Abstract
Keywords:
harmonic starlike function; growth theorem; distortion theorem1 Introduction
Let Ω be the family of functions
which are regular in
and satisfy the conditions
,
for all
; denote by
the family of functions
regular in
, such that
is in
if and only if
Next, let
and
be regular functions in
, if there exists
such that
for all
, then we say that
is subordinated to
and we write
, then
.
Moreover, univalent harmonic functions are generalizations of univalent regular functions; the point of departure is the canonical representation
of a harmonic function f in the unit disc
as the sum of a regular function
and the conjugate of a regular function
. With the convention that
, the representation is unique. The power series expansions of
and
are denoted by
If f is a sense-preserving harmonic mapping of
onto some other region, then, by Lewy theorem, its Jacobian is strictly positive,
i.e.,
Equivalently [1], the inequality
holds for all
. This shows, in particular, that
, so there is no loss of generality in supposing that
and
. The class of all sense-preserving harmonic mappings of the disc with
and
will be denoted by
. Thus
contains the standard class S of regular univalent functions. Although the regular part
of a function
is locally univalent, it will become apparent that it need not be univalent. The
class of functions
with
will be denoted by
. At the same time, we note that
is a normal family and
is a compact normal family [2].
Finally, let
be an element
(or
). If f satisfies the condition
then f is called harmonic starlike function. The class of such functions is denoted by
(or
). Also, let
be an element
(or
). If f satisfies the condition
then f is called a convex harmonic function. The class of convex harmonic functions is denoted
by
(or
).
For the aim of this paper, we will need the following lemma and theorem.
Lemma 1.1 ([2], p.51])
If
, then there exist anglesαandβsuch that
Theorem 1.2 ([2], p.108])
If
is a starlike function and if
and
are the regular functions defined by
,
,
, then
is a convex function.
2 Main results
Lemma 2.1Let
be an element of
, then
where
Proof Using Theorem 1.2, we write
On the other hand, since
is regular and satisfies the condition
, with
, the function
is an element of
[4]. Therefore, we have
After simple calculations from (2.3), we get (2.1). □
Corollary 2.2Let
be an element of
, then
Proof Since
, then
and the second dilatation
satisfies the condition of Schwarz lemma, then the inequality (2.1) can be written
in the form
which is given in (2.4) and (2.5). □
Corollary 2.3Let
be an element of
, then
Proof Using Theorem 1.2 and Corollary 2.2, we obtain (2.7) and (2.8). □
Theorem 2.4If
is in
andais in
, then
then we have
(2.11)Letting
and
in (2.11) and after the straightforward calculations, we obtain
and we conclude that
is in
for every admissible ρ. From the compactness of
[2] and (2.11), we infer that
is in
. We also note that this theorem is a generalization of the theorem of Libera and
Ziegler [3]. □
Corollary 2.5Let
be an element of
, then
(2.13)
(2.14)Proof Using Theorem 2.4, we have
If we apply Corollary 2.3 to
and
by taking
,
and after straightforward calculations, we get (2.13) and (2.14). □
Competing interests
The authors declare that they have no competing interests.
Authors’ contributions
All authors contributed equally and significantly to writing this paper. All authors read and approved the final manuscript.
Acknowledgements
The authors are very grateful to the referees for their valuable comments and suggestions. They were very helpful for our paper.
References
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Clunie, J, Sheil-Small, T: Harmonic univalent functions. Ann. Acad. Sci. Fenn., Ser. A 1 Math.. 9, 3–25 (1984)
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Duren, P: Harmonic Mappings in the Plane, Cambridge University Press, Cambridge (2004)
-
Libera, RJ, Ziegler, MR: Regular functions
for which
is α-spirallike. Trans. Am. Math. Soc.. 166, 361–370 (1972)

































