|Sj(x)−Sj(y)|

|x−y| , the following inequalities hold (see [2, 3, 9]):

Rij≤RiRj, rij≤Rirj, rij≤riRj,

rij≥rirj, Rij≥riRj, Rij≥Rirj, (2.6) which will be used repeatedly in the rest of this paper.

Assumption A. Throughout this paper we assume that ri >0 for eachi, equivalently, Si, i∈I, are bi-Lipschitz mappings with respect to Euclidean metric. In particular,r >0when I is finite.

Remark 2.3. It is possible that R ≥ 1. Since Si, i ∈ I, are essential contractions, Ri converges uniformly to 0 as |i|tends to infinity. As a consequence, we also have 0≤r <1 and R <+∞.

For anyE ⊂Rd, we use dimH(E),dimP(E),dimB(E),Hs(E),Ld,|E|, andE to denote, respectively, the Hausdorff dimension, packing dimension, box dimension, s-dimensional Hausdorff measure, d-dimensional Lebesgue measure, Euclidean diameter, and interior of E. For any set A, we let #Adenote its cardinality. A set U ⊂X is said to be open if it is open in the relative Euclidean topology of X.

Fix an invariant setU ⊂X and let 0< b <1. Define SI,b :={i= (i1, . . . , in)∈I :Ri ≤b < Ri},

SI,b (U) :={i= (i1, . . . , in)∈I:Ld(Si(U))≤bdLd(U)<Ld(Si(U)}, AI,b :={Si:i∈SI,b},

AI,b (U) :={Si :i∈SI,b (U)}.

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Remark 2.4. SinceRcan be greater than 1, for (i1, i2, . . .)∈I, there could be more than one prefix i = (i1, . . . , in) ∈ I such that i ∈ SI,b (resp. SI,b (U)). However, by Remark 2.3, the number of such prefixes must be finite.

Remark 2.5. It is possible that Si = Si0 for distinct i,i0 ∈ I; we identify such Si and Si0. For IFSs of contractive similitudes, SI,b =SI,b (U) and so AI,b =AI,b (U). In general, however, they need not be the same. For an IIFS, both AI,b and AI,b (U) are countably infinite sets.

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Definition 2.6. LetX ⊂Rd be nonempty compact subset with X 6=∅ and let Si :X → X, i∈I, be bi-Lipschitz essential contractions.

(a) We say that {Si}i∈I has the logarithmic distortion property (LDP) if there is a constantξ >0 such that

b→0lim+ sup

i∈SI,b

b

ri|lnb|ξ = 0.

(b) LetU ⊂X be an invariant set. We say that{Si}i∈I has thelogarithmic* distortion property (L*DP) if there is a constant ζ >0 such that

lim

b→0+ sup

i∈SI,b (U)

b

ri|lnb|ζ = 0 and lim

b→0+ sup

i∈SI,b (U)

Ri

ri|lnb|ζ = 0. (2.8) Mauldin and Urba´nski [10] defined thebounded distortion property (BDP) of an IFS of injectiveC1 conformal contractions. We extend this definition directly to IFSs of essential contractions as follows.

Definition 2.7. An IFS{Si}i∈I of essential contractions as in Definition 2.1 is said to have thebounded distortion property (BDP) if there exists a constantc >0 such that

Ri

ri ≤c for all i∈I.

Remark 2.8. In the above definitions, we do not assume that the IFS maps are differen- tiable.

Definition 2.9. Let X and {Si}i∈I satisfy the hypotheses of Definition 2.6, U ⊂X be a bounded invariant set that is open in the relative topology ofX withLd(U)>0, and Φ be a subset of {Si :i ∈I}. We call a subcollection{ϕj}j∈J ⊂Φ a packing family of Φ with respect toU if it satisfies the following two conditions:

(i) ϕj(U), j∈J, are pairwise disjoint;

(ii) for anyϕ∈Φ, ϕ(U) intersects at least oneϕj(U).

We denote by PI,U(b) the class of all packing families of AI,b with respect to U, and denote byPI,U (b) the class of all packing families ofAI,b (U).

Remark 2.10. The definition of packing familiy here is a generalization of that in [3] to the case I is countably infinite.

For an index set I, we define, throughout the rest of this paper,

F =F(I) :={J ⊂I : Jis finite}. (2.9) LetJ ∈ F and{Si}i∈J be the associated FIFS. For any 0< b <1, letPJ,U(b) andPJ,U (b) be the corresponding packing families as in Definition 2.9.

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Definition 2.11. Let X,{Si}i∈I and U satisfy the hypotheses of Definition 2.9. We say that{Si}i∈I satisfies cardinality growth condition (CGC) with respect toU if

γ := sup

J∈F b→0+lim

ln(supΦ∈PJ,U(b)#Φ)

−lnb <∞. (2.10)

We generalize the definition of topological pressure functions in [3] as follows.

Definition 2.12. Let X,{Si}i∈I and U satisfy the hypotheses of Definition 2.9 and fix λ∈(0,1). Define

Qλ(s) := sup

J∈F

lim

n→∞

1 nln

Φ∈PinfJ,Un)

X

ϕ∈Φ

Rsϕ

, s∈R, Qλ(s) := sup

J∈F

n→∞lim 1 nln

sup

Φ∈PJ,Un)

X

ϕ∈Φ

Rsϕ

, s∈R.

We callQλ (resp. Qλ) thelower (resp. upper)topological pressure function with scale λ. If Qλ =Qλ, we denote byQλ the common function and call it atopological pressure function with scale λ. Note that λis fixed and sis the variable of the functions Qλ(s) and Qλ(s).

Similar to Definition 2.12, we define Qλ(s) := sup

J∈F

lim

n→∞

1 nln

Φ∈PinfJ,U n)

X

ϕ∈Φ

[Ld(ϕ(U))]s/d

, s∈R, Qλ(s) := sup

J∈F

n→∞lim 1 nln

sup

Φ∈PJ,U n)

X

ϕ∈Φ

[Ld(ϕ(U))]s/d

, s∈R.

Definition 2.13. LetX and {Si}i∈I satisfy the hypotheses of Definition 2.6. We say that {Si}i∈I satisfies the weak separation condition (WSC) if there exist an invariant subset D⊂X withD 6=∅, called aWSC-region, and a constant κ∈N such that

sup

x∈X

#

ϕ∈AI,b :x∈ϕ(D) ≤κ for allb∈(0,1). (2.11) IfE ⊂X is an invariant subset and (2.11) holds, we callE aWSC-set.

For any J ∈ F, we denote by KJ the attractor of the FIFS {Si}i∈J and write αJ :=

dimHKJ.

Definition 2.14. LetX and {Si}i∈I satisfy the hypotheses of Definition 2.6. We callK a quasi s-set ifHαJ(KJ)<∞ for any J ∈ F.

Remark 2.15. If{Si}i∈Isatisfies (BDP) and (WSC), then it follows from [9, Theorem 3.2]

thatK is a quasis-set.

We now state the first two main results of this paper.

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Theorem 2.16. Let X,{Si}i∈I, U satisfy the hypotheses of Definition 2.9. Assume that (LDP) and (CGC) hold. Then for any λ ∈ (0,1) and any sequence of packing families {Sin,j}kj=1Jn ∈PJ,Un), n∈N, the following hold:

(a) for all s∈R,

Qλ(s) =Qλ(s) = sup

J∈F

n→∞lim 1 nln

k

Jn

X

j=1

Rsin,j

= (s−dimHK) lnλ;

(b) let γ be defined in Definition 2.11, then

dimHK = dimPK= dimBK =γ = sup

J∈F

n→∞lim lnknJ

−nlnλ

.

Theorem 2.17. Let X,{Si}i∈I, U satisfy the hypotheses of Definition 2.9. Assume that (LDP), (L*DP) and (CGC) hold. Then for any λ ∈ (0,1) and any sequence of packing families {Sin,j}kj=1Jn ∈PJ,Un), n∈N, we have

Qλ(s) = Qλ(s) = sup

J∈F

n→∞lim 1 nln

knJ

X

j=1

[Ld(Sin,j(U)]s/d

=Qλ(s)

= s−dimHK

lnλ for alls∈R.

LetX⊂Rdbe nonempty compact subset withX6=∅, and{Si}i∈I be a IFS of essential contractions on X (I is finite or countably infinite). Following Zerner [12], we define the growth dimension of an FIFS{Si}i∈I as

dG= lim

b→0+

ln #AI,b

−lnb .

For each finite set J ⊂ I, we denote by dJG the growth dimension of the associated FIFS {Si}i∈J. Following [11], we define the growth dimension of the IIFS{Si(x)}i∈I (In this case,

#(AI,b) =∞ for any b∈(0,1)) as

dG= sup{dJG :J ⊂Iis finite}. (2.12) Theorem 2.18. Let X,{Si}i∈I, U satisfy the hypotheses of Definition 2.9 and let K be the associated limit set. Assume that (LDP), (WSC) and (CGC) hold, and K is both a WSC-set and a quasi s-set. Then

dimHK= dimPK = dimBK=γ=dG, where dG is the growth dimension of K.

3. (LDP), (L*DP), and Topological Pressure Functions

3.1. Properties of (LDP) and (L*DP). For any E ⊂X and any i∈ I, the following inequalities will be used repeatedly,

ri|E| ≤ |Si(E)| ≤Ri|E|,

ri(Ld(E))1/d ≤(Ld(Si(E)))1/d≤Ri(Ld(E))1/d. (3.1)

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Lemma 3.1. Assume the same hypotheses on X and {Si}i∈I as in Definition 2.9, and assume that (LDP) holds. Let Ri and ri be defined as in (2.4), and ξ > 0 be defined as in Definition 2.6(a). Then for all b0 > 0 sufficiently small, there exists a constant c1 =c1(b0)>0 such that

b

c1|lnb|ξ ≤ri≤Ri≤bfor all i∈SI,b and b∈(0, b0). (3.2) Moreover, c1(b0)→0 as b0 →0.

Proof. By Definition 2.6, for sufficiently smallb0 >0, 0< c1 := sup

b∈(0,b0)

sup

i∈SI,b

b

ri|lnb|ξ <∞.

This implies that b

ri|lnb|ξ ≤ c1 for any b ∈ (0, b0). Thus the conclusion follows from the

definition ofSI,b and the factri≤Ri.

Lemma 3.2. Assume the same hypotheses onX, {Si}i∈I andU as in Definition 2.9, and assume that (L*DP) holds. LetRiandribe as in (2.4), andζ >0be defined as in Definition 2.6(b). Then for allb0 >0 sufficiently small, there is a constant c2 =c2(b0)>0 such that

b

c2|lnb|ζ ≤ri ≤Ri ≤c2|lnb|ζb for alli∈SI,b (U) and b∈(0, b0). (3.3) Moreover, c2(b0)→0 asb0 →0.

Proof. By Definition 2.6(b), there exists a constantc3 > 0 such that for sufficiently small b0 >0,

0< c3 = sup

b∈(0,b0)

sup

i∈SI,b (U)

b

ri|lnb|ζ <∞ and a constantc4>0 such that

0< c4= sup

b∈(0,b0)

sup

i∈SI,b (U)

Ri

ri|lnb|ζ <∞.

This implies that for anyb∈(0, b0), b

ri|lnb|ζ ≤c3 and Ri

ri|lnb|ζ ≤c4. (3.4) By the definition ofSI,b (U) and (3.1),i∈SI,b (U) implies that

ri

Ld(Si(U)) Ld(U)

1/d

≤b. (3.5)

By lettingc2 := max{c3, c4}and combining (3.4), (3.5), and the fact thatri≤Ri, we obtain

(3.3).

Remark 3.3. If{Si}i∈I satisfies (BDP), then there is a constantc >0 such thatRi/ri ≤c for alli∈SI,b∪SI,b (U). Thus from (3.2) and (3.3), respectively, (LDP) and (L*DP) hold.

Examples of IFSs satisfying (LDP) and (L*DP) but not (BDP) will be given in Section 6.

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Let σ : I → I denote the left shift map on I, i.e., σ(i) = i2i3· · · for i =i1i2· · ·. Since it is possible thatRij≥Ri for some i,j∈I (see Remark 2.4), we have the following property.

Proposition 3.4. Letr <1andSI,Ribe defined as in (2.5)and (2.7)respectively. Assume thatr >0. Then there exists an integer k0>0 such that for anyi∈I with |i|> k0, there is a decomposition i=i1i2 with |i2| ≤k0 such thati1 ∈SI,Ri.

Proof. As mentioned in Remark 2.3, Ri → 0 uniformly as |i| → ∞. Thus there exists an integerk0 >0 such thatRi≤rfor alli∈Iwith|i| ≥k0. Leti∈Iwith|i|=n > k0. First we check Ri−1. IfRi< Ri−1, then we takei1 =i andi2 =∅, and thus the conclusion holds.

If not, we check Ri−2. If Ri < Ri−2, then Ri−1 ≤Ri< Ri−2. Thus the conclusion holds by lettingi1 =i−1 andi2n−1(i). Continue. Note that there exists some 1≤k≤n−1 such thatR2−k+1 ≤Ri< R−ki , for otherwise, one would getr ≤Rin−1 ≤Ri < r, a contradiction.

We further claim that there exists somek∈Nwith 1≤k≤k0suchRi−k+1 ≤Ri< Ri−k. To see this we suppose on the contrary that there exists some`∈Nsatisfyingk0+1≤`≤n−1 such thatRi−(`−1) ≤Ri< Ri−`. Then one would get

Ri−(`−1) ≤Ri≤Ri−(`−1)Rσn−(`−1)(i)≤Ri−(`−1)r < Ri−(`−1),

where the third inequality is because |σn−(`−1)(i)|=`−1≥k0. This contradiction proofs the claim. The asserted result now follows by letting i1 =i−k and i2n−k(i).

Lemma 3.5. Assume the same hypotheses on X, {Si}i∈I and U as in Definition 2.9 and r be defined as in (2.5). If r >0, then (LDP) implies (L*DP).

Proof. Letk0 be as in Proposition 3.4. For t∈ I with |t|=n≥k0, let n=lk0+t with 0≤t < k0. Then rn≤rt≤Rt≤rl. Taking logarithm, we have

nlnr≤lnrt≤lnRt≤llnr≤ nlnr

k0 , |t| ≥k0. This implies that

lnRt lnrt ≥ 1

k0 >0. (3.6)

Let ξ > 0 be as in Definition 2.6(a) and b0 ∈ (0,1) be sufficiently small. Since (LDP) holds, we have from Lemma 3.1 that there is a constantc1 >0 such that

b

c1|lnb|ξ ≤ri≤Ri≤b for all i∈SI,b andb∈(0, b0). (3.7) To prove (2.8), we assume, without loss of generality, that|j|> k0 for anyj∈SI,b (U) and Rj < b0, since we need only consider sufficiently small b >0. By the definition ofSI,b (U), we have

Ld(Sj(U)) Ld(U)

1/d

≤b <

Ld(Sj−1(U)) Ld(U)

1/d

, and thus rj ≤b < Rj−1. AsRj ≥Rj−1r, we get

rj ≤b < r−1Rj. (3.8)

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Combining (3.6) and (3.8), we see that exists some constant ˜c≥1 such that

˜

c−1≤ lnRj

lnb ≤˜c. (3.9)

As|j|> k0, Proposition 3.4 implies that there exists a decompositionj=j1j2 with|j2| ≤k0 such that j1 ∈ SI,Rj. As Rj < b0, substituting b and i in (3.7) by Rj and j1 respectively yields

Rj

rj1|lnRj|ξ ≤c1.

Using (2.6) and the fact thatj1∈SRj and |j2| ≤k0, we have

rk0rj1 ≤rj1rj2 ≤rj≤rj1R|j2|. (3.10) Combining (3.8)–(3.10), we get

b

rj|lnb|ξ ≤ r−1Rjξ

rk0rj1|lnRj|ξ ≤ c1˜cξ

rk0+1 =:c3<∞ (3.11) and

Rj

b|lnb|ξ ≤ Rj

rj|lnb|ξ ≤ Rjξ

rk0rj1|lnRj|ξ ≤ c1˜cξ

rk0 ≤ c1˜cξ

rk0+1 =c3 <∞. (3.12) Furthermore, we can see from the proof of Lemma 3.1 that c1 → 0 as b0 → 0. Therefore c3 → 0 as b0 → 0, and thus the (L*DP) holds from the (3.11), (3.12) and the fact b ∈

(0, b0).

3.2. Properties of topological pressures.

Proposition 3.6. Let X,{Si}i∈I and U satisfy the hypotheses of Definition 2.9. Let λ∈ (0,1)and r be defined as in (2.5). Assume that r >0 and (CGC) holds. Then both Qλ(s) and Qλ(s) are real-valued, strictly decreasing, and continuous functions on R that tend to

−∞ and ∞ as s tends to ∞ and −∞, respectively. Moreover, Qλ(0) ≥ Qλ(0) ≥ 0 and Qλ(s) is convex on R.

Proof. Let k0 be described as in Proposition 3.4. Write C := sup{Ri : |i| < k0}. Then C < ∞. For any J ∈ F, let ϕ = Si1···ik ∈ Φ ∈ PJ,Un). Let k−1 = lk0 +m with 0≤m < k0, wherel∈N∪ {0}. Then we haveRi1···ik−1 ≤Crl≤C0rk/k0 for some constant C0. Hence

rk≤rϕ≤Rϕ≤λn< Ri1···ik−1 ≤C0rk/k0. (3.13) It follows that

k < nk0logrλ−k0logrC0, (3.14) and thus

Rϕ ≥rnk0logrλ−k0logrC0. (3.15) It follows that from (3.13) and (3.15) that whens≥0,

r(nk0logrλ−k0logrC0)s≤ X

ϕ∈Φ

Rϕs ≤#Φλns,

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and when s <0,

λns≤ X

ϕ∈Φ

Rsϕ≤#Φr(nk0logrλ−k0logrC0)s. Thus ifs≥0,

sk0lnλ−sk0lnC0

n ≤ ln(infΦ∈PJ,Un)

P

ϕ∈ΦRϕs) n

≤ ln(supΦ∈PJ,Un)

P

ϕ∈ΦRsϕ) n

≤ ln(supΦ∈PJ,Un)#Φ)

n +slnλ

≤ ln(supΦ∈PJ,Un)#Φ)

−lnλn (−lnλ) +slnλ;

ifs <0,

slnλ ≤ ln(infΦ∈PJ,Un)

P

ϕ∈ΦRsϕ) n

≤ ln(supΦ∈PJ,Un)

P

ϕ∈ΦRsϕ) n

≤ ln(supΦ∈PJ,Un)#Φ)

n +sk0logrλlnr−sk0logrC0lnr n

= ln(supΦ∈PJ,Un)#Φ)

−lnλn (−lnλ) +sk0lnλ−sk0lnC0

n .

Lettingn→ ∞ and using (2.10) and the definitions ofQλ(s) and Qλ(s), we get sk0lnλ≤ Qλ(s)≤ Qλ(s)≤(s−γ) lnλ, ifs≥0;

slnλ≤ Qλ(s)≤ Qλ(s)≤(sk0−γ) lnλ, ifs <0.

HenceQλ(s) andQλ(s) are real-valued, Qλ(0)≥ Qλ(0)≥0. Moreover, since 0< λ <1, we have lims→∞Qλ(s) = lims→∞Qλ(s) =−∞ and lims→−∞Qλ(s) = lims→−∞Qλ(s) =∞.

Next, since Qλ(s) and Qλ(s) are real-valued, for any δ >0, we have Qλ(s+δ) ≤ sup

J∈F

n→∞lim 1 nln

sup

Φ∈PJ,Uλn

X

ϕ∈Φ

Rsϕλ

= Qλ(s) +δlnλ <Qλ(s), (3.16) and by (3.15),

Qλ(s+δ) ≥ sup

J∈F

n→∞lim 1 nln

sup

Φ∈PJ,Uλn

X

ϕ∈Φ

Rϕsrδ(nk0logrλ−k0logrC0)

= Qλ(s) +δk0lnλ, that is,

Qλ(s) +δk0lnλ≤ Qλ(s+δ)≤ Qλ(s) +δlnλ <Qλ(s). (3.17)

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Moreover, for anyδ >0, we also have Qλ(s−δ) ≤ sup

J∈F

n→∞lim 1 nln

sup

Φ∈PJ,Uλn

X

ϕ∈Φ

Rϕsr−δ(nk0logrλ−k0logrC0)

≤ Qλ(s))−δk0lnλ, Qλ(s−δ) ≥ sup

J∈F

n→∞lim 1 nln

sup

Φ∈PJ,Uλn

X

ϕ∈Φ

Rsϕλ−nδ

≥ Qλ(s)−δlnλ >Qλ(s), that is,

Qλ(s)<Qλ(s)−δlnλ≤ Qλ(s−δ)≤ Qλ(s))−δk0lnλ. (3.18) From (3.17) and (3.18), we see that Qλ(s) is strictly decreasing and continuous on R. We can get analogous results for Qλ(s) in the same way.

Finally, for any 0< t < 1, s1, s2 ∈R, we have by using Young’s inequality and the fact that lnx is convex,

Qλ(ts1+ (1−t)s2) = sup

J∈F

n→∞lim 1 nln

sup

Φ∈PJ,Uλn

X

ϕ∈Φ

Rtsϕ1R(1−t)sϕ 2

= sup

J∈F

n→∞lim 1 nln

sup

Φ∈PJ,Uλn

X

ϕ∈Φ

(Rϕs1)t(Rsϕ2)1−t

≤ tsup

J∈F

n→∞lim 1 nln

sup

Φ∈PJ,Uλn

X

ϕ∈Φ

Rs1

+ (1−t) sup

J∈F

n→∞lim 1 nln

sup

Φ∈PJ,Uλn

X

ϕ∈Φ

Rs2

= tQλ(s1) + (1−t)Qλ(s2). (3.19) ThusQλ(s) is convexity on R. This completes the proof.

We define the effective domains ofQλ as

domQλ :={s∈R:−∞<Qλ(s)<∞}.

The effective domain of Qλ is defined analogously, denoted by dom(Qλ). We have the following property without assumingr >0.

Proposition 3.7. Let X,{Si}i∈I and U satisfy the hypotheses of Definition 2.9. Assume thatλ∈(0,1)and (CGC) holds. ThenQλ(s)(resp. Qλ(s)) is strictly decreasing ondomQλ (resp. domQλ) that tends to −∞ as s tends to∞. Moreover,Qλ(s) is convex ondomQλ, and hence continuous on(domQλ), 0≤ Qλ(0)≤ Qλ(0) =−γlnλ <∞, whereγ is defined as in (2.10).

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Proof. It follows from (CGC) holds and the definitions ofQλ(s) andQλ(s) that 0 ≤ Qλ(0)≤ Qλ(0) = sup

J∈F

n→∞lim

ln(supΦ∈PJ,Un)#Φ) n

= sup

J∈F

n→∞lim

ln(supΦ∈PJ,Un)#Φ)

−lnλn (−lnλ)

=−γlnλ <∞.

Next, for any s ∈ domQλ and δ > 0 with s+δ ∈ domQλ, we can see from the proof of Proposition 3.6 that (3.16) holds forQλ, and exactly the same inequality as (3.16) holds for Qλ. Moreover, we have from the proof of Proposition 3.6 that (3.19) holds forQλ. Hence

the rest of conclusions hold.

The next Lemma follows from [3, Proposition 18] and Assumption A.

Lemma 3.8. Let X and {Si}i∈I satisfy the hypotheses of Theorem 2.16. Then for any nonempty invariant open set U ⊂ X with Ld(U) > 0 and sequence of packing families {Sin,j}kjJn of AJ,λn, we have

Qλ(s) = sup

J∈F

lim

n→∞

1 nln

knJ

X

j=1

Rsin,j

= sup

J∈F

lim

n→∞

1 nln

kJn

X

j=1

rsin,j

, s∈R

Qλ(s) = sup

J∈F

n→∞lim 1 nln

kJn

X

j=1

Rsi

n,j

= sup

J∈F

n→∞lim 1 nln

kJn

X

j=1

ris

n,j

, s∈R.

The above Lemma implies that for IFSs satisfying (LDP) and (CGC), the definitions of the topological pressures are independent of the choice of the invariant open setU and the packing families ofAJ,λn.

4. Proof of Theorem 2.16 and Theorem 2.17

LetX,{Si}i∈I andρ be described as in Definition 2.1. We assume that there exists a set p={pi :i∈I} with 0< pi <1 and P

i∈Ipi = 1. Let S ={Si}i∈I,Mbe the set of Borel regular probability measures having bounded support onX. Let

BC(X) ={f :X→R:fis continuous and bounded on bounded subsets}.

Forµ∈ M, φ∈ BC(X), define µ(φ) =R

φdµ. For ν∈ M, we define S:M → Mby S(ν)(A) =X

i∈I

piν(Si−1(A)), for any Borel setA⊂X.

We say that ν is variant with respect to (S,p) if S(ν) =ν. Using a proof similar to that of [8, Theorem 4.4(1)], we have

Lemma 4.1. Let X, {Si}i∈I and ρ be described as in Definition 2.1. Then there exists a unique Borel regular probability measure µsuch that µ=P

i∈Ipiµ◦Si−1.

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Let X and {Si}i∈I be described as in Definition 2.1. We say that {Si}i∈I satisfies the open set condition (OSC)if there exists a nonempty bounded invariant open set O⊂X (in the relative Euclidean topology of X), called an OSC-set, such that Si(O)∩Sj(O) =∅for all i6=j.

Using Lemma 4.1 and a similar proof as that of [3, Proposition 20], we have the following result.

Proposition 4.2. Let K be the attractor of an FIFS {Si}i∈I satisfying the hypotheses of Definition 2.6, and assume that (LDP) holds. If (OSC) holds with an OSC-set U ⊇K and P

j∈Irsj >1 withrj <1, then dimHK≥s.

Proposition 4.3. LetK be the limit set of the IFS{Si}i∈I, andAI,b be defined as in (2.7).

Then K=S

ϕ∈AI,bϕ(K).

Proof. For any i ∈ I, we have Si(K) ⊂ K since K = S

i∈ISi(K). This implies that for any ϕ = Si1···in ∈ AI,b, ϕ(K) ⊂ K. Thus S

ϕ∈AI,bϕ(K) ⊂ K. Notice that the following consequences:

K = [

i∈I

Si(K) =[

i∈I

Si([

j∈I

Sj(K)) = [

i,j∈I

Sij(K) =· · ·

= [

i1,...,ip∈I

Si1···ip(K).

Similarly,

Si1···ip(K) = Si1···ip

[

ip+1∈I

Sip+1(K)

= [

ip+1∈I

Si1···ipip+1(K).

Thus if x ∈ K, then there exists i = i1i2· · · ∈ I such that K ⊃ Si1(K) ⊃ Si1i2(K) ⊃

· · · ⊃ {x}. Since there exists n such that i|n ∈ SI,b, we have x ∈ Si|n(K), and thus K ⊂S

ϕ∈AI,bϕ(K). This completes this proof.

Proposition 4.4. Let K be the limit set of the IFS {Si}i∈I and F be defined as in (2.9).

Then K=S

J∈FKJ.

Proof. Since KJ ⊂ K, we haveS

J∈FKJ ⊂K. Next we prove reverse inclusion. For any x∈K, it follows from the definition of π and Definition 2.2 that there exists i1i2· · · ∈I such that

x=

\

p=1

Si1···ip(X).

We write {x} = xi1i2···. Let i\1· · ·ip denote the infinite sequence i1· · ·ipi1· · ·ip· · · ∈ I with recurrent blocki1· · ·ip. Since

Sj1···jq(xi1i2···)∈Sj1···jq(

\

p=1

Si1···ip(X)) =

\

p=1

Sj1···jqi1···ip(X) =xj1···jqi1···ip···,

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we have Si1···ip(xi\

1···ip) = xi\

1···ip. It follows that xi\

1···ip is the unique fixed point si1···ip of Si1···ip. Thus bothsi1···ipandxi1···ip···belong toSi1···ip(X). Since limp→∞diam(Si1···ip(X)) = 0, we have limp→∞si1···ip =xi1···ip···. For anyp≥1, we chooseJ ∈ F such that (i1, . . . , ip)∈ Jp ={(i1, . . . , ip) : ij ∈J, 1≤j ≤p}. Then si1···ip ∈ KJ, and thus x∈S

J∈FKJ. Notice that S

J∈FKJ is a close set, and for any y ∈K, there exists a sequence {xn} of points in K such that limn→∞xn=y. We see that K ⊂S

J∈FKJ. This completes the proof.

Proof of Theorem 2.16. By Lemma 3.8, we first requireK⊂U. By Proposition 3.7,Qλ(0) and Qλ(0) are real numbers. We first prove that domQ= domQ=R, and for any s∈R,

Qλ(s) =Qλ(0) +slnλ= (s−α) lnλ,

Qλ(s) =Qλ(0) +slnλ= (s−β) lnλ, (4.1) whereα, β are the unique zeroes ofQλ(s) andQλ(s), respectively. Substitutingb=λn and i=in,j into (3.2) yields

λn

c1(n|lnλ|)ξ ≤rin,j ≤Rin,j ≤λn, n= 1,2, . . . , j= 1, . . . , knJ. Hence

kJnλns≥PkJn j=1Rsi

n,j ≥knJ c 1

1(n|lnλ|)ξ

s

λns, ifs≥0;

kJnλns≤PkJn j=1Rsi

n,j ≤knJ c 1

1(n|lnλ|)ξ

s

λns, ifs <0.

Since

n→∞lim 1 nln

1 c1(n|lnλ|)

s

= 0,

by using Proposition 3.8 and the fact that Qλ(0) andQλ(0) are real numbers, we have Qλ(s) = sup

J∈F

lim

n→∞

1 nln

k

Jn

X

j=1

Risn,j

= sup

J∈F

lim

n→∞

1

nln(knJλns)

= Qλ(0) +slnλ Qλ(s) = sup

J∈F

n→∞lim 1 nln

kJn

X

j=1

Risn,j

= sup

J∈F

n→∞lim 1

nln(knJλns)

= Qλ(0) +slnλ. (4.2)

This implies that domQ = domQ =R. Moreover, by the properties of slnλ, Qλ(s) and Qλ(s) are strictly decreasing and continuous on R that tend to −∞ and ∞ as s tends to ∞ and −∞, respectively. So, Qλ(s) and Qλ(s) have unique zero, denote by α and β, respectively. Thus we have Qλ(0) =−αlnλand Qλ(0) =−βlnλ, and thus (4.1) holds.

Next, we prove

β≤dimHK.

Suppose, on the contrary, β > dimHK. Assume dimHK < s < β. By (4.1), Qλ(s) = (s−β) lnλ >0. This implies, by Proposition 3.8, that there exists J ∈ F such that

n→∞lim 1 nln

kJn

X

j=1

rsin,j ≥ Qλ(s) 2 >0,

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Thus there exists an integern >0 depending onJ, such that 1

nln

kJn

X

j=1

rsin,j ≥ Qλ(s) 2 >0.

Let KnJ denote the attractor of the new FIFS {Sin,j}kj=1Jn . Then this FIFS satisfies (OSC) with U being an OSC-set. Since U ⊃ KnJ, by applying Proposition 4.2 to the new FIFS {Sin,j}kj=1Jn , we get dimHKnJ ≥s. Notice that KnJ ⊂KJ and the fact

KJ = [

i∈J

\

m=1

Si|m(X)⊂ [

i∈I

\

n=1

Si|n(X) =K,

we get dimHK≥dimHKJ ≥dimHKnJ ≥s, a contradiction. Thus dimHK ≥β.

Now, we prove

Qλ(s) =Qλ(s) = (s−dimHK) lnλ. (4.3) To this end we first prove α ≥dimHK. Let s > α. Then by (4.1), Qλ(s) <0, and thus s > 0 by Proposition 3.7. By assumption, for each integer n > 0, {Sin,j}kj=1nJ is a packing family of AJ,λn with respect to U, where J ∈ F. This implies from Definition 2.9 that for eachϕ∈AJ,λn, there is at least onejsuch thatϕ(U)∩Sin,j(U)6=∅. Choosexn,j ∈Sin,j(U).

By (3.1), both |ϕ(U)| and

Sin,j(U)

are less than λn|U|. Thus ϕ(U) is contained in the ballBn|U|(xn,j) with radius 2λn|U|. It follows from Proposition 4.3 and the factKJ ⊂U that

KJ = [

ϕ∈AJ,λn

ϕ(KJ)⊂ [

ϕ∈AJ,λn

ϕ(U)⊂

kJn

[

j=1

Bn|U|(xn,j).

This implies that{Bn|U|(xn,j)}kj=1Jn is a 4λn|U|cover ofKJ. Thus {Bn|U|(xn,j) :j= 1,2, . . . , knJ, J ∈ F } is a 4λn|U|cover ofS

J∈FKJ. Notice thatK =S

J∈FKJ (Proposition 4.4). This implies that

{Bn|U|(xn,j) :j= 1,2, . . . , knJ, J ∈ F }

is a 6λn|U|cover ofK. By the compactness ofK, there existJ1, . . . , Jp such that K⊂

p

[

i=1 kJin

[

j=1

Bn|U|(xn,j). (4.4)

It follows from Proposition 3.8 and (4.2) that sup

J∈F

lim

n→∞

1

nln[kJn(6λn|U|)s]

=Qλ(0) +slnλ=Qλ(s)<0.

There exists infinitely many integersnsuch thatkJn(6λn|U|)s<1. Notice thatK⊂K and there existsJ∈ F such that

kJn1 +· · ·+kJnp ≤kJn. (4.5)

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