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Purpose

Since weighted shifts play a vital role in linear dynamics so in 2021 Chan & Sanders considered weighted shift operators on p(Z) that are not hypercyclic and proved that under certain conditions they can be factorized as products of hypercyclic shifts. The purpose of this article is to extend their results to operator weighted shifts on 2(K) by using the concept of generalized shift of higher multiplicity developed herein.

Design/methodology/approach

Traditionally, an operator T is considered as a shift on a space H if there is some canonical basis for H such that T shifts every basis vector to the immediate next basis vector, maybe with some weight attached to it. This clearly indicates that an operator which is a shift with respect to a basis for H may not remain a shift if the basis is changed. This motivates the definition of a generalized shift operator. We begin with the case of multiplicity one and then extend it to higher finite multiplicity. We then develop the idea so that we can frame conditions under which a bilateral shift can be factorized as product of hypercyclic generalized shifts.

Findings

A generalized bilateral backward weighted shift (GBBWS) is defined in terms of a bijection on Z and it is shown that if there are two bijections σ and ρ which generate the same generalized shift, then there exists a unique c such that σ(i) = ρ(i + c) for all integers i. We determine conditions under which the direct sum of generalized shifts is again a generalized shift. We also show that for a uniformly bounded sequence of invertible diagonal operators {Ai} on a separable complex Hilbert space K of finite dimension, if W is bilateral backward weighted shift on 2(K) with weight sequence {Ai} then there exists hypercyclic GBBWS T and P on 2(K) such that W = TP.

Originality/value

The idea of generalized shift of multiplicity one was introduced by Chan & Sanders in 2018. However, we have developed the idea further, particularly extending it to the case of shifts of higher multiplicity. The factorization of shifts as product of hypercyclic shifts was also done by them. We have extended their result to higher dimension, and our approach to the problem is completely different from theirs.

Consider an infinite dimensional complex Hilbert space H. Recall that a bounded linear operator T on H is said to be cyclic if hH such that {p(T)h: p a polynomial} is dense in H; T is said to be hypercyclic if xH such that Orbit{Tnx: n ≥ 0} is dense in H. The study of hypercyclicity is specific to infinite dimensional spaces because no operator on a finite dimensional space is ever hypercyclic. The first examples of hypercyclic operators constructed on a Hilbert space were multiples λB with |λ| > 1, where B is the unweighted unilateral backward shift [1].

In [2] Wu proved that even if an operator is not cyclic it can still be expressed as the sum of cyclic operators. In Ref. [3] Grivaux showed that a bounded linear operator T can be expressed as the sum of two hypercyclic operators. Again in Ref. [2] Wu proved that even when T is not cyclic it can be factorized as product of cyclic operators. Hence it is natural to explore operator factorization in the stronger setting of hypercyclicity. Since weighted shifts play a vital role in linear dynamics (refer [4]) so in Refs. [5, 6] Chan & Sanders considered weighted shift operators on p(Z) that are not hypercyclic and proved that under certain conditions they can be factorized as products of hypercyclic shifts. In this article we extend their results to operator weighted shifts on 2(K) by using the concept of generalized shift of higher multiplicity developed in Sections 3 and 4.

Shift operators on separable Hilbert and Banach spaces have always been a subject of interest since the first systematic study done by Shields [7]. One of the reasons for this continued exploration and interest is because they provide a fertile domain for examples and counter examples. Traditionally, an operator T is considered as a shift on a space H if there is some canonical basis for H such that T shifts every basis vector to the immediate next basis vector, maybe with some weight attached to it. This clearly indicates that an operator which is a shift with respect to a basis for H may not remain a shift if the basis is changed. Given a space H, it is common practice to identify a cannonical basis B of H and throughout the particular study the action of all linear operators on H are considered with respect to this arbitrary fixed basis B.

For example, let H=2(C), the space of all two way scalar sequences which are square summable. Let {en}nZ be an orthonormal basis for H. Given a bounded sequence of non-zero scalars {αn}nZ, an operator T is a shift on H if Ten=αnen+1nZ. In this case T is called bilateral forward weighted shift (abbreviated as BFWS) with weight sequence {αn}. If Ten=αn1en1nZ, then T is called bilateral backward weighted shift (or BBWS) with weight sequence {αn}.

Now consider the operator T on H such that Ten=e0, if n=2e1, if n=0e1, if n=1en1, otherwise. 

Clearly, T is not a shift on H with respect to basis {en}nZ. However, if we re-arrange the basis vectors and consider the basis {fn}nZ where f1 = e0, f0 = e1 and fn = en for n ≠ 0, 1, then Tfn=fn1nZ, and so T is a shift on H with respect to basis {fn}nZ. In this case, T is called a generalized shift on H with respect to basis {en}nZ.

Thus, given a basis {en}nZ of H if there exists a bijection σ on Z such that an operator T on H is a shift with respect to basis {eσ(n)}nZ then T is called a generalized shift on H with respect to bijection σ. References to generalized shifts on 2(C) can be found in Refs. [5, 6].

In this article, we consider generalized shifts of multiplicity higher than 1. For this we consider a separable complex Hilbert space K and define 2(K) to be the space of all two way sequences {xn}nZ in K such that nZxn2<. In Section 3, we define generalized bilateral backward weighted shifts (GBBWS) on 2(K) and prove the following:

  1. If T is a GBBWS on 2(K) with respect to the bijection σ then there exists infinitely many bijections on Z distinct from σ, such that T is a GBBWS with respect to each of these bijections. However, there exists only one such bijection ρ for which ρ(0) = 0, and in this sense the bijection corresponding to GBBWS T is unique.

  2. Every GBBWS on 2(K) is similar to the BBWS on 2(K) with same sequence of weights.

In Section 4, we consider 2(K1) ⊕ 2(K2) for separable complex Hilbert spaces K1 and K2. We show that if T1, T2 are GBBWS on 2(K1), 2(K2) respectively then T1T2 is again a GBBWS. Conversely, if T is a GBBWS on 2(K1K2) with weight sequence {An}nZ then T = T1T2, where T1, T2 are GBBWS on 2(K1), 2(K2) respectively provided An = BnCn, where Bn, Cn are non zero bounded linear operators on K1, K2 respectively.

The main objective of the paper is addressed in Section 5. Here we apply the results developed in Sections 3 and 4 to provided conditions under which a BBWS W on 2(K) can be factorized as W = AB where A and B are hypercyclic GBBWS.

Let C denote the complex space and Z denote the set of integers. 2(C) denotes the space of all two way square summable sequences {αn}nZ in C. If {αn}nZ is in 2(C) then it is denoted as (…, α−1, [α0], α1, …) where [.] denotes the 0th position of the sequence with respect to index set Z. Thus,

For x = (…, α−1, [α0], α1, …) and y = (…, y−1, [y0], y1, …) in 2(C), define x,y=iZxiy¯i. Then 2(C) is a Hilbert space with respect to this inner product.

If ei denotes the sequence (…, δ−1,i, [δ0,i], δ1,i, …) where δj,i=1, if j=i0, otherwise then {ei}iZ is an orthonormal basis for 2(C) and x = (…, α−1, [α0], α1, …) in 2(C) can be written as x=iZαiei.

Let K be a separable complex Hilbert space and 2(K) denote the space of all two way square summable sequences {xn}nZ in K. If {xn}nZ is in 2(K), we denote it as (…, x−1, [x0], x1, …) so that 2(K){x=(,x1,[x0],x1,):xiK,iZxi2<}.

For x = (…, x−1, [x0], x1, …) and y = (…, y−1, [y0], y1, …) in 2(K), we define x + y = (…, x−1 + y−1, [x0 + y0], x1 + y1, …) and λx = (…, λx−1, [λx0], λx1, …) for λC. Also, x,y=iZxi,yi and 2(K) is a separable Hilbert space with respect to these operations.

For t ∈ K, we follow the convention of denoting the sequence (…, 0, [t], 0, …) as te0. In fact, for iZ, if x = (…, x−1, [x0], x1, …) ∈ 2(K) with xi = t and xj = 0 for ji, then we denote x as tei. Therefore, x = (…, x−1, [x0], x1, …) ∈ 2(K) can be written as iZxiei.

Definition 1.

Let {An}nZ be a sequence of non-zero bounded linear operators on K such that supnAn‖ < . Let W: 2(K) → 2(K) be defined as follows:

Equivalently, W(iZxiei)=iZAi1xiei1. Then W is called bilateral backward weighted shift (BBWS) on 2(K) with weight sequence {An}nZ.

Similarly, if for each x=iZxiei2(K), we have W(xiei)=Aixiei+1iZ, then W is called bilateral forward weighted shift (BFWS) on 2(K) with weight sequence {An}nZ.

If dim(K) = 1, then 2(K) is isomorphic to 2(C) and is therefore considered as identical with 2(C). Let σ be a bijection on Z. For y = (…, y−1, [y0], y1, …) in 2(K), let zjyσ(j). Then {yj} and {zj} are same as sets but different as sequences since the order of the elements in {yj} have been changed in the sequence {zj}. We use the notation (,z1,[z0],z1,)σ to understand that jZzjeσ(j)2(K). Let us define 2(K)σ as follows:

So, if z=(,z1,[z0],z1,)σ2(K)σ then

Similarly, if y = (…, y−1, [y0], y1, …) ∈ 2(K) then

Definition 2.

For a uniformly bounded sequence {An}nZ of non-zero operators on K, T: 2(K)σ2(K)σ is said to be a BBWS with weight sequence {An}nZ if for each z=(,z1,[z0],z1,)σ2(K)σ,T(,z1,[z0],z1,)σ=(,A1z0,[A0z1],A1z2,)σ.

Definition 3.

An operator T on 2(K) is said to be a generalized bilateral backward weighted shift (GBBWS) if there exists a bijection σ on Z and a uniformly bounded sequence {An}nZ of non-zero operators on K such that T is BBWS on 2(K)σ with weight sequence {An}nZ. In this case, we say that T is a GBBWS on 2(K) with respect to bijection σ and weight sequence {An}nZ. Thus, for x=iZxiei2(K),

or equivalently, T(xσ(i)eσ(i))=Ai1xσ(i)eσ(i1)iZ.

Example 1.

Let T on 2(K) be defined as follows:

For x=iZxieil2(K),Tx=(,x1,x0,[x2],x3,x1,x4,x5,).

Equivalently,

Figure 1 below gives a pictoral representation of the action of T on x = (…, x−1, [x0], x1, …).

Consider the bijection σ on Z given by:

It can easily be verified that Txσ(i)eσ(i)=xσ(i)eσ(i1)iZ where x=iZxiei2(K). Thus, T is a GBBWS on 2(K) with respect to bijection σ and weight sequence {An}nZ, where each An is the identity operator on K.

Proposition 1.

Let {Dn}nZ be a uniformly bounded sequence of non-zero operators on K. Let T be an operator on 2(K) such that for each x=iZxiei2(K),T(xiei)=Di1xieτ(i), where τ is a bijection on Z. If T is a GBBWS on 2(K) with respect to bijection σ and weight sequence {An}nZ then (τσ)(i) = σ(i − 1) and Ai1=Dσ(i)1iZ.

Proof. For x=iZxiei2(K), we have, T(xσ(i)eσ(i)) = Ai−1xσ(i)eσ(i−1).

Also, T(xσ(i)eσ(i)) = Dσ(i)−1xσ(i)eτ(σ(i)).

Thus, Ai1xσ(i)eσ(i1)=Dσ(i)1xσ(i)eτσ(i)iZ which implies that

σ(i1)=(τσ)(i)iZ and Ai1xσ(i)=Dσ(i)1xσ(i)iZ

As xσ(i) is an arbitrary element of K so we must have Ai−1 = Dσ(i)−1 ∀ i. □

Using the above proposition, we will give an example of an operator T on 2(K) such that T is not a GBBWS.

Example 2.

Let T on 2(K) be defined as follows:

Figure 2 below gives a pictoral representation of the action of T on x ∈ 2(K).

We will show that T is not a GBBWS on 2(K).

Let if possible there exists a bijection σ on Z and a weight sequence {An}nZ of operators on K such that T is a GBBWS on 2(K) with respect to σ and weight sequence {An}nZ.

From the definition of T, we have Txiei = xieτ(i), where τ(i)2, if i=1,0, if i=3,i1,otherwise.

So, by P1, we should have each An to be the identity operator on K, and (τσ)(i)=σ(i1)iZ.

Claim 1.

If τσ(i) = σ(i − 1) ∀i then jZ such that σ(j) = 1.

To establish our claim, suppose j0Z such that σ(j0) = 1.

Then σ(j0 − 1) = (τσ)(j0) = τ(σ(j0)) = τ(1) = 2

and σ(j0 − 2) = (τσ)(j0 − 1) = τ(σ(j0 − 1)) = τ(2) = 1.

Therefore, σ(j0) = 1 = σ(j0 − 2), and since σ is injective, we must have j0 = j0 − 2, a contradiction. Thus, our claim is established.

Now, by Claim1, σ is not surjective which contradicts the fact that σ is a bijection on Z. Hence,any bijection σ on Z such that T is a GBBWS on 2(K) with respect to σ.

Example 3.

Consider the operator given in Example1 where it was shown that  a bijection σ on Z such that T is GBBWS on 2(K) with respect to σ.

Consider the bijection φ on Z given by φ(i)=i+4, if i4 or i12, if i=31, if i=2.

It follows easily that T is a GBBWS on 2(K) with respect to bijection φ.

Remark 1.

  1. From examples 1 and 3, we can conclude that for a bounded linear operator T on 2(K) there may exist different bijections σ and φ on Z such that T is GBBWS on 2(K) with respect to both σ and φ. In other words, σ corresponding to T is not unique.

  2. In examples 1 and 3, we observe that φ(i)=σ(i+4)iZ. This observation leads us to the next few results.

Theorem 2.

Let T be a GBBWS on 2(K) with respect to bijection σ and weight sequence {An}nZ. Let cZ and φ(i)σ(i+c)iZ. Then T is a GBBWS on 2(K) with respect to bijection φ and weight sequence {Bn} where Bi=Ai+ciZ.

Proof. For x=iZxiei2(K) we have Txσ(i)eσ(i)=Ai1xσ(i)eσ(i1)iZ. Therefore Txσ(i+c)eσ(i+c)=Ai+c1xσ(i+c)eσ(i+c1)iZ which implies that Txφ(i)eφ(i) = Ai+c−1xφ(i)eφ(i−1). Let BiAi+c so that Bi−1 = Ai+c−1. Thus, we have Txφ(i)eφ(i)=Bi1xφ(i)eφ(i1)iZ, and so T is GBBWS on 2(K) with respect to φ and weight sequence {Bn}nZ. □

Theorem 3.

Let T be a bounded linear operator on 2(K) such that T is GBBWS on 2(K) with respect to bijection σ and weight sequence {An}nZ and T is also a GBBWS on 2(K) with respect to bijection φ and weight sequence {Bn}nZ. Then there exists a unique cZ such that φ(i)=σ(i+c)iZ. Also, Bi=Ai+ciZ.

Proof. Existence:

  • Step 1: We show that if m,nZ such that σ(m) = φ(n) then σ(m − λ) = φ(n − λ) for all positive integers λ. For this, let x=iZxiei2(K) and suppose σ(m) = φ(n) = i0. Then Txi0ei0=Txσ(m)eσ(m)=Am1xσ(m)eσ(m1) and Txi0ei0=Txφ(n)eφ(n)=Bn1xφ(n)eφ(n1). Thus, Am1xi0eσ(i1)=Bn1xi0eφ(n1) which implies that σ(m − 1) = φ(n − 1).

Therefore σ(m) = φ(n) ⇒ σ(m − 1) = φ(n − 1). Applying this argument repeatedly we get σ(m − λ) = φ(n − λ) for every positive integer λ, and Step1 is proved.

As 1Z and σ and φ are surjective, so m0,n0Z such that σ(m0) = 1 = φ(n0). Together with the conclusion of Step1 we can say that integers m0 and n0 such that σ(m0 − λ) = φ(n0 − λ) for all non negative integers λ.

  • Step 2: To show σ(m0 + λ) = φ(n0 + λ) for all positive integers λ.

Let S1{σ(m0λ):λN{0}} and S2={φ(n0λ):λN{0}}.

Since, σ(m0 − λ) = φ(n0 − λ) so S1 = S2.

Now, let λ be a positive integer and j0 = σ(m0 + λ). Since φ is surjective n1Z such that φ(n1) = j0. Also j0S1 implies j0S2 and so n1 > n0.

Thus, φ(m0 + λ) = φ(n1) and so, by applying the conclusion of Step1, we get σ(m0) = φ(n1 − λ). This together with the fact that σ(m0) = φ(n0) gives φ(n0) = φ(n1 − λ). Since φ is injective, so this implies that n0 = n1 − λ, or equivalently, n1 = n0 + λ. Thus, σ(m0 + λ) = j0 = φ(n0 + λ), and Step2 is established.

Thus, there exist integers m, n such that σ(m+λ)=φ(n+λ)λZ. If c ≔ m − n then for iZ, we have σ(i + c) = σ(m + (i − n)) = φ(n + (i − n)) = φ(i).

Uniqueness:

Suppose there exists c1,c2Z such that φ(i)=σ(i+c1)=σ(i+c2)iZ. Then by injectivity of σ, we must have c1 = c2.

  • Step 3: To show Bi=Ai+ciZ. Since for x=iZxiei2(K), we have

Txφ(i)eφ(i) = Bi−1xφ(i)eφ(i−1) = Bi−1xσ(i+c)eσ(i+c−1) and

Txφ(i)eφ(i) = Txσ(i+c)eσ(i+c) = Ai+c−1xσ(i+c)eσ(i+c−1),

therefore we must have Bi−1 = Ai+c−1, or equivalently, Bi=Ai+ciZ. □

Remark 2.

In view of theorems 2 and 3, given a GBBWS T on 2(K) with respect to σ we can always choose σ(0) = 0 without any loss of generality. If we follow this convention then we can say that σ corresponding to T is unique. Henceforth, in the sequel we will always assume σ(0) = 0 so that σ corresponding to T is unique.

Theorem 4.

Let T be a GBBWS on 2(K) with respect to bijection σ and weight sequence {An}nZ. Then T is similar to the BBWS on 2(K) with weight sequence {An}nZ.

Proof. Define P, Q: 2(K) → 2(K) as follows: for x=iZxiei2(K),

PxiZxieσ(i) and QxiZxieσ1(i).

Therefore, PQ and QP are both identity on 2(K)and so P, Q are invertible and Q = P−1. As T is a BBWS on 2(K)σ, so for y=(,y1,[y0],y1,)σ2(K)σ,T(,y1,[y0],y1,)σ=(,A1y0,[A0y1],A1y2,)σ. Now for x=(,x1,[x0],x1,)2(K),

Thus, W = P−1TPT is similar to W. □

We can apply Theorem 4 to show that a given operator is not a GBBWS on 2(K).

Example 4.

For simplicity, we consider dim(K) = 1. So 2(K) is replaced with 2(C). From [Ref. 7], we know that the bilateral backward shift W on 2(C) have no eigen values, or the point spectrum of W is empty.

Now consider T as defined in Example 2, where Te1 = e2 and Te2 = e1. So for x=e1+e22(C), we have Tx = x and so 1 is an eigen value of T. Thus, the point spectrum of T is non-empty.

But if two operators are similar then they must have the same point spectrum. Thus, T is not similar to W and so by Theorem 4, T cannot be a GBBWS on 2(C).

We end the section with the following question:

Suppose we have two separable complex Hilbert spaces K1 and K2 such that K = K1K2. If T is a GBBWS on 2(K) then can we express T as T1T2 where T1 and T2 are GBBWS on 2(K1) and 2(K2) respectively?”

In the next section, we address this and other related questions.

Let K = K1K2. Then for a sequence of elements {xi} in K, we get sequences {yi} and {zi} in K1 and K2 respectively where xi = yizi. Also we define ‖xi2 = ‖yi2 + ‖zi2 so that {xi} is square summable if and only if {yi} and {zi} are square summable.

Following the notation introduced in Section 3, if x = (…, x−1, [x0], x1, …) ∈ 2(K) where K = K1K2, we have the representation x=iZxiei. But each xi = yizi where yiei ∈ 2(K1), ziei ∈ 2(K2). So, in this case xiei actually has to be interpreted as yieiziei. To avoid confusion, we introduce a new notation in case K = K1K2. For each iZ, define fi = eiei and for αβ ∈ K1K2, let (αβ)fi = αeiβei. So, x = (…, x−1, [x0], x1, …) ∈ 2(K1K2) will now be represented as x=iZxifi=iZ(yizi)fi=iZ(yieiziei). Also, note that if H1 and H2 are two Hilbert spaces then for xy and ξη in H1H2, addition in H1H2 is conventionally defined as (xy) + (ξη) = (x + ξ) ⊕ (y + η).

Following the same rule in 2(K1) ⊕ 2(K2), we have x=iZ(yieiziei)=(iZyiei)(iZziei), i.e., x = yz where y=iZyiei2(K1) and z=iZziei2(K2). Thus, we can define 2(K1K2) as (,x1,[x0],x1,):xi=yiziK1K2,iZyiei2(K1),iZziei2(K2) so that 2(K1K2) = 2(K1) ⊕ 2(K2). Equivalently, for y=iZyiei2(K1) and z=iZziei2(K2), we have yz=iZ(yizi)fi2(K1K2).

Definition 4.

Let K = K1K2 and {An} be a uniformly bounded sequence of non-zero operators on K. Linear operator W: 2(K1K2) → 2(K1K2) is called bilateral backward weighted shift (BBWS) on 2(K1K2) with weight sequence {An} if W(iZxifi)=iZAi1xifi1.

Theorem 5.

Let W be BBWS on 2(K1K2) with weight sequence {An}nZ, where An = BnCn, Bn, Cn non zero bounded linear operators on K1, K2 respectively and supnAn‖ < . Then W = W1W2, where W1 is BBWS on 2(K1) with weight sequence {Bn}nZ and W2 is BBWS on 2(K2) with weight sequence {Cn}nZ.

Proof. Let x=iZxifi2(K1)2(K2). Then xi = yizi ∈ K1K2, and

(1)

As y=iZyiei2(K1) so W1y=iZBi1yiei1, and as z=iZyiei2(K2) so W2z=iZCi1ziei1. Observe that yz ∈ 2(K1) ⊕ 2(K2) and so (W1W2)(yz) ≔ W1yW2z. Using this in (1) we get Wx = W1yW2z = (W1W2)(yz) = (W1W2)x. Thus, W = W1W2. □

Theorem 6.

If W1 and W2 are BBWS on 2(K1) and 2(K2) with weight sequences {Bn} and {Cn} respectively, then W ≔ W1W2 is BBWS on 2(K1K2) with weight sequence {An}, where An ≔ BnCn.

Proof. Let x=iZxiei2(K1K2). Then xi = yizi ∈ K1K2. Also y=iZyiei2(K1),z=iZziei2(K2) and x = yz ∈ 2(K1K2).

Therefore,

Thus, W is BBWS on 2(K1K2) with weight sequence {An}nZ. □

Now for K = K1K2 let W be a GBBWS on 2(K) with bijection σ and weight sequence {An}nZ, where {An}nZ is a sequence of uniformly bounded non-zero operators on K. Then for each x=iZxifi2(K), W(,xσ(1),[xσ(0)],xσ(1),)σ=(,A1xσ(0),[A0xσ(1)],A1xσ(2),)σ i.e., W(iZxσ(i)fσ(i))=iZAi1xσ(i)fσ(i1) where fσ(i) = eσ(i)eσ(i). Let us assume that each An = BnCn, where Bn and Cn are non zero bounded linear operators on K1 and K2 respectively. Also since xi ∈ K1K2 so there exists yi ∈ K1 and zi ∈ K2 such that xi = yizi. Thus, x = yz, where y=iZyiei2(K1) and z=iZziei2(K2).

Let W1 be GBBWS on 2(K1) with respect to bijection σ and weight sequence {Bi}, W2 be GBBWS on 2(K2) with respect to bijection σ and weight sequence {Ci}. Then W1y=iZBi1yσ(i)eσ(i1) and W2z=iZCi1zσ(i)eσ(i1).

∴ we have

Thus, Wx = (W1W2)(yz) = (W1W2)x. So, we can represent W as W1W2, where W1 and W2 are GBBWS on 2(K1) and 2(K2) respectively both with respect to bijection σ. We can summarize this in the following theorem.

Theorem 7.

Let W be a GBBWS on 2(K1K2) with respect to bijection σ and weight sequence {An}nZ where An = BnCn with Bn, Cn being non-zero bounded linear operators on K1 and K2 respectively. Then W = W1W2 where W1 is GBBWS on 2(K1) with respect to bijection σ and weight sequence {Bn}nZ and W2 is GBBWS on 2(K2) with respect to bijection σ and weight sequence {Cn}nZ.

Let us consider the converse of the above result by taking GBBWS W1 and W2 on 2(K1) and 2(K2) respectively and defining W = W1W2 on 2(K1) ⊕ 2(K2) = 2(K1K2). As W1 is a GBBWS on 2(K1), so there exists a bijection σ on Z and a weight sequence {Bn}nZ of non-zero operators such that for each y=iZyiei2(K1),W1(iZyσ(i)eσ(i))=iZBi1yσ(i)eσ(i1). Similarly, W2 is a GBBWS on 2(K2) and so there exists a bijection ρ on Z and weight sequence {Cn}nZ of non-zero operators such that for each z=iZziei2(K2),W2(iZyρ(i)eρ(i))=iZCi1yρ(i)eρ(i1).

As it is not necessary that ρ = σ, hence the steps that proved Theorem 7 cannot be reversed. To address this issue, we proceed to introduce a new bijection τ to represent the pair (σ, φ). For this, let τ:ZZ be defined as τ(σ(i)) = φ(i), i.e. τ = φσ−1. Then τ is a bijection on Z. We define (fτ)i=eσ(i)eφ(i). For αβ ∈ K1K2, we set (αβ)(fτ)i=αeσ(i)βeφ(i). Thus for each xi = yizi ∈ K1K2 we use the representation x=(,x1,[x0],x1,)τ to understand

Thus, we can define 2(K1K2)τ={(,x1,[x0],x1,)τ:xi=yiziK1K2,iZyieσ(i)2(K1),iZzieφ(i)2(K2)}, so that 2(K1K2)τ=2(K1)σ2(K2)φ. Equivalently, for y=(,y1,[y0],y1,)σ2(K1)σ and z=(,z1,[z0],z1,)φ2(K2)φ, we have yz=iZ(yizi)(fτ)i2(K1K2)τ.

Remark 3.

(i) Note that when φ(i)=i=σ(i)iZ, i.e. φ and σ are the identity bijections on Z, then (fτ)i=fi.

  • (ii) If σ = φ, not necessarily identity on Z, then

(fτ)i=eσ(i)eφ(i)=eσ(i)eσ(i)=fσ(i).

  • (iii) If x=iZ(yizi)fi=(,y1z1,[y0z0],y1z1,)2(K1K2) then 

Notational Summary:

  1. 2(K1K2) = 2(K1) ⊕ 2(K2) where fi = eiei, and if x = i(yizi)fi ∈ 2(K1K2) then x = yz where y = iyiei ∈ 2(K1), z = iziei ∈ 2(K2).

  2. For bijections σ and ρ let τρσ−1.

     Then 2(K1K2)τ=2(K1)σ2(K2)ρ. Also (fτ)ieσ(i)eρ(i), and if x = i(yizi)fi ∈ 2(K1K2) then x=iZ(xτ)i(fτ)i=(,(xτ)1,[(xτ)0],(xτ)1,)τ2(K1K2)τ where (xτ)i=yσ(i)zρ(i).

Definition 5.

A bounded linear operator T on 2(K1K2) is said to be a generalized bilateral backward weighted shift (GBBWS) with respect to bijection τ and weight sequence {An} if the following conditions hold:

  1. There exist bijections σ and ρ on Z such that τ = ρσ−1 and 2(K1K2)τ=2(K1)σ2(K2)ρ.

  2. For x=iZ(yizi)fi2(K1K2), we have T(iZ(xτ)i(fτ)i)=iZAi1(xτ)i(fτ)i1, where (xτ)i=yσ(i)zρ(i), (fτ)i=eσ(i)eρ(i).

Theorem 8.

Let T1 be GBBWS on 2(K1) with respect to bijection σ and weight sequence {Bn}nZ, and T2 be GBBWS on 2(K2) with respect to bijection ρ and weight sequence {Cn}nZ. If An = BnCn and τρσ−1 then T = T1T2 is GBBWS on 2(K1K2) with respect to bijection τ and weight sequence {An}nZ.

Proof. Let T ≔ T1T2 on 2(K1) ⊕ 2(K2) = 2(K1K2) and x=iZxifi2(K1K2). Then xi = yizi ∈ K1K2 and x = yz ∈ 2(K1) ⊕ 2(K2), where y=iZyiei and z=iZziei.

Thus x=iZ(xτ)i(fτ)i2(K1K2)τ, where (xτ)iyσ(i)zρ(i).

Also T1y=T1(iZyσ(i)eσ(i))=iZBi1yσ(i)eσ(i1) and

T2z=T2(iZzρ(i)eρ(i))=iZCi1zρ(i)eρ(i1).

Let An ≔ BnCn on K1K2. Then for x=iZxifi2(K1K2), it follows that T(iZ(xτ)i(fτ)i)=iZAi1(xτ)i(fτ)i1. Therefore, T is a GBBWS on 2(K1K2) with respect to bijection τ and weight sequence {An}nZ. □

Finally, the following result gives an affirmative answer to the question raised at the end of Section 3.

Theorem 9.

Let K = K1K2 and An = BnCn where Bn and Cn are non-zero bounded linear operators on K1 and K2 respectively. Also, let supnAn‖ < . If T is a GBBWS on 2(K1K2) with respect to bijection τ and weight sequence {An}nZ then the following holds:

  1. There exist bijections σ and φ on Z such that τ = φσ−1,

  2.  GBBWS T1 on 2(K1) with respect to bijection σ and weight sequence {Bn}nZ and GBBWS T2 on 2(K2) with respect to bijection φ and weight sequence {Cn}nZ such that T = T1T2.

Proof. Let σ be a bijection on Z and φ = τσ. Then 2(K1K2)τ=2(K1)σ2(K2)φ. Also for each x=iZ(yizi)fi2(K1K2),

Tx=T(iZ(xτ)i(fτ)i), [where (xτ)i=yσ(i)zφ(i)]

=iZAi1(xτ)i(fτ)i1]

=(iZBi1yσ(i)eσ(i1))(iZCi1zφ(i)eφ(i1)).

Now as x = yz where y=iZyiei2(K1),z=iZziei2(K2),

therefore T1y=T1(iZyσ(i)eσ(i))=iZBi1yσ(i)eσ(i1) and

T2z=T2(iZzφ(i)eφ(i))=iZCi1zφ(i)eφ(i1). Thus we get

Tx = T1yT2z = (T1T2)x which implies that T = T1T2. □

Theorem 10.

Let K = K1K2 and An = BnCn where Bn and Cn are non-zero bounded linear operators on K1 and K2 respectively. If T is a GBBWS on 2(K1K2) with respect to bijection τ and weight sequence {An}nZ then T is similar to the BBWS W on 2(K1K2) with weight sequence {An}nZ.

Proof. By Theorem 9, bijections σ and φ on Z such that τ = φσ−1 and T = T1T2 where T1 is GBBWS on 2(K1) with respect to bijection σ and weight sequence {Bn}nZ, and T2 is GBBWS on 2(K2) with respect to bijection φ and weight sequence {Cn}nZ.

Again by Theorem 4, T1 is similar to BBWS W1 on 2(K1) with weight sequence {Bn}nZ, and T2 is similar to BBWS W2 on 2(K2) with weight sequence {Cn}nZ. So, T1T2 is similar to W1W2. By Theorem 6, W = W1W2 is BBWS on 2(K1K2).

Thus, T is similar to BBWS W on 2(K1K2) with weight sequence {An}nZ. □

Weighted shift operators play a vital role in linear dynamics (refer [4]). Beginning with Kitai [8], several studies have been conducted to determine necessary and sufficient conditions for hypercyclicity of weighted shift operators, refer [9–13]. Very often a weighted shift which is not hypercyclic turns out to be Cesaro-hypercyclic and vice versa, refer [14–16]. With weighted shifts serving as a testing ground for hypercyclicity, it is natural to examine hypercyclic factorization with this class of operators.

In Theorem 2.4 [6], it was shown that if T is a BBWS on 2(C) then there exists GBBWS A and B such that A and B are hypercyclic and T = AB. Using the results from Section 4, we will show that this result by Chan & Sanders [6] can be extended to BBWS of any finite higher multiplicity but with some restrictions on the operator weights. We begin by considering BBWS of multiplicity 2, and for this we consider K=CC. Also for easy reference Theorem 2.4 [6] is stated below.

Theorem 11.

[6] Let 1 ≤ p < . If T:p(Z)p(Z) is a bilateral weighted shift, then there are hypercyclic bilateral weighted shifts A,B:p(Z)p(Z) such that T = AB. Furthermore, for any ϵ > 0, the weighted shifts A and B can be chosen so that their normsA‖, ‖Bare no larger than (1 + ϵ) max{1, ‖T‖}.

Theorem 12.

Let K be a complex Hilbert space of dimension 2 and {An} be a uniformly bounded sequence of invertible diagonal operators on K. If W is BBWS on 2(K) with weight sequence {An}nZ, then there exists hypercyclic GBBWS T and P on 2(K) such that W = TP.

Proof. We consider K = K1K2, where K1=K2=C and An = BnCn where Bn and Cn are non zero scalar multiples of identity operator on C. By Theorem 5, we have W = W1W2 where W1 is BBWS on 2(K1) with weight sequence {Bn}nZ and W2 is BBWS on 2(K2) with weight sequence {Cn}nZ.

Since K1=K2=C so by Theorem 11, there are hypercyclic GBBWS T1, P1 on 2(K1) and T2, P2 on 2(K2) such that W1 = T1P1 and W2 = T2P2. Also for any ϵ > 0, the weighted shifts T1, T2 and P1, P2 can be chosen so that

(2)

For i = 1, 2, let Ti be GBBWS on 2(Ki) with respect to bijection σi and weight sequence {Dn(i)}nZ, and let Pi be GBBWS on 2(Ki) with respect to bijection φi and weight sequence {Qn(i)}nZ. Let τ1=φ1σ11 and τ2=φ2σ21. Also let Dn=Dn(1)Dn(2) and Qn=Qn(1)Qn(2). Then by Theorem 8, T = T1T2 is GBBWS on 2(K1K2) with respect to bijection τ1 and weight sequence {Dn}nZ. Similarly, P = P1P2 is GBBWS on 2(K1K2) with respect to bijection τ2 and weight sequence {Qn}nZ.

First we show that T is hypercyclic. For this let L1 and L2 be BBWS on 2(C) with weight sequence {Dn(1)} and {Dn(2)} respectively. Then by Theorem 4, L1 is similar to T1, and L2 is similar to T2. As mentioned in Ref. [4], hypercyclicity is preserved under similarity, and as T1, T2 are hypercyclic so L1, L2 are also hypercyclic. This together with (1) implies that L1L2 must also be hypercyclic, by [12, Theorem 2.5]. Let L ≔ L1L2. Then L is a hypercyclic BBWS on 2(K) with weight sequence {Dn}. Since by Theorem 10, T is similar to L, so T is also hypercyclic.

By a similar argument it follows that P is hypercyclic.

Claim: (T1T2)(P1P2) = T1P1T2P2.

To establish the claim, let x = yz ∈ 2(K1) ⊕ 2(K2).

Then

Therefore (T1T2)(P1P2) = T1P1T2P2, and the claim is established.

So, we have W = W1W2 = TIP1T2P2 = (T1T2)(P1P2) = TP, where T and P are hypercyclic GBBWS on 2(K). □

Now suppose BBWS W with weight sequence {An} is of multiplicity 3. Then we can consider K = K1K2, where dim(K1) = 1 and dim(K2) = 2. If An = BnCn on K1K2 then we have W = W1W2 where W1, W2 are BBWS on 2(K1) and 2(K2) respectively. We will then have W1 = T1P1 by Theorem 2.4 [6]. We can also apply Theorem 12 and have W2 = T2P2, but for this Cn must be an invertible diagonal operator on K2. In other words, we need to assume that each An is an invertible diagonal operator on K with respect to some common basis. This leads us to the following result:

Theorem 13.

Let K be a separable complex Hilbert space of finite dimension n, and {Ai} be a uniformly bounded sequence of invertible diagonal operators on K. If W is BBWS on 2(K) with weight sequence {Ai} then there exists hypercyclic GBBWS T and P on 2(K) such that W = TP.

Proof. We prove the result by induction on n.

By Theorem 2.4 [6], the result is true for n = 1. Suppose the result is true for n. We will show that it is true for n + 1.

For this we first express K as K = K1K2 where dim(K1) = 1 and dim(K2) = n. Since An is invertible diagonal, we can express An as An = BnCn where Bn, Cn are invertible diagonal operators on K1, K2 respectively. So by Theorem 5, W = W1W2 where W1, W2 are BBWS on 2(K1), 2(K2) with weight sequences {Bn}, {Cn} respectively.

So by our assumption we have W1 = T1P1 and W2 = T2P2 where Ti, Pi are hypercyclic GBBWS on 2(Ki) for each i = 1, 2. Let T ≔ T1T2 and P ≔ P1P2. Then following an argument similar to what was done in Theorem 12, we can conclude that W = TP where T and P are hypercyclic GBBWS on 2(K).

Thus, by induction on n, the conclusion of the theorem follows. □

1.
Rolewicz
 
S
.
On orbits of elements
.
Studia Math
.
1969
;
32
(
1
):
17
-
22
. doi: .
2.
Wu
 
PY
.
Sums and products of cyclic operators
.
Proc Amer Math Soc
.
1994
;
122
(
4
):
1053
-
63
. doi: .
3.
Grivaux
 
S
.
Sums of hypercyclic operators
.
J Funct Anal
.
2003
;
202
(
2
):
486
-
503
. doi: .
4.
Bayert
 
F
,
Matheron
 
E
. Dynamics of linear operators. In:
Cambridge Tracts in Math
,
179
.
Cambridge
:
Cambridge Univ. Press
;
2009
.
5.
Chan
 
KC
,
Sanders
 
R
.
Hypercyclic shift factorizations for unilateral weighted backward shift operators
.
J Oper Theor
.
2018
;
80
(
2
):
349
-
74
.
6.
Chan
 
KC
,
Sanders
 
R
.
Hypercyclic shift factorizations for bilateral weighted shift operators
.
J Oper Theor
.
2021
;
85
(
2
):
323
-
45
. doi: .
7.
Sheilds
 
AL
. Weighted shift operators and analytic function theory. In:
Topics of Operator Theory, Math. Surveys Monographs
,
49–178
.
Providence, RI
:
Amer. Math. Soc.
;
1974
.
8.
Kitai
,
C
.
Invariant closed sets for linear operators
,
Thesis, Univ. of Toronto
.
1982
.
9.
Feldman
 
N
.
Hypercyclicity and supercyclicity for invertible bilateral weighted shifts
.
Proc Amer Math Soc
.
2003
;
131
(
2
):
479
-
85
. doi: .
10.
Hazarika
 
M
,
Arora
 
SC
.
Hypercyclic operator-weighted shifts
.
Bull Korean Math Soc
.
2004
;
41
(
4
):
589
-
98
. doi: .
11.
Liang
 
Y
,
Zhou
 
Z
.
Hereditarily hypercyclicity and supercyclicity of weighted shifts
.
J Korean Math Soc
.
2014
;
51
(
2
):
363
-
82
. doi: .
12.
Salas
 
HN
.
Hypercyclic weighted shifts
.
Trans Amer Math Soc
.
1995
;
347
(
3
):
993
-
1004
. doi: .
13.
Wang
 
Y
,
Zhou
 
Z
.
A note on the hypercyclicity of operator-weighted shifts
.
Ann Funct Anal
.
2018
;
9
(
3
):
322
-
33
. doi: .
14.
Berrag
 
ME
,
Tajmouati
 
A
.
Cesaro-hypercyclic and hypercyclic operators
.
Commun Korean Math Soc
.
2019
;
34
(
2
):
557
-
63
.
15.
Leon-Saavendra
 
F
.
Operators with hypercyclic Cesaro means
.
Stud Math
.
2002
;
152
:
201
-
15
.
16.
Tajmouati
 
A
,
Berrag
 
ME
.
Weyl type theorems for Cesaro-hypercyclic operators
.
Filomat
.
2019
;
33
(
17
):
5639
-
44
. doi: .
Published in the Arab Journal of Mathematical Sciences. Published by Emerald Publishing Limited. This article is published under the Creative Commons Attribution (CC BY 4.0) license. Anyone may reproduce, distribute, translate and create derivative works of this article (for both commercial and non-commercial purposes), subject to full attribution to the original publication and authors. The full terms of this license may be seen at Link to the terms of the CC BY 4.0 licence.

Data & Figures

Figure 1
A diagram showing the action of T on x.The diagram illustrates the action of T on x, with elements x negative 2, x negative 1, x 0, x 1, x 2, x 3, and x 4. Arrows indicate the relationships and flow between these elements.

Action of T on x = (…, x−1, [x0], x1, …)

Figure 1
A diagram showing the action of T on x.The diagram illustrates the action of T on x, with elements x negative 2, x negative 1, x 0, x 1, x 2, x 3, and x 4. Arrows indicate the relationships and flow between these elements.

Action of T on x = (…, x−1, [x0], x1, …)

Close modal
Figure 2
A diagram showing the action of T on x 2(K).A diagram illustrating the action of T on x 2(K). The diagram includes a sequence of elements labeled as x minus 2, x minus 1, x 0, x 1, x 2, x 3, and x 4. Arrows indicate the direction of action or flow between these elements, with x 1 and x 2 having a bidirectional relationship.

Action of T on x  2(K)

Figure 2
A diagram showing the action of T on x 2(K).A diagram illustrating the action of T on x 2(K). The diagram includes a sequence of elements labeled as x minus 2, x minus 1, x 0, x 1, x 2, x 3, and x 4. Arrows indicate the direction of action or flow between these elements, with x 1 and x 2 having a bidirectional relationship.

Action of T on x  2(K)

Close modal

Supplements

References

1.
Rolewicz
 
S
.
On orbits of elements
.
Studia Math
.
1969
;
32
(
1
):
17
-
22
. doi: .
2.
Wu
 
PY
.
Sums and products of cyclic operators
.
Proc Amer Math Soc
.
1994
;
122
(
4
):
1053
-
63
. doi: .
3.
Grivaux
 
S
.
Sums of hypercyclic operators
.
J Funct Anal
.
2003
;
202
(
2
):
486
-
503
. doi: .
4.
Bayert
 
F
,
Matheron
 
E
. Dynamics of linear operators. In:
Cambridge Tracts in Math
,
179
.
Cambridge
:
Cambridge Univ. Press
;
2009
.
5.
Chan
 
KC
,
Sanders
 
R
.
Hypercyclic shift factorizations for unilateral weighted backward shift operators
.
J Oper Theor
.
2018
;
80
(
2
):
349
-
74
.
6.
Chan
 
KC
,
Sanders
 
R
.
Hypercyclic shift factorizations for bilateral weighted shift operators
.
J Oper Theor
.
2021
;
85
(
2
):
323
-
45
. doi: .
7.
Sheilds
 
AL
. Weighted shift operators and analytic function theory. In:
Topics of Operator Theory, Math. Surveys Monographs
,
49–178
.
Providence, RI
:
Amer. Math. Soc.
;
1974
.
8.
Kitai
,
C
.
Invariant closed sets for linear operators
,
Thesis, Univ. of Toronto
.
1982
.
9.
Feldman
 
N
.
Hypercyclicity and supercyclicity for invertible bilateral weighted shifts
.
Proc Amer Math Soc
.
2003
;
131
(
2
):
479
-
85
. doi: .
10.
Hazarika
 
M
,
Arora
 
SC
.
Hypercyclic operator-weighted shifts
.
Bull Korean Math Soc
.
2004
;
41
(
4
):
589
-
98
. doi: .
11.
Liang
 
Y
,
Zhou
 
Z
.
Hereditarily hypercyclicity and supercyclicity of weighted shifts
.
J Korean Math Soc
.
2014
;
51
(
2
):
363
-
82
. doi: .
12.
Salas
 
HN
.
Hypercyclic weighted shifts
.
Trans Amer Math Soc
.
1995
;
347
(
3
):
993
-
1004
. doi: .
13.
Wang
 
Y
,
Zhou
 
Z
.
A note on the hypercyclicity of operator-weighted shifts
.
Ann Funct Anal
.
2018
;
9
(
3
):
322
-
33
. doi: .
14.
Berrag
 
ME
,
Tajmouati
 
A
.
Cesaro-hypercyclic and hypercyclic operators
.
Commun Korean Math Soc
.
2019
;
34
(
2
):
557
-
63
.
15.
Leon-Saavendra
 
F
.
Operators with hypercyclic Cesaro means
.
Stud Math
.
2002
;
152
:
201
-
15
.
16.
Tajmouati
 
A
,
Berrag
 
ME
.
Weyl type theorems for Cesaro-hypercyclic operators
.
Filomat
.
2019
;
33
(
17
):
5639
-
44
. doi: .

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