The Schur class, denoted by S(D)\documentclass[12pt]{minimal}
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\begin{document}$${\mathcal {S}}({\mathbb {D}})$$\end{document}, is the set of all functions analytic and bounded by one in modulus in the open unit disc D\documentclass[12pt]{minimal}
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\begin{document}$${\mathbb {D}}$$\end{document} in the complex plane C\documentclass[12pt]{minimal}
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\begin{document}$${\mathbb {C}}$$\end{document}, that is S(D)=φ∈H∞(D):‖φ‖∞:=supz∈D|φ(z)|≤1.\documentclass[12pt]{minimal}
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\begin{document}$$\begin{aligned} {\mathcal {S}}({\mathbb {D}}) = \left\{ \varphi \in H^\infty ({\mathbb {D}}): \Vert \varphi \Vert _{\infty } := \sup _{z \in {\mathbb {D}}} |\varphi (z)| \le 1\right\} . \end{aligned}$$\end{document}The elements of S(D)\documentclass[12pt]{minimal}
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\begin{document}$${\mathcal {S}}({\mathbb {D}})$$\end{document} are called Schur functions. A classical result going back to I. Schur states: A function φ:D→C\documentclass[12pt]{minimal}
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\begin{document}$$\varphi : {\mathbb {D}} \rightarrow {\mathbb {C}}$$\end{document} is in S(D)\documentclass[12pt]{minimal}
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\begin{document}$${\mathcal {S}}({\mathbb {D}})$$\end{document} if and only if there exist a Hilbert space H\documentclass[12pt]{minimal}
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\begin{document}$${\mathcal {H}}$$\end{document} and an isometry (known as colligation operator matrix or scattering operator matrix) V=aBCD:C⊕H→C⊕H,\documentclass[12pt]{minimal}
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\begin{document}$$\begin{aligned} V = \begin{bmatrix} a &{}\quad B \\ C &{}\quad D \end{bmatrix} : {\mathbb {C}} \oplus {\mathcal {H}} \rightarrow {\mathbb {C}} \oplus {\mathcal {H}}, \end{aligned}$$\end{document}such that φ\documentclass[12pt]{minimal}
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\begin{document}$$\varphi $$\end{document} admits a transfer function realization corresponding to V, that is φ(z)=a+zB(IH-zD)-1C(z∈D).\documentclass[12pt]{minimal}
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\begin{document}$$\begin{aligned} \varphi (z) = a + z B (I_{{\mathcal {H}}} - z D)^{-1} C \quad \quad (z \in {\mathbb {D}}). \end{aligned}$$\end{document}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\documentclass[12pt]{minimal}
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\begin{document}$${\mathbb {C}}^n$$\end{document} is a well-known “analogue” of Schur functions on D\documentclass[12pt]{minimal}
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\begin{document}$${\mathbb {D}}$$\end{document}. 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.
