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Discrete Analogs of Canonical Systems with Pseudo-exponential Potential. Definitions and Formulas for the Spectral Matrix Functions

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Abstract

We first review the theory of canonical differential expressions in the rational case. Then, we define and study the discrete analogue of canonical differential expressions. We focus on the rational case. Two kinds of discrete systems are to be distinguished: one-sided and two-sided. In both cases the analogue of the potential is a sequence of numbers in the open unit disk (Schur coefficients). We define the characteristic spectral functions of the discrete systems and provide exact realization formulas for them when the Schur coefficients are of a special form called strictly pseudo-exponential.

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... Recall that discrete and continuous systems with the potentials, which belong to the subclass of the strictly pseudo-exponential potentials, have been actively studied in [1]- [6], [8]- [10]. In particular, direct and inverse problems for Szegö recurrence on the semiaxis with the scalar (p = 1) strictly pseudo-exponential potentials have been treated in [5,6]. Direct and inverse problems for the pseudo-exponential potentials (continuous case) have been studied in a series of Gohberg-Kaashoek-Sakhnovich papers [21,22] (see references therein and see also [17] for the case of the generalized pseudo-exponential potentials). ...
... The case of the discrete skewself-adjoint Dirac system have been studied in [24]. Notice that similar to [21,31] (see also [5,6,8,21,24]) we start our explicit constructions with the explicit formula for the fundamental solution. ...
... Notice that our matrices C k belong to the class of the so called pseudoexponential potentials. An important subclass of the strictly pseudoexponential potentials, that is, a subclass with an additional requirement σ(A) ⊂ C − (σ -spectrum), have been treated for p = 1 in [5,6]. In particular, for the strictly pseudoexponential subcase the inequality |ϕ(λ)| < 1 for λ ∈ C − is true. ...
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Discrete Dirac type self-adjoint system is equivalent to the block Szeg\"o recurrence. Representation of the fundamental solution is obtained, inverse problems on the interval and semi-axis are solved. A Borg-Marchenko type result is obtained too. Connections with the block Toeplitz matrices are treated.
... Remark 2.3 When m 1 = m 2 = 1, one easily removes the factor (1 − |ρ k | 2 ) −1/2 in (2.12) to obtain systems as in [4,5], where direct and inverse problems for the case of scalar strictly pseudo-exponential potentials have been treated. The square matrix version (i.e., the version where m 1 = m 2 ) of Szegö recurrence, its connections with Schur coefficients and applications are discussed in [8,9] (see also references therein). ...
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Chapter
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Chapter
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Book
1 Schur Parameters and Positive Block Matrices.- 1.1 Preliminaries.- 1.2 Renorming Hilbert Spaces and Elementary Rotations.- 1.3 Kolmogorov Decompositions. I.- 1.4 Row and Column Contractions.- 1.5 The Structure of Positive Definite Kernels.- 1.6 Kolmogorov Decompositions. II.- 1.7 Notes.- 2 Models for Triangular Contractions.- 2.1 Preliminaries.- 2.2 The Structure of Triangular Contractions.- 2.3 Realization of Triangular Contractions.- 2.4 Unitary Couplings and Operator Ranges.- 2.5 Modeling Families of Contractions.- 2.6 Notes.- 3 Moment Problems and Interpolation.- 3.1 A Survey on Completion Problems.- 3.2 Extensions of Partial Isometries.- 3.3 Krein's Formula.- 3.4 Moment Problems.- 3.5 The Commutant Lifting Method.- 3.6 Notes.- 4 Displacement Structures.- 4.1 Structured Matrices.- 4.2 Generalized Schur Algorithm.- 4.3 Discrete Transmission-Line Models.- 4.4 Displacement Structure and Completion Problems.- 4.5 Other Applications.- 4.6 Notes.- 5 Factorization of Positive Definite Kernels.- 5.1 Spectral Factors.- 5.2 Examples.- 5.3 Schur's Algorithm, Szego's Theory and Spectral Factors.- 5.4 Maximum Entropy.- 5.5 Notes.- 6 Nonstationary Processes.- 6.1 Modeling Nonstationary Processes.- 6.2 Kolmogorov-Wiener Prediction.- 6.3 Other Prediction Problems.- 6.4 Szego's Limit Theorems.- 6.5 Notes.- 7 Graphs and Completion Problems.- 7.1 Preliminaries.- 7.2 Completing Positive Partial Matrices. I.- 7.3 Completing Positive Partial Matrices. II.- 7.4 Completing Contractive Partial Matrices.- 7.5 Notes.- 8 Determinantal Formulae and Optimization.- 8.1 Determinantal Formulae.- 8.2 Maximum Determinant Formulae.- 8.3 Maximum Determinant for Nonchordal Graphs.- 8.4 Inheritance Principles.- 8.5 Notes.- References.
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We obtain explicit formula for the reflexivity coefficient function (or potential) of an ordinary differential operator if its reflection coefficient is a rational matrix valued function. The solution is given in terms of a realization of the reflection coefficient function.
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We solve the inverse problems associated with a differential expression of the form (1.1) for the Weyl coefficient function and the reflection coefficient function in the case of potentials k(t) of the special form (1.2).
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A differential expression of the type (Dx)(r)=W * (r)J(d/dr)(W(r)x(r))(r∈[0,∞)); where J is (2n×2n)-matrix with the properties J * =-J, J 2 =-I 2n and W(r) is a continuous (2n×2n)-matrix function with J-unitary values (W * (r)JW(r)=J ∀r∈[0,∞)) is considered. An expression of this type generalizes the canonical differential expression (D v x)(r)=J(dx(r)/dr)-V(r)x(r) with Hermitian potential V(r)V * (r)=V(r). For the special class of equations (Dx)(r,λ)=λx(r,λ) which include equations (D v x)(r,λ)=λx(r,λ) with summable potential V(r) (V∈L 2n×2n 1 (0,∞)), the problems of scattering and spectral theory are solved.
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A number of results in the theory of inverse problems for polynomials on the line and on the circle will be reviewed. Analogues of the methods of Gelfand-Levitan, Krein, and Marchenko will be presented with special emphasis on the role played by factorization and Toeplitz operators.
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For rational and analytic matrix functions new formulas are obtained for the limits in the Szegö-Kac-Achiezer limit theorems. In the rational case the new expressions are given in terms of finite matrices which come from special representations of the matrix functions. These representations are known as realizations in mathematical systems theory.
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The main theme of the first half of this paper rests upon the fact that there is a reproducing kernel Hilbert space of vector valued functions B (X) associated with each suitably restricted matrix valued analytic function X. The deep structural properties of certain classes of these spaces, and the theory of isometric and contractive inclusion of pairs of such spaces, which originates with de Branges, partially in collaboration with Rovnyak, is utilized to develop an algorithm for constructing a nested sequence B(X) ⊃ B(X 1) ⊃... of such spaces, each of which is included isometrically in its predecessor. This leads to a new and pleasing viewpoint of the Schur algorithm and various matrix generalizations thereof. The same methods are used to reinterpret the factorization of rational J inner matrices and a number of related issues, from the point of view of isometric inclusion of certain associated sequences of reproducing kernel Hilbert spaces.
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We prove a trace formula for pairs of self-adjoint operators associated to canonical differential expressions. An important role is played by the associated Weyl function.
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The Factorization of Rational Matrix Functions.- Decomposing Algebras of Matrix Functions.- Canonical Factorizations of Continuous Matrix Functions.- Factorization of Triangular Matrix Functions.- Factorization of Continuous Self-Adjoint Matrix Functions on the Unit Circle.- Miscellaneous Results on Factorization Relative to a Contour.- Generalized Factorization.- Further Results Concerning Generalized Factorization.- Local Principles in the Theory of Factorization.- Perturbations and Stability.
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Explicit formulas are given for the solutions of the direct and inverse scattering problems for a canonical differential system with a strictly pseudo–exponential potential. The proofs are self–contained and employ state space techniques from mathematical system theory. The paper supplements an earlier paper of the first two authors where explicit formulas were given using Marchenko's approach, and an earlier paper of the last three authors where self–contained proofs were given for the corresponding direct and inverse spectral problems. Two types of factorizations of the scattering matrix function appear and connections between them are considered.
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This paper solves explicitly the direct spectral problem of canonical differential systems for a special class of potentials. For a potential from this class the corresponding spectral function may have jumps and its absolutely continuous part has a rational derivative possibly with zeros on the real line. A direct and self-contained proof of the diagonalization of the associated differential operator is given, including explicit formulas for the diagonalizing operator and the spectral function. This proof also yields an explicit formula for the solution of the inverse problem. As an application new representations are derived for a large class of solutions of nonlinear integrable partial differential equations. The method employed is based on state space techniques and uses the idea of realization from mathematical system theory.
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We study the connections between the Carathodory-Toeplitz extension problem and the Nehari extension problem in the discrete scalar case. This is the discrete counterpart of our previous paper [4].
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The Schur algorithm and its time-domain counterpart, the fast Cholseky recursions, are some efficient signal processing algorithms which are well adapted to the study of inverse scattering problems. These algorithms use a layer stripping approach to reconstruct a lossless scattering medium described by symmetric two-component wave equations which model the interaction of right and left propagating waves. In this paper, the Schur and fast Chokesky recursions are presented and are used to study several inverse problems such as the reconstruction of nonuniform lossless transmission lines, the inverse problem for a layered acoustic medium, and the linear least-squares estimation of stationary stochastic processes. The inverse scattering problem for asymmetric two-component wave equations corresponding to lossy media is also examined and solved by using two coupled sets of Schur recursions. This procedure is then applied to the inverse problem for lossy transmission lines.
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This paper develops a method for obtaining linear fractional representations of a givennn matrix valued function which is analytic and contractive in either the unit disc or the open upper half plane. The method depends upon the theory of reproducing kernel Hilbert spaces of vector valued functions developed by de Branges. A self-contained account of the relevant aspects of these spaces to this study is included. In addition, the methods alluded to above are used in conjunction with some ideas of Krein, to develop models for simple, closed symmetric [resp. isometric] operators with equal deficiency indices. A number of related issues and applications are also discussed.
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We develop the theory of orthogonal polynomials on the unit circle based on the Szegő recurrence relations written in matrix form. The orthogonality measure and C-function arise in exactly the same way as Weyl's function in the Weyl approach to second order linear differential equations on the half-line. The main object under consideration is the transfer matrix which is a key ingredient in the modern theory of one-dimensional Schrödinger operators (discrete and continuous), and the notion of subordinacy from the Gilbert–Pearson theory. We study the relations between transfer matrices and the structure of orthogonality measures. The theory is illustrated by the Szegő equations with reflection coefficients having bounded variation.
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The paper extends earlier results of the authors for canonical systems with spectral functions of which the absolutely continuous part has a rational derivative to a class of differential systems with skew selfadjoint potentials. The corresponding direct and inverse spectral problems are solved explicitly, using state space methods from mathematical system theory. Applications to nonlinear integrable partial differential equations are included.
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We show that the multitude of applications of the Weyl–Titchmarsh m-function leads to a multitude of different functions in the theory of orthogonal polynomials on the unit circle that serve as analogs of the m-function.
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The main result is that forevery J-unitary 2×2-matrix polynomial on the unit circle is an essentially unique product of elementary J-unitary 2×2-matrix polynomials which are either of degree 1 or 2k. This is shown by means of the generalized Schur transformation introduced in [Ann. Inst. Fourier 8 (1958) 211; Ann. Acad. Sci. Fenn. Ser. A I 250 (9) (1958) 1–7] and studied in [Pisot and Salem Numbers, Birkhäuser Verlag, Basel, 1992; Philips J. Res. 41 (1) (1986) 1–54], and also in the first two parts [Operator Theory: Adv. Appl. 129, Birkhäuser Verlag, Basel, 2000, p. 1; Monatshefte für Mathematik, in press] of this series. The essential tool in this paper are the reproducing kernel Pontryagin spaces associated with generalized Schur functions.
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In this paper we study the inverse scattering problem for linear canonical differential equations of a special type in the case when the scattering function is a rational matrix—valued function. The main result here is the form of the potential in terms of a realisation of the scattering function. The difference between this publication and the previous one [3] consists in the fact that here is used the Marchenko method instead of Kreĭn’s method. For rational scattering functions we also prove the equivalence of the two methods.
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"Lectures form the CBMS regional conference held at Case Western University, September 10-14, 1984." Incluye bibliografía
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We present a novel technique to calculate the transmission and reflection properties of inhomogeneous lossy transmission lines. It is based on a perturbation expansion of the relevant telegrapher's equation around the homogeneous solution. The method reveals that the transmission properties are unaffected to first order in the impedance and admittance, while reflection properties are modified by first-order terms. Extending the analysis to second order, we find correction terms for both transmission and reflection. These allow us to understand the statistical properties of the information bearing capacity and the echo of the inhomogeneous transmission line. The correction to the transmission properties is fully reciprocal, despite the absence of any symmetry properties. We compute scaling laws for echo and capacity
Schur parameters, factorization and dilation problems, volume 82 of Operator Theory: Advances and Applications
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Invariant subspaces of matrices with applications. Canadian Mathematical Society Series of Monographs and Advanced Texts
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General theorems on the factorization of operatorvalued functions with respect to a contour. I. Holomorphic functions
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On the spectral theory of a class of canonical systems of differential equations
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Toeplitz operators with rational symbols and realizations: an alternative version
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Über die Potenzreihen, die im Innern des Einheitkreises beschränkten sind, I. Journal für die Reine und Angewandte Mathematik English translation in: I. Schur methods in operator theory and signal processing. (Operator theory
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On a class of canonical differential operators. Izvestya Akademii Nauk English translation inMATHMathSciNet
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