New Subclasses of Univalent Mappings in Several Complex Variables: Extension Operators and Applications

Abstract

In this paper we define new subclasses of univalent mappings in the case of several complex variables. We will focus our attention on a particular class, denoted \(E_{1}^{\ast}\), and observe that in the case of one complex variable, \(E_{1}^{\ast}(U)\)\ coincides with the class of convex functions \(K\) on the unit disc. However, if \(n\geq2\), then \(E_{1}^{\ast (\mathbb{B}^{n})\) is different from the class of convex mappings \(K(\mathbb{B}^{n})\) on the Euclidean unit ball \(\mathbb{B}^{n}\) in \(\mathbb{C}^{n}\). Along with this, we will study other properties of the class \(E_{1}^{\ast}\) on the unit polydisc, respectively on the Euclidean unit ball in \(\mathbb{C}^{n}\). In the second part of the paper we discuss the Graham–Kohr extension operator n,\U{3b1} (defined by Graham and Kohr in Complex Variab. Theory Appl. 47:59-72, 2002). They proved that the extension operator \(\Psi_{n,\U{3b1} }\) does not preserve convexity for \(n\geq2\) for all \(\U{3b1} \in \lbrack0,1]\). However, in this paper we prove that \(\Psi_{n,0}(K)\) and \(\Psi_{n,1}(K)\) are subsets of the class \(E_{1}^{\ast}\left( \mathbb{B}^{n}\right)\) which is different from the class \(K(\mathbb{B}^{n})\) for the Euclidean case.

Authors

Eduard Ştefan Grigoriciuc
Department of Mathematics, Faculty of Mathematics and Computer Science, Babeş-Bolyai University, Cluj-Napoca, Romania

Keywords

Biholomorphic mapping; Convex mapping; Starlike mapping; Extension operator.

Paper coordinates

E.S. Grigoriciuc, New subclasses of univalent mappings in several complex variables: extension operators and applications, Computational Methods and Function Theory, 23 (2023), pp. 533–555, https://doi.org/10.1007/s40315-022-00467-z

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Computational Methods and Function Theory

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Springer

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1617-9447
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2195-3724

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New Subclasses of Univalent Mappings in Several Complex Variables. Extension Operators and Applications
\jyear

2021

[1]\fnmEduard Ştefan \surGrigoriciuc

[1]\orgdivDepartment of Mathematics, \orgnameFaculty of Mathematics and Computer Science, Babeş-Bolyai University, \orgaddress\street1 M. KogΔƒlniceanu Str., \cityCluj-Napoca, \postcode400084, \stateCluj, \countryRomania

New Subclasses of Univalent Mappings in Several Complex Variables. Extension Operators and Applications

Abstract

In this paper we define new subclasses of univalent mappings in the case of several complex variables. We will focus our attention on a particular class, denoted E1βˆ—, and observe that in the case of one complex variable, E1βˆ—β’(U) coincides with the class of convex functions K on the unit disc. However, if nβ‰₯2, then E1βˆ—β’(𝔹n) is different from the class of convex mappings K⁒(𝔹n) on the Euclidean unit ball 𝔹n in β„‚n. Along with this, we will study other properties of the class E1βˆ— on the unit polydisc, respectively on the Euclidean unit ball in β„‚n. In the second part of the paper we discuss about Graham-Kohr extension operator Ξ¨n,Ξ± (defined by I. Graham and G. Kohr in Complex Variables Theory Appl. 47 (2002), 59–72). They proved that the extension operator Ξ¨n,Ξ± does not preserve convexity for nβ‰₯2 for all α∈[0,1]. However, in this paper we prove that Ξ¨n,0⁒(K) and Ξ¨n,1⁒(K) are subsets of the class E1βˆ—β’(𝔹n) which is different from the class K⁒(𝔹n) for the Euclidean case.

keywords:
Biholomorphic mapping, Convex mapping, Starlike mapping, Extension operator
pacs:
[

MSC Classification]32H02, 30C45

1 Introduction

Let β„‚n denote the space of n complex variables z=(z1,…,zn) equipped with an arbitrary norm βˆ₯β‹…βˆ₯βˆ—. Let Bn={zβˆˆβ„‚n:β€–zβ€–βˆ—<1} be the unit ball in β„‚n with respect to the arbitrary norm βˆ₯β‹…βˆ₯βˆ—. In the case of one complex variable, B1 is denoted by U.

Let H⁒(Bn) denote the set of all holomorphic mappings from Bn into β„‚n. If f∈H⁒(Bn), we say that f is normalized if f⁒(0)=0 and D⁒f⁒(0)=In, where D⁒f⁒(z) is the complex Jacobian matrix of f at z and In is the identity operator in β„‚n. Let S⁒(Bn) be the set of all normalized univalent mappings in H⁒(Bn). In the case of one complex variable we denote the class of normalized univalent functions by S.

A mapping f∈S⁒(Bn) is called convex (starlike) if its image is a convex (starlike with respect to the origin) set in β„‚n. The class of normalized convex mappings is denoted by

K⁒(Bn)={f∈S⁒(Bn):f⁒(Bn)⁒ is a convex set in ⁒ℂn}

and the class of normalized starlike mappings is denoted by

Sβˆ—β’(Bn)={f∈S⁒(Bn):f⁒(Bn)⁒ is a starlike set with respect to zero in ⁒ℂn}.

In the case of one complex variable, the sets K⁒(U) and Sβˆ—β’(U) are denoted by K and Sβˆ—. For details, one may consult Dur , Goo , GrKo1 or Ko1 . In Rob Robertson introduced the class of starlike (respectively convex) functions of order Ξ± on the unit disc U, where α∈[0,1). Hence, we denote by

K⁒(Ξ±)={f∈S:Re⁒[1+΢⁒f′′⁒(ΞΆ)f′⁒(ΞΆ)]>Ξ±,΢∈U}

the class of convex functions of order Ξ± on U and by

Sβˆ—β’(Ξ±)={f∈S:Re⁒[΢⁒f′⁒(ΞΆ)f⁒(ΞΆ)]>Ξ±,΢∈U}

the class of starlike functions of order Ξ± on U. There are also generalizations of these classes in several complex variables (see Curt Cu1 , Kohr Ko2 or Ko3 , Liu Liu1 ). When we refer to these classes in the context of several complex variables, then K⁒(Bn;Ξ±) denotes the class of all normalized biholomorphic convex mappings of order Ξ± on Bn and Sβˆ—β’(Bn;Ξ±) denotes the class of all normalized biholomorphic starlike mappings of order Ξ± on Bn.

Remark 1.

Notice that, throughout this paper, we denote by β„€+=β„•βˆͺ{0} the set of non-negative integers and by β„€+βˆ—=β„•={1,2,3,…} the set of natural numbers (positive integers).

Remark 2.

During this paper we are working on different domains (unit balls in β„‚n with respect to different norms), as follows:

  • β€’

    𝔹n – the Euclidean unit ball in β„‚n with respect to the Euclidean norm β€–zβ€–=βˆ‘j=1n|zj|2, for all z=(z1,…,zn)βˆˆβ„‚n.

For the Euclidean case, we denote the Euclidean norm simply βˆ₯β‹…βˆ₯ without any index. Hence, in this paper, when we use the notation βˆ₯β‹…βˆ₯, we automatically refer to the Euclidean norm.

  • β€’

    π•Œn – the unit polydisc in β„‚n with respect to the maximum norm β€–zβ€–βˆž=max⁑{|zj|:j=1,nΒ―}, for all z=(z1,…,zn)βˆˆβ„‚n.

  • β€’

    Bpn – the unit ball in β„‚n with respect to the p-norm β€–zβ€–p=[βˆ‘j=1n|zj|p]1/p, for all z=(z1,…,zn)βˆˆβ„‚n and p∈[1,∞).

In the case of one complex variable, each of the sets 𝔹1, π•Œ1 and Bp1 coincides with U. Mention that when we work with an arbitrary norm, it will be denoted βˆ₯β‹…βˆ₯βˆ—. But, when the domains are those described above, we use the particular notations for unit balls and norms presented for every case. For details one may consult GrKo1 or Ko1 .

Another important result that we will refer to during this paper is Alexander’s duality theorem which says that f∈K if and only if ΢⁒f′⁒(ΞΆ)∈Sβˆ—, ΢∈U (see (Dur, , Theorem 2.12), (Goo, , Chapter 8, Theorem 5) or (GrKo1, , Theorem 2.2.6)).

Remark 3.

It is important to notice that the Alexander’s duality theorem is no longer true in the case of several complex variables (for details one may consult (GrKo1, , Remark 6.3.15) and examples given in (GrKo1, , Problem 6.2.5), (GrKo1, , Problem 6.3.2) and (Suf1, , Example 3)).

When we refer to the starlikeness of a mapping of several complex variables, we can use the following analytical characterization result given by Matsuno (see (GrKo1, , Theorem 6.2.2) or Mat ):

Theorem 1.

Let f:𝔹nβ†’β„‚n be a locally biholomorphic mapping such that f⁒(0)=0. Then f is starlike if and only if

Re⁒⟨[D⁒f⁒(z)]βˆ’1⁒f⁒(z),z⟩>0,zβˆˆπ”Ήnβˆ–{0}. (1)

A very useful tool in the geometric function theory of one and several complex variables are the Loewner chains. Next we present the definition of the Loewner chains in β„‚n, as well as their connection with univalent mappings (for details, one may consult (ArBrHaKo , GrKo1 or GrKoKo1 ).

Definition 1.

(see ArBrHaKo , GrKo1 or GrKoKo1 ) A mapping L=L⁒(z,t):𝔹nΓ—[0,∞)β†’β„‚n is called a Loewner chain (normalized univalent subordination chain) if the following conditions hold:

  1. 1.

    eβˆ’t⁒L⁒(β‹…,t)∈S⁒(𝔹n), for all t∈[0,∞);

  2. 2.

    L⁒(𝔹n,s)βŠ†L⁒(𝔹n,t), for all 0≀s≀t<∞.

Remark 4.

In (Pom1, , Theorem 6.1) (see also GrKo1 ) we can find a very important result in the case of one complex variable which says that for every f∈S there exists a Loewner chain L=L⁒(΢,t) such that f⁒(΢)=L⁒(΢,0), for all ΢∈U.

In order to extend the previous result in the case of several complex variables, I. Graham, H. Hamada and G. Kohr (see GrHaKo1 or GrKo1 ) defined the family S0⁒(𝔹n) of normalized univalent mappings which have parametric representation as follows

S0(𝔹n)={f∈S(𝔹n):βˆƒL(z,t)Β a Loewner chain such that the family

{eβˆ’tL(β‹…,t)}tβ‰₯0Β is a normal family on 𝔹nΒ andΒ f=L(β‹…,0)}

Remark 5.

Recall that a family β„± is called a normal family if each sequence in β„± either has a subsequence that converges locally uniformly or else has a subsequence that is compactly divergent (see (Ko1, , Definition 1.3.4)).

Remark 6.

It is clear that if n=1, then S0⁒(𝔹1)=S. However, if nβ‰₯2, then S0⁒(𝔹n)β«‹S⁒(𝔹n) (for details, one may consult GrHaKo1 , GrKo1 or GrKoKo1 ). Another important results regarding to the family of normalized univalent mappings which have parametric representation S0⁒(𝔹n) can be found in GrHaKoKo1 , GrKoKo1 and GrKoPf1 .

The problem of constructing examples of starlike (respectively convex) mappings in β„‚n is partially solved in terms of extension operators. Two of the most important extension operators are defined by K. Roper and T.J. Suffridge (in 1995, see RoSuf0 ), respectively by I. Graham and G. Kohr (in 2002, see GrKo2 ). Such operators extend classes of univalent functions to some classes of univalent mappings in β„‚n. For more details about extension operators and properties of them one may consult GrHaKoSuf1 , GrKo3 and GrKoPf1 .

Let α∈[0,1]. In 2002, I. Graham and G. Kohr (see GrKo2 ) introduced the extension operator Ψn,α defined for normalized locally univalent functions on U by

Ξ¨n,α⁒(f)⁒(z)=(f⁒(z1),[f⁒(z1)z1]α⁒zβˆ—),z=(z1,zβˆ—)βˆˆπ”Ήn, (2)

where f⁒(z1)β‰ 0, for z1∈Uβˆ–{0} and the branch of the power function is chosen such that (f⁒(z1)z1)Ξ±|z1=0=1.

Remark 7.

In (GrKo2, , Corollary 3.3) Graham and Kohr proved that Ξ¨n,α⁒(Sβˆ—)βŠ†Sβˆ—β’(𝔹n), for all α∈[0,1]. Also in (GrKo2, , Remark 3.6) the authors shows that Ξ¨n,Ξ± does not preserve convexity for nβ‰₯2, for all α∈[0,1].

In the second section of our paper, we introduce two new subclasses Ek and Ekβˆ— of univalent mappings of one and several complex variables. We will give the definitions in a general setting (on the unit ball Bn in β„‚n with respect to an arbitrary norm) and some particular examples on the Euclidean unit ball 𝔹n.

The third section contains some general properties of the previously defined subclasses of univalent mappings. We will highlight the fact that in the case of one complex variable, E1βˆ—β’(U) coincides with the class of convex functions K on the unit disc U, but this result is not longer true in the case of several complex variables.

In the last part of this paper, we discuss about the preservation of some new subclasses of univalent mappings by the Graham-Kohr extension operator Ξ¨n,Ξ± defined in (2). It is interesting that although the operator Ξ¨n,Ξ± does not keep the convexity, still in some particular cases, the class K is taken to a class that we will define in the next section.

2 New Subclasses of Univalent Mappings

This section is dedicated to the study of new subclasses of univalent mappings in several complex variables. We will give the definitions in a general setting (on the unit ball Bn in β„‚n with respect to an arbitrary norm βˆ₯β‹…βˆ₯βˆ—), but a few properties will be presented on some particular domains, especially, on the Euclidean unit ball 𝔹n.

Definition 2.

Let kβˆˆβ„€+ and let f:Bnβ†’β„‚n be a holomorphic mapping such that f⁒(0)=0 and D⁒f⁒(0)=In. Also, let f⁒(z)=z+βˆ‘m=2∞Pm⁒(z) be the power series expansion of f on the unit ball Bn, where

Pm⁒(z)=1m!⁒Dm⁒f⁒(0)⁒(zm),z∈Bn.

Then we define

(Gk⁒f)⁒(z)={Dk⁒f⁒(z)⁒(zk)+z+βˆ‘m=2kβˆ’1Pm⁒(z),kβ‰₯3D2⁒f⁒(z)⁒(z2)+z,k=2D⁒f⁒(z)⁒(z),k=1f⁒(z),k=0, (3)

for all z∈Bn.

Definition 3.

Let kβˆˆβ„€+. We define the following subclasses of normalized univalent mappings on Bn:

Ekβˆ—β’(Bn)={f∈S⁒(Bn):Gk⁒f∈Sβˆ—β’(Bn)} (4)

and

Ek⁒(Bn)={f∈S⁒(Bn):Gk⁒f∈K⁒(Bn)}. (5)
Remark 8.

According to the previous definition, it is clear than we obtain the following particular cases:

  1. 1.

    If k=0, then

    E0βˆ—β’(Bn)=Sβˆ—β’(Bn)andE0⁒(Bn)=K⁒(Bn).
  2. 2.

    If k=1, then

    E1βˆ—β’(Bn)={f∈S⁒(Bn):G1⁒f∈Sβˆ—β’(Bn)}

    and

    E1⁒(Bn)={f∈S⁒(Bn):G1⁒f∈K⁒(Bn)},

where G1⁒f⁒(z)=D⁒f⁒(z)⁒(z), for z∈Bn.

An important remark on the previous subclasses of biholomorphic mappings in β„‚n is based on the fact that Alexander’s duality theorem is no longer true in higher dimensions (see Remark 3). According to this, we obtain the following remarks:

Remark 9.

If nβ‰₯2, then

K⁒(B1n)⊊E1βˆ—β’(B1n)andK⁒(π•Œn)⊊E1βˆ—β’(π•Œn), (6)

where B1n is the unit ball in β„‚n with respect to the 1-norm, respectively π•Œn is the unit polydisc in β„‚n.

Proof.

For the sake of brevity, let us consider n=2. Notice that the arguments for the case nβ‰₯2 are similar.

  1. 1.

    First, let us consider the case of the unit ball B12 with respect to the 1-norm. According to (GrKo1, , Theorem 6.3.11.a) and (GrKo1, , Remark 6.3.15), we have that if f∈K⁒(B12), then D⁒f⁒(z)⁒z is starlike on B12. Hence, G1⁒f∈Sβˆ—β’(B12) and in view of Definition 3 we obtain that f∈E1βˆ—β’(B12).

    In order to prove that the inclusion K⁒(B12)⊊E1βˆ—β’(B12) is strict, it is enough to consider the mapping f:B12β†’β„‚2 given by

    f⁒(z)=(z11βˆ’z1,z2),z=(z1,z2)∈B12.

    Then D⁒f⁒(z)⁒(z)=(z1/(1βˆ’z1)2,z2) is starlike on B12 (in view of (GrKo1, , Problem 6.2.5)) and hence, f∈E1βˆ—β’(B12). However, f is not convex on B12 (see (GrKo1, , Problem 6.3.2)). Then, f∈E1βˆ—β’(B12)βˆ–K⁒(B12) and we conclude that

    K⁒(B12)⊊E1βˆ—β’(B12).
  2. 2.

    On the other hand, in view of (GrKo1, , Theorem 6.3.11.b) and (GrKo1, , Remark 6.3.15), we have that if f∈K⁒(π•Œ2), then D⁒f⁒(z)⁒z is starlike on π•Œ2. Hence, G1⁒f∈Sβˆ—β’(π•Œ2) and in view of Definition 3 we obtain that f∈E1βˆ—β’(π•Œ2).

    Again, to prove that the inclusion K⁒(π•Œ2)⊊E1βˆ—β’(π•Œ2) is strict, we can consider the mapping f:π•Œ2β†’β„‚2 given by

    f⁒(z)=(z1+a2⁒z22,z2),z=(z1,z2)βˆˆπ•Œ2.

    Then D⁒f⁒(z)⁒(z)=(z1+a⁒z22,z2) is starlike on π•Œ2 for |a|≀1 (see (Suf1, , Example 3)). In view of Definition 3, we deduce that f∈E1βˆ—β’(π•Œ2). However, f is not convex for aβ‰ 0 (see (Suf1, , Example 3)). Hence, there exists a mapping f∈E1βˆ—β’(π•Œ2)βˆ–K⁒(π•Œ2). Then

    K⁒(π•Œ2)⊊E1βˆ—β’(π•Œ2)

    and this completes the proof.

∎

Remark 10.

In addition to Remark 9, we can also prove (see Theorem 2) that

E1βˆ—β’(𝔹n)β‰ K⁒(𝔹n),nβ‰₯2, (7)

where 𝔹n is the Euclidean unit ball in β„‚n. Hence, it is not trivial to define the subclasses Ekβˆ— and Ek of univalent mappings in the case of several complex variables. Even the simplest case k=1 is interesting for the Euclidean unit ball 𝔹n in view of the difference provided by relation (7).

Next we present two examples of mappings which belongs to the class E1βˆ—β’(Bpn) for the general case of the unit ball Bpn with respect to a p-norm. These examples was also considered in (BrGrHaKo, , Example 3.2), (HaKo1, , Remark 3.3), (RoSuf1, , Example 5) and (RoSuf1, , Example 6).

Example 1.

Let f:Bp2βŠ‚β„‚2β†’β„‚2 be given by

f⁒(z)=(z1+a⁒z22,z2),z=(z1,z2)∈Bp2.

Then f∈E1βˆ—β’(Bp2) if and only if

|a|≀12⁒(p2βˆ’14)1/p⁒(p+1pβˆ’1),p>1. (8)
Proof.

We have that f⁒(0)=0 and D⁒f⁒(0)=In, where

D⁒f⁒(z)=(12⁒a⁒z201),z=(z1,z2)∈Bp2.

Moreover,

g⁒(z)=D⁒f⁒(z)⁒(z)=(z1+2⁒a⁒z22,z2),z=(z1,z2)∈Bp2.

In view of (RoSuf1, , Example 5) we know that g=G1⁒f∈Sβˆ—β’(Bp2) if and only if

|2⁒a|≀(p2βˆ’14)1/p⁒(p+1pβˆ’1),p>1.

Hence, f∈E1βˆ—β’(Bp2) if and only if condition (8) holds and this completes the proof. ∎

Remark 11.

It is clear that in view of the previous example, we can construct another example on the Euclidean unit ball 𝔹2. Indeed, for the particular case p=2, we obtain that f∈E1βˆ—β’(𝔹2) if and only if |a|≀3⁒34.

Example 2.

Let f:Bp2βŠ‚β„‚2β†’β„‚2 be given by

f⁒(z)=(z1+a⁒z1⁒z2,z2),z=(z1,z2)∈Bp2.

Then f∈E1βˆ—β’(Bp2) if and only if |a|≀1/2, for all 1≀pβ‰€βˆž.

Proof.

We have that f⁒(0)=0 and D⁒f⁒(0)=In, where

D⁒f⁒(z)=(1+a⁒z2a⁒z101),z=(z1,z2)∈Bp2.

Moreover,

g⁒(z)=D⁒f⁒(z)⁒(z)=(z1+2⁒a⁒z1⁒z2,z2),z=(z1,z2)∈Bp2.

In view of (RoSuf1, , Example 6) we know that g=G1⁒f∈Sβˆ—β’(Bp2) if and only if |2⁒a|≀1, for all 1≀pβ‰€βˆž. Hence, f∈E1βˆ—β’(Bp2) if and only if |a|≀12, and this completes the proof. ∎

Similarly, we can construct examples of mappings in the class E1⁒(𝔹2) for the case of the Euclidean unit ball. We present these very simple examples without proofs, but for details, one may consult (RoSuf1, , Examples 7 and 8) (cf. BrGrHaKo , (HaKo1, , Remark 3.3)).

Example 3.

Let f:𝔹2β†’β„‚2 be given by f⁒(z)=(z1+a⁒z22,z2) for all zβˆˆπ”Ή2. Then f∈E1⁒(𝔹2) if and only if |a|≀14.

Example 4.

Let f:𝔹2β†’β„‚2 be given by f⁒(z)=(z1+a⁒z1⁒z2,z2) for all zβˆˆπ”Ή2. Then f∈E1⁒(𝔹2) if and only if |a|≀24.

3 General Properties

In the third section we present some general properties of the previously defined subclasses of univalent mappings. We will highlight the connection between subclasses E1βˆ— (respectively E1) on the unit disc U and the class of convex mappings K⁒(Bpn) in β„‚n. It is very interesting that results from the case n=1 are not longer true in the case of several complex variables.

Theorem 2.

Regarding to the class E1βˆ—, the following statements are true:

  1. 1.

    If n=1, then E1βˆ—β’(U)=K⁒(U)=K.

  2. 2.

    If nβ‰₯2, then E1βˆ—β’(𝔹n)∩K⁒(𝔹n)β‰ βˆ… and E1βˆ—β’(𝔹n)β‰ K⁒(𝔹n).

Proof.
  1. 1.

    Let us first consider the case n=1. Then we can rewrite the definition of the class E1 in the following way

    E1βˆ—β’(𝔹1)=E1βˆ—β’(U)={f∈S⁒(𝔹1):G1⁒f∈Sβˆ—β’(𝔹1)},

    where S⁒(𝔹1)=S, Sβˆ—β’(𝔹1)=Sβˆ— and G1⁒f⁒(ΞΆ)=΢⁒f′⁒(ΞΆ), for all ΞΆβˆˆπ”Ή1=U. Hence,

    E1βˆ—β’(U)={f∈S:Re⁒[΢⁒(G1⁒f)′⁒(ΞΆ)G1⁒f⁒(ΞΆ)]>0,΢∈U}

    which means that

    E1βˆ—β’(U)={f∈S:Re⁒[f′⁒(ΞΆ)+΢⁒f′′⁒(ΞΆ)f′⁒(ΞΆ)]>0,΢∈U}.

    Now, it is clearly that

    E1βˆ—β’(U)={f∈S:Re⁒[1+΢⁒f′′⁒(ΞΆ)f′⁒(ΞΆ)]>0,΢∈U}=K.

    Another simple argument for the equality between these two classes is given by the fact that Alexander’s Duality Theorem holds in the case of one complex variable. Then, in view of Definition 3 and Remark 8, we have that

    E1βˆ—β’(U)={f∈S:΢⁒f′⁒(ΞΆ)∈Sβˆ—,΢∈U}=K.
  2. 2.

    For the second part of the proof it is enough to consider some examples which shows us that, in the case of several complex variables, E1βˆ—β’(𝔹n)∩K⁒(𝔹n)β‰ βˆ… and E1βˆ—β’(𝔹n)β‰ K⁒(𝔹n). For simplicity, let us consider the case n=2, but notice that for nβ‰₯2 the arguments are similar. Indeed, according to

    • β€’

      Example 1 for p=2 and a=12, we can construct f:𝔹2β†’β„‚2 given by

      f⁒(z)=(z1+a⁒z22,z2),z=(z1,z2)βˆˆπ”Ή2.

      Because |a|=12<3⁒34 we obtain that f∈E1βˆ—β’(𝔹2). Moreover, in view of (RoSuf1, , Example 7), we have that f∈K⁒(𝔹2) because |a|≀12.

    Hence, we obtain that E1βˆ—β’(𝔹n)∩K⁒(𝔹n)β‰ βˆ…. On the other hand, in view of

    • β€’

      Example 1 for p=2 and b=3⁒34, we can construct g:𝔹2β†’β„‚2 given by

      g⁒(z)=(z1+b⁒z22,z2),z=(z1,z2)βˆˆπ”Ή2.

      Because |b|=3⁒34≀3⁒34 we obtain that g∈E1βˆ—β’(𝔹2). But, according to (RoSuf1, , Example 7), we have that gβˆ‰K⁒(𝔹2) because 3⁒34>12.

    Hence, we have that there exists g∈E1βˆ—β’(𝔹2)βˆ–K⁒(𝔹2), i.e. g belongs to class E1βˆ—β’(𝔹2), but g is not a convex mapping on 𝔹2. Finally, in view of

    • β€’

      Example 2 for p=2 and c=22, we can construct h:𝔹2β†’β„‚2 given by

      h⁒(z)=(z1+c⁒z1⁒z2,z2),z=(z1,z2)βˆˆπ”Ή2.

      Because |c|=22≀12 we obtain that h∈K⁒(𝔹2) (according to (RoSuf1, , Example 8)). However, hβˆ‰E1βˆ—β’(𝔹2) because G1⁒hβˆ‰Sβˆ—β’(𝔹2), where

      G1⁒h⁒(z)=D⁒h⁒(z)⁒(z)=(z1+2⁒z1⁒z2,z2),z=(z1,z2)βˆˆπ”Ή2.

      Indeed, in view of (RoSuf1, , Example 6) it is easy to prove that G1⁒fβˆ‰Sβˆ—β’(𝔹2).

    Hence, we obtain that h∈K⁒(𝔹2)βˆ–E1βˆ—β’(𝔹2), i.e. h is a convex mapping on 𝔹2, but h does not belong to class E1βˆ—β’(𝔹2). In view of all arguments presented above, we conclude that E1βˆ—β’(𝔹n)β‰ K⁒(𝔹n) and this completes the proof.

∎

Remark 12.

According to Theorem 2, it is clear that if n=1, then K⁒(U)=E1βˆ—β’(U). However, if nβ‰₯2, then K⁒(B1n)⊊E1βˆ—β’(B1n) and K⁒(π•Œn)⊊E1βˆ—β’(π•Œn) in view of Remark 9 and K⁒(𝔹n)β‰ E1βˆ—β’(𝔹n) in view of Theorem 2.

Next, we present an example given by M.S. Liu in Liu1 . He obtained a very nice condition for a function to be convex of order Ξ± on the unit ball Bp2 (with respect to a p-norm, where pβ‰₯2). We will use this example given by Liu to prove that E1⁒(𝔹n)∩K⁒(𝔹n;1/2)β‰ βˆ… and K⁒(𝔹n;1/2)βˆ–E1⁒(𝔹n)β‰ βˆ….

Example 5.

(see (Liu1, , Example 1)) Let α∈[0,1), pβ‰₯2 and kβˆˆβ„€+βˆ—={1,2,3,…} such that k<p≀k+1. Also, let g:Bp2β†’β„‚2 be given by

g⁒(z)=(z1+a⁒z2k+1,z2),z=(z1,z2)∈Bp2, (9)

where Bp2={zβˆˆβ„‚2:β€–zβ€–p=(|z1|p+|z2|p)1/p}. If a satisfies the inequality |a|≀1βˆ’Ξ±k⁒(k+1), then g∈K⁒(Bp2,Ξ±).

Theorem 3.

Regarding to the class E1, the following statements are true:

  1. 1.

    If n=1, then E1⁒(U)⊊K⁒(1/2).

  2. 2.

    If nβ‰₯2, then E1⁒(𝔹n)∩K⁒(𝔹n;1/2)β‰ βˆ… and K⁒(𝔹n;1/2)βˆ–E1⁒(𝔹n)β‰ βˆ…, i.e. there exists also convex mappings of order 1/2 on 𝔹n which does not belong to class E1⁒(𝔹n).

Proof.
  1. 1.

    Let us first consider the case n=1.

    • β€’

      Let f∈E1⁒(U). Then, in view of Definition 3, we have that G1⁒f∈K. According to a result given by Sheil-Small and Suffridge (see (GrKo1, , Theorem 2.2.4)) we know that

      Re⁒[2⁒΢⁒(G1⁒f)′⁒(ΞΆ)(G1⁒f)⁒(ΞΆ)βˆ’(G1⁒f)⁒(ΞΆ0)βˆ’ΞΆ+ΞΆ0ΞΆβˆ’ΞΆ0]β‰₯0,βˆ€ΞΆ,ΞΆ0∈U.

      For ΞΆ0=0, we obtain that

      Re⁒[΢⁒(G1⁒f)′⁒(ΞΆ)(G1⁒f)⁒(ΞΆ)]β‰₯12,΢∈U.

      But, (G1⁒f)⁒(ΞΆ)=΢⁒f′⁒(ΞΆ), for all ΢∈U and using the minimum principle for harmonic functions we have that

      Re⁒[΢⁒(G1⁒f)′⁒(ΞΆ)(G1⁒f)⁒(ΞΆ)]=Re⁒[ΞΆ2⁒f′′⁒(ΞΆ)+΢⁒f′⁒(ΞΆ)΢⁒f′⁒(ΞΆ)]=Re⁒[1+΢⁒f′′⁒(ΞΆ)f′⁒(ΞΆ)]>12,΢∈U.

      In view of the definition of the class K⁒(Ξ±) (see (Goo, , Chapter 9) or Rob ), we obtain that f∈K⁒(1/2). Hence, E1⁒(U)βŠ†K⁒(1/2).

    • β€’

      However, we can prove that the previous inclusion is strict, i.e. there is a function f∈K⁒(1/2) which does not belog to class E1⁒(U). Indeed, if we consider f:Uβ†’β„‚ given by f⁒(ΞΆ)=ΞΆ+a⁒΢2 for all ΢∈U with a=16, then according to (MeRoSco, , Theorem 2) (for Ξ±=1/2) we have that

      βˆ‘n=2∞(nβˆ’12)⁒n⁒|an|=(2βˆ’12)β‹…2β‹…|a|=12≀12

      and then f∈K⁒(1/2) by Alexander’s duality theorem. On the other hand, let us consider

      g⁒(ΞΆ)=G1⁒f⁒(ΞΆ)=΢⁒f′⁒(ΞΆ)=ΞΆ+2⁒a⁒΢2,΢∈U,a=1/6 (10)

      and h:U→ℂ given by

      h⁒(ΞΆ)=1+΢⁒g′′⁒(ΞΆ)g′⁒(ΞΆ)=4⁒΢+32⁒΢+3,΢∈U. (11)

      Then h is a MΓΆbius transformation on U such that h⁒(βˆ’3/2)=∞, h⁒(0)=1, h⁒(1)=75 and h⁒(i)=1713+613⁒i. Then

      h⁒(U)=𝒰⁒(1/5,6/5)={x+i⁒yβˆˆβ„‚:(xβˆ’0.2)2+y2<1.44},

      where 𝒰⁒(1/5,6/5) is the open disc of center w0=1/5 and radius r=6/5, as we can observe in Figure 1.

      Refer to caption
      Figure 1: The open disc 𝒰⁒(1/5,6/5) of center w0=1/5 and radius r=6/5

      Moreover, for every point wβˆˆπ’°β’(1/5,6/5)∩{x+i⁒yβˆˆβ„‚:x<0}, we have that Rew<0, i.e. βˆƒΞΆ0∈U such that Re[h⁒(ΞΆ0)]<0. For example, if ΞΆ0=βˆ’910, then ΞΆ0∈U and simple computations show that

      Re⁒[h⁒(ΞΆ0)]=Re⁒[1+ΞΆ0⁒g′′⁒(ΞΆ0)g′⁒(ΞΆ0)]=Re⁒[4⁒΢0+32⁒΢0+3]=βˆ’12<0.

      Hence, according to the behavior of the function h on U and the analytical characterization of convexity (see for example (GrKo1, , Theorem 2.2.3)), we deduce that g=G1⁒fβˆ‰K, and then fβˆ‰E1⁒(U). Finally, we obtain that f∈K⁒(1/2)βˆ–E1⁒(U).

  2. 2.

    For the second part of the proof, let us consider n=2. However, notice that for nβ‰₯2, the arguments are similar.

    • β€’

      First, we can use the example given by Liu (see (Liu1, , Example 1)) in the particular case n=2 and Ξ±=12. For this, let us consider f:𝔹2β†’β„‚2 given by

      f⁒(z)=(z1+a⁒z22,z2),z=(z1,z2)βˆˆπ”Ή2.

      According to the result given by Liu and Example 3, we obtain that

      f∈E1⁒(𝔹2)∩K⁒(𝔹2;1/2)

      for |a|≀14. Hence,

      E1⁒(𝔹n)∩K⁒(𝔹n;1/2)β‰ βˆ….
    • β€’

      In order to prove that βˆƒf∈K⁒(𝔹n;1/2)βˆ–E1⁒(𝔹n), i.e. there is a convex mapping of order 1/2 on 𝔹n such that fβˆ‰E1⁒(𝔹n), we can use a particular form of the example considered by Liu and Zhu in the general case of complex Hilbert spaces in (LiuZhu, , Example 2). Notice that, the example considered fits better with the example used in the case n=1, in the first part of the proof.

      Let us consider Ξ±=12 and a=16. Also, let

      f⁒(z)=z+a⁒⟨z,u⟩2⁒u,z=(z1,z2)βˆˆπ”Ή2,u=(1,0)βˆˆβ„‚2.

      Then, according to (LiuZhu, , Example 2), we have that f∈K⁒(𝔹2;1/2). On the other hand, if

      g⁒(z)=G1⁒f⁒(z)=D⁒f⁒(z)⁒(z)=(z1+2⁒a⁒z12,z2)=z+2⁒a⁒⟨z,u⟩2⁒u,

      for zβˆˆπ”Ή2 and u=(1,0)βˆˆβ„‚2, then |2⁒a|=13>14. In view of (LiuZhu, , Example 2), we deduce that g=G1⁒fβˆ‰K⁒(𝔹2) and hence fβˆ‰E1⁒(𝔹2). Finally, we conclude that f∈K⁒(𝔹n;1/2)βˆ–E1⁒(𝔹n) and this completes the proof.

∎

Remark 13.

Let us consider f⁒(z)=(z1+a⁒z2k+1,z2) with |a|≀12⁒k⁒(k+1) and kβˆˆβ„€+βˆ—. In view of the Example 5 (for Ξ±=1/2) we obtain that f∈K⁒(Bp2,1/2). On the other hand,

D⁒f⁒(z)⁒(z)=(z1+(k+1)⁒a⁒z2k+1,z2),z=(z1,z2)∈Bp2

and

|(k+1)⁒a|=(k+1)⁒|a|≀(k+1)⁒12⁒k⁒(k+1)=12⁒k.

To prove that f∈E1⁒(Bp2), we must obtain some conditions for G1⁒f to be convex on Bp2. According to Example 5 (for Ξ±=0) we can impose condition 12⁒k≀1k⁒(k+1) which leads us to k≀1. Hence

f∈E1⁒(Bp2)∩K⁒(Bp2;1/2),

for kβˆˆβ„€+βˆ— with k≀1. It is clear that k=1 and then the only possible value for p is p=2 (this means that we have to use the Euclidean norm βˆ₯β‹…βˆ₯).

This remark together with Example 5 shows us that a function defined by relation (9) belongs to the both classes E1⁒(Bpn) and K⁒(Bpn;1/2) if k=1, p=2 and |a|≀14, as we saw in the proof of Theorem 3.

Definition 4.

Let kβˆˆβ„€+ and α∈[0,1). In view of Definition 3, we define

Ekβˆ—β’(Bn;Ξ±)={f∈S⁒(Bn):Gk⁒f∈Sβˆ—β’(Bn;Ξ±)}, (12)

where Sβˆ—β’(Bn,Ξ±) is the family of starlike mappings of order Ξ± in β„‚n (see Cu1 or Ko2 ).

Using the previous definition, we can obtain another form of the Marx-Strohhacker theorem (see (GrKo1, , Theorem 2.3.2) for n=1 and (GrKo1, , Theorem 6.3.19) for the case of several complex variables) in the context of classes Ek and Ekβˆ—.

Theorem 4.

Let kβˆˆβ„€+. Then

Ek⁒(Bn)βŠ†Ekβˆ—β’(Bn;1/2)βŠ†Ekβˆ—β’(Bn), (13)

where Bn is the unit ball of β„‚n with respect to an arbitrary norm βˆ₯β‹…βˆ₯βˆ—.

Proof.

Let f∈Ek⁒(Bn). In view of Definition 3, we have that Gk⁒f is a convex mapping on Bn. In view of (GrKo1, , Theorem 6.3.18 and Theorem 6.3.19) we obtain that Gk⁒f is starlike of order 1/2 and this means that f∈Ekβˆ—β’(Bn;1/2). It is obvious that Ekβˆ—β’(Bn;1/2)βŠ†Ekβˆ—β’(Bn) and this completes the proof. ∎

Corollary 5.

Let kβˆˆβ„€+ and n=1. Then Ek⁒(U)βŠ†Ekβˆ—β’(U;1/2)βŠ†Ekβˆ—β’(U).

Corollary 6.

Let us consider k∈{0,1}.

  1. 1.

    If n=1, then

    K=E0⁒(U)βŠ†E0βˆ—β’(U;1/2)=Sβˆ—β’(1/2)βŠ†Sβˆ— (14)

    and

    E1⁒(U)βŠ†E1βˆ—β’(U;1/2)=K⁒(1/2)βŠ†K. (15)
  2. 2.

    On the other hand, if nβ‰₯2, then

    E0⁒(Bpn)=K⁒(Bpn)βŠ†E0βˆ—β’(Bpn;1/2)=Sβˆ—β’(Bpn;1/2)βŠ†Sβˆ—β’(Bpn) (16)

    and

    E1⁒(Bpn)βŠ†E1βˆ—β’(Bpn;1/2),for1≀p<∞, (17)

    where Bpn is the unit ball in β„‚n with respect to the p-norm and

    E1⁒(π•Œn)βŠ†E1βˆ—β’(π•Œn;1/2), (18)

    where π•Œn is the unit polydisc in β„‚n.

Proof.
  1. 1.

    First, according to Theorem 4 (for n=1, k=0, respectively k=1) we obtain immediately the inclusions from relations (14) and (15). Moreover, in view of Definition 3 and the Alexander’s duality theorem for the classes Sβˆ—β’(Ξ±) and K⁒(Ξ±), we have that

    E0βˆ—β’(U;1/2)={f∈S:G0⁒f∈Sβˆ—β’(1/2)}={f∈S:f∈Sβˆ—β’(1/2)}=Sβˆ—β’(1/2)

    and

    E1βˆ—β’(U;1/2)={f∈S:G1⁒f∈Sβˆ—β’(1/2)}={f∈S:f∈K⁒(1/2)}=K⁒(1/2),

    where G1⁒f⁒(ΞΆ)=΢⁒f′⁒(ΞΆ) for all ΢∈U. Relation (14) is also proved in (GrKo1, , Theorem 2.3.2) and relation (15) follows from Theorem 3.

  2. 2.

    Next, let us consider nβ‰₯2.

    • β€’

      In view of Definitions 3 and 4, Remark 8 and Theorem 4, we obtain the inclusions and equalities from relation (16).

    • β€’

      The inclusions from relations (17) and (18) are based on Theorem 4 for the unit ball Bpn in β„‚n with respect to the p-norm, where p∈[0,∞), respectively for the unit polydisc π•Œn in β„‚n, and this completes the proof.

∎

4 Extension Operators and Applications

In last part of this paper we consider two particular cases of the Graham-Kohr extension operator Ξ¨n,Ξ± defined by relation (2) for Ξ±=0 and Ξ±=1. Although the operator Ξ¨n,Ξ± does not preserve convexity, we can still observe an interesting property related to the subclass E1βˆ— in the particular cases mentioned above.

Proposition 7.

Let us consider the Graham-Kohr extension operator Ξ¨2,0 defined in (2) for n=2 and Ξ±=0. Then

Ξ¨2,0⁒(K)=Ξ¨2,0⁒(E1βˆ—β’(U))βŠ†E1βˆ—β’(𝔹2)β‰ K⁒(𝔹2). (19)
Proof.

Let us consider the case n=2 and f∈K. Also, let F:𝔹2β†’β„‚2 be given by

F⁒(z)=Ψ2,0⁒(f)⁒(z)=(f⁒(z1),z2),

for all z=(z1,z2)βˆˆπ”Ή2. We want to prove that

F∈E1βˆ—β’(𝔹2)⇔F∈S⁒(𝔹2)andG1⁒F∈Sβˆ—β’(𝔹2).
  1. 1.

    In (GrHaKoSuf1, , Theorem 2.1) or (GrKo2, , Theorem 3.2) the authors proved that F∈S0⁒(𝔹2), so according to this result it is clear that F∈S⁒(𝔹2).

  2. 2.

    For the second part, let us consider the mapping G:𝔹2β†’β„‚2 given by

    G⁒(z)=D⁒F⁒(z)⁒(z)=(f′⁒(z1)001)⁒(z1z2)=(z1⁒f′⁒(z1),z2),

    for all zβˆˆπ”Ή2. To prove that G is starlike on 𝔹2 it is enough to observe that

    G⁒(z)=(G1⁒(z1),G2⁒(z2)),

    where Gj⁒(zj)∈Sβˆ— for j∈{1,2}. Indeed, according to Alexander’s duality theorem we have that G1∈Sβˆ— if and only if f∈K. Moreover, it is clear that G2 is a starlike function on the unit disc. Hence, G=G1⁒F∈Sβˆ—β’(𝔹2) and this completes the proof.

∎

Remark 14.

Notice that we proved the previous result in the case n=2. However, the arguments in the case nβ‰₯2 are similar.

Another proof of Proposition 7 can be given using a surprising property of the mapping Gk. It seems that the relationship between Gk and Ξ¨n,Ξ± is commutative (in the sense presented in the following lemma).

Lemma 8.

Let us consider n=2, α=0 and k0∈{0,1,2}. Then

Ψ2,0⁒(Gk0⁒f)=Gk0⁒(Ψ2,0⁒(f)). (20)
Proof.
  1. 1.

    Let k0=0. In view of Definition 2 it is clear that for k0=0 we obtain

    Ψ2,0⁒(G0⁒f)=Ψ2,0⁒(f)=G0⁒(Ψ2,0⁒(f)).
  2. 2.

    Let k0=1. Then

    Ξ¨2,0⁒(G1⁒f)⁒(z)=(G1⁒f⁒(z1),z2)=(z1⁒f′⁒(z1),z2),

    for all z=(z1,z2)βˆˆπ”Ή2 and

    G1⁒(Ξ¨2,0⁒(f))⁒(z)=D⁒Ψ2,0⁒(f)⁒(z)=(f′⁒(z1)001)⁒(z1z2)=(z1⁒f′⁒(z1),z2),

    for all z=(z1,z2)βˆˆπ”Ή2. Hence,

    Ψ2,0⁒(G1⁒f)=G1⁒(Ψ2,0⁒(f)).
  3. 3.

    For the last part of the proof, let us consider k0=2. Then

    Ξ¨2,0⁒(G2⁒f)⁒(z)=(G2⁒f⁒(z1),z2)=(z12⁒f′′⁒(z1)+z1,z2),

    for all z=(z1,z2)βˆˆπ”Ή2. On the other hand,

    G2⁒(Ξ¨2,0⁒(f))⁒(z) =D2⁒Ψ2,0⁒(f)⁒(z)⁒(z2)+z=(z1⁒f′′⁒(z1)000)⁒(z1z2)+z
    =(z12⁒f′′⁒(z1)+z1,z2),

    for all z=(z1,z2)βˆˆπ”Ή2 and then

    Ψ2,0⁒(G2⁒f)=G2⁒(Ψ2,0⁒(f)).

Hence, we proved the commutative property of the mapping Gk for the particular cases k∈{0,1,2} and this completes the proof. ∎

Remark 15.

According to the previous proof we deduce that Lemma 8 is true also in the case nβ‰₯2, Ξ±=0 and k0∈{0,1,2}.

Remark 16.

Using Lemma 8 we can prove Proposition 7 for the case nβ‰₯2 in the following alternative way:

f∈K⇔f∈E1βˆ—β’(U)⇔f∈SandG1⁒f∈Sβˆ—

which implies that

Ξ¨n,0⁒(f)∈S⁒(𝔹n)andΞ¨n,0⁒(G1⁒f)∈Sβˆ—β’(𝔹n),

where the last implication follows from the property that Ψn,0 preserves the starlikeness (see Remark 7). But, Ψn,0⁒(G1⁒f)=G1⁒(Ψn,0⁒(f)). Then

Ξ¨n,0⁒(f)∈S⁒(𝔹n)andG1⁒(Ξ¨n,0⁒(f))∈Sβˆ—β’(𝔹n)⇔Ψn,0⁒(f)∈E1βˆ—β’(𝔹n),

in view of Definition 3. Hence,

f∈K=E1βˆ—β’(U)β‡’Ξ¨n,0⁒(f)∈E1βˆ—β’(𝔹n)

and this completes the proof.

Corollary 9.

Let us consider the Graham-Kohr extension operator Ψn,0 defined in (2) for α=0. Then, for any k∈{0,1,2}, we have the embedding

Ξ¨n,0⁒(Ekβˆ—β’(U))βŠ†Ekβˆ—β’(𝔹n).
Theorem 10.

Let us consider the Graham-Kohr extension operator Ξ¨2,1 defined in (2) for n=2 and Ξ±=1. Then

Ξ¨2,1⁒(K)=Ξ¨2,1⁒(E1βˆ—β’(U))βŠ†E1βˆ—β’(𝔹2)β‰ K⁒(𝔹2). (21)
Proof.

Let us consider the case n=2 and f∈K. Let F:𝔹2β†’β„‚2 be given by

F⁒(z)=Ψ2,1⁒(f)⁒(z)=(f⁒(z1),z2⁒f⁒(z1)z1), (22)

for all z=(z1,z2)βˆˆπ”Ή2. We want to prove that

F∈E1βˆ—β’(𝔹2)⇔F∈S⁒(𝔹2)andG1⁒F∈Sβˆ—β’(𝔹2).
  1. 1.

    In (GrHaKoSuf1, , Theorem 2.1) or (GrKo2, , Theorem 3.2) the authors proved that F∈S0⁒(𝔹2), so according to this result it is clear that F∈S⁒(𝔹2).

  2. 2.

    In order to show that G1⁒F∈Sβˆ—β’(𝔹2), let us consider the mapping G:𝔹2β†’β„‚2 given by

    G⁒(z)=D⁒F⁒(z)⁒(z)=(f′⁒(z1)0z2z1⁒[f′⁒(z1)βˆ’f⁒(z1)z1]f⁒(z1)z1)⁒(z1z2),

    where F is given by (22) and z=(z1,z2)βˆˆπ”Ή2. Hence

    G⁒(z)=(z1⁒f′⁒(z1),z2⁒f′⁒(z1)), (23)

    for all z=(z1,z2)βˆˆπ”Ή2. Next, to prove that G1⁒F=G∈Sβˆ—β’(𝔹2), we can use the analytical characterization of starlikeness from Theorem 1.

It is clear that G∈H⁒(𝔹2), G⁒(0)=0 and D⁒G⁒(0)=I2, where

D⁒G⁒(z)=(f′⁒(z1)+z1⁒f′′⁒(z1)0z2⁒f′′⁒(z1)f′⁒(z1)),

for z=(z1,z2)βˆˆπ”Ή2. Also G is locally biholomorphic on 𝔹2 since

JG⁒(z)=det[D⁒G⁒(z)]=f′⁒(z1)β‹…[f′⁒(z1)+z1⁒f′′⁒(z1)]β‰ 0,z1∈U

in view of the fact that f∈K. Moreover, we have that

[D⁒G⁒(z)]βˆ’1 =1f′⁒(z1)⁒[f′⁒(z1)+z1⁒f′′⁒(z1)]⁒(f′⁒(z1)0βˆ’z2⁒f′′⁒(z1)f′⁒(z1)+z1⁒f′′⁒(z1))
=(1f′⁒(z1)+z1⁒f′′⁒(z1)0βˆ’z2⁒f′′⁒(z1)f′⁒(z1)⁒[f′⁒(z1)+z1⁒f′′⁒(z1)]1f′⁒(z1)),zβˆˆπ”Ή2.

Thus,

[D⁒G⁒(z)]βˆ’1⁒G⁒(z) =(z1⁒f′⁒(z1)f′⁒(z1)+z1⁒f′′⁒(z1),z2βˆ’z1⁒z2⁒f′′⁒(z1)f′⁒(z1)+z1⁒f′′⁒(z1))
=(z1⁒f′⁒(z1)f′⁒(z1)+z1⁒f′′⁒(z1),z2⁒f′⁒(z1)+z1⁒z2⁒f′′⁒(z1)βˆ’z1⁒z2⁒f′′⁒(z1)f′⁒(z1)+z1⁒f′′⁒(z1))
=(z1⁒f′⁒(z1)f′⁒(z1)+z1⁒f′′⁒(z1),z2⁒f′⁒(z1)f′⁒(z1)+z1⁒f′′⁒(z1)),zβˆˆπ”Ή2. (24)

Then

Re⁒⟨[D⁒G⁒(z)]βˆ’1⁒G⁒(z),z⟩ =Re⁒⟨(z1⁒f′⁒(z1)f′⁒(z1)+z1⁒f′′⁒(z1),z2⁒f′⁒(z1)f′⁒(z1)+z1⁒f′′⁒(z1)),(z1,z2)⟩
=Re⁒[z1⁒zΒ―1⁒f′⁒(z1)f′⁒(z1)+z1⁒f′′⁒(z1)+z2⁒zΒ―2⁒f′⁒(z1)f′⁒(z1)+z1⁒f′′⁒(z1)]
=|z1|2β‹…Re⁒[f′⁒(z1)f′⁒(z1)+z1⁒f′′⁒(z1)]+|z2|2β‹…Re⁒[f′⁒(z1)f′⁒(z1)+z1⁒f′′⁒(z1)]
=β€–zβ€–2β‹…Re⁒[f′⁒(z1)f′⁒(z1)+z1⁒f′′⁒(z1)],

for all zβˆˆπ”Ή2βˆ–{0}. Hence,

Re⁒⟨[D⁒G⁒(z)]βˆ’1⁒G⁒(z),z⟩=β€–zβ€–2β‹…Re⁒[11+z1⁒f′′⁒(z1)/f′⁒(z1)]>0,

for all zβˆˆπ”Ή2βˆ–{0} according to the fact that f∈K. Using the characterization of starlikeness in 𝔹n (see Theorem 1), we obtain that G∈Sβˆ—β’(𝔹2), i.e. G1⁒F∈Sβˆ—β’(𝔹2). Hence, F=Ξ¨2,1⁒(f)∈E1βˆ—β’(𝔹2) and this completes the proof. ∎

Remark 17.

Notice that Theorem 10 is true also in the case nβ‰₯2, but for the sake of brevity we give the proof only in the case n=2. A general alternative proof of Theorem 10 can be given using the following arguments:

  1. 1.

    Let f∈K and F=Ξ¨n,1⁒(f). Then F∈S⁒(𝔹n) according to (GrKo2, , Theorem 3.2).

  2. 2.

    If we define h⁒(w)=w⁒f′⁒(w), for all w∈U, then f∈K implies that h∈Sβˆ— (in view of Alexander’s theorem).

  3. 3.

    Let G⁒(z)=D⁒F⁒(z)⁒(z), for zβˆˆπ”Ήn. According to relation (23) and the previous step, we have that

    G⁒(z)=(z1⁒f′⁒(z1),zβˆ—β’f′⁒(z1))=(h⁒(z1),zβˆ—β’h⁒(z1)z1),z=(z1,zβˆ—)βˆˆπ”Ήn.
  4. 4.

    Now it is clear that G⁒(z)=Ψn,1⁒(h)⁒(z).

  5. 5.

    I. Graham and G. Kohr proved in (GrKo2, , Corollary 3.3) that h∈Sβˆ— implies Ξ¨n,1⁒(h)=G∈Sβˆ—β’(𝔹n).

  6. 6.

    Hence, F∈S⁒(𝔹n) and G=G1⁒F∈Sβˆ—β’(𝔹n). In view of Definition 3, we obtain that F∈E1βˆ—β’(𝔹n).

Lemma 11.

Let us consider n=2, α=1 and k0∈{0,1,2}. Then

Ψ2,1⁒(Gk0⁒f)=Gk0⁒(Ψ2,1⁒(f)). (25)
Proof.
  1. 1.

    Let k0=0. In view of Definition 2 it is clear that for k0=0 we obtain

    Ψ2,1⁒(G0⁒f)=Ψ2,1⁒(f)=G0⁒(Ψ2,1⁒(f)).
  2. 2.

    Let k0=1. Then

    Ξ¨2,1⁒(G1⁒f)⁒(z)=(G1⁒f⁒(z1),G1⁒f⁒(z1)z1⁒z2)=(z1⁒f′⁒(z1),z2⁒f′⁒(z1)),

    for all z=(z1,z2)βˆˆπ”Ή2 and

    G1⁒(Ξ¨2,1⁒(f))⁒(z) =D⁒Ψ2,1⁒(f)⁒(z)⁒(z)=(f′⁒(z1)0z2⁒z1⁒f′⁒(z1)βˆ’f⁒(z1)z12f⁒(z1)z1)⁒(z1z2)
    =(z1⁒f′⁒(z1),z2z1⁒[z1⁒f′⁒(z1)βˆ’f⁒(z1)]+z2z1⁒f⁒(z1))
    =(z1⁒f′⁒(z1),z2⁒f′⁒(z1)),

    for all z=(z1,z2)βˆˆπ”Ή2. Hence,

    Ψ2,1⁒(G1⁒f)=G1⁒(Ψ2,1⁒(f)).
  3. 3.

    For the last part of the proof, let us consider k0=2. Then

    Ψ2,1⁒(G2⁒f)⁒(z) =(G2⁒f⁒(z1),z2⁒G2⁒f⁒(z1)z1)
    =(z12⁒f′′⁒(z1)+z1,z2⁒z1⁒f′′⁒(z1)+z2)
    =[z1⁒f′′⁒(z1)+1]β‹…(z1,z2),

    for all z=(z1,z2)βˆˆπ”Ή2. On the other hand,

    G2⁒(Ψ2,1⁒(f))⁒(z) =D2⁒Ψ2,1⁒(f)⁒(z)⁒(z2)+z
    =(z12⁒f′′⁒(z1)+z1,z2⁒z1⁒f′′⁒(z1)+z2)
    =[z1⁒f′′⁒(z1)+1]β‹…(z1,z2),

    where

    D2⁒Ψ2,1⁒(f)⁒(z)⁒(z2)=(z1⁒f′′⁒(z1)0z2⁒f′′⁒(z1)βˆ’z2z1⁒f′⁒(z1)+z2z12⁒f⁒(z1)f′⁒(z1)βˆ’f⁒(z1)z1)⁒(z1z2),

    for all z=(z1,z2)βˆˆπ”Ή2. Thus,

    Ψ2,1⁒(G2⁒f)=G2⁒(Ψ2,1⁒(f)).

Hence, we proved the commutative property given by (25) for the particular cases k∈{0,1,2} and this completes the proof. ∎

Remark 18.

Notice that, for the sake of brevity, we considered in the previous lemma the case n=2, but the arguments in the case nβ‰₯2 are similar.

Remark 19.

Using Lemma 11 in the general case nβ‰₯2, Remark 7 and Definition 3, we can prove Theorem 10 in the following alternative way:

f∈K⇔f∈E1βˆ—β’(U)⇔f∈SandG1⁒f∈Sβˆ—

which implies that

Ξ¨n,1⁒(f)∈S⁒(𝔹n)andΞ¨n,1⁒(G1⁒f)∈Sβˆ—β’(𝔹n).

But, Ψn,1⁒(G1⁒f)=G1⁒(Ψn,1⁒(f)). Then

Ξ¨n,1⁒(f)∈S⁒(𝔹n)andG1⁒(Ξ¨n,1⁒(f))∈Sβˆ—β’(𝔹n)⇔Ψn,1⁒(f)∈E1βˆ—β’(𝔹n).

Hence,

f∈K=E1βˆ—β’(U)β‡’Ξ¨n,1⁒(f)∈E1βˆ—β’(𝔹n)

and this completes the proof.

2023

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