This paper extends the theory of weighted translation semigroups to multivariable settings, developing analytic models, spectral descriptions, and examples in higher dimensions, generalizing previous one-variable work.
Contribution
It introduces a multivariable generalization of weighted translation semigroups, constructs an analytic model, and explores spectral properties in higher-dimensional spaces.
Findings
01
Developed a toral analogue of the analytic model.
02
Described the spectral picture of multivariable semigroups.
03
Provided numerous examples in multi-variable cases.
Abstract
M. Embry and A. Lambert initiated the study of a weighted translation semigroup {Stβ} in B(L2(R+β)), with a view to explore a continuous analogue of a weighted shift operator. We continued the work, characterized some special types of semigroups and developed an analytic model for the left invertible weighted translation semigroup. The present paper deals with the generalization of the weighted translation semigroup in multi-variable set up. We develop the toral analogue of the analytic model and also describe the spectral picture. We provide many examples of weighted translation semigroups in multi-variable case. Further, we replace the space L2(R+β) by L2(R+dβ) and explore the properties of weighted translation semigroup {StΛβ} in B(L2(R+dβ)), in both one and multi variable cases.
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Topicsadvanced mathematical theories Β· Quantum chaos and dynamical systems Β· Spectral Theory in Mathematical Physics
Full text
Weighted Translation Semigroups: Multivariable Case
M. Embry and A. Lambert initiated the study of a weighted translation semigroup {Stβ} in B(L2(R+β)), with a view to explore a continuous analogue of a weighted shift operator. We continued the work, characterized some special types of semigroups and developed an analytic model for the left invertible weighted translation semigroup. The present paper deals with the generalization of the weighted translation semigroup in multi-variable set up. We develop the toral analogue of the analytic model and also describe the spectral picture. We provide many examples of weighted translation semigroups in multi-variable case. Further, we replace the space L2(R+β) by L2(R+dβ) and explore the properties of weighted translation semigroup {Stβ} in B(L2(R+dβ)), in both one and multi variable cases.
Key words and phrases:
weighted translation semigroup, completely hyperexpansive, analytic, Taylor spectrum
2010 Mathematics Subject Classification:
Primary 47B20, 47B37; Secondary 47A10, 46E22
1. Introduction
The class of weighted shift operators has been systematically studied in [12] and generalized to multivariable set up in [9]. With a view to study a continuous analogue of weighted shifts, M. Embry and A. Lambert initiated the study of a semigroup of operators {Stβ} indexed by a non-negative real number t in [7], [8] and termed it as weighted translation semigroup. The operators Stβ are defined on L2(R+β) by using a weight function.
This work is continued in [10], where we characterized some special types of weighted translation semigroups, especially, hyperexpansive weighted translation semigroups. In [11], we proved that the weighted translation semigroup {Stβ} is analytic and possesses wandering subspace property. Also we proved that a left invertible operator Stβ is modeled as a multiplication by z on a suitable reproducing kernel Hilbert space. It turned out that the spectrum of a left invertible operator Stβ is a closed disc and the point spectrum is empty.
In section 2, we introduce the commuting tuple Stβ whose components are weighted translation semigroups in B(L2(R+β)) and discuss its properties. We present several examples in this section.
In section 3, we prove that the tuple Stβ is analytic and possesses wandering subspace property. We also prove that the tuple Stβ is unitarily equivalent to a commuting operator valued multishift. Further, we describe the toral analytic model for the toral left invertible tuple Stβ. At the end of this section, the Taylor spectrum of the toral left invertible tuple Stβ is discussed.
The major part of the work in section 3 is devoted to the comparison of the commuting d-tuple Stβ under consideration and a multishift SΞ»β on directed cartesian product of rooted directed trees as described in [5]. At the end of this paper, a comparative analysis of these two classes of operator tuples has been summarized.
The techniques used in the proofs of results in section 3 are similar to those in [5]. However, the intrinsic differences in the classes of operators get reflected in the proofs accounting for some subtle differences. In the recent work in [3], S. Chavan developed toral and spherical analytic models for a commuting tuple of operators.
In section 4, we define the weighted translation semigroup {Stβ} in B(L2(R+dβ)) and discuss its properties. In fact, the weighted translation semigroup {Stβ} is a special case where d=1.
In section 5, we introduce the special commuting tuple whose components are weighted translation semigroups in B(L2(R+dβ)) and discuss several properties. In this case, we observe that the symbols of the semigroups under consideration are multi-variable functions. This consideration results in some differences in properties of weighted translation semigroups studied earlier.
2. The Commuting tuple
2.1. Prelude
Let T=(T1β,β―,Tdβ) be a tuple of commuting bounded linear operators Tiβ(1β€iβ€d) on a Hilbert space H. Then Tβ represents (T1ββ,β―,Tdββ) and for p=(p1β,β―,pdβ)βNd,Β Tp denotes T1p1βββ―Tdpdββ.
The open polydisc centered at the origin and of polyradius r=(r1β,β―,rdβ) with r1β,β―,rdβ>0 denoted by Drdβ is
Drdβ:={z=(z1β,β―,zdβ)βCdΒ :Β β£z1ββ£<r1β,β―,β£zdββ£<rdβ}.
The class of completely hyperexpansive operators is explored in [14] and generalised to multi variable set up in [2]. We first recall some definitions useful in the sequel ([1],[4]).
Definition 2.1 :
(1)
A d-tuple S=(S1β,β―,Sdβ) of commuting operators Siβ in B(H) is subnormal if there exist a Hilbert space K containing H and a d-tuple N=(N1β,β―,Ndβ) of commuting normal operators Niβ in B(K) such that NiβHβH and Niββ£H=Siβ for 1β€iβ€d.
2. (2)
Let H1β,β―,Hdβ be commuting operators on H. The tuple (H1β,β―,Hdβ) is called hyponormal if the dΓd operator matrix ([Hjββ,Hiβ])β₯0, where
[TABLE]
3. (3)
A commuting d-tuple Q=(Q1β,β―,Qdβ) of positive operators Q1β,β―,Qdβ in B(H) is called as the generating d-tuple on H.
4. (4)
For a commuting d-tuple T=(T1β,β―,Tdβ) of operators on H, the spherical generating 1-tuple associated with T is given by
[TABLE]
5. (5)
For a fixed integer pβ₯1, the tuple T is said to be spherical p-expansion (resp. spherical p-contraction) if
[TABLE]
where Qs0β(I)=I.
6. (6)
The tuple T is called spherical p-hyperexpansion (resp. spherical p-hypercontraction) if T is a spherical k-expansion (resp. spherical k-contraction) for all k=1,β―,p.
If Bpβ(Qsβ)=0, then T is a spherical p-isometry.
7. (7)
The tuple T is said to be spherical complete hyperexpansion (resp. spherical complete hypercontraction) if T is a spherical p-expansion (resp. spherical p-contraction) for all positive integers p.
8. (8)
Let Qsβ be the spherical generating 1-tuple associated with T. Then T is jointly left-invertible if there exists Ξ±>0 such that Qsβ(I)β₯Ξ±I. Let T be a jointly left-invertible d-tuple of bounded operators on H. The spherical Cauchy dual of T is defined as the d-tuple Ts=(T1sβ,β―,Tdsβ), where Tisβ=Tiβ(Qsβ(I))β1(i=1,β―,d).
9. (9)
Given a commuting d-tuple T=(T1β,β―,Tdβ) on H, a toral generating d-tuple is given by
[TABLE]
10. (10)
Let Qtβ be the toral generating d-tuple associated with T. Then T is toral left-invertible if there exists Ξ±>0 such that Qiβ(I)β₯Ξ±I, for 1β€iβ€d. Let T be a toral left-invertible d-tuple of bounded operators on H. The toral Cauchy dual of T is defined as the d-tuple Tβ²=(T1β²β,β―,Tdβ²β), where Tiβ²β=Tiβ(TiββTiβ)β1(i=1,β―,d).
11. (11)
The tuple T is called toral complete hyperexpansion if
[TABLE]
where Qtqβ(I)=(Q1q1ββββ―βQdqdββ)(I) for q=(q1β,β―,qdβ)βNd.
In definitions (5), (6) and (7), if p=1 then by convention, the prefix 1 is dropped and if m=1 then we drop the term spherical.
We now define the operator Stβ as defined in [10], but in a notation suitable to multi-variable set up.
For a fixed positive integer i, let Οiβ be a measurable, positive function on R+β such that for each fixed tiββR+β, the function Οiβtiββ defined by
[TABLE]
is essentially bounded.
Definition 2.2 :
For a fixed positive integer i and each fixed tiββR+β, we define Siβtiββ on L2(R+β) by
[TABLE]
The family Giβ={Siβtiββ:tiββR+β} in B(L2(R+β)) is a semigroup with Siβ0β=I, the identity operator and for all tiβ,riβΒ βR+β, SiβtiβββSiβriββ=Siβtiβ+riββ. Observe that the family G1βΓβ―ΓGdβ is also a semigroup.
We say that Οiβtiββ is a weight function corresponding to the operator Siβtiββ. Further, the semigroup Giβ={Siβtiββ:tiββR+β} is referred to as the weighted translation semigroup with symbol Οiβ. Throughout this article, we assume that the symbol Οiβ,1β€iβ€d is a continuous function on R+β.
Remark 2.3 :
Consider a tuple of operators (S1βt1ββ,β―,Sdβtdββ).
It can be seen that for 1β€i,jβ€d,
[TABLE]
if and only if
[TABLE]
for all xβ₯tiβ+tjβ.
Observe that if Οiβ=Οjβ, then the operators Siβtiββ and Sjβtjββ commute.
Example 2.4 :
The pair (S1βt1ββ,S2βt2ββ) is commuting for the following symbols:
(1)
Ο1β(x)=c,Β Β Ο2β(x)=ex
2. (2)
Ο1β(x,y)=eβx,Β Β Ο2β(x,y)=ex
Recall that
[TABLE]
Also
[TABLE]
Note that the semigroup G1βΓβ―ΓGdβ is a toral isometry if every commuting d-tuple Stβ=(S1βt1ββ,β―,Sdβtdββ) in G1βΓβ―ΓGdβ is a toral isometry.
Remark 2.5 :
The commuting d-tuple (S1βt1ββ,β―,Sdβtdββ) is a toral isometry if and only if
[TABLE]
This is true if and only if
[TABLE]
Therefore the semigroup G1βΓβ―ΓGdβ is a toral isometry if and only if Οiβ is a constant function for 1β€iβ€d.
Using the characterization of a toral isometry as stated above, we prove that the toral left invertible commuting d-tuple Stβ admits a polar decomposition.
Proposition 2.6**.**
If Stβ=(S1βt1ββ,β―,Sdβtdββ) is a toral left invertible commuting d-tuple, then there exist a toral isometry (U1βt1ββ,β―,Udβtdββ) and a commuting d-tuple (D1βt1ββ,β―,Ddβtdββ) of diagonal, positive, invertible bounded operators on L2(R+β) such that Siβtiββ=UiβtiββDiβtiββ,Β Β Β Β 1β€iβ€d. Further, this decomposition is unique.
Proof.
For a fixed positive integer i,Β 1β€iβ€d, define the operators Uiβtiββ and Diβtiββ on L2(R+β) as follows:
[TABLE]
and
[TABLE]
It can be seen that Siβtiββ=UiβtiββDiβtiββ,Β Β Β Β 1β€iβ€d and this decomposition is unique. β
We now quote the proposition which is useful in constructing examples of spherical hyperexpansion using toral hyperexpansion [4, Proposition 3.7].
Proposition 2.7**.**
Let T=(T1β,β―,Tmβ) be an m-tuple on a Hilbert space H and set S=(T1β/mβ,β―,Tmβ/mβ). If T is a toral complete hyperexpansion (resp. toral p-expansion, toral p-isometry) then S is a spherical complete hyperexpansion (resp. spherical p-expansion, spherical p-isometry).
Note that if T is a complete hyperexpansion (resp. p-isometry) then the m-tuple (T,β―,T) is a toral complete hyperexpansion (resp. toral p-isometry). By Propostion 2.7, (T/mβ,β―,T/mβ) is a spherical complete hyperexpansion (resp. spherical p-isometry).
We here quote proposition useful in constructing hyponormal tuples.
Proposition 2.8**.**
[1, Proposition 3]** Let SβB(H). Then S is subnormal if and only if (I,S,β―,Spβ1) is hyponormal for every pβ₯1.
Example 2.9 :
We here present examples of some special tuples.
(1)
Recall that functions Ο1β(x)=log(x+2),Ο2β(x)=x+1x+Ξ»β(0<Ξ»<1),
Ο3β(x)=2βeβx are completely alternating. Therefore each operator Siβtiββ in a weighted translation semigroup Giβ with symbol Οiβ,Β Β 1β€iβ€3 is completely hyperexpansive. Hence the pair (Siβtiββ,Siβtiββ) is a toral complete hyperexpansion and the pair (Siβtiββ/2β,Siβtiββ/2β) is a spherical complete hyperexpansion for 1β€iβ€3.
2. (2)
Let Ο1β(x)=x+1β. Since the function Ο1β is concave, each operator S1βt1ββ in a weighted translation semigroup G1β with symbol Ο1β is 2-hyperexpansion. Hence the pair (S1βt1ββ,S1βt1ββ) is a toral 2-hyperexpansion and the pair
(S1βt1ββ/2β,S1βt1ββ/2β) is a spherical 2-hyperexpansion.
3. (3)
Observe that each operator Siβtiββ in a weighted translation semigroup Giβ with symbol Οiβ,Β Β 1β€iβ€2 is an isometry, where Ο1β(x)=c,Ο2β(x)=d. Therefore the pair (S1βt1ββ,S2βt2ββ), is a toral isometry and the pair
(S1βt1ββ/2β,S2βt2ββ/2β) is a spherical isometry.
4. (4)
Observe that each operator S1βt1ββ in a weighted translation semigroup G1β with symbol Ο1β(x,y)=x+1 is a 2-isometry. Hence the pair (S1βt1ββ,S1βt1ββ) is a toral 2-isometry and the pair (S1βt1ββ/2β,S1βt1ββ/2β) is a spherical 2-isometry.
5. (5)
Recall that functions Ο1β(x)=x+11β,Ο2β(x)=x+1x+Ξ»β(Ξ»>1),Ο3β(x)=eβx are completely monotone. Therefore each operator Siβtiββ in a weighted translation semigroup Giβ with symbol Οiβ,Β Β 1β€iβ€3 is subnormal contraction. Hence the pair (I,Siβtiββ) is hyponormal.
3. Analytic Model and Taylor Spectrum
In this section, we prove that a commuting d-tuple Stβ=(S1βt1ββ,β―,Sdβtdββ) is analytic and possesses wandering subspace property. Also a toral left invertible commuting d-tuple Stβ is modeled as a multiplication by coordinate functions ziβ on a suitable reproducing kernel Hilbert space.
Recall that the Cauchy dual Stβ²β of a left invertible operator Stβ is given by
[TABLE]
Let Stβ=(S1βt1ββ,β―,Sdβtdββ) be a toral left invertible commuting d-tuple. Then the toral Cauchy dual tuple Stβ²β=(S1βt1ββ²β,β―,Sdβtdββ²β) of Stβ is given by for 1β€iβ€d,
[TABLE]
Note that the toral Cauchy dual d-tuple (S1βt1ββ²β,β―,Sdβtdββ²β) is commuting if and only if the toral left invertible d-tuple (S1βt1ββ,β―,Sdβtdββ) is commuting.
A commuting d-tuple Stβ=(S1βt1ββ,β―,Sdβtdββ) is analytic.
Proof.
Suppose k=(k1β,β―,kdβ)βNd.
For simplicity, we use notation
[TABLE]
Observe that for fβL2(R+β)
[TABLE]
if xβ₯k1βt1β+β―+kdβtdβ and
[TABLE]
Hence
[TABLE]
The result follows from the fact that
[TABLE]
β
The following Lemma follows in similar manner as [11, Lemma 3.5].
Lemma 3.2**.**
Let Stβ=(S1βt1ββ,β―,Sdβtdββ) be a toral left invertible commuting d-tuple in G1βΓβ―ΓGdβ and let E be the joint kernel of Stββ. Then the multisequence {StkβE}kβNdβ is mutually orthogonal.
Remark 3.3 :
Using similar argument, it can be proved that the multisequence {Stβ²βkE}kβNdβ is also mutually orthogonal.
We say that a commuting d-tuple T=(T1β,β―,Tdβ) on a Hilbert space H possesses wandering subspace property if H=[E]Tβ, where E is the joint kernel of Tβ and [E]Tβ=β¨Ξ±βNdβTΞ±E.
The following Proposition follows in similar manner as [11, Proposition 3.4].
Proposition 3.4**.**
A commuting d-tuple Stβ=(S1βt1ββ,β―,Sdβtdββ) in G1βΓβ―ΓGdβ possesses wandering subspace property.
Remark 3.5 :
Using same technique given in the proof of [11, Proposition 3.4], it can be proved that the commuting d-tuple Stβ²β also possesses wandering subspace property.
We first define operator valued multishift.
Let M be a nonzero complex Hilbert space and let lM2β(Nd) denote the Hilbert space of square summable multisequence {hΞ±β}Ξ±βNdβ in M. If {WΞ±(j)β}Ξ±βNdββB(M) for j=1,β―,d, then the linear operator Wjβ in lM2β(Nd) is defined by Wjβ(hΞ±β)Ξ±βNdβ=(kΞ±β)Ξ±βNdβ for (hΞ±β)Ξ±βNdββD, where
[TABLE]
and D:={(hΞ±β)Ξ±βNdββlM2β(Nd)Β :Β (kΞ±β)Ξ±βNdββlM2β(Nd)}.
The d-tuple W=(W1β,β―,Wdβ) is called an operator valued multishift with operator weights {WΞ±(j)βΒ :Β Ξ±βNd,j=1,β―,d}.
The proof of the following proposition follows in a similar way as given in [5, Corollary 4.1.12].
Proposition 3.6**.**
Let Stβ=(S1βt1ββ,β―,Sdβtdββ) be a toral left invertible commuting d-tuple in G1βΓβ―ΓGdβ. Let E be the joint kernel of Stββ. Then Stβ is unitarily equivalent to a commuting operator valued multishift W on lE2β(Nd).
We now define the kernel condition useful in constructing the analytic model.
Definition 3.7 :
Let T=(T1β,β―,Tdβ) be a toral left invertible d-tuple on a Hilbert space H and let E denote the joint kernel of Tβ. Let Tβ² be the toral Cauchy dual of T. We say that T satisfies kernel condition if EβkerTjββTβ²[j]Ξ±β for all j=1,β―,d and for all Ξ±βNd, where, for Ξ±βNd and j=1,β―,d,
[TABLE]
Note that the toral left invertible commuting d-tuple Stβ=(S1βt1ββ,β―,Sdβtdββ) satisfies kernel condition [5, Remark 4.2.3(iii)].
The following theorem is a multivariable analogue of Shimorinβs analytic model developed in [11, Theorem 3.7]. The reader may compare this theorem with [5, Theorem 4.2.4] for a similar model developed in the context of multishifts on directed cartesian product of rooted directed trees.
Theorem 3.8**.**
Let Stβ=(S1βt1ββ,β―,Sdβtdββ) be a toral left invertible commuting d-tuple in G1βΓβ―ΓGdβ. Let E be the joint kernel of Stββ and let
[TABLE]
where r(T) denotes the spectral radius of the bounded operator T. Then there exist a reproducing kernel Hilbert space H of E-valued analytic functions defined on the polydisc Drdβ with center origin and polyradius r and a unitary operator U:L2(R+β)βH such that USjβtjββ=MzjββU for j=1,β―,d.
Proof.
For fβL2(R+β), define
[TABLE]
where P is the orthogonal projection on E. The power series Ufβ converges absolutely on the polydisc Drdβ. Let H denote the complex vector space of E-valued analytic functions of the form Ufβ. We now define a map U:L2(R+β)βH given by U(f)=Ufβ. By definition, U is onto. We now need to show that U is injective.
Let U(f)=Ufβ=0 for some fβL2(R+β). Then βkβNdβ(PStβ²ββkf)zk=0. This implies that PStβ²ββkf=0 for all kβNd. The fact kerΒ Sjβtjββ²ββ=kerΒ Sjβtjβββ, implies that the joint kernel of the tuple Stβ²ββ=E.
By the wandering subspace property of the d-tuple Stβ²β [Remark 4.6], we have βkβNdβStβ²βk=L2(R+β).
By taking orthogonal complement on both sides, we get βkβNdβ(Stβ²βk(E))β₯={0}. Note that (Stβ²βk(E))β₯=kerΒ PStβ²ββk for every kβNd. Thus βkβNdβkerΒ PStβ²ββk={0}. Recall that PStβ²ββkf=0 for all kβNd. Therefore fββkβNdβkerΒ PStβ²ββk. This implies that f=0. Hence U is injective.
Note that by kernel condition, βkβNd,kjβ=0β(PSt[j]β²ββkSjβtjββf)zk=0.
Since the toral Cauchy dual tuple Stβ²β is commuting and Sjβtjββ²ββSjβtjββ=I, the sum on the right hand side of the last step is equal to zjββkβNdβ(PStβ²ββkf)zk=zjβUfβ(z)=MzjββU(f)(z).
Hence USjβtjββ=MzjββU.
We now compute the reproducing kernel for the RKHS H associated to the pair (S1βt1ββ,S2βt2ββ) in some special cases.
(1)
Let Ο1β(x)=a,Ο2β(x)=b. Then the pair (S1βt1ββ,S2βt2ββ) is a toral isometry.
For eβE,Β z,Ξ»βDr2β and xβR+β,
[TABLE]
2. (2)
Let Ο1β(x)=Ο2β(x). For eβE,Β z,Ξ»βDr2β and xβR+β,
[TABLE]
3.1. Taylor Spectrum
For the definition and basic properties of Taylor spectrum, the reader is referred to [6].
Proposition 3.10**.**
Let Stβ=(S1βt1ββ,β―,Sdβtdββ) be a commuting d-tuple in G1βΓβ―ΓGdβ. For every ΞΈβR there exists a unitary operator MΞΈβ on L2(R+β) such that MΞΈββSjβtjββMΞΈβ=eβiΞΈtjβSjβtjββ for j=1,β―,d.
Proof.
For ΞΈβR, define the map MΞΈβ:L2(R+β)βL2(R+β) as
[TABLE]
Then clearly MΞΈβ is a unitary operator. It can be seen that the operator Sjβtjββ is unitarily equivalent to the operator eβiΞΈtjβSjβtjββ.
β
Remark 3.11 :
By the Proposition 3.10, the commuting d-tuples (S1βt1ββ,β―,Sdβtdββ) and (eβiΞΈt1βS1βt1ββ,β―,eβiΞΈtdβSdβtdββ) are unitarily equivalent.
Hence the Taylor spectrum of a commuting d-tuple Stβ has poly-circular symmetry, that is, for any w=(w1β,β―,wdβ)βΟ(Stβ) and z=(z1β,β―,zdβ)βTd,z.w=(z1βw1β,β―,zdβwdβ)βΟ(Stβ). In particular, Ο(Stββ)=Ο(Stβ).
For proving the connectedness of a Taylor spectrum of a commuting d-tuple Stβ, we need a lemma.
Given a positive integer d, we set Hβd:=Hββ―βH (d times). For a commuting d-tuple T=(T1β,β―,Tdβ) of operators on a Hilbert space H, consider the linear transformation DTβΒ :Β HβHβd given by for hβH
Let Stβ=(S1βt1ββ,β―,Sdβtdββ) be a commuting d-tuple. For iβN, let T(i) denote the commuting d-tuple (S1βt1βββi,β―,Sdβtdβββi). Then βͺiβNβkerΒ DT(i)β is dense in L2(R+β).
Proof.
Note that ker DT(i)β=Ο[0,itrβ)βL2(R+β), where trβ=min{t1β,β―,tdβ}.
It is sufficient to prove that βͺiβNβkerΒ DT(i)β contains some orthonormal basis of L2(R+β).
Let {Οjkββ}, where j is an integer and k is a non-negative integer be an orthonormal basis of L2(R+β) as described in [11, Theorem 3.7(iv)]. For fixed j and k, if 2jk+1β<itrβ, then ΟjkβββkerΒ DT(i)β. Therefore each ΟjkβββkerΒ DT(i)β for some non-negative integer i. Hence the orthonormal basis {Οjkββ}ββͺiβNβkerDT(i)β. β
Now proof of the following proposition follows on the lines similar to the proof of [5, Proposition 3.2.4].
Proposition 3.13**.**
The Taylor spectrum of a commuting d-tuple Stβ=(S1βt1ββ,β―,Sdβtdββ) is connected.
Remark 3.14 :
Recall that the point spectrum of each operator Sjβtjββ is empty [11, Proposition 4.3(1)]. This implies that the point spectrum of a commuting d-tuple Stβ is empty.
Remark 3.15 :
Recall that Drdβ is the polydisc with center origin and polyradius r, where r=(r(S1βt1ββ²β)β1,β―,r(Sdβtdββ²β)β1). Note that the polydisc Drdβ is contained in the point spectrum of Stββ for a toral left invertible commuting d-tuple Stβ. The proof of this fact is similar to the proof of [11, Proposition 4.3(2)]. By the poly-circular symmetry of the Taylor spectrum, DrdββΟ(Stβ). Suppose R is the polyradius R=(r(S1βt1ββ),β―,r(Sdβtdββ)). Then by the projection property of the Taylor spectrum, Ο(Stβ)βΟ(S1βt1ββ)Γβ―ΓΟ(Sdβtdββ)=DRdβ. Also the Taylor spectrum of Stβ is connected [Proposition 3.13].
If the commuting d-tuple Stβ is a toral isometry, then r=R=(1,β―,1). In this case, the Taylor spectrum is a polydisc.
3.2. Comparative Analysis
We now summarize the comparative analysis of the commuting d-tuple Stβ under consideration and a multishift SΞ»β on directed cartesian product of rooted directed trees as described in [5].
(1)
The joint kernel of the tuple Stββ is always infinite dimensional but the joint kernel of SΞ»ββ may be finite dimensional [5, Corollary 3.1.16].
2. (2)
The toral Cauchy dual tuple Stβ²β is always commuting but the toral Cauchy dual tuple SΞ»β²β may not be commuting [5, Proposition 5.1.1].
3. (3)
The tuple Stβ admits polar decomposition. However, the multishift SΞ»β admits polar decomposition if and only if the toral Cauchy dual tuple of SΞ»β is commuting [5, Proposition 5.1.1].
4. (4)
The multisequence {StkβE}kβNdβ is mutually orthogonal but, the multisequence {SΞ»kβE}kβNdβ may not be mutually orthogonal.
5. (5)
The toral left invertible commuting d-tuple Stβ satisfies kernel condition but the multishift SΞ»β may not satisfy kernel condition. (refer to paragraph after [5, Remark 4.2.3]).
6. (6)
The Taylor spectrum of the tuple Stβ has poly circular symmetry. However, the operator tuple SΞ»β is strongly circular [5, Proposition 3.2.1].
4. Weighted Translation semigroups in B(L2(R+dβ))
All the properties of the weighted translation semigroup {Stβ} in B(L2(R+β)) proved in [10] and [11], are also shared by the semigroup {Stβ} in B(L2(R+dβ)).
For positive integer d, let L2(R+dβ) denote the Hilbert space of complex valued square integrable Lebesgue measurable functions on R+dβ. Let B(L2(R+dβ)) denote the algebra of bounded linear operators on L2(R+dβ).
Definition 4.1 :
For a measurable, positive function Ο defined on R+dβ and
t=(t1β,β―,tdβ),x=(x1β,β―,xdβ)βR+dβ define the function
Οtβ:R+dββR+β by
[TABLE]
Here, xβt=(x1ββt1β,β―,xdββtdβ).
Suppose that Οtβ is essentially bounded for every tβR+dβ.
Definition 4.2 :
For each fixed tβR+dβ, we define Stβ on L2(R+dβ) by
[TABLE]
Remark 4.3 :
It is easy to see that for every tβR+dβ,Β Stβ is a bounded linear operator on L2(R+dβ) with β₯Stββ₯=β₯Οtββ₯ββ, where β₯Οtββ₯ββ stands for the essential supremum of Οtβ.
The family {Stβ:tβR+dβ} in B(L2(R+dβ)) is a semigroup with S0β=I, the identity operator and for all t,sΒ βR+dβ, StββSsβ=St+sββ. Here, 0 is the d-tuple (0,β―,0) in R+dβ.
We say that Οtβ is a weight function corresponding to the operator Stβ. Further, the semigroup {Stβ:tβR+dβ} is referred to as the weighted translation semigroup with symbol Ο.
Throughout this work, we assume that the symbol Ο is a continuous function on R+dβ.
By similar computations as in the case of an operator Stβ in B(L2(R+β)), it is easy to see that the adjoint of Stβ is given by
[TABLE]
and
[TABLE]
Here, x+t=(x1β+t1β,β―,xdβ+tdβ).
We now present the special types of weighed translation semigroups by choosing some special types of symbols. The characterizations of weighed translation semigroups in this case are similar to those as described in [10, Corollary 3.3].
Example 4.4 :
Let {Stβ} be a weighted translation semigroup with symbol Ο.
(1)
Let Ο1β(x,y)=e(x+y),Ο2β(x,y)=exyβ.
All these functions are log convex. Thus the semigroups {Stβ} corresponding to symbols Οiβ,i=1,2 are hyponormal.
2. (2)
Let Ο1β(x,y)=2xβyβx2+2xyβy2+1,Ο2β(x,y)=Axayb+1(A>0,a,bβ₯0,a+bβ€1).
All these functions are concave. Thus the semigroups {Stβ} corresponding to symbols Οiβ,i=1,2 are 2-hyperexpansive.
3. (3)
The semigroup {Stβ} is an m-isometry if Ο is a polynomial of degree mβ1.
4. (4)
Let Ο1β(x,y)=log(x+y+2),Ο2β(x,y)=(x+1)(y+1)β,Ο3β(x,y)=x+y+1.
All these functions are completely alternating.
Thus the semigroups {Stβ} corresponding to symbols Οiβ,i=1,2,3 are completely hyperexpansive.
5. (5)
Let Ο1β(x,y)=x+y+11β,Β Ο2β(x,y)=x+y+1β1β,Β Ο3β(x,y)=eβ(x+y). All these functions are completely monotone. Thus the semigroups {Stβ} corresponding to symbols Οiβ,i=1,2,3 are subnormal contractions.
6. (6)
Let Ο1β(x,y)=yex+xey+1,Ο2β(x,y)=exy.
All these functions are absolutely monotone.
Thus the semigroups {Stβ} corresponding to symbols Οiβ,i=1,2 are alternatingly hyperexpansive.
7. (7)
Let Ο(x,y)=x+y+1x+y+Ξ»β,Β Ξ»β₯0.
Then βxk1ββyk2ββnΟβ=(x+y+1)n+1(1βΞ»)(β1)nβ1n!β, where
n=k1β+k2β.
If 0<Ξ»<1, then Ο is a completely alternating function and the semigroup {Stβ} is completely hyperexpansive.
If Ξ»>1, then Ο is a completely monotone function and the semigroup {Stβ} is a subnormal contraction.
We now describe the kernel of the adjoint Stββ, for tξ =0.
Lemma 4.5**.**
For tξ =0, ker Stββ=E=Ο[0,t1β)Γβ―Γ[0,tdβ)βL2(R+dβ). In particular, ker Stββ is infinite dimensional.
Remark 4.6 :
The following properties of Stβ are analogues of the corresponding properties of Stβ. Let tξ =0.
(1)
An operator Stβ is analytic.
2. (2)
An operator Stβ possesses wandering subspace property.
3. (3)
A left invertible operator Stβ possesses an analytic model.
4. (4)
A left invertible operator Stβ is an operator valued weighted shift.
5. (5)
The spectrum of a left invertible operator Stβ is a disc and the point spectrum is empty.
5. The Special Tuple
We now define a tuple of a special type. Recall that a commuting d-tuple Stβ defined in Section 2, is a toral isometry if and only if each symbol Οiβ,
1β€iβ€d is a constant function [Remark 2.5]. However, in the special case, defined below we do have non-constant functions as symbols for a commuting tuple which is a toral isometry.
Let Οiβ be a measurable, positive function on R+dβ such that for each fixed tiββR+β, the function Οiβtiββ defined by
[TABLE]
is essentially bounded.
Definition 5.1 :
For each fixed tiββR+β, we define Siβtiββ on L2(R+dβ) by
[TABLE]
Remark 5.2 :
It is easy to see that for every tiββR+β,Β Siβtiββ is a bounded linear operator on L2(R+dβ) with β₯Siβtiβββ₯=β₯Οiβtiβββ₯ββ, where β₯Οiβtiβββ₯ββ stands for the essential supremum of Οiβtiββ.
The family Giβ={Siβtiββ:tiββR+β} in B(L2(R+dβ)) is a semigroup with Siβ0β=I, the identity operator. Note that the family G1βΓβ―ΓGdβ is also a semigroup.
We say that Οiβtiββ is a weight function corresponding to the operator Siβtiββ. Further, the semigroup Giβ={Siβtiββ:tiββR+β} is referred to as the weighted translation semigroup with symbol Οiβ. Throughout this work, we assume that the symbol Οiβ,1β€iβ€d is a continuous function on R+dβ.
Remark 5.3 :
Observe that Siβtiββ=Stβ, where t=(0,β―,0,tiβ,0,β―,0). Here, the ith component of the d-tuple t is tiβ and all other entries are zero.
Therefore by Remark 4.6, each operator Siβtiββ is analytic and possesses wandering subspace property. Also the spectrum of each left invertible operator Siβtiββ is a closed disc and the point spectrum is empty.
Consider a tuple (S1βt1ββ,β―,Sdβtdββ)βG1βΓβ―ΓGdβ.
It is easy to see that for 1β€i,jβ€d,
[TABLE]
if and only if
[TABLE]
[TABLE]
for all xiββ₯tiβ,xjββ₯tjβ.
Note that if Οiβ=Οjβ, then above condition is satisfied.
Example 5.4 :
Let b,c,Ξ» be positive real numbers. The pair (S1βt1ββ,S2βt2ββ) is commuting for the following symbols:
We say that the semigroup G1βΓβ―ΓGdβ is a toral isometry if every commuting d-tuple (S1βt1ββ,β―,Sdβtdββ) in G1βΓβ―ΓGdβ is a toral isometry.
Remark 5.5 :
The commuting d-tuple (S1βt1ββ,β―,Sdβtdββ) is a toral isometry if and only if
[TABLE]
A simple calculation reveals that this condition holds if and only if
[TABLE]
Therefore the semigroup G1βΓβ―ΓGdβ is a toral isometry if and only if
[TABLE]
But this condition holds if and only if Οiβ is independent of xiβ for 1β€iβ€d.
Remark 5.6 :
The toral left invertible commuting d-tuple (S1βt1ββ,β―,Sdβtdββ) also admits polar decomposition as given in the Proposition 2.6.
We now turn our attention towards constructing examples of different classes of operator tuples. The definitions of classes of operator tuples under consideration are given in Section 2. We use Proposition 2.7 to construct following examples.
Example 5.7 :
(1)
The functions Ο1β(x,y)=x+y+1β,Ο1β(x,y)=log(x+y+2),
Ο1β(x,y)=x+y+1x+y+Ξ»β(0<Ξ»<1) are completely alternating. Therefore each weighted translation semigroup S1βt1ββ with symbol Ο1β is completely hyperexpansive. Hence each pair (S1βt1ββ,S1βt1ββ) is a toral complete hyperexpansion and the pair (S1βt1ββ/2β,S1βt1ββ/2β) is a spherical complete hyperexpansion.
2. (2)
The pair (S1βt1ββ,S2βt2ββ), where Ο1β(x,y)=y+1,Ο2β(x,y)=x+1 is a toral isometry. Then the pair (S1βt1ββ/2β,S2βt2ββ/2β) is a spherical isometry.
3. (3)
The pair (S1βt1ββ,S2βt2ββ), where Ο1β(x,y)=c,Ο2β(x,y)=x+1 is a toral 2-isometry. Then the pair (S1βt1ββ/2β,S2βt2ββ/2β) is a spherical 2-isometry.
4. (4)
The weighted translation semigroup corresponding to the symbol
Ο1β(x,y)=x+y+1 is 2-isometry. Hence the pair (S1βt1ββ,S1βt1ββ) is a toral 2-isometry and the pair (S1βt1ββ/2β,S1βt1ββ/2β) is a spherical 2-isometry.
We here quote a proposition useful in constructing hyponormal tuples.
Proposition 5.8**.**
[1, Remark 7]** If H1β,β―,HmββB(H),Β Β HiββHjβ=HjββHiβ for iξ =j and each Hiβ is hyponormal, then the tuple (H1β,β―,Hmβ) is hyponormal.
Note that the above proposition is not useful to construct hyponormal tuples of the type Stβ defined in Section 2.
Consider the pair (S1βt1ββ,S2βt2ββ). It is easy to see that
[TABLE]
if and only if
[TABLE]
and
[TABLE]
if and only if
[TABLE]
Example 5.9 :
We now construct examples of hyponormal tuples.
(1)
Let b,c be positive real numbers. The pair (S1βt1ββ,S2βt2ββ) is hyponormal for the following pair of functions:
(a)
Ο1β(x,y)=c,Β Β Ο2β(x,y)=b
2. (b)
Ο1β(x,y)=ex,Β Β Ο2β(x,y)=ey
3. (c)
Ο1β(x,y)=c,Β Β Ο2β(x,y)=ex+y
4. (d)
Ο1β(x,y)=eβxβy,Β Β Ο2β(x,y)=ex+y
5. (e)
Ο1β(x,y)=eβy,Β Β Ο2β(x,y)=eβx
2. (2)
The functions Ο1β(x,y)=eβ(x+y),Ο1β(x,y)=x+y+11β are completely monotone. Therefore each weighted translation semigroup S1βt1ββ with symbol Ο1β is subnormal. Hence by Proposition 2.8, each tuple (I,S1βt1ββ,S1βt1β2β,β―,S1βt1βpβ1β),
pβ₯1 is hyponormal.
Using similar techniques as discussed in Section 3, the toral analytic model for the special tuple can be constructed. Further, the properties of Taylor spectrum are similar.
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