Open Access

A note on the Königs domain of compact composition operators on the Bloch space

Journal of Inequalities and Applications20112011:31

Received: 31 January 2011

Accepted: 10 August 2011

Published: 10 August 2011


Let be the unit disk in the complex plane. We define to be the little Bloch space of functions f analytic in which satisfy lim|z|→1(1 - |z|2)|f'(z)| = 0. If is analytic then the composition operator C φ : f f φ is a continuous operator that maps into itself. In this paper, we show that the compactness of C φ , as an operator on , can be modelled geometrically by its principal eigenfunction. In particular, under certain necessary conditions, we relate the compactness of C φ to the geometry of , where σ satisfies Schöder's functional equation σ φ = φ'(0)σ.

2000 Mathematics Subject Classification: Primary 30D05; 47B33 Secondary 30D45.

1 Introduction

Let be the unit disk in the complex plane and its boundary. We define the Bloch space to be the Banach space of functions, f, analytic in with

This space has many important applications in complex function theory, see [1] for an overview of many of them. We denote by the little Bloch space of functions in that satisfy lim|z|→1(1 - |z|2)|f '(z)| = 0. This space coincides with the closure of the polynomials in .

Suppose now that is analytic, then we may define the operator, C φ , acting on as f f φ. It was shown in [2] that every such operator maps continuously into itself. Moreover, it was proved that C φ is compact on if and only if φ satisfies
Recall that the hyperbolic geometry on is defined by the distance

where the infimum is taken over all sufficiently smooth arcs that have endpoints z and w.

Here, is the Poincaré density of . The hyperbolic derivative of φ is given by φ'(z)/(1 - |φ(z)|2) and functions that satisfy (1) are called little hyperbolic Bloch functions or written .

The Schröder functional equation is the equation

Note that this is just the eigenfunction equation for C φ . Kœnigs' theorem states that if φ has fixed point at the origin then (2) has a unique solution for γ = φ'(0) which we call the Kœnigs function and denote by σ from here on. In the study of the geometric properties of φ in relation to the operator theoretic properties of C φ , it has become evident that the Kœnigs function is much more fruitful to study than φ itself. In particular, see [3] for a discussion of the Kœnigs function in relation to compact composition operators on the Hardy spaces.

If we let be the Kœnigs domain of φ, then (2) may be interpreted as implying that the action of φ on is equivalent to multiplication by γ on Ω. It is due to this that the pair (Ω, γ ) is often called the geometric model for φ.

In this paper, we study the geometry of Ω when . In order to do this, we will use the hyperbolic geometry of Ω. If is a universal covering map and Ω is a hyperbolic domain in , then the Poincaré density on Ω is derived from the equation

which is independent of the choice of f. Since this equation, in terms of differentials, is (for w = f (z)), we see that the hyperbolic distance on defined above carries over to a hyperbolic distance on Ω. For a more thorough treatment of the hyperbolic metric, see [4].

In [5], the Königs domain of a compact composition operator on the Hardy space was studied and the following result was proved.

Theorem A. Let φ be a univalent self-map of with a fixed point in . Suppose that for some positive integer n0there are at most finitely many points of at which has an angular derivative. Then the following are equivalent.

  1. 1.

    Some power of C φ is compact on the Hardy space H2;

  2. 2.

    σ lies in H p for every p < ∞;

  3. 3.

    does not contain a twisted sector.

Here, Ω is said to contain a twisted sector if there is an unbounded curve Γ Ω with

for some ε > 0 and all w Γ, where δΩ is the distance from w to the boundary of Ω as defined below. The purpose of this paper is to provide a similar result to this in the context of the Bloch space.

2 Simply connected domains

Throughout this section, we assume that Ω is an unbounded simply connected domain in with 0 Ω. As in the previous section, σ represents the Riemann mapping of onto Ω with σ(0) = 0 and σ'(0) > 0. We will also define φ via the Schröder functional equation. Throughout we let

so that δΩ(w) is the Euclidean distance from w to the boundary of Ω.

Theorem 1. Let φ be a univalent function mapping into , φ(0) = 0. Suppose that the closure of intersects only at finitely many fixed points and is contained in a Stolz angle of opening no greater than απ there.

If |φ'(0)| > 16 tan(απ/ 2) then the following are equivalent

1. C φ is compact on ;

2. ;

3. For every n > 0, .

Remark: It has recently been shown by Smith [6] that compactness of C φ on is equivalent to compactness of C φ on , BMOA and VMOA when φ is univalent and so in the above theorem, the first condition could read: C φ is compact on , , BMOA and VMOA Before proceeding, we prove the following lemma.

Lemma 1. Under the hypotheses of the theorem, w and γw tend to the same prime end at ∞, and ∂γ Ω Ω.

Proof. The first assertion follows from the fact that the closure of touches only at fixed points. Suppose now that the second assertion is false and there are distinct prime ends ρ1 and ρ2 with ρ1 = γρ2. Then under the boundary correspondence given by σ there are distinct points η, with

It follows that and therefore ζ is a fixed point of φ. Hence, we have the contradiction ρ1 = ρ2.    □

Proof. We first prove that 1 is equivalent to 2.

By the results of Madigan and Matheson [2], and Smith [6] cited above C φ is compact on if and only if
However, by Schröder's equation
Since Ω is simply connected, λΩ (w) 1/δΩ (w) and so C φ is compact on if and only if
Since γ Ω Ω, γw → ∂Ω implies that w → ∂Ω. Therefore, (3) holds if and only if

By the Lemma, we see that γw → ∂Ω means w → ∞ and w γ Ω, and we have shown that 1 and 2 are equivalent.

Suppose that 2 holds and let ε > 0 be given. Then we can find a R > 0 so that δΩ (w) <εδΩ (γw) for all |w| > R, since there are only a finite number of prime ends at . Choose w Ω arbitrarily with modulus greater than R and let n satisfy |γ| -n R < |w| ≤ |γ |-n -1R.

Then we have that δΩ (w) < ε n δΩ (γ n w) and hence
Now as w → ∞ in γ Ω, γ n w lies in a closed set properly contained in Ω and therefore δΩ (γ n w) is bounded below by a constant independent of w. We thus have that

and since ε was arbitrary, the left-hand side of the above inequality must tend to ∞. Hence, we have shown that limw→∞|w| β δΩ (w) = 0 for every β > 0.

Now may be interpreted geometrically as limw→∂Ωn|w| n-1δΩ (w) = 0 and this follows from the above argument. Therefore, 2 implies 3.

To show that 3 implies 2, we need to show that if

then 2 holds.

To complete the proof, we require the following lemma whose proof we merely sketch.

Lemma 2. Under the hypotheses of the theorem,
Sketch of Proof. First note that
Now if lies in a non-tangential angle of opening απ at ζ, then a short calculation shows that

and the assertion follows.    □

Now with f defined above, we have
for large enough w. Hence,

as w → ∞ and so 2 holds.    □

It is of interest to consider the growth of σ since condition 3 would imply that it has very slow growth. The following corollary follows from 3 and the fact that functions in grow at most of order log 1/(1 - |z|).

Corollary 1. Suppose that φ satisfies the hypotheses of the Theorem and that any of the equivalent conditions holds, then for r = |z|.

We also provide the following restatement of the hypotheses of Theorem 1 to illustrate the main properties of the Königs domain.

Corollary 2. Let Ω be an unbounded domain in with γ Ω Ω and 0 Ω. Suppose that has Ω only finitely many prime ends atand

In addition, suppose thatγ Ω Ω. If , σ(0) = 0, σ'(0) > 0, and φ is defined by Schröder's equation, then the following are equivalent.

1. C φ is compact on ;

2. ;

3. For every n > 0, .

The hypothesis on the boundary of Ω is vital. If we do not assume that ∂γ Ω Ω, then we deduce from the proof of the Theorem that is equivalent to

In this situation, the finite part of the boundary of Ω plays a complicated role in the behaviour of φ. We conclude this section by constructing a domain that displays very bad boundary properties. This answers a question of Madigan and Matheson in [2].

In [2] it was shown that if ∂φ(D) touches in a cusp, then . However, it is not sufficient that ∂φ(D) touches at an angle greater that 0. The question was raised of whether or not it is possible that can be infinite.

With the hypothesis that ∂γ Ω Ω the prime ends at ∞ correspond to points of that touch . Therefore, is at most countable. A natural question to ask is whether or not can ever be positive, where Λ represents linear measure.

This example is well known in the setting of the unit disk, see [7, Corollary 5.3]. We describe here the construction in terms of the Königs domain.

Theorem 2. There is a univalent function such that .

Proof. We construct the domain Ω so that it satisfies (4). Let 0 < γ < 1 be given. We will define a nested sequence , n = 1, 2, ... so that

where Θ n Θn+1for all n = 1, 2, ....

First let N > 2 be chosen arbitrarily and let Θ1 = {2πk/N : k = 0, ..., N - 1}.

Suppose now that Θ n has been defined, then let Θn+1be such that Θ n Θn+1and whenever θ Θ n is isolated, we define a sequence θ k Θn+1, k = 1, 2, ..., so that θ k θ as k → ∞ and for each k there is a j so that θ - θ k = θ j -θ . Moreover, assume that

In this way, we define the sequence of sets Θ n , n = 1, 2, .... We will, furthermore, assume that for each , there is a sequence θ n Θ n , n = 1, 2, ...., such that θ n θ.

We claim that this gives the desired domain Ω with boundary defined by (5).

To see this, let γw Ω be arbitrary, then by construction, we may find a ζ ∂Ω so that δΩ (γw) = |ζ - γw|. It is readily seen that for such ζ, there is an n so that ζ {reiθ: rγ-n} for some θ Θ n and moreover, θ is isolated in Θ n .

If we now consider w, we may find a sequence θ k θ as k → ∞ so that for all k hence we may fix a k so that δΩ (w) = |w - n| for .

By estimating the line segment [w, η] by the arc of joining w to η, we see that δΩ (w) |w|| α - θ k | where w = re.Therefore, we have the estimate δΩ (w) ≤ |w||θk+1- θ k |. By a similar argument, we deduce the estimate δΩ (γw) |γw||θ - θ k | and so

by (6) and so the construction is complete.

We claim that if is defined as usual and φ is given by Schröder's equation, then .

In fact, if θ Θ n is isolated, then the ray R = {reiθ: rγ-n-1} is contained in a single prime end of Ω. Therefore, to each such ray, there exists a point that corresponds to R under σ. Since γR ∂Ω, we thus have that ζ corresponds to a prime end p under φ with .

On the other hand, if θ Θ n is isolated, then R' = {reiθ: γ-nr < γ-n-1} satisfies γR'∩ ∂Ω = , and so there is an arc such that σ (ρ θ ) = R' and ρ θ has an end-point in .

Hence, each is contained in a prime end of and

The result follows.    □

3 Multiply connected domains

The geometric arguments of the previous section potentially lend themselves to multiply connected domains in the following way. Suppose that Ω is a domain in with 0 Ω and γ Ω Ω for some . Let σ be a universal covering map of onto Ω with σ(0) = 0. Then σ'(0) ≠ 0 and we may define φ via (2). Now we have

However, if Ω is not simply connected, then σ is an infinitely sheeted covering of Ω and therefore the equation σ (z) = 0 has infinitely many distinct solutions, z n , n = 0, 1, ....

Now, since

for all n ≥ 0, we see that . Thus, we have proved the following result.

Proposition 1. Suppose that Ω is a domain satisfying 0 Ω and γ Ω Ω, and let be a universal covering map with σ(0) = 0.

If φ, as defined by (2) is in then Ω is simply connected.


Authors’ Affiliations

Department of Mathematics, Middlesex University, The Burroughs


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© Jones; licensee Springer. 2011

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