Elsevier

Applied Mathematics and Computation

Volume 267, 15 September 2015, Pages 805-809
Applied Mathematics and Computation

Harmonic mappings related to the m-fold starlike functions

https://doi.org/10.1016/j.amc.2014.10.016Get rights and content

Abstract

In the present paper we will give some properties of the subclass of harmonic mappings which is related to m-fold starlike functions in the open unit disc D={z||z|<1}. Throughout this paper we restrict ourselves to the study of sense-preserving harmonic mappings. We also note that an elegant and complete treatment theory of the harmonic mapping is given in Durens monograph (Duren, 1983). The main aim of us to investigate some properties of the new class of us which represented as in the following form,SH(m)=f=h(z)+g(z)|fSH(m),g(z)h(z)b1p(z),h(z)S(m),p(z)P(m),where h(z)=z+n=1amn+1zmn+1, g(z)=n=0bmn+1zmn+1,|b1|<1.

Introduction

Let Ω be the family of functions ϕ(z) which are analytic in D and satisfying the conditions ϕ(0)=0,|ϕ(z)|<1 for every zD. Let P(m) denote the set of functions of the form p(z)=1+pmzm+p2mz2m+ for which Rep(z)>0 in D. For brevity we say that p(z) has m-fold symmetry. A function is called m-fold symmetric is its power series has the form [1], [4], [5].s(z)=n=0dmn+1zmn+1

This condition on the power series is equivalent to the condition se2πimz=e2πims(z) for zD. The class of such functions is denoted by S(m). We denote by S(m) the families m-fold symmetric starlike functions. That iss(z)S(m)Rezs(z)s(z)>0[1], [4], [5]. Let s1(z)=z+d2z2+ and s2(z)=z+e2z2+ be analytic functions in D. If there exists a function ϕ(z)Ω such that s1(z)=s2(ϕ(z)) for every zD. Then we say that s1(z) is subordinate to s2(z) and we write s1(z)s2(z). Specially if s2(z) is univalent in D, then s1(z)s2(z) if and only if s1(D)s2(D) and s1(0)=s2(0) implies s1(Dr)s2(Dr) where Dr=z||z|<r,0<r<1 [1], [4].

A planar harmonic mapping in the open unit disc D is a complex valued harmonic function f, which maps D onto the some planar domain f(D). Since D is a simply connected domain the mapping f has a canonical decomposition f=h(z)+g(z), where h(z) and g(z) are analytic in D and have the following power series expansions,h(z)=z+n=2anzn,g(z)=n=1bnznas usual, we call h(z) the analytic part and g(z) is the co-analytic part of f, respectively and let the class of such harmonic mappings is denoted by SH, (see [2]) proved in 1936 that the harmonic mapping f is locally univalent in D if and only if its Jacobian Jf=(|h(z)|2-|g(z)|2) is strictly positive in D. In view of this result, locally univalent harmonic mapping in the unit disc are either sense-reversing if g(z)>h(z) or sense-preserving if h(z)>g(z) in D. Throughout this paper we restrict ourselves to the study of sense-preserving harmonic mappings. We also note that an elegant and complete treatment theory of the harmonic mapping is given Duren’s monograph [2].

The main aim of this paper is to investigate the some properties of the following class.SH(m)=f=h(z)+g(z)|fSH(m),g(z)h(z)b1p(z),h(z)S(m),p(z)P(m),where

h(z)=z+n=1amn+1zmn+1, g(z)=n=0bmn+1zmn+1,b1<1. and for this aim we will need the following lemmas.

Lemma 1.1 [4]

Let m1 be a fixed integer and assume thatϕ(z)=B2mz2m+B2m+1z2m+1+=n=2mBnznsatisfies the conditions of Schwarz Lemma. If 0<r<1, thenϕ(z)r2mIf equality occurs in (1.3) for one point z0=reiθ with 0<r<1, then ϕ(z)=eiαz2m and the equal sign holds in (1.3) for all zD.

Lemma 1.2 [3]

Let ϕ(z)=αnzn+αn+1zn+1+(αn0,n1) be analytic in D. If the maximum value of ϕ(z) on the circle z=r<1 is attained at z=z0, then we have z0ϕ(z0)=mϕ(z0),mn and every zD.

Lemma 1.3 [4]

Let p(z) be an element of p(m), then P(Dr) is the open disc with diameter end points w1=1-rk1+rk and w2=1w1.

Lemma 1.4 [5]

Let h(z)=z+am+1zm+1+a2m+1z2m+1+ be a starlike function on D. Thenr(1+rm)2mh(z)r(1-rm)2m(1-rm)1m(1+rm)2mh(z)(1+rm)1m(1-rm)2m

Section snippets

Main results

Theorem 2.1

Let f=h(z)+g(z) be an element of SH(m), thenw(z)-b1(1-r2m)1-b12r2m(1-b1)2rm1-b12r2m,where w(z) is the second dilatation of f.

Proof

Since f=h(z)+g(z)SH(m) then we have,w(z)=g(z)h(z)=b1+(m+1)bm+1zm+(2m+1)b2m+1z2m+(3m+1)b3m+1z3m+1+(m+1)am+1zm+(2m+1)a2m+1z2m+(3m+1)a3m+1z3m+thus,ϕ(z)=w(z)-w(0)1-w(0)w(z)=[(m+1)bm+1-b1(m+1)am+1]zm+=w(z)-b11-b1w(z)

Therefore ϕ(z) satisfies the conditions of Schwarz Lemma. Using Lemma 1.1, we can writew(z)-b11-b1w(z)zmw(z)-b1zm1-b1w(z)u2+v2-2α1(1-r2m)1-b12r2m

References (5)

  • P. Duren

    Univalent Functions

    (1983)
  • P. Duren

    Harmonic Mappings in the Plane

    (2004)
There are more references available in the full text version of this article.

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