Schur functions in complex function theory
The Schur class in complex analysis is the set of holomorphic functions which are defined and satisfy
on the unit disc
in the complex plane (cf. also Analytic function). The Schur class arises in diverse areas of classical analysis and operator theory, and it has applications in linear system theory and mathematical engineering.
The Schur algorithm [a15] is an iterative construction that associates a sequence of complex numbers with a given function
in the Schur class. The numbers are defined in terms of a sequence of Schur functions which is constructed recursively by setting
and
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If for some
,
reduces to a constant and one sets
for all
. The sequence
,
, thus consists of numbers of modulus at most one, and if some term of the sequence has unit modulus, all subsequent terms vanish; the numbers
are called the Schur parameters of
. Every sequence of complex numbers of modulus at most one and having the property that if some term has unit modulus then all subsequent terms vanish, occurs as the Schur parameters of a unique function in the Schur class.
The Schur class plays a prominent role in classical moment and interpolation problems. One of the best known is the Schur problem, also known as the Carathéodory–Fejér problem: Find a Schur function whose first
Taylor coefficients coincide with given numbers
.
The Schur algorithm provides a means to describe all such functions because the first Schur parameters of a Schur function
depend only on the first
Taylor coefficients of
. A solution exists if and only if the matrix
![]() |
has norm at most one as an operator on in the Euclidean metric. Similar results hold for the Nevanlinna–Pick problem: Find a Schur function
such that
,
, where
are given points in the unit disc and
are complex numbers.
A solution to the Nevanlinna–Pick problem exists if and only if the matrix
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is non-negative as an operator on in the Euclidean metric. For example, see [a1], Chap. 3.
Many such classical problems are subsumed in abstract operator problems. There are several approaches in common use. To describe one approach, let be multiplication by a Schur function
on the Hardy class
for the unit disc (cf. also Hardy classes) [a7], and let
be multiplication by
on
. Then
is a contraction which commutes with
, and every contraction on
which commutes with
has this form for some Schur function
. The commutation relation
is preserved under compressions of
and
to certain subspaces of
. Let
be an invariant subspace for
, and let
and
, where
is the projection of
onto
. Then
. The Sarason generalized interpolation theorem [a5] asserts that every contraction
on
which commutes with
has this form and is therefore associated with some Schur function
. Particular choices of the invariant subspace
lead to solutions to the Schur and Nevanlinna–Pick problems. The generalized interpolation theorem has an abstract extension in the commutant lifting theorem [a8], p. 66, which extends the conclusion to arbitrary Hilbert space contraction operators
,
, and
which are connected by a commutation relation
. In turn, the commutant lifting theorem is part of a broader theory of extensions and completions of Hilbert space operators [a14], which is motivated in part by connections with linear system theory and mathematical engineering [a11]. In such generalizations, scalar-valued functions are often replaced by matrix- or operator-valued functions. In tangential interpolation problems, only certain components of the data are specified. The approach of V.P. Potapov [a10] to tangential problems has diverse applications, as discussed, for example, in [a3]. See [a12] for realization theory. See [a16] for an overview of operator methods in interpolation theory.
Schur functions arise in operator theory in other ways, such as in invariant subspace theory and its generalizations. For any Schur function , the kernel
is non-negative on the unit disc in the sense that
for all
,
, and
. Therefore,
is the reproducing kernel for a Hilbert space
of holomorphic functions on
. The transformations
![]() |
are well defined, and the colligation
![]() |
is co-isometric on , that is,
. The characteristic function of the colligation is
:
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The class of Hilbert space operators which are unitarily equivalent to a transformation which arises in this way from some Schur function can be characterized [a6], p. 39. Schur functions thus encode structural information for contraction operators. For example, the study of invariant subspaces is intimately related to factorizations
of a Schur function into a product of two Schur functions. The transformation
is an example of a canonical model, that is, a concrete operator which is unitarily equivalent to an abstract operator of some prescribed type. A canonical model due to B. Sz.-Nagy and C. Foiaş is given in [a8]; see [a2] for a general notion of canonical model and operator-theoretic applications. Function-theoretic properties of a Schur function
, in turn, may be studied with the aid of model operators [a13].
More generally, a meromorphic function , holomorphic in a subregion
of
which contains the origin, is a generalized Schur function with
negative squares if the kernel
has
negative squares, that is, if every matrix
, where
,
, and
, always has at most
negative eigenvalues, and at least one such matrix has exactly
negative eigenvalues [a9]. A space
having reproducing kernel
exists now as a Pontryagin space. Transformations
,
,
,
can be defined as before, giving rise to a co-isometric colligation
in the same way. The main results of the Hilbert space theory have extensions to this situation [a4]. The indefinite theory has new elements. An example is the existence of a
-dimensional non-positive invariant subspace for the contraction
on
. The existence of such a subspace leads to the Krein–Langer factorization
for the generalized Schur function
. Here,
is a Blaschke product having
factors and
belongs to the classical Schur class and is non-vanishing at the zeros of
. To say that
is a Blaschke product of
factors means that it has the form
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where are (not necessarily distinct) points of
and
is a constant of unit modulus [a7]. The case
is included by interpreting an empty product as one. Conversely, every function of the form
with
and
as above is a generalized Schur function, with
negative squares.
References
[a1] | N.I. Akhiezer, "The classical moment problem" , Hafner (1965) |
[a2] | N. Nikolski, V. Vasyunin, "Elements of spectral theory in terms of the free function model. I. Basic constructions" , Holomorphic spaces (Berkeley, CA, 1995) , Cambridge Univ. Press (1998) pp. 211–302 |
[a3] | L.A. Sakhnovich, "Interpolation theory and its applications" , Kluwer Acad. Publ. (1997) |
[a4] | D. Alpay, A. Dijksma, J. Rovnyak, H.S.V. de Snoo, "Reproducing kernel Pontryagin spaces" , Holomorphic spaces (Berkeley, CA, 1995) , Cambridge Univ. Press (1998) pp. 425–444 |
[a5] | D. Sarason, "Generalized interpolation in ![]() |
[a6] | L. de Branges, J. Rovnyak, "Square summable power series" , Holt, Rinehart&Winston (1966) |
[a7] | P.L. Duren, "Theory of ![]() |
[a8] | B. Sz.-Nagy, C. Foiaş, "Harmonic analysis of operators on Hilbert space" , North-Holland (1970) |
[a9] | M.G. Krein, H. Langer, "Über einige Fortsetzungsprobleme, die eng mit der Theorie hermitescher Operatoren im Raume ![]() |
[a10] | V.P. Potapov, "Collected papers" , Hokkaido Univ. Research Inst. Applied Electricity, Division Appl. Math., Sapporo (1982) (Edited and transl. by T. Ando) |
[a11] | T. Kailath, "A theorem of I. Schur and its impact on modern signal processing" , I. Schur methods in operator theory and signal processing , Oper. Th. Adv. Appl. , 18 , Birkhäuser (1986) pp. 9–30 |
[a12] | J.A. Ball, I. Gohberg, L. Rodman, "Interpolation of rational matrix functions" , Oper. Th. Adv. Appl. , 45 , Birkhäuser (1990) |
[a13] | D. Sarason, "Sub-Hardy Hilbert spaces in the unit disk" , Wiley (1994) |
[a14] | C. Foias, A.E. Frazho, I. Gohberg, M.A. Kaashoek, "Metric constrained interpolation, commutant lifting and systems" , Oper. Th. Adv. Appl. , 100 , Birkhäuser (1998) |
[a15] | I. Schur, "Über Potenzreihen, die im Innern des Einheitskreises beschränkt sind. I-II" J. Reine Angew. Math. , 147–148 (1917-1918) pp. 205–232; 122–145 (Also: Gesammelte Abh. II, no. 29–30. English transl.: I. Schur methods in operator theory and signal processing, Vol. 18 of Oper. Th. Adv. Appl., Birkhäuser, 1986, pp. 31–59; 61–88) |
[a16] | H. Dym, "The commutant lifting approach to interpolation problems, by Ciprian Foias and Arthur E. Frazho (book review)" Bull. Amer. Math. Soc. , 31 (1994) pp. 125–140 |
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