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R E S E A R C H

Open Access

A note on the Königs domain of compact

composition operators on the Bloch space

Matthew M Jones

Correspondence: m.m.jones@mdx. ac.uk

Department of Mathematics, Middlesex University, The Burroughs, London, NW4 4BT, UK

Abstract

LetDbe the unit disk in the complex plane. We define B0to be the little Bloch space of functionsfanalytic inDwhich satisfy lim|z|®1(1-|z|2)|f’(z)| = 0. If ϕ:DDis analytic then the composition operatorC:f↦f∘is a continuous operator that mapsB0into itself. In this paper, we show that the compactness ofC , as an operator onB0, can be modelled geometrically by its principal eigenfunction. In particular, under certain necessary conditions, we relate the compactness ofCto the geometry of=σ(D), wheressatisfies Schöder’s functional equation s∘= ’(0)s.

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

1 Introduction

LetD={z∈ C:|z|<1}be the unit disk in the complex plane andTits boundary. We define the Bloch spaceBto be the Banach space of functions,f, analytic inDwith

||f||B=|f(0)|+ sup zD(1− |z|

2)|f(z)|<.

This space has many important applications in complex function theory, see [1] for an overview of many of them. We denote byB0the little Bloch space of functions inB

that satisfy lim|z|®1 (1 -|z|2)|f ’(z)| = 0. This space coincides with the closure of the

polynomials inB.

Suppose now thatϕ:DDis analytic, then we may define the operator,C, acting onB0asf↦f∘. It was shown in [2] that every such operator mapsB0continuously

into itself. Moreover, it was proved thatCis compact onB0if and only ifsatisfies

lim

|z|→1

1− |z|2 1− |ϕ(z)|2|ϕ

(z)|= 0. (1)

Recall that the hyperbolic geometry onDis defined by the distance

disk(z,w) = inf

λD(η)|dη|

where the infimum is taken over all sufficiently smooth arcs that have endpointsz

andw.

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Here, λD(η) = (1− |η|2)−1is the Poincaré density ofD. The hyperbolic derivative of is given by’(z)/(1 -|(z)|2) and functions that satisfy (1) are called little hyperbolic Bloch functions or writtenϕBH0.

The Schröder functional equation is the equation

σϕ=γ σ. (2)

Note that this is just the eigenfunction equation forC. Kœnigs’theorem states that if has fixed point at the origin then (2) has a unique solution for g=’(0) which we call theKœnigs functionand denote bysfrom here on. In the study of the geometric properties of in relation to the operator theoretic properties ofC, it has become evident that the Kœnigs function is much more fruitful to study thanitself. In parti-cular, see [3] for a discussion of the Kœnigs function in relation to compact composi-tion operators on the Hardy spaces.

If we let=σ(D)be the Kœnigs domainof, then (2) may be interpreted as imply-ing that the action of onDis equivalent to multiplication bygonΩ. It is due to this that the pair (Ω,g) is often called the geometric model for.

In this paper, we study the geometry ofΩwhenϕB0H. In order to do this, we will use the hyperbolic geometry ofΩ. If f :Dis a universal covering map andΩis a hyperbolic domain in ℂ, then the Poincaré density onΩis derived from the equation

λ(f(z))|f(z)|=λD(z),

which is independent of the choice of f. Since this equation, in terms of differentials, is λ(w)|dw|=λD(z)|dz|(for w =f (z)), we see that the hyperbolic distance onD defined above carries over to a hyperbolic distance on Ω. For a more thorough treat-ment 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.Letbe a univalent self-map ofDwith a fixed point inD. Suppose that for some positive integer n0 there are at most finitely many points ofTat whichϕn0has

an angular derivative. Then the following are equivalent.

1. Some power of Cis compact on the Hardy space H2;

2.slies in Hpfor every p <∞;

3.=σ(D)does not contain a twisted sector.

Here, Ωis said to contain a twisted sectorif there is an unbounded curveΓ Î Ω with

δ(w)≥ε|w|

for someε> 0 and allwÎ Γ, whereδΩis the distance fromwto the boundary ofΩ 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

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onto Ωwiths(0) = 0 ands’(0) > 0. We will also define via the Schröder functional equation. Throughout we let

δ(w) = inf

ζ|wζ|,

so thatδΩ(w) is the Euclidean distance fromwto the boundary ofΩ.

Theorem 1.Letbe a univalent function mappingDintoD, (0) = 0.Suppose that the closure ofϕ(D)intersectsTonly at finitely many fixed points and is contained in a Stolz angle of opening no greater than aπthere.

If|’(0)| > 16 tan(aπ/2)then the following are equivalent

1.Cis compact onB;

2. lim w→∞

wγ δ(w) δ(γw) = 0; 3.For every n > 0,σnB

0.

Remark: It has recently been shown by Smith [6] that compactness of ConB is

equivalent to compactness of ConB0, BMOAandVMOAwhenis univalent and so

in the above theorem, the first condition could read: Cis compact onB,B0,BMOA

and VMOABefore proceeding, we prove the following lemma.

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

Proof. The first assertion follows from the fact that the closure of ϕ(D)touchesT only at fixed points. Suppose now that the second assertion is false and there are dis-tinct prime ends r1 andr2 with r1 =gr2. Then under the boundary correspondence

given by sthere are distinct pointsh,ζTwith

σ(η) =γ σ(ζ) =σ(ϕ(ζ)).

It follows thatϕ(ζ)∈Tand thereforeζ is a fixed point of . Hence, we have the contradiction r1=r2. □

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

By the results of Madigan and Matheson [2], and Smith [6] cited above Cis

com-pact onBif and only if

lim

|z|→1

1− |z|2 1− |ϕ(z)|2|ϕ

(z)|= 0.

However, by Schröder’s equation

1− |z|2

1− |ϕ(z)|2|ϕ(z)|=

λD(ϕ(z)) λD(z) |ϕ

(z)|

= λ(σϕ(z)) λ(σ(z))

|σϕ(z)ϕ(z)| |σ(z)|

=|γ|λw) λ(w)

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lim w

δ(w)

δ(γw)= 0. (3)

Since gΩ⊂Ω,gw® ∂Ωimplies thatw®∂Ω. Therefore, (3) holds if and only if

lim γw

δ(w) δ(γw) = 0.

By the Lemma, we see that gw ® ∂Ω means w ® ∞ and w Î gΩ, and we have shown that 1 and 2 are equivalent.

Suppose that 2 holds and letε> 0 be given. Then we can find aR> 0 so thatδΩ(w)

<εδΩ (gw) for all |w| >R, since there are only a finite number of prime ends at ∞. ChoosewÎ Ωarbitrarily with modulus greater than Rand let nsatisfy |g|-nR< |w|≤ |g|-n-1R.

Then we have that δΩ(w)<εnδΩ(gnw) and hence

−logδ(w) log|w| >

nlogε−logδ(γnw)

−(n+ 1) log|γ|+ logR.

Now as w®∞ingΩ,gnwlies in a closed set properly contained inΩand therefore

δΩ(gnw) is bounded below by a constant independent ofw. We thus have that

lim w→inf∞

−logδ(w) log|w| >

−logε

−log|γ|

and sinceεwas arbitrary, the left-hand side of the above inequality must tend to∞. Hence, we have shown that limw®∞|w|bδΩ(w) = 0 for everyb> 0.

Now σnB

0may 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

lim

w→∞f(w) = limw→∞

−logδ(w) log|w| =∞

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,

lim sup w→∞

δ(w)

δ(γw)≤K <1.

Sketch of Proof. First note that

lim sup

|w|→1

δ(w) δw)≤

16

|ϕ(0)|lim sup|z|→1

δϕ(D)(z) δD(z) .

Now ifϕ(D)lies in a non-tangential angle of openingaπat ζ, then a short calcula-tion shows that

lim sup zζ

δϕ(D)(z) δD(z) ≤tan

απ 2

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Now with fdefined above, we have

f(γw)−f(w) = −logδ(γw) log|γw|

−logδ(w) log|w|

∼ logδ(w)/δ(γw)

log|w| <0

for large enoughw. Hence,

δ(w) δw) =

|γ|f(γw)

|w|f(w)fw) ≤ |γ|

f(γw)0

asw®∞and so 2 holds. □

It is of interest to consider the growth of ssince condition 3 would imply that it has very slow growth. The following corollary follows from 3 and the fact that functions in B0grow at most of order log 1/(1-|z|).

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

log|σ(z)|=o

log log 1 1−r

.

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

Corollary 2.LetΩbe an unbounded domain inℂwithgΩ⊂Ωand0Î Ω. Suppose that hasΩonly finitely many prime ends at∞and

lim sup w→∞

δ(w) δ(γw)<1.

In addition, suppose that ∂gΩ ⊂ Ω. If σ:D, s(0) = 0, s’(0) > 0, and is defined by Schröder’s equation, then the following are equivalent.

1.Cis compact onB;

2.wlim→∞

wγ δ(w) δw) = 0; 3.For every n > 0,σnB

0.

The hypothesis on the boundary of Ωis vital. If we do not assume that ∂gΩ ⊂Ω, then we deduce from the proof of the Theorem thatϕB0His equivalent to

lim γw

δ(w)

δ(γw) = 0. (4)

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

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With the hypothesis that ∂gΩ ⊂Ω the prime ends at ∞ correspond to points of

ϕ(D) that touchT. Therefore, ϕ(D)∩Tis at most countable. A natural question to ask is whether or not(ϕ(D)∩T)can ever be positive, whereΛ 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 functionϕBH0such thatϕ(D)∩T=T.

Proof. We construct the domainΩso that it satisfies (4). Let 0 <g< 1 be given. We will define a nested sequencenT, n= 1, 2, ... so that

=∪n≥1

reiθ:γnr<∞,θn, (5)

whereΘn⊂Θn+1for alln= 1, 2, ....

First let N> 2 be chosen arbitrarily and letΘ1 = {2πk/N:k= 0, ...,N -1}.

Suppose now that Θn has been defined, then letΘn+1 be such thatΘn⊂ Θn+1and

whenever θÎΘnis isolated, we define a sequenceθk ÎΘn+1, k= 1, 2, ..., so thatθk®

θ ask®∞and for eachkthere is ajso thatθ-θk=θj -θ. Moreover, assume that

lim k→∞

θk+1θk

(θθk)2 = 0. (6)

In this way, we define the sequence of sets Θn, n = 1, 2, .... We will, furthermore, assume that for each e T, there is a sequenceθnÎ Θn,n= 1, 2, ...., such that θn®

θ.

We claim that this gives the desired domainΩwith boundary defined by (5). To see this, let gwÎ Ωbe arbitrary, then by construction, we may find aζÎ ∂Ωso thatδΩ(gw) = |ζ-gw|. It is readily seen that for suchζ, there is annso thatζÎ {reiθ:

r ≥g-n} for someθÎ Θnand moreover,θis isolated inΘn.

If we now consider w, we may find a sequence θk ® θ as k ® ∞ so that

{reiθk :rγn−1} ∈for all khence we may fix a kso that δΩ (w) = |w - n| for η=reiθk.

By estimating the line segment [w,h] by the arc ofrTjoining wtoh, we see thatδΩ (w)≍ |w||a -θk| wherew =reia.Therefore, we have the estimate δΩ (w)≤|w||θk+1

-θk|. By a similar argument, we deduce the estimateδΩ(gw)≍ |gw||θ-θk| and so

δ(w) δw) ≤γ

−1θk+1θk θθk

γ−1|θθk|

by (6) and so the construction is complete.

We claim that if σ:Dis defined as usual and is given by Schröder’s equa-tion, thenϕ(D)∩T=T.

In fact, ifθÎ Θnis isolated, then the rayR= {reiθ:r≥g-n-1} is contained in a single prime end of Ω. Therefore, to each such ray, there exists a pointζTthat corre-sponds toRunders. Since gR⊂∂Ω, we thus have that ζcorresponds to a prime end

punderwithpT=∅.

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Hence, eachηTis contained in a prime end ofϕ(D)and

ϕ(D) =D\ θnisolated

ρθ.

The result follows. □

3 Multiply connected domains

The geometric arguments of the previous section potentially lend themselves to multi-ply connected domains in the following way. Suppose that Ωis a domain in ℂwith 0 Î ΩandgΩ⊂Ωfor someγD\{0}. Letsbe a universal covering map ofDontoΩ withs(0) = 0. Thens’(0)≠0 and we may definevia (2). Now we have

1− |z|2

1− |ϕ(z)|2|ϕ(z)|=|γ| λ(γw)

λ(w) .

However, if Ωis not simply connected, thensis an infinitely sheeted covering ofΩ and therefore the equations(z) = 0 has infinitely many distinct solutions,zn,n= 0, 1, ....

Now, since

1− |zn|2 1− |ϕ(zn)|2|ϕ

(zn)|=|γ|>0

for all n≥0, we see thatϕBH0. Thus, we have proved the following result.

Proposition 1.Suppose thatΩ ⊂ℂis a domain satisfying0Î ΩandgΩ⊂Ω, and letσ :Dbe a universal covering map withs(0) = 0.

If, as defined by (2) is inBH0thenΩis simply connected.

4 Competing interests

The author declares that they have no competing interests.

Received: 31 January 2011 Accepted: 10 August 2011 Published: 10 August 2011

References

1. Anderson, JM: Bloch Functions: The Basic Theory. Operators and Function Theory. D Reidel. 1–17 (1985)

2. Madigan, K, Matheson, A: Compact Composition Operators on the Bloch Space. Trans Am Math Soc.347, 2679–2687 (1995). doi:10.2307/2154848

3. Shapiro, JH: Composition Operators and Classical Function Theory. Springer. (1993) 4. Ahlfors, LV: Conformal Invariants, Topics in Geometric Function Theory. McGraw-Hill. (1973)

5. JH, Shapiro, W, Smith, A, Stegenga: Geometric models and compactness of composition operators. J Funct Anal.127, 2162 (1995). doi:10.1006/jfan.1995.1002

6. Smith, W: Compactness of composition operators on BMOA. Proc Am Math Soc.127, 2715–2725 (1999). doi:10.1090/ S0002-9939-99-04856-X

7. Bourdon, P, Cima, J, Matheson, A: Compact composition operators on BMOA. Trans Am Math Soc.351, 2183–2196 (1999). doi:10.1090/S0002-9947-99-02387-9

doi:10.1186/1029-242X-2011-31

Cite this article as:Jones:A note on the Königs domain of compact composition operators on the Bloch space.

References

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