Spectral properties of block Jacobi matrices
Grzegorz \'Swiderski

TL;DR
This paper investigates the spectral characteristics of block Jacobi matrices with operator entries, providing conditions for continuous spectra, asymptotic behaviors of eigenvectors, and criteria for indeterminacy.
Contribution
It introduces new conditions for the spectrum to be continuous and analyzes eigenvector asymptotics for block Jacobi matrices with operator entries.
Findings
Conditions for continuous spectrum established
Asymptotic behavior of eigenvectors characterized
Criteria for spectral indeterminacy provided
Abstract
We study the spectral properties of bounded and unbounded Jacobi matrices whose entries are bounded operators on a complex Hilbert space. In particular, we formulate conditions assuring that the spectrum of the studied operators is continuous. Uniform asymptotics of generalised eigenvectors and conditions implying complete indeterminacy are also provided.
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Spectral properties of block Jacobi matrices
Grzegorz Świderski
Instytut Matematyczny
Uniwersytet Wrocławski
Pl. Grunwaldzki 2/4
50-384 Wrocław
Poland
Abstract.
We study the spectral properties of bounded and unbounded Jacobi matrices whose entries are bounded operators on a complex Hilbert space. In particular, we formulate conditions assuring that the spectrum of the studied operators is continuous. Uniform asymptotics of generalised eigenvectors and conditions implying complete indeterminacy are also provided.
Key words and phrases:
Block Jacobi matrix, asymptotics of generalised eigenvectors, total variation
2010 Mathematics Subject Classification:
Primary: 47B25, 47B36, 42C05.
1. Introduction
Let be a complex Hilbert space. Consider two sequences and of bounded linear operators on such that for every the operator has a bounded inverse and is self-adjoint. Then one defines the symmetric tridiagonal matrix by the formula111By we denote the adjoint operator to .
[TABLE]
The action of on any sequence of elements from is defined by the formal matrix multiplication. Let the operator be the minimal operator associated with . Specifically, by we mean the closure in of the restriction of to the set of the sequences of finite support. Let us recall that
[TABLE]
The operator is called a block Jacobi matrix. It is self-adjoint provided the Carleman condition is satisfied, i.e.
[TABLE]
where is the operator norm (see [2, Theorem VII-2.9]).
Block Jacobi matrices are related to such topics as: matrix orthogonal polynomials (see [8]), the matrix moment problem (see [13]), difference equations of finite order (see [10]), partial difference equations (see [2]), level dependent quasi-birth–death processes (see [9] and references therein). For further applications we refer to [20, 25].
The theory of block Jacobi matrices is much less developed than the scalar ones, i.e. corresponding to . The aim of this paper is to provide extensions of results obtained in [26, 28] for to the case of arbitrary . It is of interest as we provide new results even for with , i.e. the most common (apart from ) studied case.
Originally, we were interested in the unbounded case, i.e.
[TABLE]
But it seems that even the bounded case is not well understood (see [19, 23]). Therefore, we present a unified treatment of both bounded and unbounded cases. In the unbounded case the formulation of our results is simpler.
In the proofs of the presenting theorems we will use the following notion. A non-zero sequence will be called a generalised eigenvector associated with if it satisfies the recurrence relation
[TABLE]
In Section 3 we show the correspondence between asymptotic behaviour of generalised eigenvectors and the spectral properties of .
The first main result of this article is Theorem 4, which generalises the results obtained in [26] to the operator case. Its formulation involves an additional parameter sequence . In Section 5 we present some of the possible choices of . The following Theorem is a special case of Theorem 4 (obtained for ).
Theorem 1**.**
Assume
[TABLE]
and222For a self-adjoint operator we define by the spectral theorem.
- (a)
** 2. (b)
** 3. (c)
**
Then the operator is self-adjoint. Moreover333By we denote spectrum of the operator , whereas is the set of its eigenvalues., and provided
[TABLE]
where is invertible.
Before we formulate the next result we need a definition. Given a positive integer , we define the total -variation of a sequence of vectors x=\big{(}x_{n}:n\geq 0\big{)} from a vector space by
[TABLE]
Observe that if has a finite total -variation then for each a subsequence is a Cauchy sequence.
The following Theorem is interesting even for . Since recently block periodic Jacobi matrices have obtained some attention (see [7, 19]) we formulate it for an arbitrary natural number .
Theorem 2**.**
Let be an integer. Assume
[TABLE]
Let
- (a)
** 2. (b)
** 3. (c)
** 4. (d)
**
for -periodic sequences , , and with invertible. Let be the set of such that444 The real part of the operator is defined by .
[TABLE]
is a strictly positive or a strictly negative operator on . Then for every compact set there are positive constants such that for every generalised eigenvector associated with and every
[TABLE]
When the Carleman condition is satisfied, the asymptotics (2) implies the similar conclusion as Theorem 1, i.e. and . In the scalar case the subordination theory (see, e.g., [6]) implies that in fact the spectrum of is purely absolutely continuous on . Unfortunately, a subordination theory for the non-scalar case has not been formulated (but there is some progress, see [5]). We expect that in our case the spectrum of is, similarly to the scalar case, purely absolutely continuous of the maximal multiplicity on .
It is also of interest to obtain a characterization when the symmetric operator is not self-adjoint (see, e.g., [12, 29]). The following Theorem shows that in the setting of Theorem 2 the Carleman condition is also necessary to the self-adjointness of .
Theorem 3**.**
Let the assumptions of Theorem 2 be satisfied with . If (1) is not satisfied, then the conclusion of Theorem 2 holds for . Consequently, for every
[TABLE]
Hence, we have the so-called complete indeterminate case. In particular, the symmetric operator is not self-adjoint but it has self-adjoint extensions.
The estimate implied by Theorem 3 is useful even in the scalar case (see [3]).
The method of the proofs of the presented theorems is based on an extension of the techniques used in [26] and [28]. In these articles one examines the positivity or the convergence of sequences of quadratic forms on acting on the vector of two consecutive values of a generalised eigenvector associated with , i.e.
[TABLE]
for a suitably chosen sequence , . In trying to extend this method one encounters several difficulties.
First of all, what is the right quadratic form for the operator case? One real number should control the norm of generalised eigenvectors, which unlike the scalar case, need not to be real. Moreover, the convergence (or at least positivity) should be easily expressible in terms of the recurrence relation. What additionally complicates the matter is the fact that in general the parameters and , unlike the scalars, are not commuting with each other. The second one need not to be even symmetric. Moreover, because of the fact that the Hilbert space can be arbitrary, we cannot assume that it is locally compact. This complicates the analysis of the proposed quadratic forms.
The second issue concerns the problem how one can express quantitatively the rate of divergence or deviation from the positivity of the parameters. As simple examples of diagonal and show, the divergence of the norms is too coarse. The scaling from Theorem 2(d) seems to be a natural one. However, there are also different possibilities known in the literature (see [11]).
The article is organized as follows. In Section 2 we present basic notions needed in the rest of the article. In Section 3 we define generalised eigenvectors and prove the correspondence of their asymptotic behaviour with the spectral properties of . In Section 4 we prove Theorem 4. Next, in Section 5, we present its special cases. In particular, the choice of the parameter sequence motivates us to define the notion of -shifted Turán determinants in Section 6. Section 6 is devoted to the proof of Theorems 2 and 3. In Section 7 we present the situations when one can compute exact asymptotics of . In the scalar case it has applications to the so-called Christoffel functions. Finally, in Section 8 we present some examples illustrating the sharpness of the assumptions.
2. Preliminaries
In this section we collect some basic notations and properties, which will be needed in the sequel.
2.1. Operators
On the space of bounded operators we consider only the norm topology. In particular, a sequence converges to provided
[TABLE]
where is the operator norm.
For a sequence of operators and we set
[TABLE]
For any bounded operator we define its real part by
[TABLE]
Direct computation shows that for any bounded operator one has
[TABLE]
and
[TABLE]
Moreover,
[TABLE]
For a number we define its negative part by the formula
[TABLE]
For a self-adjoint operator we define by the spectral theorem.
For any bounded operator we define its absolute value by
[TABLE]
2.2. Total variation
Given a positive integer , we define the total -variation of a sequence of vectors x=\big{(}x_{n}:n\in\mathbb{N}\big{)} from a vector space by
[TABLE]
Observe that if has a finite total -variation then for each a subsequence is a Cauchy sequence.
Proposition 1**.**
If is a normed algebra, then
[TABLE]
Proof.
Observe
[TABLE]
Hence,
[TABLE]
Consequently,
[TABLE]
Summing by the result follows. ∎
3. generalised eigenvectors and the transfer matrix
For a number , a non-zero sequence will be called a generalised eigenvector provided that it satisfies
[TABLE]
For each non-zero there is a unique generalised eigenvector such that555We employ the following notation: . . If the recurrence relation (6) holds also for , with the convention that , then is a formal eigenvector of the matrix associated with .
For each and we define the transfer matrix by
[TABLE]
Then for any generalised eigenvector corresponding to we have
[TABLE]
It is easy to verify that
[TABLE]
The rest of this section concerns relations between generalised eigenvectors and spectral properties of block Jacobi matrices.
The proof of [1, Lemma 2.1] implies that the adjoint operator to can be described as the restriction of to , i.e. for , where
[TABLE]
The following Proposition is essential in examining properties of .
Proposition 2**.**
Let . The sequence satisfies if and only if
[TABLE]
Proof.
It immediately follows from the direct computations. ∎
The following Corollary describes some of the situations when we can describe the deficiency spaces of the operator explicitly.
Corollary 1**.**
Let . If every generalised eigenvector associated with belongs to , then
[TABLE]
In particular, if (12) is satisfied for , then the symmetric operator is not self-adjoint, but it has self-adjoint extensions.
Proof.
Observe that the space is a Hilbert space. Indeed, since (see, e.g., [24, formula (7.1.45)]) it is a closed subspace of .
Define the operator by . Then by (11) implies , hence, is injective. To prove the surjectivity take , then the sequence defined by (11) is a generalised eigenvector associated with . Therefore, it belongs to . Hence, by (10) , and consequently, is surjective. Since the mapping is a contraction, it is a bounded linear bijection. By the inverse mapping theorem the operator is a linear isomorphism.
The assertion about the self-adjoint extensions of follows from von Neumann’s Extension Theorem (see, e.g., [24, Theorem 7.4.1]). ∎
Remark 1*.*
The proof of [21, Theorem 1] shows that the same conclusion holds if every generalised eigenvector associated with belongs to . As it was pointed out in [4] the formulation of [21, Theorem 1] has a typo.
The following Proposition is an adaptation of [26, Proposition 2.1]. We include it for the sake of self-containment.
Proposition 3**.**
Let . If every generalised eigenvector associated with does not belong to then and .
Proof.
Let be such that , then by Proposition 2 is a generalised eigenvector associated with . By the assumption . Therefore, , and consequently, .
Observe that the vector such that , where has to satisfy the following recurrence relation
[TABLE]
Hence is a generalised eigenvector, thus . Therefore, , and consequently, the operator is not surjective, i.e. . ∎
Remark 2*.*
In the scalar case, if the assumptions of Proposition 3 are satisfied for , then the operator is self-adjoint. We expect the same behaviour for every .
4. A commutator approach
The aim of this Section is to prove the following Theorem.
Theorem 4**.**
Let be a Jacobi matrix. Assume that there is a sequence of elements from such that
- (a)
** 2. (b)
** 3. (c)
** 4. (d)
**
Let be the set of such that the following limit exists in the norm and defines a strictly positive operator on
[TABLE]
Then and .
Given sequence of elements from and we define a sequence of binary quadratic forms on by the formula
[TABLE]
Moreover, we define the sequence of functions by the formula
[TABLE]
where is the generalised eigenvector corresponding to such that .
The first proposition provides a different representation of .
Proposition 4**.**
An alternative formula for is
[TABLE]
Proof.
By (8) one has
[TABLE]
Then formula (9) implies
[TABLE]
Hence, by formula (3)
[TABLE]
what ends the proof. ∎
The next proposition provides assumptions on the quadratic form under which it controls the norm of generalised eigenvectors.
Proposition 5**.**
Let be the set of such that the following limit exists in the operator norm and defines a strictly positive operator
[TABLE]
Then for every there is an integer and positive constants such that for every generalised eigenvector associated with and
[TABLE]
Proof.
Fix . Let
[TABLE]
where
[TABLE]
Hence,
[TABLE]
But from the definition of we have
[TABLE]
which are positive numbers. Therefore, there is and such that for every
[TABLE]
and the proof is complete. ∎
The next corollary together with Proposition 3 suggest the method of proving that every is not an eigenvalue of but belongs to .
Corollary 2**.**
Under the assumptions of Proposition 5, together with
[TABLE]
if
[TABLE]
then does not belong to .
Proof.
By Proposition 5
[TABLE]
for a positive constant . Therefore, there exists a constant such that
[TABLE]
which cannot be summable. ∎
The following Lemma is the main algebraic part of the proof of Theorem 4.
Lemma 1**.**
Let be a generalised eigenvector associated with and . Then
[TABLE]
Proof.
By Proposition 4 and formula (13) we have
[TABLE]
for
[TABLE]
Hence,
[TABLE]
By the Schwarz inequality the result follows. ∎
We are ready to prove Theorem 4.
Proof of Theorem 4.
By virtue of Corollary 2 and Proposition 3 it is enough to show that for every and a non-zero .
Fix and a non-zero . By Proposition 5 there exists such that for every holds . Let us define
[TABLE]
Then
[TABLE]
and consequently,
[TABLE]
Hence,
[TABLE]
implies . By Proposition 5
[TABLE]
for some constant . Hence, by Lemma 1
[TABLE]
which is summable by assumptions (a), (b) and (c). This shows (14). The proof is complete. ∎
5. Special cases of Theorem 4
In this section we show several choices of the sequence . In this way we show the flexibility of our approach. For the simplification of the condition for we assume that the sequence tends to infinity, i.e.
[TABLE]
This condition implies that does not depend on .
The first theorem is an extension of [18, Theorem 1.6] to the operator case. Since Section 6 is devoted to the proof of a far reaching extension of this result, we omit the details.
Theorem 5**.**
Assume
- (a)
** 2. (b)
** 3. (c)
** 4. (d)
**
and defined for is a positive operator on . Then the assumptions of Theorem 4 are satisfied.
We are ready to prove Theorem 1. Let us note that this result is a vector valued version of [26, Theorem 4.3]. In the scalar case it has far reaching applications (see [26, Section 5]).
Proof of Theorem 1.
Take . It is sufficient to show that . We have
[TABLE]
which is clearly positive for . Hence, . ∎
To formulate the last example we need a definition. Let
[TABLE]
and
[TABLE]
The following Theorem is a vector valued version of [26, Theorem 4.3] and its proof is inspired by the techniques employed in the proof of [17, Theorem 3].
Theorem 6**.**
Assume that for positive integers and a non-negative summable sequence
- (a)
** 2. (b)
* for ,* 3. (c)
the sequence is bounded and 4. (d)
**
Then the assumptions of Theorem 4 are satisfied with .
Proof.
We can assume that . Let
[TABLE]
We have to compute the set and check the assumptions (a), (b), (c) of Theorem 4.
Let us begin with the computation of . We have
[TABLE]
which by the hypotheses (a) and (b) tends to
[TABLE]
which is clearly a positive operator on for any . Hence, .
Let us show the assumption (a). We have
[TABLE]
The above expression has been estimated in the proof of [26, Theorem 4.3].
Next, since
[TABLE]
the hypothesis (c) implies that the assumption (b) will be satisfied if we show that the assumption (c) holds.
We have
[TABLE]
where
[TABLE]
By virtue of the hypothesis (d), the assumption (c) will be satisfied as long as
[TABLE]
for a constant and a non-negative summable sequence . Because
[TABLE]
the non-negativity of and , the inequality (16) will be satisfied if
[TABLE]
The spectral theorem applied to implies that the above inequality will be satisfied if
[TABLE]
for every , which by the hypothesis (b) corresponds to
[TABLE]
But
[TABLE]
and the above expression has been estimated in the proof of [26, Theorem 4.3]. This shows (17) and ends the proof. ∎
6. Turán determinants
Let us note that for the expression for (see (13)) is known as the -shifted Turán determinant (see [14]). Hence, Theorem 5 motivates us to the following construction. Fix a positive integer and a Jacobi matrix . Let us define a sequence of quadratic forms on by the formula
[TABLE]
where
[TABLE]
Then we define the -shifted Turán determinants by
[TABLE]
where is the generalised eigenvector corresponding to such that .
The rest of this section is devoted to the analysis of the sequence . Since the proof of the uniform convergence of is quite involved, we divide it into 3 subsections. The method used here is an adaptation of the techniques employed in [28].
6.1. Almost uniform non-degeneracy
Let be a subset of . In this section we consider the family defined in (18).
We say that is uniformly non-degenerated on if there are and such that for all , and
[TABLE]
We say that is almost uniformly non-degenerated on if it is uniformly non-degenerated on each compact subset of .
We begin with two simple auxiliary results which will be needed in the proof of the non-degeneracy of the considered quadratic forms.
Lemma 2**.**
For every and one has
[TABLE]
Proof.
Using (9) and (7) one can compute that both sides are equal to
[TABLE]
and the result follows. ∎
Proposition 6**.**
Let be an integer. Assume
- (a)
** 2. (b)
**
for -periodic sequences of invertible operators and . Then
[TABLE]
In particular,
[TABLE]
for a positive -periodic sequence
[TABLE]
Proof.
We have
[TABLE]
Hence,
[TABLE]
and the result follows. ∎
In the next proposition we examine the limiting behaviour of the considered quadratic forms.
Proposition 7**.**
Let be an integer. Assume
- (a)
** 2. (b)
** 3. (c)
** 4. (d)
**
for -periodic sequences and such that for every the operators and are invertible. Then on every compact subset of the sequence is uniformly bounded. Moreover,
[TABLE]
uniformly on compact subsets of , where
[TABLE]
Proof.
Let us define
[TABLE]
We have
[TABLE]
which tends to [math] uniformly on compact subsets of . Consequently, since every function is continuous, one has
[TABLE]
uniformly on the compact subsets of . In particular, it implies (20) and the uniform boundedness of on every compact subset of . ∎
Finally, in the last proposition, we formulate the conditions under which the sequence is almost uniformly non-degenerated.
Proposition 8**.**
Let the assumptions of Proposition 7 be satisfied. If for every and every there is such that
[TABLE]
then is almost uniformly non-degenerated. Moreover, if , then the same conclusion follows provided (21) holds only for .
Proof.
By (20) and (21) we have that for every compact there is a constant such that for sufficiently large and all
[TABLE]
It implies the uniform non-degeneracy of .
Consider . According to Lemma 2 we have
[TABLE]
Let and let us compute the limit of both sides as tends to . By Propositions 6 and 7 we have
[TABLE]
where
[TABLE]
and the convergence is uniform on every compact subset of . By (3) it implies that if for some
[TABLE]
then for every
[TABLE]
The proof is complete. ∎
6.2. Asymptotics of generalised eigenvectors
This section is devoted to show the implications of the non-degeneracy of together with the positivity of to the asymptotics of the generalised eigenvectors.
Theorem 7**.**
Let the family defined in (18) be uniformly non-degenerated on a compact set . Suppose that there are and such that for all such that , and
[TABLE]
Then there is such that for all , and for every generalised eigenvector corresponding to
[TABLE]
Proof.
Let and let be a generalised eigenvector corresponding to such that , . Since is uniformly non-degenerated, there are and such that for all
[TABLE]
which together with (22) implies that there is such that for all
[TABLE]
For the general non-zero we use the fact that
[TABLE]
and generalised eigenvectors depend linearly on the initial conditions. ∎
Corollary 3**.**
Suppose that the assumptions of Theorem 7 are satisfied. Let be a bounded closed set and let be a compact set. Assume that for -periodic sequence of self-adjoint operators
[TABLE]
uniformly on and
[TABLE]
uniformly on . Then
[TABLE]
uniformly on .
Proof.
Fix . By (23) there is such that for all , and
[TABLE]
Hence,
[TABLE]
uniformly on . By Theorem 7 there is a constant such that
[TABLE]
uniformly on . The proof is complete. ∎
6.3. The proof of the convergence
In this section we are going to prove that the sequence is convergent, which leads to the proofs of Theorem 2 and 3.
Let us begin with the main algebraic part of the proof.
Lemma 3**.**
Let be a generalised eigenvector associated with and . Then
[TABLE]
Proof.
The formula (8) implies
[TABLE]
Therefore, by the formulas (3) and (4)
[TABLE]
where
[TABLE]
By using , we can write
[TABLE]
Hence,
[TABLE]
Now we can compute
[TABLE]
Therefore,
[TABLE]
In particular we can estimate
[TABLE]
Therefore, by the last inequality together with (24), Schwarz inequality and (5) the result follows. ∎
The main result of this section is the following theorem.
Theorem 8**.**
Assume that for an integer
- (a)
\begin{aligned} \mathcal{V}_{N}\bigg{(}a_{n}^{-1}:n\geq 0\bigg{)}+\mathcal{V}_{N}\bigg{(}a_{n}^{-1}b_{n}:n\geq 0\bigg{)}+\mathcal{V}_{N}\bigg{(}a_{n}^{-1}a_{n-1}^{*}:n\geq 1\bigg{)}<\infty;\end{aligned}** 2. (b)
* for a constant and all ;* 3. (c)
the family defined in (18) \begin{aligned} \big{\{}Q^{z}:z\in K\big{\}}\end{aligned} is uniformly non-degenerated on a compact connected set .
Then there is such that for every , for all and for every generalised eigenvector corresponding to we have
[TABLE]
Moreover, if
[TABLE]
then the same conclusion holds for .
Proof.
Let be a connected bounded closed set. Let be a sequence of functions defined by (19). In view of Theorem 7, it is enough to show that there are and such that
[TABLE]
for all , and . The study of the sequence is motivated by the method developed in [28].
Given a generalised eigenvector corresponding to such that , we can easily see that for each , considered as a function of and , is continuous on . As a consequence, the function is continuous on . Since is uniformly non-degenerated, there is such that for each the function has no zeros and has the same sign for all and . Otherwise, by the connectedness of , there would be and such that , which would contradict the non-degeneracy of .
Next, we define a sequence of functions on by setting
[TABLE]
Then
[TABLE]
First of all, let us show that
[TABLE]
for a constant independent of and . If it is the case, then by (27) and the fact that each function is continuous, to conclude (26) it is enough to show that the product
[TABLE]
converges uniformly on to a limit that is bounded away from [math], which will be satisfied if we prove that
[TABLE]
Let us observe that by (19) and (5)
[TABLE]
Moreover, by (8)
[TABLE]
for
[TABLE]
Hence,
[TABLE]
For every the function is continuous on the compact set . Hence, it is uniformly bounded. Furthermore, by the boundedness of one has that is bounded as well. It shows that the right-hand side of (33) is uniformly bounded on . Similarly,
[TABLE]
is uniformly bounded. It implies that the right-hand side of (30) is uniformly bounded as well. Thus, the upper bound in the inequality (28) is proved. To prove the lower bound, let us see that the uniform non-degeneracy implies
[TABLE]
for a constant independent of and . So by (31) it remains to show that is a strictly positive operator uniformly with respect to . It will be implied by the uniform bound on . According to (32)
[TABLE]
and by (9), as in (33), the right-hand side of this inequality is uniformly bounded on . Hence, by (31) there is a constant such that
[TABLE]
Consequently, by the positive distance of to [math] and (34), we proved the remaining lower bound in (28).
It remains to prove (29). Let be a generalised eigenvector corresponding to such that . In view of (a), each subsequence is uniformly convergent, and consequently, the norms are uniformly bounded with respect to and . Moreover, since is uniformly non-degenerated
[TABLE]
for . Therefore, by Lemma 3
[TABLE]
for every . Using (b), we can estimate
[TABLE]
Thus, (a) and (25) implies (26). If condition (25) is not satisfied consider instead in the last inequality. The proof is complete. ∎
The following Corollary provides an estimate, which in the scalar case expresses the bound on the rate of the convergence of Turán determinants to the density of the spectral measure of (see [27]). It follows from the standard proof of the convergence of infinite products of numbers.
Corollary 4**.**
Under the hypothesis of Theorem 8, for every bounded and closed the sequence of continuous functions converges uniformly on (or on if (25) is satisfied) to the function bounded away from [math]. Moreover, by (35) there is a constant such that for all
[TABLE]
Finally, we are ready to prove Theorems 2 and 3.
Proof of Theorem 2.
By Propositions 6 and 8 we have that the assumptions of Theorem 8 are satisfied. Therefore, the result follows from Theorem 7. ∎
Proof of Theorem 3.
Since every is invertible, we have
[TABLE]
Hence, for some
[TABLE]
Consequently,
[TABLE]
and (25) is satisfied. Moreover, it implies that so, in the notation of Proposition 7, every is constant. Hence, Proposition 8 implies the almost uniform non-degeneracy of . Since is constant on Proposition 8 implies that is almost uniformly non-degenerated as well. Thus, the assumptions of Theorem 8 are satisfied, and consequently, Theorem 7 implies the requested asymptotics. Finally, Corollary 1 finishes the proof. ∎
7. Exact asymptotics of generalised eigenvectors
The following Theorem is a vector valued version of [27, Corollary 1].
Theorem 9**.**
Let be a bounded and closed set and let (or whether the Carleman condition is not satisfied) be a compact set. Let be an odd integer. Let the hypotheses of Theorem 2 be satisfied. Assume further that
[TABLE]
Then and
[TABLE]
uniformly on , where
[TABLE]
for defined in (19).
Proof.
We have
[TABLE]
Hence,
[TABLE]
Consequently,
[TABLE]
Therefore, by Proposition 6 for . It implies that . Taking norms we obtain , and consequently, . Moreover, by Corollary 4, is a continuous function on which is bounded away from [math]. Hence, by Corollary 3 the result follows. ∎
In the scalar case, and under stronger assumptions, the similar results were obtained in [16]. To obtain the complete information of the asymptotics it is of interest to identify the function . In the scalar case is related to the density of the spectral measure of (see [27, Corollary 1]).
The following Corollary is an extension of [27, Corollary 3] to the operator case. In the scalar case it provides exact asymptotics of the so-called Christoffel functions, which have applications, e.g. in random matrix theory (see [22]) or signal processing (see [15]). We believe that in the operator case it will also have some applications.
Corollary 5**.**
Let the assumptions of Theorem 9 be satisfied. Assume further that
[TABLE]
Then
[TABLE]
uniformly on , where
[TABLE]
for defined in (19).
Proof.
By Stolz–Cesàro theorem (also known as L’Hôpital’s rule for sequences)
[TABLE]
Theorem 9 implies that , and consequently, Proposition 6 shows that tends to . Therefore, by Theorem 9 the result follows. ∎
8. Examples
8.1. Examples to Theorem 4
In this section we show examples to the special cases of Theorem 4 presented in Section 5, i.e. to Theorems 1 and 6. Since Theorem 5 is a weaker version of Theorem 2, the examples to it are postponed to the next section.
Example 1*.*
Assume that and are bounded non-commuting operators on such that is invertible normal and is self-adjoint. Let
[TABLE]
Denote
[TABLE]
i.e. the th repetition of and . We define in the block form
[TABLE]
Then for
[TABLE]
the assumptions of Theorem 1 are satisfied.
Proof.
We have
[TABLE]
which by the monotonicity of and normality of is positive. Hence, the hypothesis (a) is satisfied.
Next, one has . Therefore, by
[TABLE]
we obtain the hypothesis (c).
Finally,
[TABLE]
and by the fact that tends to , the hypothesis (b) is will be satisfied if is summable. But
[TABLE]
and the result follows. ∎
Example 2*.*
Let be an integer and be such that (see (15)). Assume that and are bounded non-commuting self-adjoint operators on such that is invertible. Let
[TABLE]
for
[TABLE]
Then the assumptions of Theorem 6 are satisfied.
Proof.
The hypotheses (a) and (d) from Theorem 6 are straightforward.
Since is self-adjoint
[TABLE]
Therefore, by [26, Example 4.5] the hypothesis (b) is satisfied.
It remains to show the hypothesis (c). We have
[TABLE]
Since tends to it remains to show that is summable. But
[TABLE]
which by the Cauchy condensation test applied times is summable. The proof is complete. ∎
8.2. Examples to Theorems 2 and 3
The following Proposition provides a simple way of the construction of sequences satisfying the bounded variation condition of Theorem 2.
Proposition 9**.**
Fix and a Hilbert space . Let and be sequences of numbers such that , and
[TABLE]
Let and be -periodic sequences of bounded operators on such that for every each is invertible and each is self-adjoint. Let us define
[TABLE]
Then
[TABLE]
Proof.
We have
[TABLE]
Therefore, it is enough to apply Proposition 1. ∎
The next Proposition provides a convenient form of for .
Proposition 10**.**
Assume
- (a)
, 2. (b)
, 3. (c)
, 4. (d)
.
Then, in the notation of Theorem 2
[TABLE]
Proof.
Since
[TABLE]
we have
[TABLE]
Hence, the direct computation shows that has the requested form. ∎
In the following Example we discuss the optimality of in the case of constant coefficients.
Example 3*.*
Let
[TABLE]
Then the assumptions of Theorem 2 are satisfied with
[TABLE]
Moreover, is the maximal set where has absolutely continuous spectrum of the multiplicity .
Proof.
Let
[TABLE]
Since and are constant it is sufficient to show that matrix is positive definite for .
According to Proposition 10 we have
[TABLE]
The determinants of its principal minors are equal to
[TABLE]
Hence, the matrix is positively definite whether . Moreover, the determinant of the last minor is negative only for .
According to [30, Theorem 3] the matrix is purely absolutely continuous on the closure of the set . Moreover, the spectrum of is of multiplicity and on and , respectively. ∎
In the next Example we consider the unbounded case for .
Example 4*.*
Let
[TABLE]
Let us assume that real sequences and such that and for every satisfy
[TABLE]
and
[TABLE]
For example: for .
Then for
[TABLE]
the assumptions of Theorem 2 are satisfied.
Proof.
In view of Proposition 9 it is enough to show that is positive definite. In the notation of Proposition 10
[TABLE]
Hence, by Proposition 10
[TABLE]
The determinants of the principal minors of this matrix are equal to
[TABLE]
Hence, this matrix is positive definite if and only if
[TABLE]
∎
Acknowledgements
I would like to thank Bartosz Trojan, Ryszard Szwarc and an anonymous referee for some helpful suggestions.
The reference list from the paper itself. Each links out to its DOI / PubMed record.
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