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Parseval frames from compressions of Cuntz algebras.

Christoffersen, Nicholas ; Dutkay, Dorin Ervin ; et al.
In: Mathematische Zeitschrift, Jg. 304 (2023-05-01), Heft 1, S. 1-36
Online academicJournal

Parseval frames from compressions of Cuntz algebras 

A row co-isometry is a family (V i) i = 0 N - 1 of operators on a Hilbert space, subject to the relation ∑ i = 0 N - 1 V i V i ∗ = I. As shown in Bratteli et al. (J Oper Theory, 43, 97–143, 2000), row co-isometries appear as compressions of representations of Cuntz algebras. In this paper we will present some general constructions of Parseval frames for Hilbert spaces, obtained by iterating the operators V i on a finite set of vectors. The constructions are based on random walks on finite graphs. As applications of our constructions we obtain Parseval Fourier bases on self-affine measures and Parseval Walsh bases on the interval.

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Introduction

Structured bases appear in harmonic analysis, operator theory, and approximation theory, among other areas. The classical example of a structure basis is an exponential (Fourier) basis, which gives rise to Fourier series expansions. A probability measure μ on Rd is spectral if there exists a sequence of exponential functions that form an orthonormal basis for L2(μ) . Lebesgue measure on the unit (hyper-)cube is spectral; remarkably, Jorgensen and Pedersen initially showed that there are fractal measures which are spectral [[26]]. Wavelet bases [[8]] are another ubiquitous class of structured bases. These arise from the action of a system of unitary operators on L2(R) —dilations and translations [[12]]—that encode natural operations on the latent space. Wavelets, however, lead a double existence between L2(R) and 2(Z) , as elucidated by Mallat [[27]]. Wavelet bases in 2(Z) are generated by the iterated action of a finite number of (co-)isometries. These co-isometries give rise to a notion of scale in 2(Z) , and the corresponding scale decomposition is referred to as the cascade algorithm.

In the case of wavelet bases, the co-isometries {Si} satisfy what are now known as the Cuntz relations:

i=0N-1SiSi=I,SjSi=δj,iI

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These relations were in fact observed by engineers—albeit without a precise mathematical formulation—in the first half of the twentieth century. Cuntz is credited with the discovery and thorough study of the algebras generated by such systems of co-isometries and the associate representation theory of those algebras [[7]]. The role played by the Cuntz algebras in wavelet theory was described in the work of Bratteli and Jorgensen [[1]–[4]]. Orthonormal wavelet bases (ONB) are constructed from various choices of quadrature mirror filters (e.g. see [[8]]). These filters are in one-to-one correspondence with certain representations of a Cuntz algebra.

The Cuntz relations give an elegant way to understand the geometry of cascade algorithms (for example the Discrete Wavelet Transform). The first identity is used to decompose a vector v into a "cascade" of bits Siv , where i indexes from 0 to N-1 . Recovery of v is obtained through the same identity: apply each Si to the bits and sum it all up. The second relation (orthogonality of operators) tells us that bit interference/overlapping is avoided.

In [[13]] new examples of orthonormal bases and also classic ones were found to be generated by Cuntz algebra representations. More precisely, a multitude of ONBs such as Fourier bases on fractals, Walsh bases on the unit interval, and piecewise exponential bases on the middle-third Cantor set can be gathered under the umbrella of Cuntz algebra representations. Moreover, in [[14]] a connection between the ONB property and irreducibility of a Cuntz algebra representation was made in the particular case of Walsh systems.

However, orthonormal bases are sometimes too restrictive—for example, not all measures are spectral [[26]], and orthogonal wavelets may lack certain desirable properties [[8]]. Non-orthogonal expansions given by frames were introduced by Duffin and Schaffer [[18]] and popularized by [[9]]. A Parseval frame for a Hilbert space H is a family of vectors {ei}iI such that

v2=iI|v,ei|2,(vH).

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Parseval frames arise naturally as images of orthonormal bases under a co-isometry; notably, by the Naimark dilation theorem, all Parseval frames have this form [[22]].

One of our main motivations and applications comes from the harmonic analysis of fractal measures. The study of orthogonal Fourier series on fractal measures began with the paper [[26]], in connection with the Fuglede conjecture [[21]]. Jorgensen and Pedersen proved that, for the Cantor measure μ4 on the Cantor set C4 with scale 4 and digits 0 and 2, the set of exponential functions

e2πiλx:λ=k=0n4kll,nN,lk{0,1},

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is an orthonormal basis of L2(μ4) . Many more examples of spectral measures have been constructed since, see, e.g., [[10], [29]]. For the classical middle-third Cantor measure, Jorgensen and Pedersen proved that this construction is not possible [[26], Section 6], so that measure is not spectral. Strichartz [[29]] posed the natural question of whether this measure has a frame of exponential functions. This question is still open! Non-orthogonal (but non-frame) Fourier series expansions for the middle-third Cantor measure were constructed in [[24]].

Motivated by Strichartz's question, in [[28]], weighted Fourier Frames were obtained for the Cantor C4 set by making the set bigger, then constructing a basis for the bigger set, and then projecting the basis onto the Cantor set. Using the same dilation technique, in [[16]], a multitude of Parseval frames of weighted exponential functions and generalized Walsh bases were constructed for self-affine measures and for the unit interval. These constructions lead naturally to reconsidering the Cuntz relations, noting that only the first relation is needed to reconstruct a signal originally decomposed by a cascade algorithm. In such a set-up the operators (Si)i=0N are called row co-isometries.

In this paper we continue with the philosophy first emphasized in [[22]]—that frames are compressions of orthogonal bases—by considering compressions of Cuntz algebras. Indeed, one key idea is a dilation result from [[5]] (Theorem 2.3 in the next section) which allows one to extend a representation of a row co-isometry (which lacks the orthogonality constraints) to a "genuine" Cuntz algebra representation. We extend this philosophy to the pair Parseval frame, row co-isometries. By doing so, we will present a general framework for the construction of Parseval frames and orthonormal bases from row co-isometries, a framework which includes both of the following settings: (i) Fourier bases on self-affine measures and (ii) Walsh bases on the interval. We show that the new results are effective and can capture and unify previously obtained examples of Parseval frames and ONBs.

In Sect. 2 we include some definitions and notations; in Sect. 3 we state the main results; in Sect. 4, we present the proofs and some related results, and in Sect. 5 we apply the theory to various classes of examples.

Preliminaries and notations

Definition 2.1

Let H be a Hilbert space. A family of N bounded operators {Si}i=0N-1 on H that satisfy the relations

i=0N-1SiSi=IH,SjSi=δj,iI,(i,j{0,,N-1})

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is called a family of Cuntz isometries, or a a representation of the Cuntz algebra ON .

Note that the second relation implies that the operators are isometries with orthogonal ranges, and the first relation implies that the sum of the ranges add up to the whole space.

Such a representation is called irreducible if the only operators A on H, that commute with Si and Si , i.e., ASi=SiA , ASi=SiA , for all i{0,,N-1} , are multiples of the identity A=cIH , for some cC . Equivalently, a representation is irreducible if and only if the only closed subspaces K of H which are invariant for the representation, i.e., SiKK , SiKK , for all i{0,,N-1} , are K={0} and K=H .

For a closed subspace K of H we will denote by PK the orthogonal projection onto K.

Definition 2.2

Let H be a Hilbert space. A family of vectors {ei:iI} in H is called a frame, if there exist constants A,B>0 , called the frame bounds such that

Av2iI|v,ei|2Bv2,for allvH.

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The family of vectors is called a Parseval frame if the frame bounds are equal to 1, A=B=1 .

Theorem 2.3

[[5], Theorem 5.1] Let K be a Hilbert space, and let V0,,VN-1 be bounded operators satisfying

2.1 i=0N-1ViVi=IK

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Then K can be embedded into a larger Hilbert space H carrying a representation S0,,SN-1 of the Cuntz algebra ON such that K is cyclic for the representation, and if PK:HK is the projection onto K we have

2.2 Si(K)K,andViPK=SiPK=PKSiPK,soPKSiPK=PKSi,Vi=PKSi|K.

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The system (H,Si,PK) is unique up to unitary equivalence, and if σ:B(K)B(K) is defined by

σ(A):=i=0N-1ViAVi,

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then the commutant {Si,i=0,,N-1} is isometrically order isomorphic to the fixed point set B(K)σ={AB(K)|σ(A)=A} , by the map APKAPK .

Definition 2.4

Let K be a Hilbert space, N2 an integer, and Vi some bounded operators on K, i=0,1,,N-1 . We say that (K,Vi)i=0N-1 is a row co-isometry if

i=0N-1ViVi=IK.

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Definition 2.5

The data in Theorem 2.3 will be referred to as the Cuntz dilation (H,Si)i=0N-1 corresponding to the row co-isometry (K,Vi)i=0N-1 .

Definition 2.6

Let denote the empty word. Let Ω be the set of all finite words with digits in {0,,N-1} , including the empty word. For ωΩ , we denote by |ω| the length of ω .

For a word ω:=ω1ωnΩ , we will denote by Vω:=Vω1Vωn and similarly for Sω . Also V=I and S=I .

Definition 2.7

Let (K,Vi)i=0N-1 be a row co-isometry. Let K0 be a closed subspace of K. Suppose the following conditions are satisfied:

  • Vi∗K0⊂K0 for all i{0,,N-1} .
  • There exists an orthonormal basis (ec)cM for K0 , with M finite, some maps νi:MC , gi:MM , i{0,,N-1} such that Viec=νi(c)egi(c) , for all i{0,,N-1} and cM .
  • The maps gi are one-to-one whenever the transitions are possible, in the sense that, for all i{0,,N-1} and all c1,c2M such that νi(c1)0 and νi(c2)0 , if gi(c1)=gi(c2) then c1=c2 .

Then we say that (Vi)i=0N-1 acts on K0 as a random walk on the graph (M,{gi},{νi}) . M is the set of vertices, the maps gi indicate an edge with label i, from a vertex cM to the vertex gi(c) , and νi(c) represents a weight for this edge, more precisely |νi(c)|2 is a probability of transition from c to gi(c) along this edge.

Indeed, since i=0N-1Viec,Viec=ec2, it follows that i=0N-1|νi(c)|2=1 .

Note that if there are exactly two distinct i,i{0,...,N-1} such that gi(c)=gi(c) , then the total probability of transition from c to gi(c) is |νi(c)|2+|νi(c)|2 . We will use the convention that when we say "the probability of transition from c to gi(c) ," we mean the probability of transition from c to gi(c) (only) through i, that is, |νi(c)|2 .

  • If, for any c1,c2M , there exists ω=ω1ωn in Ω such that gω(c1):=gωngωn-1gω1(c1)=c2 and νω(c1):=νω1(c1)νω2(gω1(c1))νωn(gωn-1gω1(c1))0 , then we say that the random walk is irreducible. In other words, one can reach c2 from c1 through ω with positive probability |νω(c1)|2 .
  • We say that (Vi)i=0N-1 is simple on K0 if the only operators T:K0K0 with
  • 2.3 PK0i=0N-1ViTViPK0=T

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  • are T=λIK0 , λC ; recall that PK0 denotes the orthogonal projection onto the subspace K0 .
  • If, for any cM and i{0,,N-1} , we have Vi(egi(c))=ν¯i(c)ec , whenever νi(c)0 , we say that {Vi} is reversing on the random walk.
  • If, for any c1c2 in M, there exists n such that, for all ωΩ with |ω|n , we have νω(c1)=0 or νω(c2)=0 , then we say that the random walk is separating.
  • A word β=β0βp-1Ω , β , is called a cycle word for cM , if gβ(c)=c , and gβkgβk-1gβ0(c)c for 0k<p-1 and νβ(c)0 . The points gβkgβk-1gβ0(c) , k=0,,p-1 are called cycle points.
  • A word βΩ is called a loop for cM if β= , or gβ(c)=c and νβ(c)0 . Note that any loop β is of the form β=β1βp , for some cycle words β1,,βp for c.

In Sect. 5, we give several examples of such co-isometries, which include Fourier series on fractal measures, Walsh bases, and a combination of the two.

Definition 2.8

Let X=(X,d) be a complete metric space. A map g:XX is called a contraction, if there exists a constant 0<c<1 , such that

d(g(x),g(y))cd(x,y),for allx,yX.

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An iterated function system (IFS) is a finite family of contractions {gi}i=0N-1 on X. By [[23], Section 3], given an iterated function system {gi}i=0N-1 on X, there exists a unique closed bounded set X0 such that

X0=i=0N-1gi(X0).

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Furthermore X0 is compact. X0 is called the attractor of the iterated function system.

Main results

Structured bases regularly arise as the orbit under the action of a system of isometries applied to a collection of vectors. Since frames are compressions of orthonormal bases, structured frames might analogously arise under the action of a system of co-isometries. In the case of row co-isometries, the question of whether their action generates a frame depends on the action of the co-isometries themselves as well as the structure of their Cuntz dilation. We describe sufficient conditions under which frames are generated by row co-isometries in our main results, Theorems 3.1 and 3.6.

Theorem 3.1

Let (K,Vi)i=0N-1 be a row co-isometry and let (H,Si)i=0N-1 be its Cuntz dilation. Suppose there is a subspace K0 of K such that {Vi} acts on K0 as an irreducible random walk (M,{gi},{νi}i) with orthonormal basis (ec)cM . Assume in addition that {Vi} is simple on K0 .

Fix a point cM . Define

Ωc(0):=ωΩ:ωdoes not end in a cycle word forc.

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(In particular, Ωc(0) .)

For n1 , define Ωc(n) to be the set of words that end in exactly n cycle words for c, i.e., words ωΩ of the form ω=ω0β1βn , ω0Ωc(0) , β1,,βn cycle words for c.

Let

Ec(n):=Sωec:ωΩc(n),Hc(n):=*span¯Ec(n),(n0).

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Then

  • Ec(n) is an orthonormal basis for Hc(n) , for all n0 .
  • Hc(n)⊆Hc(n+1) for all n0 .
  • ∪n≥0Ec(n)={Sωec:ω∈Ω}.
  • Let V:=*span¯{Sωec:ωΩ}=n0Hc(n)¯ . Then V is invariant for the Cuntz representation {Si} . Also (V,Si|V)i=0N-1 is the Cuntz dilation of the row co-isometry (K0,PK0ViPK0)i=0N-1 and it is irreducible.

In addition, the following statements are equivalent

  • *span¯{Sωec:ω∈Ω}=H.
  • The Cuntz representation (H,Si)i=0N-1 is irreducible.
  • The only operators T:KK with
  • ∑i=0N-1ViTVi∗=T,

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  • are T=λIK , λC .

If {Vi} is reversing, then we also have:

  • For all n0 and all vK ,
  • 3.1 PHc(n)v2=ωΩc(0)Vω0ec,v2=PHc(0)v2=PVv2.

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and the previous statements are equivalent to

  • {Vωec:ω∈Ωc(0)} is a Parseval frame for K.

For the second part of the paper, we will impose some extra conditions on the co-isometry (K,Vi)i=0N-1 .

Assumption 3.2

Let (K,Vi)i=0N-1 be a row co-isometry. We make the following assumptions

3.2 There exists a continuous mape:TKfrom a complete metric spaceT,such that

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*span¯{e(t):tT}=K , and et=1 for all tT .

3.3 For anyi{0,,N-1}andtT,Viet=νi(t)egi(t),for someνi(t)Candgi(t)T.

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where et:=e(t) .

3.4 The mapsgiare contractions.

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Under these assumptions, one can define a random walk on the set T , where the transition from t to gi(t) is given probability |νi(t)|2 . Note that,

1=et2=i=0N-1Viet,Viet=i=0N-1|νi(t)|2et,et=i=0N-1|νi(t)|2.

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An important role in the study of the Cuntz dilation associated to the co-isometry {Vi} and the Parseval frames generated by it, is played by the minimal invariant sets associated to this random walk. We define these and more here.

Definition 3.3

For a point tT , and i{0,,N-1} , we say that the transition tgi(t) is possible throughi if νi(t)0 . We also write tigi(t) or tgi(t) .

Remark 3.4

Note that if t=gi(t)=gi(t) , the transition from tt may be possible through either i or i . We will make the convention that if we write " tgi(t) is possible", we mean " tgi(t) is possible through i," to distinguish the paths along i and i .

Given a word ω=ω1ωn , we define gω=gωngω1 . We say that the transition tgω(t) is possible (in several steps) through ω , if all the transitions tgω1(t)gω2gω1(t)gωngω1(t) are possible.

We define

νω(t)=νω1(t)νω2(gω1(t))νωn(gωn-1gω1(t)).

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|νω(t)|2 is the probability of transition from t to gω(t) through ω (passing through gω1(t) , gω2gω1(t),,gωngω1(t) ).

Note that the transition tgω(t) is possible in several steps, if and only if νω(t)0 .

A subset M of T is called invariant, if, for all t in M and i{0,,N-1} , if the transition tgi(t) is possible, then gi(t) is in M. We define the orbit of tT to be

O(t)=tT:There existsωΩsuchthatthetransitiontgω(t)=tis possible.

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A closed invariant subset M of T is minimal if there does not exist any proper closed invariant subset of M. Equivalently, as in Lemma 4.23, M=O(x0)¯ for any x0M .

Given an invariant set M, we define the subspaces K(M) of K and H(M) of H by

K(M)=*span¯{et:tM},H(M)=*span¯{Sωet:tM,ωΩ}.

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Theorem 3.5

Suppose that the assumptions (3.2)–(3.4) hold. Then there are finitely many minimal compact invariant sets. If M1,,Mp is the complete list of minimal compact invariant sets, then the spaces K(Mj) are invariant for Vi , i=0,,N-1 and the spaces H(Mj) are invariant for the representation (Si)i=0N-1 . The spaces H(Mj) are mutually orthogonal and

j=1pH(Mj)=H.

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The sub-representations (Si)i=0N-1 on H(Mj) , j=1,,p are irreducible and disjoint. (Recall that two representations (H,Si)i , (H,Si)i are called disjoint if there is no non-zero intertwining operator W:HH , WSi=SiW , WSi=SiW for all i.)

Theorem 3.6

Assume in addition that the maps {gi} are one-to-one and that all the minimal compact invariant sets are finite. Pick a point cj in Mj for every j=1,,p . Then {Vi} acts as an irreducible, separating random walk (Mj,{gi|Mj},{νi|Mj}) on the spaces K(Mj) . If {Vi} is reversing on each K(Mj) , then {Vωecj:ωΩcj(0),j=1,,p-1} is a Parseval frame for K.

Proofs

Proof of Theorem 3.1

We begin with a general lemma which shows that projections of iterations of the Cuntz dilation isometries are the corresponding iterations of the row co-isometries.

Lemma 4.1

Let (H,Si)i=0N-1 be the Cuntz dilation of the system (K,Vi)i=0N-1 , and PK:HK the projection onto K. For ωΩ ,

4.1 Vω(k)=PKSω(k)for allkK

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Proof

Let ω=ω1ω2 and kK . Using (2.2) and PKSi(k)K , we have

Vω1Vω2(k)=Vω1PKSω2(k)=PKSω1PKSω2(k)=PKSω1Sω2(k)

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By induction, (4.1) follows.

We will also need the next general result which shows when the vectors Sωv are orthogonal.

Lemma 4.2

If (H,Si)i=0N-1 is a representation of the Cuntz algebra, v,vH , ω,ωΩ and Sωv,Sωv0 , then ω is a prefix of ω or vice-versa, i.e., there exists a word βΩ such that ω=ωβ or ω=ωβ .

Proof

Let n=|ω| , n=|ω| . If there exists k such that ωkωk then take the smallest such k, and we have

Sω1ωk-1ωkωnv,Sω1ωk-1ωkωnv=Sωkωnv,Sωkωnv=0.

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This is impossible, therefore ω is a prefix of ω or vice-versa.

To prove item (a) in the theorem, we will use the next Lemma:

Lemma 4.3

If ω1,ω2Ω and Sω1ec,Sω2ec0 , then there exists a loop β for c such that ω1=ω2β or ω2=ω1β .

Proof

First, an easy computation shows that, for cM and ωΩ ,

4.2 Vωec=Sωec=νω(c)egω(c).

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By Lemma 4.2, either ω1=ω2β or ω2=ω1β for some βΩ . Assume the first. We prove that β is a loop. We have

0Sω1ec,Sω2ec=Sω2βec,Sω2ec=Sβec,ec=ec,Sβec=ν¯β(c)ec,egβ(c).

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This implies that gβ(c)=c and νβ(c)0 so β is a loop for c.

Lemma 4.4

Suppose ω1β1=ω2β2 for some cycle words β1 and β2 for c and some words ω1 and ω2 ; then β1=β2 and ω1=ω2 . Also, every word can be written uniquely as ω0β1β2βn for some cycle words β1,,βn for c, (n could be 0) and some word ω0Ωc(0) .

Proof

Suppose |β1|>|β2| . Then, if we read the words ω1β1=ω2β2 from the right, we see that β1=γβ2 for some non-empty word γ . We have gβ2(c)=c=gβ1(c)=gβ2(gγ(c)) . Since all these transitions are possible and the maps gi are one-to-one in this case, it follows that gγ(c)=c , but this contradicts the fact that β1 is a cycle word for c. Thus β1=β2 and ω1=ω2 .

Now take an arbitrary word ω . If it does not end in a cycle word, it is in Ωc(0) . If it ends in a cycle word, by the previous statement, it can be written uniquely as ω=ω1β1 , with β1 cycle word. Repeat for ω1 and use induction, to obtain the last statement in the lemma.

See Remark 4.5, where we point out why the condition that the maps gi are injective is important in this context.

Now take ω1ω2 in Ωc(n) for some n0 . If Sω1ec,Sω2ec0 then, with Lemma 4.3, there exists a loop β such that ω2=ω1β or ω1=ω2β . Assume that ω1=ω2β . Since β is a loop, β , we have that β=β1βp for some cycle words β1,,βp for c. Since ω2 ends in n cycle words for c, it follows that ω1=ω2β ends in n+p cycle words for c, which, by Lemma 4.4, is impossible since ω1Ωc(n) . This shows that Ec(n) is an orthonormal basis for Hc(n) .

Remark 4.5

The condition that the maps gi be one-to-one when the transitions are possible is important in Lemma 4.4, and to guarantee that the vectors Sωec with ec in Ωc(n) are orthogonal. Indeed, if we do not assume this condition, it is possible that a word ends both in a cycle word for c and in two cycle words for c. Consider

V0:=121200,V1:=0012-12.

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A simple check shows that (V0,V1) is a row co-isometry on C2 , and if {e1,e2} is the standard basis for C2 , then, this co-isometry acts as a random walk on M={1,2} , with g0(1)=1 , g0(2)=1 , g1(1)=2 , g1(2)=2 , ν0(1)=12 , ν0(2)=12 , ν1(1)=12 , ν1(2)=-12 .

The random walk is clearly irreducible and, if T=T11T12T21T22 with T=V0TV0+V1TV1 , we obtain that T=12(T11+T22)I2 , so the co-isometry is simple on C2 .

Note that both 0 and 10 are cycle words for c:=1M . Therefore the word ω=1010 ends the cycle word 0 for c, since 1, 01 and 101 are not cycle words for c. At the same time ω ends in two cycle words for c, ω=(10)(10) .

(b) We will need some key lemmas.

Lemma 4.6

Define the random walk/Markov chain Xn , n0 on M by

*Prob(Xn=gi(t)|Xn-1=t)=|νi(t)|2,(tM).

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Then

*Prob(Xn=gωngω1(t),Xn-1=gωn-1gω1(t),,X1=gω1(t)|X0=t)=|νω1ωn(t)|2.

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Also the random walk is recurrent.

Proof

The first equality follows from a simple computation.

Since M is finite and the random walk is irreducible by hypothesis (see Definition 2.7), the random walk is also recurrent (see, e.g., [[19], Theorem 6.4.4] or [[20], Section XV.6]).

Definition 4.7

Let t,cM and ωΩ , ω=ω1ωn . We say that gω(t)=c for the first time if gω(t)=c , νω(t)0 , and gω1ωk(t)c for 1k<n . In particular, if t=c and ω , then gω(t)=c for the first time if and only if ω is a cycle word for c.

Lemma 4.8

Let t,cM . Then

4.3 gω(t)=cfor the first time|νω(t)|2=1.

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Proof

By Lemma 4.6, the random walk on M is recurrent, so *Prob(Xever entersc|X0=t)=1 . But

*Prob(Xeverentersc|X0=t)=n=1*Prob(Xn=c,Xn-1c,,X1c|X0=t)=n=1ω=ω1...ωn*Prob(Xn=gωngω1(t)=c,Xk=gωkgω1(t)cfor1k<n|X0=t)=gω(t)=cforthefirsttime|νω(t)|2.

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Lemma 4.9

Let t,cM . Then

et=gω(t)=cfor the first timeνω(t)Sωec.

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Proof

Using the Cuntz relations, and that Siex=νi(x)egi(x) for all i=0,,N-1 and xT , we have

et=ω1=0N-1Sω1Sω1et=ω1νω1(t)Sω1egω1(t)=ω1:gω1(t)=cνω1(t)Sω1ec+ω1:gω1(t)cνω1(t)Sω1egω1(t)=ω1:gω1(t)=cνω1(t)Sω1ec+ω1:gω1(t)cνω1(t)ω2Sω1Sω2Sω2egω1(t)=ω1:gω1(t)=cνω1(t)Sω1ec+ω1ω2:gω1(t)c,gω1ω2(t)=cνω1ω2(t)Sω1ω2ec+ω1ω2:gω1(t)c,gω1ω2(t)cνω1ω2(t)Sω1ω2egω1ω2(t).

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Continuing, by induction we get, for nN ,

4.4 et=1|ω|n,gω(t)=cfor the first timeνω(t)Sωec+|ω|=ngω1ωk(t)cfor any1knνω(t)Sωegω(t)

Graph

Note that if we take two different ω1,ω2 that appear in the first sum, then one can not be the prefix of the other, by the definition of " gω(t)=c for the first time". Also if ω1 appears in the first sum, and ω2 appears in the second, then ω1 is not a prefix of ω2 because gω1(t)=c . Using Lemma 4.2, it follows that all the terms in the first sum are mutually orthogonal, and they are orthogonal to all the terms in the second sum. Denote the second sum by An . Since the norms are equal, we get

4.5 1=1|ω|n,gω(t)=cfor the first time|νω(t)|2+An2.

Graph

From Lemma 4.8,

limn1|ω|n,gω(t)=cfor the first time|νω(t)|2=1,

Graph

therefore An0 and this proves the lemma.

Let n0 and ωΩc(n) , then with Lemma 4.9

Sωec=Sωβcycle word forcνβ(c)Sβec=βνβ(c)Sωβec.

Graph

But ωβΩc(n+1) so SωecHc(n+1) . Thus Hc(n)Hc(n+1) . (c) is trivial. (d) Using Lemma 4.9, it follows that, for every tM , etV , thus K0V . Clearly V is invariant for all the operators Si . To see that it is also invariant for the operators Si , let ωΩ . If ω=ω1ωn , then SiSωec=δiω1Sω2ωnecV . If ω= , then Siec=νi(c)eg(c)V , according to the previous argument. Thus V is invariant for the Cuntz representation and it contains K0 .

Since K0 is invariant for all Vi , we have PK0ViPK0=ViPK0 and PK0ViPK0=PK0Vi . Let Wi:=PK0ViPK0 . Then

i=0N-1WiWi=PK0.

Graph

Since {Sωec:ωΩ} spans V it follows that K0 is cyclic for the representation {Si} . Thus (V,Si|V)i=0N-1 is the Cuntz dilation of the row co-isometry (K0,Wi)i=0N-1 . By Theorem 2.3, it follows that the Cuntz representation (V,Si|V)i=0N-1 is irreducible, since {Vi} is simple on K0 .

(e) We assume now that {Vi} is reversing. If ωΩc(n) , then ω=ω0β1βn , with ω0Ωc(0) and β1,,βn cycle words for c.

If β is a cycle word for c, then Vβec=Vβegβ(c)=ν¯β(c)ec . So

Vωec=Vω0Vβ1Vβnec=ν¯βn(c)ν¯βn-1(c)ν¯β1(c)Vω0ec.

Graph

Let vK . Then, with (a), we have

PHc(n)v2=ωΩc(n)Sωec,v2=ωΩc(n)PKSωec,v2=ωΩc(n)Vωec,v2=ω0Ωc(0)cycle words forcβ1,βnVω0β1βnec,v2=ω0Ωc(0)β1,,βn|νβ1(c)|2|νβn(c)|2Vω0ec,v2.

Graph

But

βicycle word forc|νβi(c)|2=1,

Graph

by Lemma 4.8, so we obtain

PHc(n)v2=ωΩc(0)Vω0ec,v2=PHc(0)v2.

Graph

But, with (b), we obtain

PVv2=limnPHc(n)v2=PHc(0)v2.

Graph

Next we prove the equivalences.

(i) (ii). If (i) holds, then H=V and (ii) follows from (d).

(ii) (i). We know from (d) that V is invariant for the representation {Si} . Since this is irreducible, we must have V=H which implies (i).

(ii) (iii). Follows from Theorem 2.3.

Assume now that {Vi} is reversing.

(i) (iv). Follows from (e), since if vK , then vH=V .

(iv) (i). For this last implication we prove first the following

Lemma 4.10

Suppose V and K are closed subspaces of the Hilbert space H and suppose {ei|iI} is an orthonormal basis for V. Then {PKei:iI} is a Parseval frame for K if and only if KV .

Proof

The sufficiency is well known. Indeed, if vKV, then v2=iv,ei2=iPKv,ei2=iv,PKei2

Assume now {PKei:iI} is a Parseval frame for K. Let kK . Then, since {ei:iI} is an orthonormal basis for V, we have

PVk2=iI|k,ei|2=iI|PKk,ei|2=iI|k,PKei|2=k2.

Graph

The last equality holds because {PKei|iI} is a Parseval frame for K. But this implies that PVk=k so kV . As k was arbitrary in K, it follows that KV .

With Lemma 4.1 we have PKSωec=Vωec for all ωΩc(0) . Then, with Lemma 4.10, we get that KHc(0)V=*span¯{Sωec:ωΩc(0)} . V is invariant for the representation {Si} therefore we obtain that K is also cyclic for the representation (V,Si|V)i=0N-1 and clearly invariant for all Si . Therefore (V,Si|V)i=0N-1 is the Cuntz dilation of the row co-isometry (K,Vi)i=0N-1 . By the uniqueness in Theorem 2.3, it must be isomorphic to the representation (H,Si)i=0N-1 . By (d), the Cuntz representation on V is irreducible, so (ii) follows. With an earlier implication this yields (i).

Proposition 4.11

Let (K,Vi)i=0N-1 be a row co-isometry which acts on the subspace K0 as a random walk (M,{gi},{νi}) which is irreducible and separating. Then {Vi} is simple on K0 .

Proof

Let T be as in (2.3). Since K0 is invariant for Vi , we have PK0ViPK0=PK0Vi , iterating (2.3) we obtain, for all nN ,

4.6 |ω|=nPK0VωTVωPK0=T

Graph

Then, take c1c2 in M. Since the random walk is separating if we take n large enough, we have that, for any ωΩ with |ω|=n , either νω(c1)=0 or νω(c2)=0 . Therefore

Tec1,ec2=|ω|=nTVωec1,Vωec2=|ω|=nνω(c1)ν¯ω(c2)Tegω(c1),egω(c2)=0.

Graph

So, T has zero off-diagonal entries.

We prove that the diagonal entries are equal. By taking the real and imaginary parts, we can assume that T is self-adjoint. Let c0M such that Tec0,ec0=max{Tec,ec:cM}.

Let cM . Since the random walk is irreducible, there exists ω0Ω such that gω0(c0)=c and νω0(c0)0 . Let n:=|ω0| . We have

Tec0,ec0=|ω|=nTVωec0,Vωec0=|ω|=n|νω(c0)|2Tegω(c0),egω(c0)|ω|=n|νω(c0)|2Tec0,ec0=Tec0,ec0.

Graph

But then, we must have equalities in all inequalities, and therefore, since νω0(c0)0 , we get that Tec,ec=Tec0,ec0 . Thus all the diagonal entries of T are the same, and T is a multiple of the identity, so {Vi} is simple on K0 .

Remark 4.12

In Proposition 4.13 we show that, in many cases, the family {Sωec:ωΩc(0)} is incomplete in H.

Proposition 4.13

As in Theorem 3.1, let (K,Vi)i=0N-1 be a row co-isometry and let (H,Si)i=0N-1 be its Cuntz dilation. Suppose there is a subspace K0 of K such that {Vi} acts on K0 as an irreducible random walk (M,{gi},{νi}) with orthonormal basis (ec)cM . Assume in addition that {Vi} is simple on K0 .

  • Suppose for all cM and all i{0,,N-1} , we have |νi(c)| is either 0 or 1. Then M is a single cycle, {Vi} is reversing, and, for cM , nN , and for ω=ω0γΩc(n) , with ω0Ωc(0) and γ a loop for c, Sωec is a unimodular constant multiple of Sω0ec ; therefore {Sωec:ωΩc(0)} is an orthonormal basis for the space V=*span¯{Sωec:ωΩ} .
  • Suppose that there exists cM such that νi(c)0 for two distinct i{0,,N-1} . Then, for all n0 , the family {Sωec:ωΩc(n)} is incomplete in V.
Proof

For (i), if the probabilities |νi(c)|2 are all 0 or 1, it follows that from each point in M there is a unique possible transition to another point in M, and since the random walk is irreducible, it follows that M has to be a cycle.

We prove that Vi is reversing. Indeed let cM and let i0 be the unique digit such that the transition cgi0(c) is possible. We have

ec=i=0N-1ViViec=i=0N-1νi(c)Viegi(c)=νi0(c)Vi0egi0(c),

Graph

so Vi0egi0(c)=ν¯i0(c)ec . Thus {Vi} is reversing.

Let cM , and let β be the unique cycle word for c. Using the same argument as before, we get that {Si} is also reversing on the random walk and so Sβec=ν¯β(c)ec . But this implies that if ωΩc(0) then Sωβec=ν¯β(c)Sωec . By induction, we obtain the last statements in (i).

For (ii), let n0 . Let β0 be a fixed cycle word for c. Let β0n:=β0β0ntimes . We prove that Sβ0n+1ec is orthogonal to Sωec , for all ωΩc(n) , ωβ0n . Indeed, if this is not true, let ω=ω0β1βn , for some ω0Ωc(0) and β1,,βn cycle words for c, then by Lemma 4.3, we have that β0n+1=ω0β1βnβn+1βn+p for some cycle words βn+1βn+p . But, from Lemma 4.4, we get that ω0= and β1==βn+p=β0 and p=1 . So ω=β0n , a contradiction.

Note also that, Sβ0nec is orthogonal to all Sωec , for all ωΩc(n) , ωβ0n , by Theorem 3.1.

Consider v=Sβ0n+1ec-Sβ0n+1ec,Sβ0necSβ0nec , which is perpendicular to Sβ0nec , but also to all Sωec with ωΩc(n) , ωβ0n . Thus v is orthogonal to the subspace Hc(n) .

We just have to check that v is not zero.

If there exist i1,i2{0,,N-1} , i1i2 , such that the transitions cgi1(c) , cgi2(c) are possible, then, since the random walk is irreducible, there are possible transitions from gi1(c) and gi2(c) , back to c. Therefore c has at least two distinct cycle words β1 , β2 , and νβ1(c)(0,1) . We take c and β0 in the previous argument to be β1 . Since v is perpendicular to Sβonec , using the Pythagorean theorem, we have:

v2=Sβ0n+1ec2-Sβ0n+1ec,Sβ0necSβ0nec2=1-|Sβ0ec,ec|2=1-|ec,Sβ0ec|2=1-|νβ0(c)|2>0.

Graph

Therefore, 0vSωec for all ωΩc(n) and so the family {Sωec:ωΩc(0)} is incomplete in H.

Let us provide an application of Theorem 3.1 in the case when a row co-isometry admits periodic points.

Definition 4.14

A non empty word β is called irreducible if there is no word ω such that β=ωωωktimes with k2 . Let Ωβ be the set of words that do not end in β , including the empty word.

Theorem 4.15

Let (H,Si)i=0N-1 be the Cuntz dilation of the row co-isometry (K,Vi)i=0N-1 . Suppose v0K is a unit vector such that Vip-1Vi0v0=v0 for some irreducible word β=i0ip-1 . Then the following are equivalent:

  • {Vωv0|ω∈Ωβ} is a Parseval frame.
  • {Sωv0|ω∈Ωβ} is ONB in H.
  • {Sωv0|ω∈Ω} spans H.
  • The representation (H,Si)i=0N-1 is irreducible.
  • The commutant of the Cuntz dilation is trivial.
  • Bσ(K)=C1K.
Proof

We will use the following lemma:

Lemma 4.16

Let S:HH with S1 , and vH then Sv=v if and only if Sv=v .

Proof

If Sv=v then, since S=S1 , we have

0Sv-v2=Sv-v,Sv-v=Sv2+v2-v,Sv-Sv,v=Sv2-v2v2-v2=0.

Graph

Therefore, Sv=v .

For the converse, replace S by S .

With the requirements of Theorem 3.1 in mind we construct the following data:

4.7 M:={v0,Vi0v0,Vi1Vi0v0,,Vip-2Vi0v0},K0:=span¯M

Graph

and ec:=c for cM .

4.8 gi:MM,gi(v0)=v0ifii0Vi0v0otherwise,gi(VikVi0v0)=VikVi0v0ifiik+1Vik+1VikVi0v0otherwise

Graph

4.9 νi:MC,νi(v0)=0ifii01otherwise,νi(VikVi0v0)=0ifiik+11otherwise

Graph

Note that the maps gi are trivially one-to-one when the transitions are possible.

Notice that for words ω containing a digit i{i0,i1,,ip-1} the transitions cgω(c) are not possible because νω(c)=0 in this case. Because v0K we see that

M={v0,Si0v0,Si1Si0v0,,Sip-2Si0v0}.

Graph

Claim 4.17

M forms an orthonormal basis for K0 .

First we notice the elements in M are unit vectors. Because Sk=1 for all 0kp-1 , we have:

1=v0=Sip-1Si0v0SikSi0v0SikSi0v01

Graph

To show, for kl

4.10 SikSi0v0,SilSi0v0=0

Graph

assume without loss of generality k<l where 0k,lp-1 .

With Lemma 4.16, Sip-1Si0v0=v0 entails Sβv0=v0 . Using the Cuntz orthogonality relations SiSi=I and v0=Sβv0=Si0Si1Sip-1v0 , the left-hand side in (4.10) can be rewritten as Sik+1Sip-1v0,Sil+1Sip-1v0 . If this last term would not vanish then with Lemma 4.3 we get that γ:=ijip-1 is a loop for v0 , for some j>k . From (4.8) we have to have Sip-1Sijv0=v0 , which then gives SijSip-1v0=v0 with Lemma 4.16. Exploiting these fixed point properties for Sγ and Sβ we have succesively in finitely many steps

v0,v0=Sβββv0,Sγβββv0.

Graph

Since the isometries (Sl)l have orthogonal ranges we have that the infinite words are equal:

ββ=γββ with γ a word shorter than β . Then γ(ββ)=γγββ==γγγββ , which implies that

γγγ=βββ,withq:=|γ|<|β|=p.

Graph

Let d=gcd(p,q)<p . Then there exists m, n in Z such that mp+nq=d . Denote γk=γkmodq and βk=ikmodp for all kZ . Then from the last equality above with infinite words, we have for γk=βk for all kZ . Then for all k:

βd+k=βmp+nq+k=βnq+k=γnq+k=γk=βk.

Graph

So ββ actually has period d, i.e. β=αααp/dtimes where α=i0id-1 . This contradicts the fact that β is irreducible. Hence (4.10) holds and the Claim is proved.

Next, we check that the notions introduced in Definition 2.7 are satisfied in this setting.

Claim 4.18

ViK0K0 for all i{0,,N-1} . Thus item (i) in Definition 2.7 holds.

From the definition of M above we see that Vik(c)M if c=Vik-1Vi0v0 . For the remaining cases we prove that Vi(c)=0 , thus finishing the Claim.

Sip-1Si0v0=v0 . Let 0kp-1 . Then Si0SikSikSi0 is the projection onto Si0SikH , and is smaller than the projection Si0Sik-1Sik-1Si0 . Hence

v02=Si0Sip-1Sip-1Si0v02Si0SikSikSi0v02v02

Graph

which implies v02=Si0SikSikSi0v02 . Since Si0SikSikSi0 is a projection, it follows that

4.11 v0=Si0SikSikSi0v0.

Graph

Then using the Cuntz relations

|ω|=k+1SωSωv0,v0=v0,v0=Si0ikSikSi0v0,v0.

Graph

It follows that SωSωv0,v0=0 ωi0ik , |ω|=k+1 . Hence

4.12 Vωv0=Sωv0=0ωi0ik,|ω|=k+1.

Graph

This concludes the Claim.

Notice that item (ii) in Definition 2.7 is satisfied because of Eq. (4.12) and the choice of M, gi and νi . Also the random walk (M,{gi},{νi}) is irreducible: if c1=VikVi0v0M and c2=VilVi0v0M with say k<l then gω(c1)=c2 and νω(c1)=1 , where ω=ik+1il .

Claim 4.19

{Vi} is reversing on the random walk (M,{gi},{νi}) .

Suppose νi(c)0 for cM . We need show Vi(gi(c))=νi(c)¯c . Because cM we have c=VikVi0v0 for some 0kp-1 . From the definition of the νi we must have i=ik+1 (the case c=v0 follows similarly). What is needed to show now is

4.13 Vik+1(Vik+1Vi0v0)=VikVi0v0.

Graph

From (4.11) with kk+1 and rewriting using the Cuntz relations SiSi=I we have

SikSi0v0=Sik+1(Sik+1Si0v0).

Graph

We apply the projection PK on both sides and use v0K and Lemma 4.1 to obtain (4.13).

Claim 4.20

The random walk (M,{gi},{νi}) is separating.

Let c1:=VikVi0v0 and c2:=VilVi0v0 in M, with 0k<lp-1 . We prove that if ω is a word with |ω|p then either νω(c1)=0 or νω(c2)=0 . Suppose by contradiction that for some ω=j0j1jt with tp both νω(c1) and νω(c2) are non zero. Using (4.9) we have j0=ik+1=il+1 , j1=ik+2=il+2 , and continuing we get ik+tmodp=il+tmodp for all tN . As a consequence the following infinite words are equal:

ik+1ip-1ββ=il+1ip-1ββ

Graph

Concatenating the word i0i1ik on the left hand side we obtain

βββ=γββwhereγ=i0i1..ikil+1ip-1.

Graph

Using the same argument as above we get a contradiction with the fact that β is irreducible.

With Proposition 4.11, it follows that {Vi} is simple on K0 .

We are done checking the settings and requirements of Theorem 3.1. We apply its item (d) and finish the proof.

In the particular case when one of the co-isometries admits a fixed point one easily obtains the following characterizations.

Corollary 4.21

Let (H,Si)i=0N-1 be the Cuntz dilation of row co-isometry (K,Vi)i=0N-1 , and v0K unit vector such that V0(v0)=v0 . The following are equivalent:

  • The family of vectors {Vωv0}ωΩ0 is a Parseval frame in K.
  • The family of vectors {Sωv0}ωΩ0 is ONB in H.
  • The family of vectors {Sωv0}ωΩ0 spans H.
  • The representation (H,Si)i=0N-1 is irreducible.
  • The commutant of the Cuntz dilation is trivial.
  • Bσ(K)=C1K.
Example 4.22

If the Cuntz dilation is not irreducible, it is possible that {Vωv0}ωΩ0 is not even a frame for its span.

Define the operators V0,V1 on l2(Q) by

V0er=λr0er/2,V1er=λr1e(r-1)/2,(rQ),

Graph

where er is the canonical basis in l2(Q) , er(q)=δr,q , r,qQ , and λ00=1 , λ01=0 , and λri=1/2 for r0 , i=0,1 . Thus |λr0|2+|λr1|2=1 for all r.

Denote

f0(r)=r2,f1(r)=r-12,(rQ),

Graph

with inverses

h0(r)=2r,h1(r)=2r+1,(rQ).

Graph

Clearly Vi defines a bounded operator on l2(Q) . We compute the adjoints

Vier,eq=er,Vieq=λ¯qiδrfi(q)=λ¯qiδhi(r)q=λ¯hi(r)iδhi(r)q=λ¯hi(r)iehi(r),eq.

Graph

Therefore

Vier=λ¯hi(r)iehi(r),(rQ,i=0,1).

Graph

Then, we have

i=01ViVier=i=01λriViefi(r)=i=01λriλ¯hi(fi(r))iehi(fi(r))=i=01|λri|2er=er.

Graph

Thus V0V0+V1V1=I.

Also, if v0=e0 then V0v0=v0 .

Now, for i1,,in{0,1} , we have

Vi1Vin(V1v0)=Vi1Vin(λ¯11e1)=Vi1Vin-1(λ¯hin(1)1λ¯11ehin(1))==λ¯hi1hin(1)i1λ¯hi2hin(1)i2λ¯hin(1)inλ¯11ehi1hin(1)=12n+1e2n+2n-1in+2n-2++i1.

Graph

Consider the vector e2m , m1 . If 2m=2n+2n-1in+2n-2++i1 , then n=m and in==i1=0 , and

e2m,Vi1Vin(V1e0)=12m+1.

Graph

If 2m2n+2n-1in+2n-2++i1 , then

e2m,Vi1Vin(V1e0)=0.

Graph

If {Vωv0}ωΩ0 is a frame,then for a frame constant A>0 , we have

A=Ae2m2ω|e2m,Vωv0|2=12m+12.

Graph

Letting m , we get A=0 , a contradiction.

Proof of Theorem 3.5

We remark first the following: suppose M1,M2 are two different minimal compact invariant sets. Then they have to be disjoint (see Lemma 4.23). Indeed, if they are not, then M1M2 is compact invariant set which is contained in M1 , and, since M1 is minimal, M1M2=M1 , and similarly for M2 , which is a contradiction.

We also note, that since the functions tViet and gi(t) are continuous, and using relation (3.3), we get

νi(t)=νi(t)egi(t),egi(t)=Viet,egi(t),

Graph

it follows that the maps νi(t) are also continuous.

Lemma 4.23

For aT , the closed orbit O(a)¯ is compact and invariant. If M is a minimal compact invariant set, and x0M , then M=O(x0)¯ . If M1,M2 are distinct compact minimal invariant sets, they are disjoint.

Proof

First, we prove that the entire orbit of a, that is O:={gω(a):ωΩ}¯ is compact. Let c(0,1) be a common contraction constant for all (gi) , i=0,,N-1 . It suffices to show that any sequence in O has a convergent subsequence. Now let (gωn(a))n1 , ωnΩ , be a sequence in the orbit of a and fix some x0X0 . By passing to a subsequence, we may assume that the sequence of lengths |ωn| , otherwise the orbit would be finite, thus one could select a constant subsequence.

Let X0 be the unique compact attractor of the iterated function sytem (gi)i=0N-1 , i.e., the unique compact subset with the property that

X0=i=0N-1gi(X0).

Graph

See [[23], Section 3] or [[25]] for details.

Because the attractor X0 is compact, one can extract a convergent subsequence of (gωn(x0))n1 . There is no loss of generality if we relabel the subsequence and still denote it by (gωn(x0))n1 . Say gωn(x0)xX0 . Let ϵ>0 and N large enough so that c|ωn|d(a,x0)<ϵ/2 and d(gωn(x0),x)<ϵ/2 whenever n>N . Using the triangle inequality, we have, for n>N :

d(gωn(a),x)d(gωn(a),gωn(x0))+d(gωn(x0),x)c|ωn|d(a,x0)+d(gωn(x0),x)<ϵ

Graph

Hence the subsequence (gωn(a))n1 is convergent.

Next we show that O(a)¯ is invariant. Note first that O(a) is invariant: indeed if bO(a) with bgi(b) possible then b=gω(a) with ab possible. So νi(b)0 and νωi(a)=νω(a)νi(b)0 . It follows that agωi(a)=gi(b) is possible, hence gi(b)O(a) . Now, if bO(a)¯ with bgi(b) possible (so νi(b)0 ) then one can find a sequence bnO(a) with limnbn=b . Hence the transitions abn=gωn(a) are possible, where ωn are words depending on n. Because gi and νi are continuous we obtain gi(b)=limngi(bn) and νi(bn)0 for n large enough. It follows that the transitions agωni(a)=gi(bn) are possible, so gi(bn)O(a) . Because gi(b)=limngi(bn) we obtain gi(b)O(a)¯ .

If x0M then O(x0) is contained in M. Since M is minimal and O(x0)¯ is invariant, we get M=O(x0)¯ .

If M1,M2 are distinct compact minimal invariant sets, and we assume that they are not disjoint, then for x0M1M2 we have M1=O(x0)¯=M2 , a contradiction.

Lemma 4.24

The minimal compact invariant sets are contained in the attractor X0 of the iterated function system {gi} .

Proof

Indeed, let M be a minimal compact invariant set. Let xM . Pick ω1,ω2, such that the transitions xgω1(x)gω1ω2(x) are possible. Then gω1ωn(x)M , for all n0 . Let x0X0 . Then, if 0<c<1 is a common contraction ratio for the maps {gi} , we have d(gω1ωn(x),gω1ωn(x0))cnd(x,x0)0 . Since gω1ωn(x0)X0 and X0 is compact, it follows that is has a convergent subsequence to a point z0 in X0 . Then the same subsequence of {gω1ωn(x)} is convergent to z0 , which means z0M . Then O(z0)¯ is a compact invariant set contained in M and in X0 . Since M is minimal M=O(z0)¯X0 .

Thus, all minimal compact invariant sets are contained in the compact attractor of the iterated function system {gi} .

Lemma 4.25

There exists a constant δ>0 such that for any two distinct minimal compact invariant sets M1 and M2 , dist(M1,M2)δ .

Proof

We follow the argument in [[6]]. Since the maps |νi|2 are uniformly continuous on the attractor X0 , there exists δ>0 such that, if d(x,y)<δ , then ||νi(x)|2-|νi(y)|2|<1N for all i.

Suppose now, that there exist xM1 and yM2 such that d(x,y)<δ . Since i|νi(x)|2=1 , it follows that there exist i1 such that |νi1(x)|21N . Then, since d(x,y)<δ , we obtain that |νi1(y)|2>0 . This means that the transitions xgi1(x) and ygi1(y) are possible, so gi1(x)M1 and gi1(y)M2 . Also d(gi1(x),gi1(y))d(x,y)<δ . Repeating the argument and using induction, we obtain some labels i1,i2,,in, such that the transitions xgi1in(x) and ygi1in(y) are possible for all n. So gi1in(x)M1 and gi1in(y)M2 . But, using the same argument as in Lemma 4.25, d(gi1in(x),gi1in(y)) converges to 0, which would mean that dist(M1,M2)=0 and this contradicts the fact that M1 and M2 are distinct minimal compact invariant sets.

Using Lemmas 4.25 and 4.24, all minimal compact invariant sets are cpntained in the compact attractor X0 and they have a distance bigger than δ between any two of them. Thus, there can be only a finite number of minimal compact invariant sets.

We start with a simple relation that we will use often. For a word ωΩ and tT ,

Sωet=Vωet=νω(t)egω(t).

Graph

We have, for tMj and i{0,,N-1} , Viet=νi(t)egi(t)K(Mj) , if the transition tgi(t) is possible, and Viet=0K(Mj) if the same transition is not possible. So K(Mj) is invariant for Vi .

The next lemma shows that the spaces H(Mi) are invariant for the Cuntz representation {Sj} .

Lemma 4.26

If K0 is a subspace of K which is invariant under the operators Vi , i=0,,N-1 , then

H(K0):=*span¯{Sωv:vK0,ωΩ},

Graph

is invariant for the representation (Si)i=0N-1 .

Proof

Clearly, the space is invariant under the operators Si , i=0,1,,N-1 . For a nonempty word ω=ω1ωn , vK0 and i{0,,N-1} we have Si(Sωv)=δi,ω1Sω2SωnvH(K0) . Also Siv=VivK0H(K0) .

Next, we prove that the spaces K(Mj) are mutually orthogonal.

Lemma 4.27

If M1 and M2 are two closed invariant subsets with dist(M1,M2)>0 then

et1,et2=0,(t1M1,t2M2).

Graph

Proof

Let ω be a word and assume that the transitions t1gω(t1) and t2gω(t2) are possible in several steps. Then gω(t1)M1 and gω(t2)M2 . Also, since the maps gi are contractions with ratio 0<c<1 , if n=|ω| then

dist(gω(t1),gω(t2))cndist(t1,t2),

Graph

so, if n is large enough then

dist(gω(t1),gω(t2))<dist(M1,M2),

Graph

and this would yield a contradiction. Thus, for ω long enough, one of the transitions t1gω(t1) or t2gω(t2) is not possible, so νω(t1)=0 or νω(t2)=0 .

Using this, with n large enough, and the co-isometry relation, we have

et1,et2=|ω|=nSωet1,Sωet2=|ω|=nνω(t1)ν¯ω(t2)egω(t1),egω(t2)=0.

Graph

Lemma 4.28

Assume that the subspaces K1 and K2 are invariant for the operators Vi , i=0,,N-1 , and are mutually orthogonal, and let H(K1) and H(K2) be the subspaces of H as in Lemma 4.26. Then H(K1) and H(K2) are orthogonal.

Proof

Given two words ω=ω1ωn and ω=ω1ωm , if there exists i such that ωiωi then, take the first such i and, for v1K1 and v2K2 :

Sωv1,Sωv2=SωiSωi+1Sωnv1,SωiSωi+1Sωmv2=0,

Graph

since the ranges of Sωi and Sωi are orthogonal.

In the remaining case, ω is a prefix of ω (or vice-versa), ω=ωβ for some word β1βp , then

Sωv1,Sωv2=Sβv1,v2=v1,Sβv2=0,

Graph

because Sβv2K2 .

Using Lemmas 4.27 and 4.28, we get the next lemma:

Lemma 4.29

If M1 and M2 are two closed invariant subsets with dist(M1,M2)>0 then the subspaces K(M1) and K(M2) are orthogonal and the subspaces H(M1) and H(M2) are orthogonal.

Thus, the spaces H(Mj) are mutually orthogonal.

To prove the irreducibility of the Cuntz representation on H(Mj) , the disjointness and the fact that the sum of these spaces is H, we will introduce the Ruelle operator:

Definition 4.30

Define the Ruelle transfer operator for functions f:TC by

4.14 Rf(t)=i=0N-1|νi(t)|2f(gi(t)),(tT).

Graph

Recall that B(K)σ is the space of bounded operators T on K with

i=0N-1ViTVi=T.

Graph

By Theorem 2.3, the commutant of the representation (H,Si)i=0N-1 is in bijective correspondence with B(K)σ by the map APKAPK .

Define the map AhA , from B(K)σ to complex valued functions defined on T , by

4.15 hA(t)=Aet,et,(tT).

Graph

For an operator A in the commutant of the representation (H,Si)i=0N-1 , the operator PKAPK is in B(K)σ , and we define hA=hPKAPK .

Lemma 4.31

The function B(K)σAhA , maps into the continuous fixed points of the Ruelle transfer operator, is linear, and order preserving. Also, R1=1 .

Proof

It is clear that, for AB(K)σ , the function hA is continuous. Also, the map AhA is clearly linear and order preserving. We check that hA is a fixed point for R. We have, using the assumptions (3.2)-(3.3),

hA(t)=Aet,et=i=0N-1AViet,Viet=i=0N-1|νi(t)|2Aegi(t),egi(t)=i=0N-1|νi(t)|2hA(gi(t))=(RhA)(t).

Graph

So hA is a fixed point for R. In particular, taking A to be the identity, since hI(t)=et2=1 for all t, it follows that R1=1 .

Lemma 4.32

Let t1,t2T and ϵ>0 . Then there exists nN such that if ωΩ has length |ω|n , then

egω(t1)-egω(t2)<ϵ.

Graph

Proof

Let X0 be the compact attractor of the iterated function system (gi)i=0N-1 . We claim that there is a δ>0 such that, if x0X0 , tT and dist(x0,t)<δ , then ex0-et<ϵ/2 .

Suppose not. Then there exists a sequence {xn} in X0 and a sequence {tn} in T , such that dist(xn,tn)<1/n and exn-etnϵ/2 . Since X0 is compact, by passing to a subsequence, we may assume that {xn} converges to some x0 in X0 . Since dist(xn,tn) converges to 0, we get that tn also converges to x0 . Since the map tet is continuous, we get that both exn and etn converge to ex0 , a contradiction.

Now, take some point in x0 in X0 . Since the maps gi are contractions, with some contraction ratio 0c<1 , if we take n large enough and ω in Ω with length |ω|=n , we have, for i=1,2 :

dist(gω(ti),gω(x0))cnd(ti,x0)<δ,

Graph

and since gω(x0) is in X0 , we get that egω(ti)-egω(x0)<ϵ/2 , which implies that egω(t1)-egω(t2)<ϵ .

Lemma 4.33

Let A be in the commutant of {Si} . If hA=0 then A=0 .

Proof

We have, for t1,t2T

Aet1,et2=|ω|=nSωAet1,Sωet2=|ω|=nνω(t1)ν¯ω(t2)Aegω(t1),egω(t2).

Graph

Suppose A0 . By Lemma 4.32, for a given ϵ>0 , for ω long enough, egω(t1)-egω(t2)<ϵA . Using hA(gω(t2))=0 we have:

|Aegω(t1),egω(t2)|=|Aegω(t1)-Aegω(t2),egω(t2)|Aegω(t1)-egω(t2)egω(t2)<ϵ

Graph

Then, using the Cauchy-Schwarz inequality

|Aet1,et2||ω|=n|νω(t1)|212|ω|=n|νω(t2)|2ϵ212=ϵ.

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Since ϵ was arbitrary, we get Aet1,et2=0 for all t1,t2 , and since these vectors span the entire space, we get A=0 on K and therefore A=0 on H.

Lemma 4.34

Let F be a compact invariant set and let h be a real valued continuous fixed point of the Ruelle operator. Then the sets

S:=x0F:h(x0)=supxFh(x)andI:=x0F:h(x0)=infxFh(x)

Graph

are compact and invariant.

Proof

Let x0S . We have that, if the transition x0gi(x0) is possible, then gi(x0)F and h(gi(x0))supxFh(x)=h(x0) . If the transition x0gi(x0) is not possible, then νi(x0)=0 . Therefore

h(x0)=i=0N-1|νi(x0)|2h(gi(x0))=i,igi(x0)possible|νi(x0)|2h(gi(x0))i,igi(x0)possible|νi(x0)|2h(x0)=h(x0).

Graph

Thus, we must have equality in the inequality, which means that h(gi(x0))=h(x0) whenever νi(x0)0 . Therefore gi(x0)S if the the transition is possible, so S is invariant. Similarly for I.

Lemma 4.35

If h is a continuous fixed point of the Ruelle operator then h is constant on minimal compact invariant sets.

Proof

If Rh=h , then the real and imaginary part of h are also fixed points of the Ruelle operator, as R is order preserving. Hence we may assume that h is real-valued. Let M be a minimal compact invariant set. By Lemma 4.34, the set

S=x0M:h(x0)=supxMh(x)

Graph

is compact invariant and contained in M. Since M is minimal, it follows that S=M , so h is constant on M.

Lemma 4.36

Let h be a continuous fixed point of the Ruelle operator. If h=0 on all minimal compact invariant sets, then h=0 on T .

Proof

Taking the real and imaginary parts, we can assume h is real valued. Let x0T . By Lemma 4.34, the set

S=xO(x0)¯:h(x)=suptO(x0)¯h(t)

Graph

is compact invariant, so, by Zorn's lemma, it contains a minimal compact invariant set M0 . Then, for all xM0 ,

0=h(x)=suptO(x0)¯h(t).

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Similarly

0=inftO(x0)¯h(t).

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So h is 0 on O(x0)¯ . Since x0 was arbitrary, h is 0 everywhere.

Lemma 4.37

Let M be a minimal compact invariant set. Then H(M) is irreducible for the representation (Si)i=0N-1 .

Proof

Suppose L is a closed subspace of H(M) which is invariant for the representation (Si) . Then, let PL be the projection from H to L, PK the projection from H to K and PM the projection from H to H(M). By Theorem 2.3 and Lemma 4.31, the function

hL(t)=PKPLPKet,et=PLet,et,(tT),

Graph

is a continuous fixed point of the Ruelle operator. Also since 0PLPM , we have, with hM(t)=PKPMPKet,et=PMet,et , 0hLhM. From Lemma 4.29 we get that hM=0 on all minimal compact invariant sets different than M. Indeed, if M is such a set then, for tM , PMet=0 , so hM(t)=PMet,et=0 .

Since 0hLhM , we get that hL is zero on all minimal compact invariant sets different than M. Also, from Lemma 4.35, hL is constant c on M. Since hM=1 on M, we get that chM-hL=0 on all minimal compact invariant sets. Therefore, by Lemma 4.36, hL=chM on T . This implies, by Lemma 4.33, that PL=cPM . Since PL and PM are projections, it follows that c=0 or c=1 , and this means that L is either {0} or H(M), so H(M) is irreducible.

Lemma 4.38

If M1,,Mp is a complete list, without repetitions, of the minimal compact invariant sets, then

i=1pH(Mi)=H.

Graph

Proof

Let H0=iH(Mi) and let PH0 be the corresponding projection. We know that PH0 commutes with the representation (Si) and we consider the fixed point of the Ruelle operator hH0(t)=PKPH0PKet,et=PH0et,et , tT .

For every i=1,,p and every tMi , since etH(Mi) , we have that hH0(t)=PH0et,et=et,et=1 . Thus 1-hH0 is 0 on every minimal compact invariant set. Thus, according to Lemma 4.36, 1-hH0 is zero everywhere, and by Lemma 4.33, I-PH0=0 , which means that H0=H .

Lemma 4.39

Let M1 , M2 be two distinct minimal compact invariant sets. Then the restrictions of the representation (Si)i=0N-1 to H(M1) and H(M2) are disjoint.

Proof

Let A:H(M1)H(M2) be an operator that intertwines the two representations. Extend A from H to H, by letting A=0 on the orthogonal complement of H(M1) . Then A commutes with the representation (Si) . We claim that the fixed point of the Ruelle operator hA(t):=PKAPKet,et=Aet,et=0 for all tT .

If tM1 , then etH(M1) and AetH(M2) , so, by Lemma 4.29, we get that hA(t)=Aet,et=0 .

If t is in a minimal compact invariant set M different than M1 , then H(M) is orthogonal to H(M1) , by Lemma 4.29, so Aet=0 by definition. Therefore hA(t)=Aet,et=0 in this case too. So, hA is zero on all the minimal compact invariant sets, therefore hA is zero everywhere, according to Lemma 4.36, which implies that A=0 , by Lemma 4.33.

Proof of Theorem 3.6

Assume now that the maps gi are one-to-one and that the minimal compact invariant sets are finite. We prove a Lemma.

Lemma 4.40

Assume that all the maps gi , i=0,,N-1 are one-to-one. Let M be a minimal finite invariant set. Then for any t1t2 in M, et1et2 .

Proof

Let d:=min{dist(x,y):x,yM,xy} . Let 0<c<1 be a common contraction ratio for the maps (gi) and let n be large enough, so that cndist(t1,t2)<d . Then, if |ω|n , and the transitions t1gω(t1) and t2gω(t2) are possible (in several steps), then gω(t1),gω(t2)M and

dist(gω(t1),gω(t2))cndist(t1,t2)<d,

Graph

so gω(t1)=gω(t2) and, since the maps gi are one-to-one, it follows that t1=t2 , a contradiction. Thus, for |ω|n one of the transitions t1gω(t1) and t2gω(t2) is not possible. Then, using the Cuntz relations

et1,et2=|ω|=nSωet1,Sωet2=|ω|=nνω(t1)ν¯ω(t2)egω(t1),egω(t2)=0.

Graph

Lemma 4.40 also shows that the random walk on M is also separating. Since in a minimal finite invariant set M, the orbit of any point is M, it follows that the random walk on M is irreducible. By Proposition 4.11, {Vi} is simple on K(M) for any minimal finite invariant set.

We know that the Cuntz representation on H(Mi) is irreducible, and therefore, with Theorem 3.1, we have that *span¯{Sωeci:ωΩ}=H(Mi) and so limnPHci(n)v=PH(Mi)v , for any vH(Mi) .

The proof that we have a Parseval frame is very similar to the end proof of Theorem 3.1.

Let vK . We have, for all n0 , using the fact that {Vj} is reversing on all the spaces K(Mi) :

i=1pPHci(n)v2=i=1pωΩci(n)Sωeci,v2=i=1pωΩci(n)PKSωeci,v2=i=1pωΩci(n)Vωeci,v2=i=1pωΩci(0)cycle words forciβ1,βnVωβ1βneci,v2=i=1pωΩci(0)cycle words forciβ1,βn|νβ1(ci)|2|νβn(ci)|2Vω0eci,v2.

Graph

But

βicycle word forci|νβi(c)|2=1,

Graph

by Lemma 4.8, so we obtain

i=1pPHci(n)v2=i=1pωΩci(0)Vω0eci,v2.

Graph

Then,

v2=limni=1pPHc(n)v2=i=1pωΩci(0)Vω0eci,v2.

Graph

The next proposition gives a sufficient condition for all the minimal compact invariant sets to be finite.

Proposition 4.41

Suppose the Assumptions 3.2 hold. Assume that at least one of the minimal compact invariant sets is finite. Let X0 be the attractor of the iterated function system {gi}i=0N-1 . Assume that the zero sets {xX0:νi(x)=0} are finite, and that all the maps gi are one-to-one, for all i{0,,N-1} . Then all the minimal compact invariant sets are finite.

Proof

Let M0 be a finite minimal invariant set and let MM0 be a minimal compact invariant set. Let x0M0 . Then, by Lemma 4.23, O(x0)¯=M0 . Since M0 is finite, we get that O(x0)=M0x0 , so, there exist i0,,ip-1 such that the transition x0gip-1gi0(x0)=x0 is possible, so |νω(x0)|>0 , where ω=i0ip-1 .

Since νω is continuous, there exists δ>0 such that, if d(x,x0)<δ then |νω(x)|>0 .

Let c be a common contraction ration for the maps {gi} . Let nN such that cnpdiam(X0)<δ . Let xM . Suppose the transition xgωn(x) is possible. Then gωn(x)M . Also,

d(gωn(x),x0)=d(gωn(x),gωn(x0))cnpd(x,x0)cnpdiam(X0)<δ,

Graph

since xM , x0M0 and M,M0X0 . Therefore |νω(gωn(x))|>0 and therefore the transition gωn(x)gωgωn(x) is possible. This means that gωn+1(x) is in M. Also,

d(gωn+1(x),x0)=d(gωgωn(x),gω(x0))cpd(gωn(x),x0)<δ.

Graph

By induction, gωn+k(x)M and d(gωn+k(x),x0)<δ for all kN .

But, as k , gωn+k(x) converges to the fixed point of gω , which is x0 . Since gωn+k(x)M and M is closed, it follows that x0M , which contradicts the fact that MM0 .

Thus, the transition xgωn(x) is not possible so νntimesωωω(x)=0 . Since xMX0 , we have

xk=0n-1j=0p-1(gijgi0)-1({yM:νij+1(y)=0}),

Graph

which is a finite set. Since x was arbitrary in M, it follows that M is finite.

Corollary 4.42

In the hypotheses of Theorem 3.5, assume in addition that the operators {Vi} are Cuntz isometries. If {Vi} is reversing on K, then for all i=1,,p , cMi , the numbers |νj(c)| are either 0 or 1, and {Vωeci:ωΩci(0),i=1,,p-1} is an orthonormal basis for K.

Proof

If {Vi} is reversing on K, then for cMi , if νj(c)0 , we have Vjegj(c)=ν¯j(c)ec . But, since Vj is an isometry Vjegj(c)=1 , so |νj(c)|=1 . This implies that νk(c)=0 for all kj .

The fact that {Vωeci:ωΩci(0),i=1,,p-1} is an orthonormal basis for K follows from Theorem 3.5 since the Cuntz dilation {Sj} of {Vj} is just {Vj} on K.

Examples

Example 5.1

We start with a general example which combines exponential functions and piecewise constant functions on the attractor of an affine iterated function system.

Definition 5.2

The Hilbert space will be the L2 -space associated to the invariant measure of an affine iterated function system.

Let R be a d×d expansive integer matrix (i.e., all eigenvalues λ have λ>1 ). Let BZd , 0B , B=N . Consider the affine iterated function system

τb(x)=R-1(x+b),(xRd,bB).

Graph

Let XB be the attractor XB of the iterated function system (τb)bB , i.e., the unique compact set with the property that

XB=bBτb(XB).

Graph

Let μB be the invariant measure of the iterated function system, i.e., the unique Borel probability measure such that

fdμB=1NbBfτbdμB,

Graph

for all bounded Borel functions on Rd . See [[23]] for details.

We say that the measure μB has no overlap if

μB(τb(XB)τb(XB))=0,for allbbinB.

Graph

Assume that μB has no overlap. Define R:XBXB by

Rx=Rx-b,xτb(XB),

Graph

so that Rτb(x)=x for all xXB , bB .

Now, to construct the co-isometry (Vi)i=0M-1 on the Hilbert space L2(μB) , suppose that there exist some points l0,,lM-1 in Zd , l0=0 and ai,bC ( i{0,,M-1},bB ) such that the matrix

5.1 1Ne2πiR-1b·liai,bi{0,,M-1},bB

Graph

has orthonormal columns (so it is an isometry). In other words, for all b,b in B:

5.2 1Ni=0M-1ai,ba¯i,be2πiR-1(b-b)·li=δb,b.

Graph

Define the function mi on XB by:

mi(x)=e2πili·xbBali,bχτb(XB)(x),(xXB,i{0,,M-1}).

Graph

Here χA is the characteristic function of the subset A.

Define the operators Vi on L2(μB) by

5.3 Vif(x)=ml(x)f(Rx),(xXB,fL2(μB)).

Graph

Proposition 5.3

We have the following:

  • For i{0,,M-1} and fL2(μB) :
  • 5.4 Vif(x)=1NbBmi¯(τb(x))f(τb(x)),(xXB).

Graph

  • In particular, for et(x)=e2πit·x ( tRd) ,
  • 5.5 Viet=1NbBe2πi(R)-1(t-li)·bai,b¯·e(R)-1(t-li)

Graph

  • {Vi}i=0M-1 is a co-isometry on L2(μB) . This shows that the Assumptions 3.2 are satisfied, with e(t)(x)=e2πit·x , t,xRd and
  • 5.6 νi(t)=1NbBe2πi(R)-1(t-li)·bai,b¯,gi(x)=(R)-1(t-li).

Graph

  • If, in addition, the matrix in (5.1) is unitary, then the operators {Vi} are Cuntz isometries.
Proof

We have that, for f,gL2(μ) ,

Vif,g=f,Vig=f(x)mi¯(x)g¯(Rx)dμB(x)=1NbBf(τbx)mi¯(τbx)g¯(Rτbx)dμB(x)=1NbBmi¯(τbx)f(τbx)g¯(x)dμB(x).

Graph

In particular, we have that

Viet(x)=1NbBmi¯(τb(x))et(τb(x))=1NbBe-2πili·R-1(x+b)ai,b¯e2πit·R-1(x+b)=1NbBe2πi(R)-1(t-li)·(x+b)ai,b¯=1NbBe2πi(R)-1(t-li)·bai,b¯e2πi(R)-1(t-li)·x=1NbBe2πi(R)-1(t-li)·bai,b¯e(R)-1(t-li)(x),

Graph

which implies (5.4).

Secondly, for fL2(μ) , a fixed b0B , and xτb0(XB) , we have

i=0M-1ViVif(x)=i=0M-1Vi1NbBmi¯(τb(x))f(τb(x))=i=0M-11NbBmi(x)mi¯(τbR(x))f(τbR(x))=1NbBi=0M-1mi(x)mi¯(τbR(x))f(τbR(x))=1NbBi=0M-1mi(x)e-2πili·τbRxai,b¯f(τbR(x))=1NbBi=0M-1e2πili·xe-2πili·(x+R-1(b-b0))ai,b0ai,b¯f(τbR(x))=bBf(τbR(x))1Ni=0M-1ai,b0ai,b¯e2πili·R-1(b0-b)=bBf(τbR(x))δb,b0=f(x).

Graph

If the matrix in (5.1) is unitary, then we have that

ViVif(x)=Vimi(x)f(Rx)=1NbBmi¯(τb(x))mi(τb(x))f(Rτb(x))=1NbBe-2πili·τb(x)ai,b¯e2πili·τb(x)ai,bf(x)=f(x)1NbBe-2πili·R-1(x+b)ai,b¯e2πili·R-1(x+b)ai,b=f(x)e2πi(R)-1(li-li)·x1NbBe-2πi(R)-1li·bai,b¯e2πi(R)-1li·bai,b=f(x)e2πi(R)-1(li-li)·xδi,i=f(x)δi,i.

Graph

Example 5.4

In this example, we consider the weighted Fourier frames studied in [[15], [28]].

As in Example 5.1, consider an affine iterated function system on Rd ,

τb(x)=R-1(x+b),(bB,xRd).

Graph

Assume now that there exist some points l0,,lM-1 in Zd , l0=0 , and some complex numbers α0,,αM-1 , α0=1 , such that the matrix

5.7 1Ne2πiR-1b·liαii{0,,M-1},bB

Graph

is an isometry, i.e.,

5.8 1Ni=0M-1e2πiR-1(b-b)·li|αi|2=δb,b,(b,bB).

Graph

By [[10], Theorem 1.6], we get that the measure μB has no overlap. Indeed, according to the cited reference, we just have to make sure that the elements in B are not congruent modulo RZd . But this follows, by contradiction, from (5.8).

Note that this corresponds to a special case in Example 5.1, when, for all i{0,,M-1} , we have ai,b=αi for all bB , that is ai,b is independent of b. Using Proposition 5.3, we obtain that the isometries Vi are given by

5.9 Vif(x)=αie2πili·xf(Rx),(fL2(μB)),

Graph

and they satisfy the Assumptions 3.2, with

5.10 gi(t)=(R)-1(t-li),νi(t)=α¯imB(gi(t)),(tRd,i{0,,M-1}),

Graph

where

5.11 mB(t)=1NbBe2πib·t,(tRd).

Graph

The set {0} is a minimal invariant set, because l0=0 and α0=1 , so the only possible transition from 0 is to 000 with probability |ν0(0)|2=1 .

In dimension d=1 , since mB is a trigonometric polynomial, it has finitely many zeros in the attractor XL of the maps {gi} , and therefore we can use Proposition 4.41, to conclude that all minimal invariant sets are finite.

We check that {Vj} is reversing on every space K(Mi) for all minimal invariant sets Mi , i=1,,p . For this, we will use [[15], Proposition 4.2], which shows that, for every tMi , b·tZ , for all bB . We include the statement of that result, because it gives a lot of information about the structure of the minimal finite invariant sets in this situation:

Proposition 5.5

[[15], Proposition 4.2] Assume αi0 for all i{0,,M-1} . Let M be a non-trivial finite, minimal invariant set. Then, for every two points t,tM the transition is possible from t to t in several steps. In particular, every point in the set M is a cycle point. The set M is contained in the interval min(-li)R-1,max(-li)R-1 .

If t is in M and if there are two possible transitions tgl1(t) and tgl2(t) , then l1l2(modR) .

Every point t in M is an extreme cycle point, i.e., |mB(t)|=1 and if tgl0(t) is a possible transition in one step, then {i:(l0-li)·R-1bZfor allbB}={i:lil0(modR)} and

5.12 i,lil0(modR)|αl|2=1.

Graph

In particular t·bZ for all bB .

Take cMi , and j{0,,M-1} such that νj(c)0 . This means that the transition cgj(c) is possible and so gj(c)Mi and b·gj(c)Z for all bB . Then, for xτb(XB) , we have:

Vjegj(c)(x)=αje2πiljxe2πigj(c)(Rx-b)=αje2πi(ljx+gj(c)·(Rx-b))=αje2πi(ljx+gj(c)·Rx)=αie2πi(ljx+cx-ljx)=αje2πicx.

Graph

Also

ν¯j(c)=αjm¯B(gj(c))=αj1NbBe-2πibgj(c)=αj.

Graph

So Vjegj(c)=ν¯j(c)ec .

Thus, we can apply Theorem 3.5. So, we pick a point ci in each minimal invariant set Mi . Recall that Ωci(0) is the set of all words in Ω that do not end in a cycle word for ci . We compute Vωeci , for ω=ω1ωnΩ , and we show that

5.13 Vωeci=αω1αωnelω1+Rlω2+Rn-1lωn+Rnci.

Graph

Indeed, using the fact that bciZ for all bB , and RZ , take xτb(XB) , and we have:

Vωneci(x)=αωne2πi(lωnx+ci(Rx-b))=αωnelωn+Rci(x).

Graph

Then

Vωn-1Vωneci=αωn-1αωnelωn-1+Rlωn+R2ci.

Graph

The relation (5.13) then follows by induction.

Thus, with Theorem 3.5 and Corollary 4.42, we obtain

Corollary 5.6

[[16], Theorem 1.6] In dimension d=1 , let Mi , i=1,,p be all the minimal finite invariant sets, and pick ciMi for each i=1,,p . The family of weighted exponential functions

αω1αωnelω1+Rlω2++Rn-1lωn+Rnci:ωΩci(0),i=1,,p

Graph

is a Parseval frame for L2(μB) .

Corollary 5.7

[[11], Theorem 8.4] In dimension d=1 , suppose that the matrix

1Ne2πiR-1b·lii{0,,N-1},bB

Graph

is unitary. Let Mi , i=1,,p be all the minimal invariant sets, and pick ciMi for each i=1,,p . The family of exponential functions

elω1+Rlω2++Rn-1lωn+Rnci:ωΩci(0),i=1,,p

Graph

is an orthormal basis for L2(μB) .

Example 5.8

In this example, we show that, in higher dimensions, it is possible to have minimal compact invariant sets which are infinite. Take

R:=4014,B:=00,03,10,13.

Graph

One can take

L:=l0=00,l1=20,l2=02,l3=22,

Graph

and all αi=1 , so that the matrix in (5.7) is unitary.

We have

mB(x,y)=14(1+e2πix+e2πi3y+e2πi(x+3y))=14(1+e2πix)(1+e2πi3y).

Graph

We note that the set S={(x,-2/3):xR} is invariant. Indeed, (R)-1=1/4-1/1601/4 . So, if li=(,0) then the second component of gi(x,-2/3) is -1/6 and so

νi(x,-2/3)=mB(gi(x,-2/3))=mB(,-1/6)=0.

Graph

If li=(,2) , then the second component of gi(x,-2/3) is -2/3 so gi(x,-2/3)S . Thus the only possible transitions from (x,-2/3) are

(x,-2/3)(0,2)(x/4+1/6,-2/3),and(x,-2/3)(2,2)(x/4-1/3,-2/3).

Graph

Let X1 be the attractor of the iterated function system σ0(x)=x/4+1/6 , σ2(x)=x/4-1/3 , i.e., the unique compact subset of R such that

X1=σ0(X1)σ2(X1).

Graph

We claim that X1×{-2/3} is a minimal compact invariant set.

If we compute the fixed points of σ0 and σ2 , which are 29 and -49 respectively, the interval [-49,29] is invariant for both σ0 and σ2 , which implies that X1[-49,29] .

Note that, if xX1 , then

mB(x,-2/3)=14(1+e2πix)=0,

Graph

if and only if x=-12 . Thus, the only points (x,-2/3)X1×{-2/3} for which not both transitions are possible, could be (σ0-1(-1/2),-2/3)=(-8/3,-2/3) and (σ1-1(-1/2),2/3)=(-2/3,-2/3) . But these points are outside the interval [-49,29]×{-2/3} so they are not in X1×{-2/3} . Therefore, for all points in X1×{-2/3} , both transitions are possible. But the closed orbit of any point in the attractor is the attractor itself, thus X1×{-2/3} is minimal compact invariant.

Remark 5.9

A lot of information about the structure of the minimal invariant sets in higher dimensions can be found in [[6]].

Example 5.10

We present here an example of a Cuntz representation, where a cycle point has two cycle words and therefore the family {Sωec:ωΩc(0)} is incomplete in the Hilbert space H(M) that corresponds to its minimal invariant set (by Proposition 5.5).

We consider an affine iterated function system on R2 , as in Definition 5.2, determined by the scaling matrix R=4002 , and digits B×B where B={0,2},B={0,1} . Let R=4,R=2 , l0=(0,0),l1=(3,0),l2=(4,0),l3=(15,0) . We will order the set B×B={(0,0),(2,0),(0,1),(2,1)} for the sake of indexing the matrices to follow. Take

14(ai,(b,b))i=0,,3,(b,b)B×B=12111111ξξ11-1-111-ξ-ξ,|ξ|=1;ξ1,-1

Graph

(this appears also in [[28]]).

14e2πi(14li1b+12l2b)ai,(b,b)i=0,,3,(b,b)B×B=1211111-1ξ-ξ11-1-11-1-ξξ

Graph

is unitary where li1,li2 denote the coordinates of li . To simplify notation, we will often identify (x, 0) with x. Define, for i=0,,3 ,

mi(x,x)=e2πili·(x,x)(b,b)B×Bai,(b,b)χτb,b(XB,XB)(x,x),

Graph

and Sif(x,x)=ml(x,x)f(Rx,Rx) .

Then from Proposition 5.3, since the matrix above is unitary, the operators (Si) form a representation of the Cuntz algebra O4 . If we denote et,t(x,x)=e2πi(tx+tx) , then we have that the Sl have the form:

Siet,t=νi(t,t)egi(t,t),whereνi(t,t)=14(b,b)B×Be2πi(14(t-li)b+12tb)ai,(b,b)¯gi(t,t)=14(t-li),12t.

Graph

We now find the compact minimal invariant sets. Assume M is a compact minimal invariant subset of T=R2 . Then if (t,t)M , then there must exist a possible transition (t,t)gi1(t,t)...gi1...in(t,t)M for all n. By compactness of M , there exists a convergent subsequence gi1i2...ink(t,t)(x0,0)M as k , since the second component of gi1i2...ink(t,t) is 12nkt , which converges to 0 as k . Since M is minimal M=O(x0,0)¯R×{0} . Thus M=M1×{0} , for some M1R (note that any transition from a point in R×{0} leads to R×{0} ). Now we calculate:

νi(t,0)=14bBe2πi(14(t-li)b)bBai,(b,b)¯.

Graph

However, we see that ai,(b,b) is independent of b, so we denote

αi=12bBai,(b,b)=12(ai,(0,0)+ai,(0,1))=12(ai,(2,0)+ai,(2,1))mB(x)=12bBe2πibx=12(1+e2πi2x).

Graph

Therefore we may write

νi(t,0)=αi¯mB(14(t-li))gi(t,0)=14(t-li),0.

Graph

Thus, M1 must be invariant for the maps gi(·,0) and the weights αi¯mB(14(·-li)) . Note that in particular, since α2=12(1+(-1))=0 , and αi0 for i2 , it suffices to see that M1 is invariant for the gi(·,0) and mB(14(·-li)),i{0,1,3} . We will show that M1=O(-1)¯={-1,-4} or M1=O(0)¯={0} .

With Proposition 5.5, we know that, for any cM1 , we must have c·bZ for all bB . So c12Z . Also, c[-153,03]=[-5,0] . Also, if cM1 and the transition to gi(c) is possible, then gi(c) is in M1 so it must be of the same form 12Z . Note that mB(x)=0 only if x is of the form 2k+14 for some kZ . Thus, if c=2j+12 for some jZ then the transition cg0(c)=2j+18 is possible and g0(c) is not in 12Z . This means that c cannot be in M1 . So we only have to check {-5,-4,-3,-2,-1,0} . {0} is the trivial invariant set. Also {-4,-1} is invariant. We have the possible transitions -5g1(-5)=-2g0(-2)=-12 and -3g1(-3)=-32 . Since -12 and -32 are not in M1 it follows that neither are -5,-3 nor -2 .

In the case of M1=O(-1)={-4,-1} , we see that -1 has two distinct cycle words, 1 and 3, 0. Indeed -1g1(-1)=-1-34=-1 and -1g3(-1)=-1-154=-4g0(-4)=-44=-1 . Thus by Proposition 4.13, we know that span¯{Sωe(-1,0):ωΩ(-1,0)(0)}H(M1) .

Example 5.11

We use Theorem 3.5 to provide a class of Parseval frames as in [[17]], Theorem 3.11. Let A be a M×N matrix such that 1NAA=IN (hence NM ) and the first row is constant α0,j=1 , j=0,,N-1 . With R(x)=Nxmod1 and k{0,1,M-1} define

mk(x):=j=0N-1akjχ[j/N,(j+1)/N)(x)Vk:L2[0,1]L2[0,1],Vkf(x):=mk(x)f(R(x)).

Graph

Note that this corresponds to the Example 5.1 when R=N , B={0,1,,N-1} , li=0 for all i=0,,M-1 and ai,b are the entries of the matrix A. Indeed, the attractor of the iterated function system (τb)bB is [0, 1] and the invariant measure μB is the Lebesgue measure on [0, 1].

By Proposition 5.3, the Assumptions 3.2 are satisfied, with

gi(t)=tN,νi(t)=1Nj=0N-1e2πij·tNa¯i,j.

Graph

We will show that the only compact minimal invariant set is M={0} then apply Theorem 3.5.

The set M={0} is invariant because the only possible transition from 0 is 000 with probability |ν0(0)|2=1 .

To show this is the only compact, minimal invariant set suppose by contradiction there is a compact minimal invariant set N with some tN , t0 . We argue that necessarily 0N thus {0}N , contradicting the minimality of N . If tN then t/NN because there must be at least one possible transition tgk(t)=t/N since k|νk(t)|2=1 . Continuing in this fashion we get an:=(t/N)nN for all nN . By compactness and invariance 0=limnanN , as desired.

Since the only cycle word for 0 is 0, with Theorem 3.5, we obtain:

Corollary 5.12

[[17], Theorem 1.4] The family of functions

{Vω1:ωΩnot ending in0}

Graph

is a Parseval frame for L2[0,1] .

Acknowledgements

We would like to thank professor Deguang Han for very helpful conversations and to the anonymous referee for a very careful and thorough review of our paper.

Publisher's Note

Springer Nature remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.

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Reported by Author; Author; Author; Author

Titel:
Parseval frames from compressions of Cuntz algebras.
Autor/in / Beteiligte Person: Christoffersen, Nicholas ; Dutkay, Dorin Ervin ; Picioroaga, Gabriel ; Weber, Eric S.
Link:
Zeitschrift: Mathematische Zeitschrift, Jg. 304 (2023-05-01), Heft 1, S. 1-36
Veröffentlichung: 2023
Medientyp: academicJournal
ISSN: 0025-5874 (print)
DOI: 10.1007/s00209-023-03259-w
Schlagwort:
  • RANDOM walks
  • ALGEBRA
  • REPRESENTATIONS of algebras
  • FOURIER series
  • Subjects: RANDOM walks ALGEBRA REPRESENTATIONS of algebras FOURIER series
  • 05C81
  • 28A80
  • 42A16
  • 42C10
  • 47L55
  • Cuntz algebra
  • Fourier series
  • Fractal measures
  • Iterated function systems
  • Parseval frame
  • Row co-isometry
  • Walsh bases
Sonstiges:
  • Nachgewiesen in: DACH Information
  • Sprachen: English
  • Document Type: Article
  • Author Affiliations: 1 = Department of Mathematics, University of Colorado, Campus Box 395, 2300 Colorado Avenue, 80309-0395, Boulder, CO, USA ; 2 = Department of Mathematics, University of Central Florida, P.O. Box 161364, 4000 Central Florida Blvd., 32816-1364, Orlando, FL, USA ; 3 = Department of Mathematical Sciences, University of South Dakota, 414 E. Clark St., 57069, Vermillion, SD, USA ; 4 = Department of Mathematis, Iowa State University, 396 Carver Hall, 411 Morrill Road, 50011, Ames, IA, USA
  • Full Text Word Count: 22499

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