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Model spaces invariant under composition operators

Published online by Cambridge University Press:  25 March 2022

P. Muthukumar
Affiliation:
Department of Mathematics and Statistics, Indian Institute of Technology Kanpur, Kanpur 208 016, India e-mail: pmuthumaths@gmail.com muthu@iitk.ac.in
Jaydeb Sarkar*
Affiliation:
Indian Statistical Institute, Statistics and Mathematics Unit, Bangalore 560 059, India e-mail: jay@isibang.ac.in
*
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Abstract

Given a holomorphic self-map $\varphi $ of $\mathbb {D}$ (the open unit disc in $\mathbb {C}$ ), the composition operator $C_{\varphi } f = f \circ \varphi $ , $f \in H^2(\mathbb {\mathbb {D}})$ , defines a bounded linear operator on the Hardy space $H^2(\mathbb {\mathbb {D}})$ . The model spaces are the backward shift-invariant closed subspaces of $H^2(\mathbb {\mathbb {D}})$ , which are canonically associated with inner functions. In this paper, we study model spaces that are invariant under composition operators. Emphasis is put on finite-dimensional model spaces, affine transformations, and linear fractional transformations.

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© The Author(s), 2022. Published by Cambridge University Press on behalf of The Canadian Mathematical Society

1 Preliminaries

Let $\mathbb {D}$ denote the open unit disk of the complex plane $\mathbb {C}$ , and let $H^2(\mathbb {D})$ denote the Hardy space over $\mathbb {D}$ . For $\varphi $ a holomorphic self-map of $\mathbb {D}$ , define the composition operator $C_\varphi $ on $H^2(\mathbb {D})$ by

$$ \begin{align*} C_\varphi f = f \circ \varphi \qquad (f \in H^2(\mathbb{D})). \end{align*} $$

It follows from the Littlewood subordination principle that $C_\varphi \in \mathcal {B}(H^2(\mathbb {D}))$ [Reference Shapiro22]. Here $\mathcal {B}(H^2(\mathbb {D}))$ denotes the set of all bounded linear operators on $H^2(\mathbb {D})$ .

The theory of composition operators is highly interdisciplinary with its natural connections to complex analysis, linear dynamics, complex geometry, and functional analysis. For instance, the question of the existence of nontrivial invariant subspaces of bounded linear operators on Hilbert spaces can be formulated in terms of minimal invariant subspaces of composition operators induced by hyperbolic automorphisms of $\mathbb {D}$ [Reference Montes-Rodríguez, Ponce-Escudero and Shkarin18Reference Nordgren, Rosenthal and Wintrobe20].

The theme of this paper is also in line with the invariant subspaces of composition operators, but restricted to model (or inner function based quotient) spaces of $H^2(\mathbb {D})$ . Recall that a function $\theta \in H^\infty (\mathbb {D})$ is said to be inner if $|\theta | = 1$ a.e. on $\partial \mathbb {D}$ in the sense of nontangential boundary values, where $H^\infty (\mathbb {D})$ denotes the commutative Banach algebra of all bounded holomorphic functions on $\mathbb {D}$ . Given an inner function $\theta $ , the model space $\mathcal {Q}_\theta $ is the quotient space

$$ \begin{align*} \mathcal{Q}_\theta = H^2(\mathbb{D}) \ominus \theta H^2(\mathbb{D}) \cong H^2(\mathbb{D})/ \theta H^2(\mathbb{D}). \end{align*} $$

The aim of this paper is to describe some results and methods of the calculation of model spaces that are invariant under composition operators. On the other hand, a celebrated result of Beurling [Reference Beurling1] states that a closed subspace $\mathcal {Q} \subseteq H^2(\mathbb {D})$ is invariant under $M_z^*$ if and only if $\mathcal {Q}$ is a model space. Here $M_zf = z f$ , $f \in H^2(\mathbb {D})$ , and $M_z^*$ is the backward shift

$$ \begin{align*} M_z^* f= \frac{f(z) - f(0)}{z} \qquad (f \in H^2(\mathbb{D})). \end{align*} $$

In other words, we are interested in joint invariant subspaces of the (noncommuting) pair $(M_z^*, C_\varphi )$ on $H^2(\mathbb {D})$ . Yet another motivation comes from the recent classification [Reference Bose, Muthukumar and Sarkar2] of joint invariant subspaces of the noncommuting pair $(M_z, C_\varphi )$ on $H^2(\mathbb {D})$ . In this context, we further remark that the concept of joint invariant subspaces of $(M_z, C_\varphi )$ was independently introduced by Chalendar and Partington [Reference Chalendar and Partington4] and Mahvidi [Reference Mahvidi16]. For recent results related to the subject we refer to [Reference Bose, Muthukumar and Sarkar2, Reference Jones14, Reference Matache17] and the references therein.

Often, results on composition operators are case-based. For instance, the theory of $C_{\varphi }$ corresponding to the holomorphic self-map of $\mathbb {D}$ as

$$ \begin{align*} \varphi(z) = az+b \text{ or } \frac{az+b}{cz+d} \end{align*} $$

is extremely demanding and complete answers to many basic questions are not known (cf. [Reference Deddens7, Reference Cowen6], and also see [Reference Gallardo-Gutiérrez and Schroderus11, Reference Lefèvre, Li, Queffélec and Rodríguez-Piazza15] for more recent accounts). Even norm computations and invariant subspaces of $C_\varphi $ for linear fractional transformations are known to be case-based (cf. [Reference Bourdon, Fry, Hammond and Spofford3, Reference Montes-Rodríguez, Ponce-Escudero and Shkarin18]). In fact, the results of this paper are also no exception. For example, Theorem 3.1 states: Let $\varphi $ be a holomorphic self-map of $\mathbb {D}$ . Fix $\alpha \in \mathbb {D}$ and $n \in \mathbb {N}$ , and consider the inner function

$$ \begin{align*} \theta(z)=\left(\frac{z- \alpha}{1-\bar{\alpha}z}\right)^n \qquad (z \in \mathbb{D}). \end{align*} $$

Then $\mathcal {Q}_\theta $ is invariant under $C_\varphi $ if and only if there exist scalars $a,b$ , and $c (\neq 0)$ such that

(1.1) $$ \begin{align} \varphi(z)= \begin{cases} a + bz, & \mbox{if } \alpha = 0 \text{ and } n> 1, \\ \frac{1-c}{\bar{\alpha}} + cz, & \mbox{if } \alpha \neq 0, \end{cases} \end{align} $$

where, $|a| + |b| \leq 1$ and $|\frac {1-c}{\bar {\alpha }}| + |c| \leq 1$ .

Note that the above model space $\mathcal {Q}_\theta $ is an n-dimensional Hilbert space. Even though we all know the structure of finite-dimensional model spaces (they are essentially parameterized by n-Blaschke products), but we do not know a general method to classify holomorphic self-maps $\varphi $ of $\mathbb {D}$ for which a given finite-dimensional model space remains invariant under $C_\varphi $ (see Question 3.3). In order to make this problem more convincing, in Proposition 3.4, we consider the two-dimensional model space $\mathcal {Q}_\theta $ corresponding to the (special) Blaschke product $\theta (z) = z \frac {z- \alpha }{1 - \bar {\alpha } z}$ , $z \in \mathbb {D}$ , and prove that $C_{\varphi } \mathcal {Q}_\theta \subseteq \mathcal {Q}_\theta $ if and only if $\varphi $ is the special Möbius map

$$ \begin{align*} \varphi(z) = \frac{(c_1 - 1) + (\bar{\alpha} + c_2) z}{\bar{\alpha}(c_1 + c_2z)} \qquad (z \in \mathbb{D}), \end{align*} $$

for some scalars $c_1$ and $c_2$ such that at least one of them is nonzero (see (3.2)). The above answers do not seem to tell us much about a possible answer to our general question.

We also put special emphasis on composition operators induced by linear fractional symbols (cf. Theorem 4.5): Let $\theta $ be an inner function, and let $\varphi (z)= \frac {az+b}{cz+d}$ be a nonconstant holomorphic self-map of $\mathbb {D}$ , where $ad - bc = 1$ . Suppose $\sigma (z)= \frac {\bar {a}z-\bar {c}}{-\bar {b}z+\bar {d}}$ and $\theta (0) = 0$ . If we denote $\psi = (\frac {\theta }{z}\circ \sigma )(\frac {\theta }{z})^{-1}$ , then the following are equivalent:

  1. (1) $\mathcal {Q}_\theta $ is invariant under $C_\varphi $ .

  2. (2) $\psi \in H^2(\mathbb {D})$ or $\psi \in H^\infty (\mathbb {D})$ .

  3. (3) $\frac {\theta }{z}H^2(\mathbb {D})$ is invariant under $C_\sigma $ .

A similar (but not same as above) consideration also holds for composition operators induced by affine transformations (see Theorem 4.3).

In the application part, we consider direct interpretations of our results to simple model spaces and reducing subspaces of composition operators. For instance, Theorem 5.3 states that:

  1. (1) $\mathcal {Q}_\theta $ is invariant under $C_\varphi $ for all inner function $\theta $ if and only if $\varphi $ is the identity map.

  2. (2) $\mathcal {Q}_\theta $ is invariant under $C_\varphi $ for all holomorphic self-map $\varphi $ if and only if $\theta (z)=\alpha z$ or $\theta \equiv \alpha $ , where $\alpha $ is an unimodular constant.

We now discuss the issue of reducing subspaces of composition operators from our perspective. Let T be a bounded linear operator on a Hilbert space $\mathcal {H}$ . A closed subspace $\mathcal {M} \subseteq \mathcal {H}$ is called reducing subspace for T (or $\mathcal {M}$ reduces T) if both $\mathcal {M}$ and $\mathcal {M}^{\bot }$ are invariant under T. It is known that $M_z$ on $H^2(\mathbb {D})$ is irreducible, that is, $M_z$ has no nontrivial reducing subspaces. In the setting of composition operators, if $\alpha \in \mathbb {C}$ with $\text {Re}(\alpha )> 0$ , then $C_{\varphi _{\alpha }}$ is also irreducible [Reference Montes-Rodríguez, Ponce-Escudero and Shkarin18, Theorem 1.3], where

$$ \begin{align*} \varphi_{\alpha}(z)=\frac{(2- \alpha )z+ \alpha}{-\alpha z+(2+ \alpha)} \qquad (z \in \mathbb{D}). \end{align*} $$

Another example is the composition operator corresponding to univalent loxodromic type self-map with nonzero Denjoy–Wolff point [Reference Guyker13, Theorem 1]. At the other extreme, we discuss reducibility of compositor operators restricted to model spaces. In Theorem 5.5, we prove the following: Let $\varphi $ be a holomorphic self-map of $\mathbb {D}$ , $\alpha \in \mathbb {D}$ , $n \geq 1$ , and suppose $\theta (z)=\left (\frac {z- \alpha }{1-\bar {\alpha }z}\right )^n$ . Then $\mathcal {Q}_\theta $ reduces $C_\varphi $ if and only if there exist a scalar c, $|c| \leq 1$ , and $\psi \in H^\infty (\mathbb {D})$ , $\|\psi \|_{\infty } \leq 1$ , such that

$$ \begin{align*} \varphi(z)= \begin{cases} z \psi, & \mbox{if } \alpha = 0 \text{ and } n = 1, \\ c z, & \mbox{if } \alpha = 0 \text{ and } n \geq 2,\\ z, & \mbox{if } \alpha \neq 0. \end{cases} \end{align*} $$

Finally, we make a general remark. Recall that a linear fractional transformation $\varphi (z) = \frac {az+b}{cz+d}$ is a self-map of $\mathbb {D}$ if and only if

$$ \begin{align*} |b \bar{d} - a \bar{c}| + |ad - bc| \leq |d|^2 - |c|^2. \end{align*} $$

In particular, since $\varphi $ is a holomorphic self-map, the inequalities following (1.1) are automatically true. In this paper, whenever no confusion can arise, we will not explicitly mention the above inequality for linear fractional transformations that are self-maps of $\mathbb {D}$ . In particular, the above inequality is applicable to Theorem 3.1, Example 3.4, and Theorem 4.3.

The rest of the paper is organized as follows. Section 2 recalls (rather a modified version of) the classification of Beurling type invariant subspaces from [Reference Bose, Muthukumar and Sarkar2]. Section 3 relates affine transformations and certain finite-dimensional model spaces. Section 4 deals with model subspaces invariant under composition operators corresponding to fractional linear transformations. The final section, Section 5, deals with some of the direct applications of our main results. We also discuss reducible composition operators at the level of model spaces.

2 Beurling type invariant subspaces

The purpose of this short section is to recall the classification of Beurling type invariant subspaces of composition operators from [Reference Bose, Muthukumar and Sarkar2].

We begin with the formal definition of Hardy space $H^2(\mathbb {D})$ . Recall that the Hardy space is the function Hilbert space of all holomorphic functions on $\mathbb {D}$ whose power series have square-summable coefficients. The following equivalent description of $H^2(\mathbb {D})$ is also well known:

$$ \begin{align*} H^2(\mathbb{D}) = \Big\{f \in \text{Hol}(\mathbb{D}): \|f\|:= \Big[\sup_{0 \leq r < 1} \frac{1}{2 \pi} \int_{0}^{2\pi} |f(r e^{it})|^2 dt\Big]^{\frac{1}{2}} < \infty\Big\}. \end{align*} $$

Also, we denote the closed unit ball of $H^\infty (\mathbb {D})$ (which is popularly known as Schur class) by

$$ \begin{align*} {\mathcal S}(\mathbb{D}) = \{\psi \in H^\infty(\mathbb{D}): \|\psi\|_\infty: = \sup_{z \in \mathbb{D}} |\psi(z)| \leq 1\}. \end{align*} $$

We will follow the standard notation: Given a bounded linear operator T on some Hilbert space $\mathcal {H}$ , the lattice of all closed T-invariant subspaces is denoted by $\mathrm{Lat} T$ , that is

$$ \begin{align*} \text{Lat} T = \{\mathcal{S} \subseteq \mathcal{H} \text{ closed subspace}: T \mathcal{S} \subseteq \mathcal{S}\}. \end{align*} $$

By Beurling’s Theorem, we know that

$$ \begin{align*} \text{Lat} M_z = \{\{0\}, \theta H^2(\mathbb{D}): \theta \text{ inner}\}, \end{align*} $$

and

$$ \begin{align*} \text{Lat} M_z^* = \{\mathcal{Q}_\theta, H^2(\mathbb{D}): \theta \text{ inner}\}. \end{align*} $$

A closed subspace $\mathcal {S} \subseteq H^2(\mathbb {D})$ is said to be a Beurling type invariant subspace if $\mathcal {S} = \theta H^2(\mathbb {D})$ for some inner function $\theta $ , or equivalently (in view of Beurling), $\mathcal {S}$ is invariant under $M_z$ . The following theorem is a simple refinement of [Reference Bose, Muthukumar and Sarkar2, Theorem 2.3]. We only prove the new component of the result.

Theorem 2.1 Let $\theta $ be an inner function and $\varphi $ be a holomorphic self-map of $\mathbb {D}$ . The following are equivalent:

  1. (1) $\theta H^2(\mathbb {D}) \in \mathrm{Lat} C_\varphi $ .

  2. (2) $\frac {\theta \circ \varphi }{\theta }\in {\mathcal S}(\mathbb {D})$ .

  3. (3) $\frac {\theta \circ \varphi }{\theta }\in H^\infty (\mathbb {D})$ .

  4. (4) $\frac {\theta \circ \varphi }{\theta }\in H^2(\mathbb {D})$ .

Proof The equivalence $(1) \Leftrightarrow (2)$ follows from [Reference Bose, Muthukumar and Sarkar2, Theorem 2.3]. Since

$$ \begin{align*} {\mathcal S}(\mathbb{D}) \subsetneq H^\infty(\mathbb{D}) \subsetneq H^2(\mathbb{D}), \end{align*} $$

it follows that $(2) \Rightarrow (3) \Rightarrow (4)$ . Therefore, it suffices to verify that $(4) \Rightarrow (2)$ . Suppose that $\frac {\theta \circ \varphi }{\theta }\in H^2(\mathbb {D})$ . Since $\theta $ is inner, we have

$$ \begin{align*} \left|\frac{\theta\circ\varphi}{\theta}(e^{it})\right|= |(\theta\circ\varphi)(e^{it})|\leq 1 \mbox{~for all~} t\in [0,2 \pi] \mbox{~a.e.} \end{align*} $$

Therefore, $\frac {\theta \circ \sigma }{\theta } \in H^\infty (\mathbb {D})$ with $\left \|\frac {\theta \circ \varphi }{\theta }\right \|_\infty \leq 1$ [Reference Duren9, Theorem 2.11], that is, $\frac {\theta \circ \varphi }{\theta }\in {\mathcal S}(\mathbb {D})$ , which completes the proof of the theorem.▪

This result will play a key role in what follows.

3 Finite-dimensional model spaces

Recall that the Hardy space $H^2(\mathbb {D})$ is a reproducing kernel Hilbert space corresponding to the Szegö kernel $k: \mathbb {D} \times \mathbb {D} \rightarrow \mathbb {C}$ , where

$$ \begin{align*} k(z, w) = (1 - z \bar{w})^{-1} \qquad (z, w \in \mathbb{D}). \end{align*} $$

Therefore, the linear span of $\{k(\cdot , w): w \in \mathbb {D}\}$ is dense in $H^2(\mathbb {D})$ , and $f(w) = \langle f, k(\cdot , w) \rangle _{H^2(\mathbb {D})}$ for all $f \in H^2(\mathbb {D})$ and $w \in \mathbb {D}$ . For each $\alpha \in \mathbb {D}$ , define the Blaschke factor $b_{\alpha }$ by

$$ \begin{align*} b_{\alpha}(z) = \frac{z - \alpha}{1 - \bar{\alpha} z} \qquad (z \in \mathbb{D}). \end{align*} $$

It is known that a model space $\mathcal {Q}_{\theta }$ is finite dimensional if and only if $\theta $ is a finite Blaschke product (cf. [Reference Radjavi and Rosenthal21, Theorem 3.8]). More specifically, if $\text {dim}\mathcal {Q}_{\theta } = n < \infty $ , then there exists $\alpha _1, \ldots , \alpha _m \in \mathbb {D}$ , and $n_1, \ldots , n_m \in \mathbb {N}$ such that $\sum _{i=1}^m n_i = n$ and

$$ \begin{align*} \theta =\prod_{i=1}^{m} b_{\alpha_i}^{n_i}. \end{align*} $$

Moreover, $\{c_{\alpha _i}^{(l_i)}: 0 \leq l_i \leq n_i-1, 1 \leq i \leq m\} $ is a basis for $\mathcal {Q}_{\theta }$ (see [Reference Garcia, Mashreghi and Ross12, Proposition 5.16]), where

$$ \begin{align*} c_{\alpha}^{(t)} := \frac{z^{t}}{(1 - \bar{\alpha} z)^{t+1}} \qquad (t \in \mathbb{Z}_+). \end{align*} $$

In the following, we prove that a “simple” finite dimensional model space is invariant under $C_\varphi $ if and only if $\varphi $ is a special affine map.

Theorem 3.1 Let $\varphi $ be a holomorphic self-map of $\mathbb {D}$ , $\alpha \in \mathbb {D}$ , $n \in \mathbb {N}$ , and suppose $\theta (z)=\left (\frac {z- \alpha }{1-\bar {\alpha }z}\right )^n$ . Then $\mathcal {Q}_\theta \in \mathrm{Lat} C_\varphi $ if and only if there exist scalars $a,b$ , and $c (\neq 0)$ such that

$$ \begin{align*} \varphi(z)= \begin{cases} a + bz, & \mbox{if } \alpha = 0 \text{ and } n> 1, \\ \frac{1-c}{\bar{\alpha}} + cz, & \mbox{if } \alpha \neq 0. \end{cases} \end{align*} $$

Proof In view of the preceding discussion, we have

$$ \begin{align*} \mathcal{Q}_\theta = \left\{ \frac{p(z)}{(1- \bar{\alpha} z)^n}: p \in \mathbb{C}[z], \text{deg } p \leq n-1 \right\}\!. \end{align*} $$

Suppose $\alpha = 0$ . Then $\theta (z)=z^n$ and

$$ \begin{align*} \mathcal{Q}_\theta=\mbox{span}\{1, z, z^2,\ldots,z^{n-1}\}. \end{align*} $$

Let $\varphi = a + bz$ . Clearly, if $f = \sum _{j=0}^{n-1} a_{j} z^{j} \in \mathcal {Q}_\theta $ , then

$$ \begin{align*} f\circ \varphi = \sum_{j=0}^{n-1} a_{j} \varphi^{j} = \sum_{j=0}^{n-1} a_{j} (a + bz)^{j}, \end{align*} $$

and hence $C_\varphi f = f\circ \varphi \in \mathcal {Q}_\theta $ . For the converse part, suppose $C_{\varphi } \mathcal {Q}_\theta \subseteq \mathcal {Q}_{\theta }$ . Since the identity map $f(z)=z$ , $z \in \mathbb {D}$ , is in $\mathcal {Q}_\theta $ , if follows that

$$ \begin{align*} f\circ \varphi=\varphi \in \mathcal{Q}_\theta, \end{align*} $$

which implies that $\varphi $ is a polynomial. Also note that $g \in \mathcal {Q}_\theta $ , where $g(z)=z^{n-1}$ , $z \in \mathbb {D}$ . Then

$$ \begin{align*} g\circ \varphi=\varphi^{n-1} \in \mathcal{Q}_\theta, \end{align*} $$

which implies that

$$ \begin{align*} (n-1) \mbox{deg}(\varphi)=\mbox{deg}(\varphi^{n-1})\leq n-1. \end{align*} $$

Since $n-1\neq 0$ , it follows that $\mbox {deg}(\varphi )\leq 1$ , and hence $\varphi $ is an affine map.

Now suppose that $\alpha \neq 0$ , and let $C_{\varphi } \mathcal {Q}_\theta \subseteq \mathcal {Q}_\theta $ . Since $k(\cdot , \alpha ) \in \mathcal {Q}_\theta $ , it follows that

$$ \begin{align*} k(\cdot, \alpha) \circ \varphi=\displaystyle\frac{1}{1-\bar{\alpha}\varphi} \in \mathcal{Q}_\theta, \end{align*} $$

and hence, there exists a polynomial p of degree $\leq n-1$ such that

$$ \begin{align*} \frac{1}{1- \bar{\alpha} \varphi}=\frac{p(z)}{(1-\bar{\alpha}z)^n}. \end{align*} $$

In particular, $\varphi $ is a nonconstant polynomial. Suppose $\mbox {deg}(\varphi )=m>0$ . Since

$$ \begin{align*} g = \frac{1}{(1-\bar{\alpha}z)^n} \in \mathcal{Q}_\theta, \end{align*} $$

we have

$$ \begin{align*} g\circ \varphi = \frac{1}{(1-\bar{\alpha}\varphi)^n}\in \mathcal{Q}_\theta. \end{align*} $$

Thus, there exists $q \in \mathbb {C}[z]$ such that

$$ \begin{align*} (1-\bar{\alpha}\varphi)^n q(z)=(1-\bar{\alpha}z)^n. \end{align*} $$

Comparing the degrees of both sides, we have $mn\leq n$ , which implies $\mbox {deg}(\varphi )=1$ . Then $\mbox {deg}(q)=0$ , and hence q is a nonzero constant. Therefore, there exists a nonzero scalar c such that $1-\bar {\alpha }\varphi =c (1-\bar {\alpha }z)$ , that is

$$ \begin{align*} \varphi(z)= \frac{1-c}{\bar{\alpha}} + cz. \end{align*} $$

We now turn to the converse direction. Let $c \neq 0$ and $\varphi (z)= \frac {1-c}{\bar {\alpha }}+cz$ . Then $1 - \bar {\alpha } \varphi = c (1 - \bar {\alpha } z)$ , and hence

$$ \begin{align*} \left(\frac{1}{1- \bar{\alpha} \varphi} \right)^l\in \mbox{span}\left\{\frac{1}{(1- \bar{\alpha} z)^j}: j =1, \ldots, n \right\} = \mathcal{Q}_\theta \end{align*} $$

for all $l=1,2,\ldots , n$ . It follows that $f\circ \varphi \in \mathcal {Q}_\theta $ for all $f\in \mathcal {Q}_\theta $ . This completes the proof of the theorem.▪

We would like to point out that even affine transformations (as symbols) play a prominent role in the complexity of composition operators (cf. Deddens [Reference Deddens7]).

Remark 3.2 In the context of Theorem 3.1, we note that if $\alpha = 0$ and $n = 1$ , then $\mathcal {Q}_z=(z H^2(\mathbb {D}))^{\bot }$ , which is the one dimensional subspace of all constant functions in $H^2(\mathbb {D})$ . Clearly, $\mathcal {Q}_z$ is invariant under every composition operator.

We do not know the answer to the following compelling question.

Question 3.3 Consider the finite Blaschke product $\prod _{i=1}^{m} b_{\alpha _i}$ corresponding to $\alpha _1, \ldots , \alpha _n \in \mathbb {D}$ . Characterize holomorphic self-maps $\varphi $ of $\mathbb {D}$ such that

$$ \begin{align*} C_{\varphi} \mathcal{Q}_{\prod_{i=1}^{m} b_{\alpha_i}} \subseteq \mathcal{Q}_{\prod_{i=1}^{m} b_{\alpha_i}}. \end{align*} $$

We also put forward the following simpler (two-dimensional) version: Suppose $\alpha \neq \beta $ in $\mathbb {D}$ , and suppose $\theta = b_{\alpha } b_{\beta }$ . Classify holomorphic self-maps $\varphi $ of $\mathbb {D}$ such that $C_\varphi \mathcal {Q}_\theta \subseteq \mathcal {Q}_\theta $ .

We do not know the complete answer to this question but the following special case ( $\alpha \neq 0$ and $\beta = 0$ ):

Proposition 3.4 Let $\alpha \in \mathbb {D}$ be a nonzero scalar, and suppose $\theta = z b_{\alpha }$ . Let $\varphi $ be a holomorphic self-map of $\mathbb {D}$ . Then $C_{\varphi } \mathcal {Q}_\theta \subseteq \mathcal {Q}_\theta $ if and only if $\varphi $ is the special Möbius map

(3.2) $$ \begin{align} \varphi(z) = \frac{(c_1 - 1) + (\bar{\alpha} + c_2) z}{\bar{\alpha}(c_1 + c_2z)} \qquad (z \in \mathbb{D}), \end{align} $$

for some scalars $c_1$ and $c_2$ such that at least one of them is nonzero.

Proof Here the two-dimensional model space $\mathcal {Q}_\theta $ is given by $\mathcal {Q}_\theta = \text {span} \{1, k(\cdot , \alpha )\}$ . As the space of all constant functions is invariant under every composition operators (see Remark 3.2), $\mathcal {Q}_\theta $ is invariant under $C_\varphi $ if and only if

$$ \begin{align*} k(\cdot, \alpha) \circ \varphi = \frac{1}{1 - \bar{\alpha} \varphi} \in \mathcal{Q}_\theta. \end{align*} $$

This is equivalent to the fact that

$$ \begin{align*} \frac{1}{1 - \bar{\alpha} \varphi} = \frac{c_1 + c_2 z}{1 - \bar{\alpha} z} \qquad (z \in \mathbb{D}), \end{align*} $$

for some scalars $c_1$ and $c_2$ such that at least one of them is nonzero, which is equivalent to (3.2). This completes the proof of the proposition.▪

Putting together the representations of linear fractional transformations from (3.2) and Theorem 3.1, it is perhaps evident that the answer to Question 3.3 will be also case-based.

4 Linear fractional symbols

Our aim in this section is to describe the structure of model invariant subspaces of composition operators whose symbols are linear fractional transformations mapping $\mathbb {D}$ into itself. We are also motivated by the intricate analysis presented in Cowen [Reference Cowen6] and Deddens [Reference Deddens7].

Before we begin with a general observation, we introduce the following (standard) notation: For each $\varphi \in H^\infty (\mathbb {D})$ , we denote by $M_\varphi $ the multiplication operator ${M_\varphi f = \varphi f}$ , $f \in H^2(\mathbb {D})$ . It is well known that $M_\varphi \in \mathcal {B}(H^2(\mathbb {D}))$ with $\|M_\varphi \| = \|\varphi \|_{\infty }$ for all $\varphi \in H^\infty (\mathbb {D})$ , and $\{M_z\}' = \{M_{\varphi }: \varphi \in H^\infty (\mathbb {D})\}$ , where $\{M_z\}'$ denotes the commutator of $M_z$ .

Let $\varphi $ be a holomorphic self-map of $\mathbb {D}$ and let $\theta $ be an inner function. Clearly, $C_\varphi \mathcal {Q}_\theta \subseteq \mathcal {Q}_\theta $ if and only if $C_\varphi ^*(\theta H^2(\mathbb {D})) \subseteq \theta H^2(\mathbb {D})$ , which is, by the Douglas range inclusion theorem [Reference Douglas8, Theorem 1] (as $\mbox {ran} (C_{\varphi }^* M_{\theta }) \subseteq \mbox {ran} M_{\theta }$ ), equivalent to the existence of some $X \in \mathcal {B}(H^2(\mathbb {D}))$ such that

$$ \begin{align*} C_\varphi^* M_\theta= M_\theta X. \end{align*} $$

Now if the above equality holds, then $\theta X(f) = C_{\varphi }^*(\theta f)$ for all $f \in H^2(\mathbb {D})$ , and hence zeros of $\theta $ are also zeros of $C_{\varphi }^*(\theta f)$ and

$$ \begin{align*} \text{multiplicity}_{w} \theta \leq \text{multiplicity}_{w} C_{\varphi}^*(\theta f), \end{align*} $$

for all $w \in \mathcal {Z}(\theta )$ (the zero set of $\theta $ ). This implies that $\frac {1}{\theta } C_\varphi ^*(\theta f)$ is a well defined holomorphic function on $\mathbb {D}$ . Therefore, we have proved the following general (but perhaps less practical) characterization.

Lemma 4.1 $Q_{\theta }$ is invariant under $C_\varphi $ if and only if $f \in H^2(\mathbb {D}) \mapsto \frac {1}{\theta } C_\varphi ^* M_\theta f$ defines a bounded linear operator on $H^2(\mathbb {D})$ .

Now we turn to linear fractional transformations. The following adjoint formula is due to Cowen [Reference Cowen6, Theorem 2]. There is a wide range of applications of Cowen’s adjoint formula (cf. [Reference Clifford and Zheng5, Reference Gallardo-Gutiérrez and Montes-Rodríguez10, Reference Gallardo-Gutiérrez and Schroderus11]).

Theorem 4.2 Let $\varphi (z)=\frac {az+b}{cz+d}$ be a nonconstant holomorphic self-map of $\mathbb {D}$ , where $ad - bc = 1$ . Then $\sigma (z) = \frac {\bar {a}z-\bar {c}} {-\bar {b}z+\bar {d}}$ is a holomorphic self-map of $\mathbb {D}$ , $g(z)= \frac {1}{-\bar {b}z+\bar {d}}$ and $h(z)=cz+d$ are in $H^\infty (\mathbb {D})$ , and $C_\varphi ^*=M_g C_\sigma M_h^*$ .

Note that if $\varphi $ is a constant map, then $\mathcal {Q}_\theta $ is invariant for $C_\varphi $ if and only if $\theta (0)=0$ . Indeed, the constant function $1 \in \mathcal {Q}_\theta $ if and only if $\theta (0) = \langle 1, \theta \rangle _{H^2(\mathbb {D})} = 0$ . Now we turn to nonconstant affine self-maps.

In what follows, we denote by $\mathcal {H}(\mathbb {D})$ either $H^2(\mathbb {D})$ or $H^\infty (\mathbb {D})$ .

Theorem 4.3 Let $\theta $ be an inner function, and let $\varphi (z)=az+b, a\neq 0$ . Suppose $\sigma (z)= \frac {\bar {a}z}{1-\bar {b}z}$ , $z \in \mathbb {D}$ . The following are equivalent.

  1. (1) $\mathcal {Q}_\theta \in \mathrm{Lat} C_\varphi $ .

  2. (2) $\frac {\theta \circ \sigma }{\theta } \in \mathcal {H}(\mathbb {D})$ .

  3. (3) $\theta H^2(\mathbb {D}) \in \mathrm{Lat} C_\sigma $ .

Proof If we apply Theorem 4.2 to the case when $c=0$ and $d = 1$ , we get

$$ \begin{align*} C_\varphi^*=M_\psi C_\sigma, \end{align*} $$

where $\psi (z)= \frac {1}{1-\bar {b}z}$ . Now suppose that $\mathcal {Q}_\theta $ is invariant under $C_\varphi $ . By Lemma 4.1, we know that the map

$$ \begin{align*} Xf= \frac{1}{\theta} C_\varphi^*M_\theta f \qquad (f \in H^2(\mathbb{D})), \end{align*} $$

defines a bounded linear operator X on $H^2(\mathbb {D})$ , and hence, using $C_\varphi ^*=M_\psi C_\sigma $ , we have

$$ \begin{align*} Xf = \frac{1}{\theta} C_\varphi^*M_\theta f = \frac{1}{\theta} \psi (\theta\circ\sigma) (f\circ\sigma) \in H^2(\mathbb{D}), \end{align*} $$

for all $f\in H^2(\mathbb {D})$ . Applying this with $f = 1$ yields

$$ \begin{align*} \psi\frac{\theta\circ\sigma}{\theta} \in H^2(\mathbb{D}). \end{align*} $$

But since $\frac {1}{\psi }= 1 - \bar {b}z \in H^\infty (\mathbb {D})$ , it follows that $\frac {\theta \circ \sigma }{\theta } \in H^2(\mathbb {D})$ . Theorem 2.1 then implies that $\theta H^2(\mathbb {D})$ is invariant under $C_\sigma $ . This proves $(1) \Rightarrow (2) \Rightarrow (3)$ .

Now we assume that $C_\sigma (\theta H^2(\mathbb {D})) \subseteq \theta H^2(\mathbb {D})$ . Again, Theorem 2.1 implies that $\frac {\theta \circ \sigma }{\theta } \in {\mathcal S}(\mathbb {D})$ , and therefore $\psi \frac {\theta \circ \sigma }{\theta } \in H^\infty (\mathbb {D})$ . Then $\frac {1}{\theta } C_{\varphi }^* M_\theta $ defines a bounded linear operator on $H^2(\mathbb {D})$ , and hence, $\mathcal {Q}_\theta $ is invariant under $C_\varphi $ . This proves that $(3) \Rightarrow (2) \Rightarrow (1)$ and completes the proof of the theorem.▪

Now we consider model spaces that are invariant under composition operators induced by linear fractional transformations. However, we will be restricted to inner functions that vanish at the origin. In fact, our main tool is the following adjoint formula [Reference Shapiro23, Equation (3.6)], which concerns functions vanishing at the origin:

Lemma 4.4 Let $\varphi (z)=\frac {az+b}{cz+d}$ be a nonconstant holomorphic self-map of $\mathbb {D}$ , where $ad - bc = 1$ . If $\sigma (z) = \frac {\bar {a}z-\bar {c}} {-\bar {b}z+\bar {d}}$ , then

$$ \begin{align*} C_\varphi^*f(z)=z\sigma'(z) \frac{f(\sigma(z))}{\sigma(z)} \qquad (f\in H^2(\mathbb{D}), f(0)=0). \end{align*} $$

As pointed our earlier, if $\theta $ is an inner function, then the constant function $1 \in \mathcal {Q}_\theta $ if and only if $\theta (0) = 0$ . In the following, under the assumption that the inner functions vanish at the origin, we present a classification of model spaces that are invariant under composition operators induced by linear fractional transformations. Recall that $\mathcal {H}(\mathbb {D})$ is either $H^2(\mathbb {D})$ or $H^\infty (\mathbb {D})$ .

Theorem 4.5 Let $\theta $ be an inner function, $\theta (0) = 0$ , and let $\varphi (z)= \frac {az+b}{cz+d}$ be a nonconstant holomorphic self-map of $\mathbb {D}$ , where $ad - bc = 1$ . Suppose $\sigma (z)= \frac {\bar {a}z-\bar {c}}{-\bar {b}z+\bar {d}}$ and

$$ \begin{align*} \psi = \frac{\frac{\theta}{z}\circ\sigma}{\frac{\theta}{z}}. \end{align*} $$

The following are equivalent:

  1. (1) $\mathcal {Q}_\theta \in \mathrm{Lat} C_\varphi $ .

  2. (2) $\psi \in \mathcal {H}(\mathbb {D})$ .

  3. (3) $\frac {\theta }{z}H^2(\mathbb {D}) \in \mathrm{Lat} C_\sigma $ .

Proof Since $\theta (0)=0$ , we see that $\frac {\theta }{z}$ is an inner function. Suppose that $\mathcal {Q}_\theta $ is invariant under $C_\varphi $ . Lemma 4.1 implies that

$$ \begin{align*} Xf = \frac{1}{\theta}C_\varphi^*(\theta f) \qquad (f \in H^2(\mathbb{D})), \end{align*} $$

defines a bounded linear operator X on $H^2(\mathbb {D})$ and $C_{\varphi }^* M_\theta = M_\theta X$ . In view of Lemma 4.4, it then follows that

$$ \begin{align*} Xf = \sigma' \frac{z (\theta\circ\sigma)}{\theta\sigma} (f\circ\sigma) = \sigma' \psi (f\circ\sigma), \end{align*} $$

where $\sigma '$ is the derivative of $\sigma $ . In particular

$$ \begin{align*} X1 = \sigma' \psi \in H^2(\mathbb{D}), \end{align*} $$

from which, using the fact that $\frac {1}{\sigma '} \in H^\infty (\mathbb {D})$ , it follows that $\psi \in H^2(\mathbb {D})$ . And finally, by Theorem 2.1, $\displaystyle \frac {\theta }{z}H^2(\mathbb {D})$ is invariant under $C_\sigma $ , which proves $(1) \Rightarrow (2) \Rightarrow (3)$ .

Now if $(3)$ is true, then Theorem 2.1 implies that $(2)$ is true, that is, $\psi \in H^\infty (\mathbb {D})$ . In particular, since $\sigma ' \in H^\infty (\mathbb {D})$ , X (defined as above) defines a bounded linear operator on $H^2(\mathbb {D})$ and satisfy the equality $C_{\varphi }^* M_\theta = M_\theta X$ . By Lemma 4.1, $\mathcal {Q}_\theta $ is invariant under $C_\varphi $ , which complete the proof of $(2) \Rightarrow (1)$ .▪

We do not know, in general, how to classify an inner function $\theta $ for which $\mathcal {Q}_\theta $ is invariant under a composition operator induced by a linear fractional transformation.

5 Applications

The main goal of this section is to discuss some direct applications of our main results to some elementary invariant subspaces of composition operators.

First, we prove that the identity map is the only self-map of $\mathbb {D}$ , which leaves all model spaces invariant.

Theorem 5.1 Let $\varphi $ be a holomorphic self-map of $\mathbb {D}$ . Then $\theta H^2(\mathbb {D})$ is invariant under $C_\varphi $ for all inner function $\theta $ if and only if $\varphi $ is the identity map.

Proof If $\varphi (z) = z$ , $z \in \mathbb {D}$ , then $C_\varphi = I_{H^2(\mathbb {D})}$ (the identity operator). In particular, $\theta H^2(\mathbb {D})$ is invariant under $C_\varphi $ . Conversely, suppose $\theta H^2(\mathbb {D})\in \mbox {Lat}C_\varphi $ for all inner function $\theta $ . Fix $\alpha \in \mathbb {D}$ . Then $\alpha $ is the only zero of the Blaschke factor (which is also an inner function) $b_\alpha (z) = \frac {\alpha - z}{1-\bar {\alpha } z}$ , $z \in \mathbb {D}$ . Since $b_\alpha H^2(\mathbb {D})\in \mbox {Lat}C_\varphi $ , by assumption, Theorem 2.1 implies that

$$ \begin{align*} \frac{b_\alpha\circ\varphi}{b_\alpha}\in {\mathcal S}(\mathbb{D}). \end{align*} $$

This forces $b_\alpha (\varphi (\alpha ))=0$ , and hence $\varphi (\alpha )=\alpha $ . Since $\alpha \in \mathbb {D}$ is arbitrary, we have that $\varphi (z)=z$ , $z\in \mathbb {D}$ , which completes the proof.▪

Before examining the other extreme property of the invariant subspaces of composition operators, we need to recall the following fact which concerns fixed points of holomorphic self-maps [Reference Bose, Muthukumar and Sarkar2, Corollary 3.4]: Let $\varphi $ be a holomorphic self-map of $\mathbb {D}$ and let $w \in \mathbb {D}$ be the fixed point of $\varphi $ . If $\theta $ is an inner function and $\theta (w)\neq 0$ , then $\theta H^2(\mathbb {D})$ is invariant under $C_\varphi $ if and only if $\theta \circ \varphi =\theta $ .

Recall that a point $w \in \mathbb {D}$ is said to be a fixed point of a holomorphic self-map $\varphi $ of $\mathbb {D}$ if $\varphi (w) = w.$

Theorem 5.2 Let $\theta $ be an inner function. Then $\theta H^2(\mathbb {D}) \in \mathrm{Lat} C_{\varphi }$ for all self-maps $\varphi $ of $\mathbb {D}$ if and only if $\theta $ is an unimodular constant.

Proof If $\theta $ is an unimodular constant, then $\frac {\theta \circ \varphi }{\theta }$ is also unimodular constant. Theorem 2.1 then implies that $\theta H^2(\mathbb {D})\in \mbox {Lat} C_\varphi $ .

Conversely, assume that $\theta H^2(\mathbb {D}) \in \mathrm{Lat} C_\varphi $ for all holomorphic self-map $\varphi $ of $\mathbb {D}$ . First, we claim that $\theta $ has no zeros in $\mathbb {D}$ . Suppose toward a contradiction that $\theta (\alpha )=0$ for some $\alpha \in \mathbb {D}$ . Since $\theta $ is an inner function, there exists $\beta \in \mathbb {D}$ such that $\theta (\beta ) \neq 0$ . Set

$$ \begin{align*} \varphi = b_{\beta} \circ b_{\alpha}. \end{align*} $$

Note that $\varphi $ is an inner function and $\varphi (\alpha ) = \beta $ . Therefore, $\frac {\theta \circ \varphi }{\theta } \notin H^\infty (\mathbb {D})$ , and hence, by Theorem 2.1, $\theta H^2(\mathbb {D})$ is not invariant under $C_\varphi $ . This contradiction completes the proof of the claim that $\theta (z)\neq 0$ for all $z\in \mathbb {D}$ . If we consider a constant function $\varphi \equiv c$ , then in view of the discussion preceding the statement of this theorem, $C_\varphi (\theta H^2(\mathbb {D})) \subseteq \theta H^2(\mathbb {D})$ implies that

$$ \begin{align*} \theta=\theta\circ\varphi\equiv\theta(c). \end{align*} $$

Since $\theta $ is an inner function, $\theta (c)$ must be unimodular, and hence $\theta $ is an unimodular constant. This completes the proof of the theorem.▪

Now we turn to special model invariant subspaces of composition operators. In the following, we will let $\theta $ and $\varphi $ denote inner function and holomorphic self-map of $\mathbb {D}$ , respectively.

Theorem 5.3 The following holds true:

  1. (1) $\mathcal {Q}_\theta \in \mathrm{Lat} C_\varphi $ for all inner function $\theta $ if and only if $\varphi $ is the identity map.

  2. (2) $\mathcal {Q}_\theta \in \mathrm{Lat} C_\varphi $ for all self-map $\varphi $ if and only if $\theta (z)=\alpha z$ or $\theta \equiv \alpha $ , where $\alpha $ is an unimodular constant.

Proof If $\mathcal {Q}_\theta \in \mathrm{Lat} C_\varphi $ for all inner function $\theta $ , then, in particular, $\mathcal {Q}_{b_{\alpha }}, \mathcal {Q}_{b_{\beta }} \in \mathrm{Lat} C_\varphi $ , where $\alpha \neq \beta $ are in $\mathbb {D} \setminus \{0\}$ . By Theorem 3.1, there exist nonzero scalars a and b such that

$$ \begin{align*} \varphi(z)= \frac{1-a}{\bar{\alpha}}+ a z = \frac{1-b}{\bar{\beta}} + b z \qquad (z \in \mathbb{D}). \end{align*} $$

Thus, comparing both sides of the above and noting the fact that $\alpha \neq \beta $ , we have $a = b =1$ , which implies that $\varphi (z)=z$ , $z\in \mathbb {D}$ . The converse part of $(1)$ is trivial.

Now we turn to prove $(2)$ . If $\theta (z)=\alpha z$ for some unimodular $\alpha $ , then $\mathcal {Q}_\theta = k(\cdot , 0) \mathbb {C}$ is the space of all constant functions, which is clearly invariant under all composition operators (cf. Remark 3.2). In the case of $\theta \equiv \alpha $ , we have $\mathcal {Q}_\theta =\{0\}$ , which is also invariant under all composition operators.

For the converse part, we first note that if $\mathcal {Q}_\theta =\{0\}$ , then $\theta H^2(\mathbb {D})=H^2(\mathbb {D})$ , and hence $\theta $ is an unimodular constant. So suppose, $\mathcal {Q}_\theta \neq \{0\}$ . Then there exist $\alpha \in \mathbb {D}$ and $f\in \mathcal {Q}_\theta $ such that $f(\alpha )\neq 0$ . By taking $\varphi \equiv \alpha $ , we see that $1 \in \mathcal {Q}_\theta $ , which implies

$$ \begin{align*} \theta(0)=\langle \theta, 1\rangle=0. \end{align*} $$

Then $\omega = \frac {\theta }{z}$ is an inner function. By Theorem 4.5, $\omega H^2(\mathbb {D})$ invariant under $C_\sigma $ for every linear fractional self-map $\sigma $ of $\mathbb {D}$ .

Now we claim that $\omega $ has no zeros in $\mathbb {D}$ . Suppose toward a contradiction that $\omega (\alpha )=0$ for some $\alpha \in \mathbb {D}$ . Since $\omega $ is an inner function, $\omega (\beta ) \neq 0$ for some $\beta \in \mathbb {D}$ . Set $\sigma = b_\beta \circ b_\alpha $ so that $\sigma (\alpha ) = \beta $ . Then

$$ \begin{align*} \frac{\omega\circ\sigma}{\omega} \notin H^\infty(\mathbb{D}), \end{align*} $$

and hence $\omega H^2(\mathbb {D})$ is not invariant under $C_\sigma $ . This is a contradiction, and hence $\omega (z)\neq 0$ , $z\in \mathbb {D}$ .

Finally, consider a nonautomorphic and holomorphic self-map $\sigma $ of $\mathbb {D}$ with a fixed point in $\mathbb {D}$ (for instance, consider $\sigma (z)= \frac {1}{2}z$ ). As $\omega H^2(\mathbb {D})$ invariant under $C_\sigma $ , by [Reference Bose, Muthukumar and Sarkar2, Corollary 3.5], it follows that $\omega $ is an unimodular constant. This implies that $\theta (z)=\alpha z$ for some unimodular constant $\alpha $ .▪

We conclude this section by proving a reducing property of composition operators. Here we will be restricted to finite-dimensional model spaces, as in Theorem 3.1. Before we begin this discussion, we recall the following result [Reference Bose, Muthukumar and Sarkar2, Corollary 2.4]:

Theorem 5.4 Let B be a Blaschke product and let $\varphi $ be a holomorphic self-map of $\mathbb {D}$ . Then $BH^2(\mathbb {D}) \in \mathrm{Lat}C_\varphi $ if and only if $\text {multiplicity}\ {}_w B \leq \text {multiplicity}\ {}_w {B\circ \varphi }$ for all $w \in \mathbb {D}$ such that $B(w)=0$ .

We are now ready for the reducing subspace property of elementary composition operators.

Theorem 5.5 Let $\varphi $ be a holomorphic self-map of $\mathbb {D}$ , $\alpha \in \mathbb {D}$ , $n \geq 1$ , and suppose $\theta (z)=\left (\frac {z- \alpha }{1-\bar {\alpha }z}\right )^n$ . Then $\mathcal {Q}_\theta $ reduces $C_\varphi $ if and only if there exist a scalar c, $|c| \leq 1$ , and $\psi \in \mathcal {S}(\mathbb {D})$ such that

$$ \begin{align*} \varphi(z)= \begin{cases} z \psi, & \mbox{if } \alpha = 0 \text{ and } n = 1 \\ c z, & \mbox{if } \alpha = 0 \text{ and } n \geq 2\\ z, & \mbox{if } \alpha \neq 0. \end{cases} \end{align*} $$

Proof Suppose $\alpha = 0$ . If $n=1$ , then the one-dimensional subspace $(z H^2(\mathbb {D}))^{\bot } = \mathcal {Q}_z$ is invariant under every composition operator (see Remark 3.2), where $z H^2(\mathbb {D})$ is invariant under $C_\varphi $ if and only if $\varphi = z \psi $ for some $\psi \in {\mathcal S}(\mathbb {D})$ (see Theorem 5.4). If $n \geq 2$ , then, by Theorem 3.1, $\mathcal {Q}_\theta $ is invariant under $C_\varphi $ if and only if $\varphi $ is an affine map. By Theorem 5.4, $\theta H^2(\mathbb {D})$ is invariant under $C_\varphi $ if and only if $\varphi = z \psi $ for some $\psi \in {\mathcal S}(\mathbb {D})$ . In particular, $\varphi (0)=0$ , and hence $\theta H^2(\mathbb {D})$ reduces $C_\varphi $ if and only if $\varphi (z)= cz$ for some $|c|\leq 1$ .

Finally, assume that $\alpha \neq 0$ . If $\varphi $ is the identity map, then $C_\varphi = I_{H^2(\mathbb {D})}$ , and hence $\mathcal {Q}_\theta $ reduces $C_\varphi $ . Next, we assume that $\mathcal {Q}_\theta $ reduces $C_\varphi $ . By Theorem 3.1, there exists a scalar $c (\neq 0)$ such that $\varphi (z)= \frac {1-c}{\bar {\alpha }} + cz$ . Again, by Theorem 5.4, $(\theta \circ \varphi )(\alpha )=0$ , and hence $\varphi (\alpha )= \alpha $ . Now

$$ \begin{align*} \frac{1-c}{\bar{\alpha}} + c \alpha = \alpha \end{align*} $$

is equivalent to

$$ \begin{align*} (1-c)(1-|\alpha|^2)=0. \end{align*} $$

As $|\alpha | < 1$ , we must have $c=1$ , that is, $\varphi (z)=z$ , $z\in \mathbb {D}$ , which completes the proof.▪

Finally, we would like to point out that the present theory of model spaces and composition operators complement the recent paper [Reference Bose, Muthukumar and Sarkar2]. The classification of Beurling type invariant subspaces of composition operators ([Reference Bose, Muthukumar and Sarkar2, Theorem 2.3] or Theorem 2.1) also plays an important role in our consideration, and evidently, some of our results are in duality (cf. Theorem 4.3 and 4.5). On the other hand, model spaces are fairly complex objects in operator theory and function theory, which also represent a large class of bounded linear operators. The present analysis clearly shows a challenging role of model spaces to the theory of composition operators (and vice versa).

Acknowledgment

The authors thank the referee for corrections and suggestions which helped to improve the presentation. The second author is supported in part by NBHM (National Board of Higher Mathematics, India) grant NBHM/R.P.64/2014, and the Mathematical Research Impact Centric Support (MATRICS) grant, File No: MTR/2017/000522, by the Science and Engineering Research Board (SERB), Department of Science & Technology (DST), Government of India.

References

Beurling, A., On two problems concerning linear transformations in Hilbert space . Acta Math. 81(1948), 239255.CrossRefGoogle Scholar
Bose, S., Muthukumar, P., and Sarkar, J., Beurling type invariant subspaces of composition operators . J. Oper. Theory 86(2021), 425438.CrossRefGoogle Scholar
Bourdon, P., Fry, E., Hammond, C., and Spofford, C., Norms of linear-fractional composition operators . Trans. Amer. Math. Soc. 356(2004), 24592480.CrossRefGoogle Scholar
Chalendar, I. and Partington, J., On the structure of invariant subspaces for isometric composition operators on ${H}^2(D)$ and ${H}^2\left({\mathbb{C}}^{+}\right)$ . Arch. Math. (Basel) 81(2003), 193207.CrossRefGoogle Scholar
Clifford, J. and Zheng, D., Composition operators on the Hardy space . Indiana Univ. Math. J. 48(1999), 15851616.Google Scholar
Cowen, C., Linear fractional composition operators on ${H}^2(D)$ . Integr. Equat. Oper. Theory 11(1988), 151160.CrossRefGoogle Scholar
Deddens, J., Analytic Toeplitz and composition operators . Canadian J. Math. 24(1972), 859865.CrossRefGoogle Scholar
Douglas, R. G., On majorization, factorization, and range inclusion of operators on Hilbert space . Proc. Amer. Math. Soc. 17(1966), 413415.CrossRefGoogle Scholar
Duren, P. L., Theory of  ${H}^p$ spaces, Academic Press, New York and London, 1970.Google Scholar
Gallardo-Gutiérrez, E. and Montes-Rodríguez, A., The role of the angle in supercyclic behavior . J. Funct. Anal. 203(2003), 2743.CrossRefGoogle Scholar
Gallardo-Gutiérrez, E. and Schroderus, R., The spectra of linear fractional composition operators on weighted Dirichlet spaces . J. Funct. Anal. 271(2016), 720745.CrossRefGoogle Scholar
Garcia, S. R., Mashreghi, J., and Ross, W. T., Introduction to model spaces and their operators, Cambridge Studies in Advanced Mathematics, 148, Cambridge University Press, Cambridge, 2016.CrossRefGoogle Scholar
Guyker, J., On reducing subspaces of composition operators . Acta Sci. Math. 53(1989), 369376.Google Scholar
Jones, M., Shift invariant subspaces of composition operators on  ${H}^p$ . Arch. Math. (Basel) 84(2005), 258267.CrossRefGoogle Scholar
Lefèvre, P., Li, D., Queffélec, H., and Rodríguez-Piazza, L., Some revisited results about composition operators on Hardy spaces . Rev. Mat. Iberoam. 28(2012), 5776.CrossRefGoogle Scholar
Mahvidi, A., Invariant subspaces of composition operators . J. Operator Theory 46(2001), 453476.Google Scholar
Matache, V., Invariant subspaces of composition operators . J. Operator Theory 73(2015), 243264.CrossRefGoogle Scholar
Montes-Rodríguez, A., Ponce-Escudero, M., and Shkarin, S., Invariant subspaces of parabolic self-maps in the Hardy space . Math. Res. Lett. 17(2010), 99107.CrossRefGoogle Scholar
Nordgren, E., Rosenthal, P., and Wintrobe, F., Composition operators and the invariant subspace problem . C. R. Math. Rep. Acad. Sci. Canada 6(1984), 279283.Google Scholar
Nordgren, E., Rosenthal, P., and Wintrobe, F., Invertible composition operators on ${H}^p$ . J. Funct. Anal. 73(1987), 324344.CrossRefGoogle Scholar
Radjavi, H. and Rosenthal, P., Invariant subspaces . In: Ergebnisse der Mathematik und ihrer Grenzgebiete, Band 77, Springer, New York and Heidelberg, 1973.Google Scholar
Shapiro, J. H., Composition operators and classical function theory, Springer, New York, 1993.CrossRefGoogle Scholar
Shapiro, J. H., Composition operators $\heartsuit$ Toeplitz operators. In: Five lectures in complex analysis, Contemp. Math., 525, American Mathematical Society, Providence, RI, 2010, pp. 117139.CrossRefGoogle Scholar