English

Factorizations of Schur functions

Functional Analysis 2021-03-08 v3 Complex Variables Operator Algebras Optimization and Control

Abstract

The Schur class, denoted by S(D)\mathcal{S}(\mathbb{D}), is the set of all functions analytic and bounded by one in modulus in the open unit disc D\mathbb{D} in the complex plane C\mathbb{C}, that is S(D)={φH(D):φ:=supzDφ(z)1}. \mathcal{S}(\mathbb{D}) = \{\varphi \in H^\infty(\mathbb{D}): \|\varphi\|_{\infty} := \sup_{z \in \mathbb{D}} |\varphi(z)| \leq 1\}. The elements of S(D)\mathcal{S}(\mathbb{D}) are called Schur functions. A classical result going back to I. Schur states: A function φ:DC\varphi: \mathbb{D} \rightarrow \mathbb{C} is in S(D)\mathcal{S}(\mathbb{D}) if and only if there exist a Hilbert space H\mathcal{H} and an isometry (known as colligation operator matrix or scattering operator matrix) V=[aBCD]:CHCH, V = \begin{bmatrix} a & B \\ C & D \end{bmatrix} : \mathbb{C} \oplus \mathcal{H} \rightarrow \mathbb{C} \oplus \mathcal{H}, such that φ\varphi admits a transfer function realization corresponding to VV, that is φ(z)=a+zB(IHzD)1C(zD). \varphi(z) = a + z B (I_{\mathcal{H}} - z D)^{-1} C \quad \quad (z \in \mathbb{D}). An analogous statement holds true for Schur functions on the bidisc. On the other hand, Schur-Agler class functions on the unit polydisc in Cn\mathbb{C}^n is a well-known "analogue" of Schur functions on D\mathbb{D}. In this paper, we present algorithms to factorize Schur functions and Schur-Agler class functions in terms of colligation matrices. More precisely, we isolate checkable conditions on colligation matrices that ensure the existence of Schur (Schur-Agler class) factors of a Schur (Schur-Agler class) function and vice versa.

Keywords

Cite

@article{arxiv.1908.01850,
  title  = {Factorizations of Schur functions},
  author = {Ramlal Debnath and Jaydeb Sarkar},
  journal= {arXiv preprint arXiv:1908.01850},
  year   = {2021}
}

Comments

27 pages, revised and compressed. To appear in Complex Analysis and Operator Theory

R2 v1 2026-06-23T10:40:17.313Z