Orthogonality of quasi-orthogonal polynomials
Cleonice F. Bracciali, Francisco Marcell\'an, Serhan Varma

TL;DR
This paper characterizes when quasi-orthogonal polynomials, formed as linear combinations of orthogonal polynomials, are themselves orthogonal, and explores implications for quadrature rules and numerical integration.
Contribution
It provides necessary and sufficient conditions for quasi-orthogonal polynomials to be orthogonal, solving an inverse problem and deriving recurrence relations for their coefficients.
Findings
Derived explicit recurrence formulas for coefficients of quasi-orthogonal polynomials.
Established conditions under which quasi-orthogonal polynomials are orthogonal.
Connected these results to various quadrature rules and provided illustrative examples.
Abstract
A result of P\'olya states that every sequence of quadrature formulas with nodes and positive numbers converges to the integral of a continuous function provided for a space of algebraic polynomials of certain degree that depends on . The classical case when the algebraic degree of precision is the highest possible is well-known and the quadrature formulas are the Gaussian ones whose nodes coincide with the zeros of the corresponding orthogonal polynomials and the numbers are expressed in terms of the so-called kernel polynomials. In many cases it is reasonable to relax the requirement for the highest possible degree of precision in order to gain the possibility to either approximate integrals of more specific continuous functions that contain a polynomial factor or to include additional fixed nodes. The construction of such quadrature processes…
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ORTHOGONALITY OF QUASI-ORTHOGONAL POLYNOMIALS
Cleonice F. Bracciali
Departamento de Matemática Aplicada
UNESP-Univ Estadual Paulista
São José do Rio Preto, SP
Brazil
,
Francisco Marcellán
Departamento de Matemáticas
Universidad Carlos III de Madrid
Leganés
Spain
and Instituto de Ciencias Matemáticas (ICMAT)
Cantoblanco
Spain
and
Serhan Varma
Department of Mathematics, Faculty of Science
Ankara University
Tandoğan
Ankara
Turkey
Abstract.
A result of Pólya states that every sequence of quadrature formulas with nodes and positive numbers converges to the integral of a continuous function provided for a space of algebraic polynomials of certain degree that depends on . The classical case when the algebraic degree of precision is the highest possible is well-known and the quadrature formulas are the Gaussian ones whose nodes coincide with the zeros of the corresponding orthogonal polynomials and the numbers are expressed in terms of the so-called kernel polynomials. In many cases it is reasonable to relax the requirement for the highest possible degree of precision in order to gain the possibility to either approximate integrals of more specific continuous functions that contain a polynomial factor or to include additional fixed nodes. The construction of such quadrature processes is related to quasi-orthogonal polynomials. Given a sequence of monic orthogonal polynomials and a fixed integer , we establish necessary and sufficient conditions so that the quasi-orthogonal polynomials defined by
[TABLE]
with , and for , also constitute a sequence of orthogonal polynomials. Therefore we solve the inverse problem for linearly related orthogonal polynomials. The characterization turns out to be equivalent to some nice recurrence formulas for the coefficients . We employ these results to establish explicit relations between various types of quadrature rules from the above relations. A number of illustrative examples are provided.
Key words and phrases:
Orthogonal polynomials, quasi-orthogonal polynomials, positive quadrature formulas, Gaussian quadrature formulas, Christoffel numbers, inverse problems.
2010 Mathematics Subject Classification:
33C45; 42C05
Research supported by the Brazilian Science Foundation CAPES under project number CSF/PVE 107/2012. The work of the author (CFB) has also been supported by Brazilian Science Foundation CNPq, grants 305208/2015-2 and 402939/2016-6. The work of the author (FM) has also been supported by Ministerio de Economía y Competitividad of Spain, grant MTM 2015-65888-C4-2-P.
1. Introduction
Some results obtained during the early development of the theory of orthogonal polynomials were motivated by the desire to build quadrature formulas with positive Christoffel numbers whose nodes are zeros of known polynomials. Nowadays these quadratures are succinctly denominated as positive quadrature formulas. The study of this kind of problems was inspired by the Gauss’ theorem on quadrature with the highest algebraic degree of precision with nodes at the zeros of the polynomials orthogonal with respect to the measure of integration as well as by the result of Pólya [38] on convergence of quadrature rules. This led Riesz, Fejér and Shohat to search for the properties of certain linear combinations of orthogonal polynomials and the further developments resulted in deep outcome. The most convincing example is the Askey and Gasper [7, 8] proof of the positivity of certain sums of Jacobi polynomials which played a key role in the final stage of de Branges’ proof of the Bieberbach conjecture. We refer to the nice survey of Askey [6] for the motivation to study positive Jacobi polynomial sums, coming from positive quadratures, and for further information about these natural connections.
The construction of positive quadrature rules is connected with the so-called quasi-orthogonal polynomials. Let be a given sequence of monic orthogonal polynomials, generated by the three-term recurrence relation
[TABLE]
with and Then, given , the polynomials defined by
[TABLE]
are said to be a sequence of quasi-orthogonal polynomials of order or, simply, -quasi-orthogonal polynomials if . Here for , are real numbers. By convention we set , , when , and also when and . Notice that for we have the standard orthogonality. This notion was introduced by Riesz while studying the moment problem and the reason for this nomenclature is rather simple: is orthogonal to every polynomial of degree not exceeding with respect to the functional of orthogonality of . M. Riesz himself considered only the case while Fejér [22] concentrated his attention on the specific case when , are the Legendre polynomials and . It seems that Shohat [41] was the first who studied the general case. The renewed recent interest on the quasi-orthogonal polynomials brought a large number of interesting results. Peherstorfer [34, 35, 36] and Xu [44] obtained results concerning the location of the zeros of the quasi-orthogonal polynomials and the positivity of the Christoffel numbers when are orthogonal on with respect to a measure that belongs to Szegő’s class. Xu [45] established general properties of quasi-orthogonal polynomials and, under the assumption that is also orthogonal, studied the relation between the Jacobi matrices associated with both sequences. The zeros of some quasi-orthogonal polynomials were studied recently by Beardon and Driver [9] and Brezinski, Driver and Redivo-Zaglia [12].
Motivated by the relation between positive quadrature rules and quasi-orthogonal polynomials, we provide necessary and sufficient conditions in order that the sequence of polynomials , obeying (1.2), is also orthogonal. The latter problem is purely algebraic in nature. We solve it via a constructive approach by taking into account classical results on Sturm sequences. It becomes evident then that one may look at the solution in terms of a relation between the Jacobi matrices associated with the sequences of orthogonal polynomials. As a result the solution is explicit in the sense that we establish the connection between the three term recurrence relations that generate the sequences and as well as between the linear functionals related to them. These results allow us to judge about the nodes of two Gaussian type quadrature formulas whose location coincides with the zeros of the polynomials and . Moreover, the Christoffel numbers of the quadrature rules are obtained explicitly as a consequence of the closed forms of the corresponding kernel polynomials which are also derived from our general approach.
The structure of the paper is as follows. In Section 2 we state the necessary and sufficient conditions of the orthogonality of a sequence of quasi-orthogonal polynomials of order as well as the expression of the polynomial associated with the Geronimus transformation of the initial linear functional. In Section 3, the proofs of those theorems are given as well as an algorithm to deduce the sequence of connection coefficients. Section 4 is focussed on the relation between the corresponding Jacobi matrices. Thus, we have a computational approach to the zeros of since they are the eigenvalues of the th principal leading submatrices of the corresponding Jacobi matrix. The Christoffel numbers are their normalized eigenvectors. We also prove some results concerning the zeros of the polynomial as well as the expression of the kernel polynomials in terms of the initial ones. In Section 5 we analyze some examples illustrating the problems considered in the previous sections. First, the case when is a symmetric linear functional is considered. The results are implemented for Chebyshev polynomials of the second kind. Second, the non-symmetric case is studied and implemented for Laguerre polynomials. Finally, we study the case of constant coefficients. In such a case, we solve a problem posed in [3] for in such a way in a symmetric case, periodic sequences for the parameters of the three term recurrence relation appear.
2. Orthogonality of quasi-orthogonal polynomials
The characterization of those quasi-orthogonal polynomials (1.2) which form a sequence of orthogonal polynomials themselves can be approached from a general point of view. Let be the linear space of algebraic polynomials with complex coefficients. Then denotes the action of the linear functional over the polynomial where denotes the algebraic dual of the linear space . The sequence of monic orthogonal polynomials (SMOP) with respect to the linear functional obeys the conditions , where for all , and is the Kronecker delta. A linear functional is said to be regular or quasi-definite (see [16]) when the leading principal submatrices of the Hankel matrix composed by the moments , , are non-singular for each . When the determinants of are positive for all nonnegative integers the functional is called positive-definite. If the linear functional is regular, then the SMOP satisfies the three-term recurrence relation (1.1) with and if is positive-definite then . Conversely, if a sequence of polynomials is generated by the recurrence relation (1.1) and , then there is a linear functional , such that is a sequence of polynomials orthogonal with respect to and this is the statement of Favard’s theorem ([16]). Moreover, if for every then the linear functional is positive-definite and it has an integral representation , , where is a positive Borel measure supported on an infinite subset of (see [16]).
The linear functional is called a rational perturbation of , if there exist polynomials and , such that
[TABLE]
Detailed information about the direct problems studied from several points of view can be found in [2, 13, 23, 30, 46]. In particular, the connection formula between the polynomials orthogonal with respect to and is called the generalised Christoffel’s formula (see [23]). The relation between the corresponding Jacobi matrices was studied in [20].
Let be a SMOP, and are positive integers. Let consider another sequence of monic polynomials related to by
[TABLE]
with , . Then the problem to find necessary and sufficient conditions so that is also a SMOP and to obtain the relation between the corresponding regular linear functionals is called an inverse problem. Observe that we adopt the convention that when either or is equal to one, then the corresponding sum does not appear, that is, we interpret it as an empty one. A vast number of interesting results have been obtained on topics related to the inverse problem (see [1, 3, 4, 5, 10, 11, 25, 26, 32, 37]).
In the present contribution we also focus our attention on the quasi-orthogonal polynomials defined by (1.2) under the only natural restriction and for . This corresponds to a very general situation when we set and in (2.1). Therefore, in what follows we consider this setting. Many particular results, when one looks for the relation between the functionals and , with respect to which the polynomial sequences and are orthogonal, are known [13, 15, 18, 19, 29, 46] but the general case that we discuss in the present contribution has not been approached in the literature yet. In this paper we provide necessary and sufficient conditions so that the sequence of monic polynomials is also orthogonal.
Let be a SMOP corresponding to a regular linear functional . Now we give the necessary and sufficient conditions ensuring the orthogonality of the monic polynomial sequence that satisfies the three-term recurrence relation
[TABLE]
with the initial conditions and , and the condition , for .
Theorem 2.1**.**
Let be a sequence of monic polynomials defined by . Then is a SMOP with recurrence coefficients and if and only if the coefficients , , , satisfy the following conditions
[TABLE]
[TABLE]
[TABLE]
and
[TABLE]
for and .
Moreover, the recurrence coefficients of are given by
[TABLE]
and the coefficients also satisfy
[TABLE]
The above relations provide a complete characterization of the orthogonality of the polynomial sequence . When you recover Theorem 1 in [3].
On the other hand, a natural question arises about the relation between the regular linear functionals and such that and are the corresponding SMOP. In this case, the functional which describes the orthogonality of the sequence is a Geronimus spectral transformation of degree of the linear functional . In other words, , where is a polynomial of degree (see [32]). Our next result furnishes a method to determine .
Theorem 2.2**.**
The coefficients of the polynomial
[TABLE]
such that , are the unique solution of a system of linear equations, where the entries of the corresponding matrix depend only on the sequences of connection coefficients , .
A detailed description of the linear system and about the explicit form of the coefficients will be done in the sequel.
It is worth pointing out that an alternative way to compute the coefficients of is via a relation between the Jacobi matrices related to the sequences and . We discuss this method in Section 4.
Since the quasi-orthogonal polynomials arise naturally in the context of quadrature formulae of Gaussian type, many properties that can be classified more than as analytic rather than algebraic, such as the behaviour of their zeros and the positivity of the Christoffel numbers have been analysed. Most of these results deal with rather specific particular cases when either is a small integer or the orthogonal polynomials belong to classical families. In Section 4.2 we obtain some results about the zeros of the polynomials and .
Many illustrative examples are analysed when the linear functional is a symmetric one, as well as when one deals with constant connection coefficients. The latter problem is motivated by a result in [24] where is the sequence of Chebyshev polynomials.
3. Proofs of Theorems 2.1 and 2.2 and the direct problem
3.1. Proof of Theorem 2.1
The core of the overall approach is a classical result of Sturm [42] on counting the number of real zeros of an algebraic polynomial. We refer to [39, Section 10.5] and [33, Sections 2.4, 2.5] for detailed information about various versions of Sturm’s result as well as about the historical background. We state the general version of Sturm’s theorem in the setting we need. Let and be polynomials of exact degree and , respectively, with monic leading coefficients. Execute the Euclidean algorithm
[TABLE]
A careful inspection of the general version of Sturm’s theorem shows that the following holds:
Theorem A*.*
(Sturm)
Under the above assumptions, the polynomials and have real and strictly interlacing zeros if and only if are positive real numbers. Furthermore, the zeros of the polynomial are all real and the zeros of two consecutive polynomials are strictly interlacing.
It follows immediately from Theorem A and Favard’s theorem that, given two polynomials and with positive leading coefficients and with real and strictly interlacing zeros, the Euclidean algorithm (3.1) generates the sequence , , such that these are the first terms of a sequence of orthogonal polynomials, which can be constructed by using the standard three term recurrence relation. In other words, any two polynomials of consecutive degrees and interlacing zeros may be “embedded” in a sequence of orthogonal polynomials. This straightforward but beautiful observation was pointed out by Wendroff [43] and the statement is nowadays called Wendroff’s theorem. Observe that and generate , uniquely “backwards” via (3.1) while the sequence , of all the polynomials can be extended “forward” in various ways. The complete characterization of the sequences of orthogonal polynomials and that are related by the relation (1.2) is obtained via Theorem A.
Proof of Theorem 2.1.
Applying the Euclidean algorithm (3.1) with “initial” polynomials and and setting , we obtain
[TABLE]
where is a polynomial of degree at most . Using (1.2) together with the recurrence relation (1.1) we conclude that
[TABLE]
where and . Moreover, when , we have for all .
Now we can determine necessary and sufficient conditions in order to the polynomial coincides with the polynomial , i.e.,
[TABLE]
Comparing the coefficients that multiply and in (3.2) and (3.3) we derive the conditions
[TABLE]
and the latter obviously correspond to (2.6) and (2.7). This means that
[TABLE]
Since , we obtain the constraint
[TABLE]
which is exactly (2.2).
Similarly, comparing the coefficients of in (3.2) and (3.3), we obtain the following conditions:
[TABLE]
and
[TABLE]
Now (2.3) follows from (3.6) and (3.7) while (2.4) is a consequence of (3.4) and (3.7). Finally, (3.4) and (3.5) imply (2.5).
It is important to check that at the last step the coefficient must be different from zero in order to be consistent with the quasi-orthogonality condition. This completes the proof.
Theorem 2.1 provides also a forward algorithm to compute the coefficients for . Starting with coefficients , from the linear combination
[TABLE]
we choose the coefficients for and write
[TABLE]
Then we compute , for , using equation (2.3) and , , , and (see the first scheme in Fig. 1). We compute , for , using equation (2.4) and , , , and (see the second scheme in Fig. 1).
We compute , for and , using equation (2.5) and , , , , and also , , , and . This is illustrated as the first scheme in Fig. 2. Alternatively, , for and , is given by
[TABLE]
using , , , , and also , , , , (see the second scheme in Fig. 2).
As we have pointed out above, after the computations at level , it is necessary to verify if , for .
The initial coefficients , , for , starting from and , are uniquely determined by the “backward” process described by the Euclidean algorithm and by Theorem A.
Let us notice the key role played by the connection coefficients for the polynomials and as initial data to run the above algorithm.
As a summary, you can generate the coefficients of quasi-orthogonal polynomials in a recursive way, assuming some initial conditions.
3.2. Proof of Theorem 2.2
The dual basis of is defined, as usual, by the conditions (see [31])
[TABLE]
It is easy to see that the elements of the basis, dual to SMOP with respect to the regular linear functional , are . Let us define the left-multiplication of a linear functional by any polynomial via
[TABLE]
Let , given by relation , be a SMOP with respect to a regular linear functional . According to [31], if we use the expansion of the linear functional in terms of the dual basis of the SMOP , in view of orthogonality properties and relation , we obtain the following relation between the corresponding linear functionals.
Lemma 3.1**.**
[TABLE]
where is a polynomial of degree because its leading coefficient is
Proof of Theorem 2.2
For we have
[TABLE]
For , we obtain
[TABLE]
Since, for
[TABLE]
assuming and using (1.2), we derive
[TABLE]
Now we write the equations (3.2) as a system of linear equations where
[TABLE]
[TABLE]
The latter can be rewritten in the form
[TABLE]
Using the backward technique for solution of systems of linear equations, we obtain, for ,
[TABLE]
In order to simplify (3.10), let be the tridiagonal matrix corresponding to the SMOP , that is,
[TABLE]
where and
[TABLE]
Notice that, for and we have
[TABLE]
where denotes the entry of the matrix . Then the equalities
[TABLE]
hold for .
Now it is clear that the inner products , , can be expressed in terms of the coefficients , , and from the value of . Indeed, we rewrite (1.2) in the form
[TABLE]
which implies
[TABLE]
for , so that
[TABLE]
Using equations (3.12), for and including the equation we obtain the following system of equations:
[TABLE]
Let us denote by the matrix of the latter system. Then the solution , , is obtained in terms of the coefficients , , and .
Replacing the solution of (3.30) into (3.2) we conclude that
[TABLE]
where is the inverse of the matrix . Finally we solve the system (3.10) and find all coefficients of the polynomial as functions of and Thus, Theorem 2.2 is proved.
The above result shows that the sequences , , defined in Theorem 2.1 must satisfy the constraints on the coefficients of the polynomial given in Theorem 2. In other words, the sequences , together with the coefficients of the three term recurrence relation, determine uniquely the polynomial . Moreover, since the matrix is nonsingular, any polynomial of the form (2.9) determines uniquely the coefficients , for . We discuss this question thoroughly in the next section.
Notice that the latter observations provide not only an algorithm to calculate , but also an alternative proof about the relation between the Geronimus transformation and the quasi-orthogonal polynomials.
It is easy to see from (3.10) that the leading coefficient of is given, in an alternatively way, by
[TABLE]
Considering and the normalization , we obtain
[TABLE]
where are given by .
The second coefficient of can also be obtained in an explicit form. Indeed, it follows from (3.10) that
[TABLE]
Now (3.2), with and , yields
[TABLE]
Since
[TABLE]
then Therefore (3.33) becomes
[TABLE]
Then (3.32) implies
[TABLE]
The computations of the remaining coefficients of are rather involved and yield extremely complex explicit expressions so that we omit them.
Remark 3.1*.*
Notice that the above result shows that you can find a direct relation between the coefficients of the polynomial the connection coefficients of the sequences and and the coefficients of the three term recurrence relation of the sequence .
4. Gaussian type quadrature formulas
4.1. An interpretation in terms of Jacobi matrices
In this section we provide an alternative approach to the above problems based on the matrix form of the three-term recurrence relations as well as of the connection coefficients between the two sequences of polynomials. Let and be the tridiagonal matrices corresponding to the SMOP and , respectively. Then the three-term recurrence relations satisfied by the SMOP and are equivalent to
[TABLE]
where and .
On the other hand, reads as
[TABLE]
where is a banded lower triangular matrix with entries and , . Combining and we obtain
[TABLE]
and then
[TABLE]
These represent a succinct matrix form of the relations obtained in Theorem 2.1.
On the other hand, Christoffel formula [23] is equivalent to
[TABLE]
where is a banded upper triangular matrix with entries , , , and , where is the polynomial defined in (3.8).
Substituting (4.1) and (4.2) into (4.4), we obtain
[TABLE]
where is a diagonal matrix of size . It is clear that the matrix is uniquely determined from . Since equalities (4.3) and (4.5) yield
[TABLE]
the matrix can be determined from (4.6). Notice that (4.6) is the factorization of the matrix while is a UL factorization of the matrix .
We also describe relations between the corresponding finite dimensional tridiagonal matrices which appear in the three-term recurrence relations (4.1) as well as on (4.2). If and , then (4.1) and (4.2) reduce to
[TABLE]
where denotes the leading principal submatrix of size of the corresponding infinite one, while here and in what follows, is the -th vector of the canonical basis in with all entries zeros except for the -th one, which is one. Replacing (4.9) and (1.2) in (4.8) yields
[TABLE]
Having in mind (4.7), the latter simplifies to
[TABLE]
Thus, we obtain
[TABLE]
This result means that is a rank-one perturbation of the matrix .
Remark 4.1*.*
The particular cases , and of the above matrix method are considered in [13], and [29], respectively.
Remark 4.2*.*
Having in mind that the zeros of the polynomial are the eigenvalues of the matrix , the above expression means that they are the eigenvalues of a rank one perturbation of the matrix . Therefore, one may estimate them using the classical theory of eigenvalue perturbations (see [45]). On the other hand, the corresponding Christoffel numbers are the first component of the normalized eigenvector associated with each eigenvalue.
4.2. Results on the zeros of orthogonal polynomials
In this section we discuss some properties of these zeros and of their location with respect to those of provided that both and are sequences of orthogonal polynomials and they are related by (1.2).
In order to obtain inequalities for the number of zeros of which are greater than the largest zero of we need a theorem on Descartes rule of signs for orthogonal polynomials due to Obrechkoff. Given a finite sequence of real numbers, let be the number of its sign changes. Recall that is counted in the following natural way. First we discard the zero entries from the sequence and then count a sign change if two consecutive terms in the remaining sequence have opposite signs. By we denote the number of the zeros, counting their multiplicities, of the function in .
Definition 4.1**.**
The sequence of functions obeys the general Descartes’ rule of signs in the interval if the number of zeros in , where the multiple zeros are counted with their multiplicities, of any real nonzero linear combination
[TABLE]
does not exceed the number of sign changes in the sequence .
More precisely, this property states that
[TABLE]
for any .
Theorem B* (Obrechkoff [33]).*
If the sequence of polynomials is defined by the recurrence relation
[TABLE]
with and , where , and denotes the largest zero of , then the sequence of polynomials obeys Descartes’ rule of signs in .
Since, by Favard’s theorem [21], the requirements on in Theorem B are equivalent to the fact that is a sequence of orthogonal polynomials, we obtain
Corollary 4.1**.**
Suppose that the orthogonal polynomials , be normalized in such a way that their leading coefficients are all of the same sign and let be the largest zero of . Then, for any set of real numbers , which are not identically zero, we get
[TABLE]
Some applications of Theorem B and Corollary 4.1 to zeros of orthogonal polynomials were discussed in [17]
Now we are ready to formulate a result concerning inequalities for largest zeros of the polynomials .
Theorem 4.1**.**
Let be a sequence of monic orthogonal polynomials and let be defined by (1.2). If the zeros of are , then
[TABLE]
Despite that in this paper we are interested in the situation when is another sequence of orthogonal polynomials, the above result about the largest zeros of does not depend on the fact that the sequence of polynomials obeys an orthogonality property or not.
Corollary 4.2**.**
If the zeros of are also real and simple, denoted by and , then
[TABLE]
In particular independently of the signs of for . Moreover, if for , then which means that all zeros of precede .
Finally, we obtain a relation between the Stieltjes functions of and Indeed, let define
[TABLE]
where and .
Since then , and
[TABLE]
Therefore, where is a polynomial of degree at most , and
[TABLE]
Since the Stieltjes function is a linear spectral modification of ([46]), assuming that is a positive definite linear functional and is a positive polynomial on the support of a positive Borel measure associated with , it is well known (see [27] and [28]) that for large enough each zero of with multiplicity attracts zeros of . On the other hand, for every fixed , at most zeros of can lie outside . These facts allow us to judge about the location of the zeros of that lie outside the support of .
4.3. Kernel polynomials and Christoffel numbers
In [14] quadrature formulas on the real line with the highest degree of accuracy, with positive weights, and with one or two prescribed nodes anywhere on the interval of integration are characterized. Next we will consider a more general problem when we deal with more prescribed nodes. We are interested in the study of Christoffel numbers assuming they are positive numbers, i.e. by choosing those nodes outside the interval of orthogonality of the initial measure.
Let and be the kernel polynomials associated with the positive definite linear functionals and , respectively, i.e.
[TABLE]
where and
First of all, we will find an algebraic relation between and .
Writing as
[TABLE]
we get
[TABLE]
If then From the reproducing property of the kernel polynomial we get
[TABLE]
On the other hand,
[TABLE]
[TABLE]
Finally,
[TABLE]
In other words,
[TABLE]
where
[TABLE]
[TABLE]
[TABLE]
and
[TABLE]
By setting we get
[TABLE]
If we commute the variables in (4.10),
[TABLE]
since the kernel polynomials are symmetric with respect to the variables, then subtracting (4.11) from (4.10), we get
[TABLE]
Substituting (4.12) in (4.10) we obtain
[TABLE]
In particular, the confluent formula holds
[TABLE]
or, alternatively from (4.10)
[TABLE]
On the other hand, from (4.10) and taking into account that
[TABLE]
where
[TABLE]
we get
[TABLE]
and using the same arguments as above to obtain formula (4.13), we get the following compact expression for the kernel polynomial.
Proposition 4.1**.**
[TABLE]
where .
Remark 4.3*.*
Proceeding as above one has the expression for the confluent formula .
Remark 4.4*.*
If then . Thus
[TABLE]
If we denote by the zeros of the polynomial , we deduce in a straightforward way the value of the Christoffel numbers in the quadrature formula by using the above zeros as nodes. Indeed,
[TABLE]
5. Examples
In this section we analyze some examples which illustrate the problems considered in the previous sections. First we focus our attention on the symmetric case which is less complex than the general one. The case when the connection coefficients are constant real numbers is also studied.
5.1. Symmetric case
Let us consider the symmetric SMOP , that is the case when for . According to Theorem 2.1, equations (2.3), (2.4) and (2.5) become
[TABLE]
[TABLE]
and for
[TABLE]
Equations (2.6) and (2.7) become
[TABLE]
or alternatively
[TABLE]
**Step 1. ** If we fix for , then from (5.1)
[TABLE]
and it is easy to conclude that for
Relation (5.2) yields
[TABLE]
**Step 2. ** If we impose the restrictions and , for , then from (5.5) and (5.4), we obtain
[TABLE]
Proposition 5.1**.**
If and , for , then
[TABLE]
This means that .
Here, for a fixed positive integer number , we denote by the sequence of polynomials satisfying the three-term recurrence relation
[TABLE]
with initial conditions , It is said to be the sequence of associated monic polynomials of order for the linear functional (see [16]).
**Step 3. ** We keep and , for , and we add the constrain , for . Since from (5.3), with ,
[TABLE]
then Thus, either or remains constant for , that is, for
If the coefficients are constants for , then is the sequence of anti-associated polynomials of order for the Chebyshev polynomials of the second kind (see [40]).
**Step 4. ** The other possibility is that , and , for . Now we add the restriction , for . Since, from (5.3) with ,
[TABLE]
we obtain
[TABLE]
and, again, either or the sequence is a periodic sequence with period 2. Thus is the sequence of anti-associated polynomials of order of a 2-periodic sequence (see [40]). We refer to [16, p.91] for the explicit expression of symmetric orthogonal polynomials defined by recurrence relations whose coefficients are 2-periodic sequences. Let , where and . Then
[TABLE]
where .
**Step 5. ** Yet another possibility is , , and , for . Following the previous reasoning let to add the restriction , for . Then (5.3), for , reads
[TABLE]
Hence,
[TABLE]
Then either or the sequence is a 3-periodic one.
We can proceed in this way up to using (5.3), and periodic sequences appear in a natural way.
We will illustrate the above method in the case of Chebyshev polynomials of the second kind.
Example 5.1**.**
Let be the sequence of monic Chebyshev polynomials of second kind orthogonal with respect to on . Then , , and , and (\ref{eq_for_b_i_sym}) become
[TABLE]
for .
Assume that for , and for . Then we have
[TABLE]
In particular, according to the fact that and for , then
[TABLE]
and, as a consequence, for every ,
[TABLE]
On the other hand, if you assume, instead of and for , that and for , a reverse situation in terms of the connection coefficients, then
[TABLE]
and
[TABLE]
In particular, this means that
[TABLE]
Notice that in this case
[TABLE]
In other words, we have constant connection coefficients, but they appear for .
Proposition 5.2**.**
Let assume that is a sequence of quasi-orthogonal polynomials of order with respect to the sequence . If either and for , or and for , then all the remaining connection coefficients are constant for . Notice that if the initial conditions are and then all coefficients are constant for . In this case,
[TABLE]
This means that the SMOP has the same sequence of ()-associated polynomials that the SMOP . In other words it is an anti-associated SMOP of order of the Chebyshev polynomials of second kind.
5.2. Non-symmetric case
Notice that key information for the sequence is given by the sequences and or, alternatively, by the sequences and because
[TABLE]
If for the coefficients and do not depend on , i.e. and , we have
[TABLE]
On the other hand, if and are constant coefficients, for , i.e. and , it follows from (2.6), (3.6) and (3.7) that
[TABLE]
Example 5.2**.**
Let be the sequence of either monic Chebyshev polynomials of third kind , orthogonal with respect to on , or monic Chebyshev polynomials of fourth kind , orthogonal with respect to on . In both cases there exists a representation
[TABLE]
where the coefficient depends on the choice of For the Chebyshev polynomials of the third kind, with , , and for the Chebyshev polynomials of the fourth kind, with , , (see [16, p.89]).
Then
[TABLE]
Thus, this problem is reduced to the one concerning Chebyshev polynomials of the second kind.
Notice that if and , for , according to Example 5.1, this yields
[TABLE]
The same analysis applies when we assume and , for .
Example 5.3**.**
Let be the sequence of monic Laguerre polynomials , orthogonal with respect to on , . In this situation, for , and for . Consider the case when and , for . It follows from that
[TABLE]
[TABLE]
**Step 1. ** If , then
[TABLE]
where does not depend on . Therefore is a polynomial of degree in .
**Step 2. ** If , then
[TABLE]
where , are, in general, complex numbers such that . Thus,
[TABLE]
Then is a rational function.
From we have
[TABLE]
Then
[TABLE]
where does not depend on , and
[TABLE]
Then is also a rational function.
Now we look at the behaviour of the coefficients for , and .
From and (\ref{eq_for_b_i}) with , we have
[TABLE]
we see that is a polynomial of degree two in .
Also, from and (\ref{eq_for_b_i}) with , we have
[TABLE]
and is a polynomial of degree three in .
Suppose that . If , then the above relations yield that is a polynomial of degree eight. On the other hand, is a polynomial of degree three, which is a contradiction. Otherwise, if , according to the above calculations, and are rational functions of the variable . However, and are polynomials of degrees two and three, respectively. This is a contradiction again.
We conclude that it is not possible that and , , are constant real numbers when you deal with Laguerre orthogonal polynomials.
5.3. All constant coefficients
Now we consider the special case when all the coefficients in (1.2) do not depend on . Let us apply Theorem 2.1 to obtain the necessary and sufficient conditions for the orthogonality of the monic polynomial sequence . Let be a SMOP with respect to a linear functional and
[TABLE]
where are real numbers, and . The above necessary and sufficient conditions become
[TABLE]
[TABLE]
where and are the coefficients of the three term recurrence relation satisfied by the SMOP , for .
These results were obtained [3]. In that paper the authors provide also a detailed study of the case with constant coefficients. The case with constant coefficients was analysed thoroughly in [29].
Now we focus our attention on the case when the sequence is symmetric, i.e., , for all . The conditions and yield the necessary and sufficient conditions, for ,
[TABLE]
Then, as a consequence of Theorem 2.1, we obtain
Corollary 5.1**.**
Let be a symmetric monic polynomial sequence and let be a monic polynomial sequence defined by relation , for . Then is a SMOP with recurrence coefficients and if and only if the sequence satisfies and . Furthermore, the recurrence coefficients of SMOP satisfy and for . In other words, , where and are the associated polynomials of order for the SMOP and respectively (see [16]).
Our next result characterizes as a periodic sequence and we also discuss its possible periods.
Theorem 5.1**.**
Under the hypothesis of Corollary 5.1, the sequence of the coefficients of the three-term recurrence relation must be a periodic sequence with period , where is a divisor of . Furthermore, if , for , then the period of the sequence is . If , for any , such that , then the period of the sequence is the greatest common divisor of , and .
Proof.
Conditions and , for , tell us that if any coefficient , for , then Hence, we conclude that
if any coefficient , for , then implies that is a periodic sequence with period ;
if any coefficient , for , then implies that is a periodic sequence with period .
As a summary, if , for any , then is a -periodic sequence.
The condition , i.e., , for , tell us that the sequence is also a -periodic sequence.
It is easy to see that a periodic sequence with both period and has, in fact, period equals to the greatest common divisor of and . Since all divisors of but itself are included in , all choices of such that yield the divisors in . Also the choice for yields as the period. ∎
Remark 5.1*.*
i) If for only one such that , then if is a multiple of , the period of the sequence is exactly .
ii) Observe that to choose values for and one needs .
iii) Notice that the coefficient is free.
Remark 5.2*.*
If we consider a SMOP , such that , for , the conditions and yield the same behaviour for as in Theorem 5.1 taking into account that it represents a shift in the variable for a symmetric SMOP.
For the case , when the sequence is not symmetric, in [29] the authors also consider the choice and they prove that both sequences and must be -periodic. When one considers either only or only , the behaviour of and is one-periodic. Finally, with both and the behaviour of and depends on the values of , and .
Remark 5.3*.*
Grinshpun [24] showed that Bernstein-Szegő’s orthonormal polynomials of -th kind, and only them, can be represented as a linear combination of Chebyshev orthonormal polynomials of -th kind, respectively, with constant coefficients, namely
[TABLE]
where denote the Bernstein-Szegő orthonormal polynomials of -th kind and are the Chebyshev orthonormal polynomials of th kind.
Sequences of Bernstein-Szegő polynomials are orthogonal with respect to the weight functions
[TABLE]
where is the Chebyshev weight function of the th kind, and is a positive polynomial of degree on . The constants are given as the real coefficients of a polynomial of degree , that appears as the Fejér-normalized representation of the positive polynomials Moreover, Grinshpun proves that if are the classical Chebyshev orthonormal polynomials of one of the four kinds, with and the polynomial either does not have any zeros in the unit disc or all its zeros are located on the unit circle, then either or , are Bernstein-Szegő polynomials of the corresponding kind.
Acknowledgements. We thank Dr. D. K. Dimitrov by his continued support. His comments and criticism have contributed to improve the presentation of the manuscript.
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