Volume 2009, Article ID 807943,12pages doi:10.1155/2009/807943
Research Article
Univalence of Certain Linear Operators Defined by
Hypergeometric Function
R. Aghalary and A. Ebadian
Department of Mathematics, Faculty of Science, Urmia University, Urmia, Iran
Correspondence should be addressed to A. Ebadian,[email protected]
Received 11 January 2009; Accepted 22 April 2009
Recommended by Vijay Gupta
The main object of the present paper is to investigate univalence and starlikeness of certain integral operators, which are defined here by means of hypergeometric functions. Relevant connections of the results presented here with those obtained in earlier works are also pointed out.
Copyrightq2009 R. Aghalary and A. Ebadian. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.
1. Introduction and Preliminaries
LetHdenote the class of all analytic functionsf in the unit diskD {z ∈C:|z|< 1}. For
n≥0, a positive integer, let
An
f∈ H:fz z ∞
k1
ankznk
, 1.1
withA1:A, whereAis referred to as the normalized analytic functions in the unit disc. A functionf∈ Ais called starlike inDiffDis starlike with respect to the origin. The class of all starlike functions is denoted byS∗:S∗0. Forα <1, we define
S∗α
f ∈ A: Re
zfz fz
> α, z∈D
, 1.2
and it is called the class of all starlike functions of orderα. Clearly,S∗α⊆ S∗for 0< α <1. For functionsfjz, given by
fjz
∞
k0
ak,jzk, j 1,2
we define the Hadamard productor convolutionoff1zandf2zby
f1∗f2z: ∞
k0
ak,1ak,2zk: f2∗f1
z. 1.4
An interesting subclass of S the class of all analytic univalent functions is denoted by
Uα, μ, λand is defined by
U α, μ, λ
f ∈ A:1−α
z fz
μ
α
z fz
μ1
fz−1< λ, z∈D
, 1.5
where 0< α≤1, 0≤μ < αn,andλ >0.
The special case of this class has been studied by Ponnusamy and Vasundhra1and Obradovi´c et al.2.
For a,b,c∈C and c/0,-1,-2,. . ., the Gussian hypergeometric series Fa,b;c;zis defined as
Fa, b;c;z ∞
n0
anbn
cn
zn
n!, z∈D, 1.6
wherean aa1a2· · ·an−1anda0 1. It is well-known thatFa, b;c;zis analytic inD. As a special case of the Euler integral representation for the hypergeometric function, we have
F1, b;c;z Γc
ΓbΓc−b
1
0
1 1−tzt
b−11−tc−b−1dt, z∈D, Rec >Reb >0. 1.7
Now by letting
φa;c;z:F1, a;c;z, 1.8
it is easily seen that
zφa;c1;zcφa;c;z−cφa;c1;z. 1.9
Forf∈ A, Owa and Srivastava3introduced the operatorΩλ:A → Adefined by
Ωλfz Γ2−λ
Γ1−λz
λ d
dz
z
0 ft
which is extensions involving fractional derivatives and fractional integrals. Using definition ofφa;c;z:F1, a;c;zwe may write
Ωλfz zφ2; 2−λ;z∗fz. 1.11
This operator has been studied by Srivastava et al.4and Srivastava and Mishra5. Also forλ <1,Reα >0,andfz z∞k2akzk, let us define the functionFby
Fz:λz1−λ α
1
0
t1/α−2ftzdt
z 1−λ ∞
k2 ak
k−1α1z
k.
1.12
This operator has been investigated by many authors such as Trimble 6, and Obradovi´c et al.7.
If we take
ψ m, γ, z1 1−m ∞
k2
1
k−1γ1z
k, 1.13
then we can rewrite operatorFdefined by1.11as
Fz z
ψλ, α, z∗fz z
. 1.14
From the definition ofψm, γ, zit is easy to check that
zψ m, γ, z 1
γψ m, γ, z
1 γ
1 1−m z
1−z
. 1.15
Forf ∈Uα, μ, λwithz/fzμ∗φa;c1;z/0 for allz∈Dwe define the transform
Gby
Gz z
1
z/fzμ∗φa
;c1;z 1/μ
, 1.16
wherea, c∈Candc /0,−1,−2, . . . .
Also for f ∈ Uα, μ, λ with z/fzμ ∗ψm, γ, z/0 for all z ∈ D we define the transformHby
Hz z
1
z/fzμ∗ψm, γ, z
1/μ
, 1.17
In this investigation we aim to find conditions on α, μ, λ such that f ∈ Uα, μ, λ
implies that the functionfto be starlike. Also we find conditions onα, μ, λ, m, γ, a, cfor each
f∈Uα, μ, λ; the transformsGandHbelong toUα, μ, λandS∗. For proving our results we need the following lemmas.
Lemma 1.1cf. Hallenbeck and Ruscheweyh8. Lethzbe analytic and convex univalent in the unit diskDwithh0 1. Also let
gz 1b1zb2z2· · · 1.18
be analytic inD. If
gz zgz
c ≺hz z∈U;c /0, 1.19
then
gz≺ψz c zc
z
0
tc−1htdt≺hz z∈D;Rec≥0;c /0. 1.20
andψzis the best dominant of 1.20.
Lemma 1.2 cf. Ruscheweyh and Stankiewicz 8. If f andg are analytic and F and G are convex functions such thatf ≺F, g≺G,thenf∗g≺F∗G.
Lemma 1.3cf. Ruscheweyh and Sheil-Small9. LetFandGbe univalent convex functions in D. Then the Hadamard productF∗Gis also univalent convex inD.
2. Main Results
We follow the method of proof adopted in1,10.
Theorem 2.1. Let n be positive integer withn≥2. Also letn1/2n < α≤1andn1−α< μ < αn. Iffz zan1zn1· · · belongs toUα, μ, λ, Thenf ∈S∗γwhenever0< λ≤ λα, μ, n, γ,
where
λ α, μ, n, γ: ⎧ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎨ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎩
αn−μ2α 1−γ−1
αn−μ2μ22α 1−γ−1
, 0≤γ≤ μ−n1−α μ1n ,
αn−μ 1−γ nμγ −μ ,
μ−n1−α
μ1n < γ <1.
2.1
Proof. Let us define
pz
z fz
μ
Sincef ∈Uα, μ, λ, we have
1−α
z fz
μ
α
z fz
μ1
fz pz−α μzf
z
1 αn−μan1zn· · · 1λωz,
2.3
whereωzis an analytic function with|ωz|<1 andω0 ω0 · · ·ωn−10 0.By
Schwarz lemma, we have|ωz| ≤ |z|n. By2.3, it is easy to check that
pz 1−μλ
α
1
0 ωtz tμ/α1dt,
1−α αzf z
fz
1λωz
1−μλ/α10ωtz/ tμ/α1dt.
2.4
Therefore
1 1−γ
zfz fz −γ
α−1−αγ
/ 1−γα−μλ10 ωtz/tμ/α1dt α/ 1−γ1λωz αα−μλ10 ωtz/tμ/α1dt .
2.5
We need to show thatf ∈S∗γ. To do this, according to a well-known result9and2.5it suffices to show that
α−1−αγ/ 1−γα−μλ01 ωtz/tμ/α1dt α/1−γ1λωz
αα−μλ10 ωtz/tμ/α1dt /−iT, T ∈R, 2.6
which is equivalent to
λ
⎡
⎣ωz μ
αγ1−α/α−i 1−γT10 ωtz/tμ/α1dt α 1−γ1iT
⎤
⎦/ −1, T∈R. 2.7
Suppose thatBndenote the class of all Schwarz functionsωsuch thatω0 ω0
· · ·ωn−10 0,and let
M sup
z∈D,ω∈Bn,T∈R
ωz μ
αγ1−α/α−i 1−γT10 ωtz/tμ/α1dt α 1−γ1iT
then,f ∈S∗γifλM ≤1. This observation shows that it suffices to findM. First we notice that
M≤sup
T∈R
⎧ ⎪ ⎨ ⎪ ⎩
1 μ/ n−μ/α αγ1−α2/α2 1−γ2T2 α 1−γ1T2
⎫ ⎪ ⎬ ⎪
⎭. 2.9
Defineφ:0,∞ →Rby
φx αn−μ
μ αγ1−α2 1−γ2α2x
αn−μα 1−γ√1x . 2.10
Differentiatingφwith respect tox, we get
φx μ αn−μ
α3 1−γ3√1x/2 αγ1−α2 1−γ2α2x αn−μ2α2 1−γ21x
−
αn−μα 1−γ αn−μμ αγ1−α2 1−γ2α2x
/2√1x αn−μ2α2 1−γ21x .
2.11
Case 1. Let 0< γ <μ−n1−α/μ1n.Then we see thatφhas its only critical point in the positive real line at
x0
1
1−γ2α2
#
μ2 2α1−γ−12
αn−μ2 − αγ1−γ
2
$
. 2.12
Furthermore, we can see thatφx >0 for 0≤ x < x0 andφx <0 forx > x0. Henceφx attains its maximum value atx0and
φx≤φx0 αn−μ
2μ22α 1−γ−1
αn−μ2α 1−γ−1 αn−μ2μ22α1−γ−12
. 2.13
Case 2. Letγ >μ−n1−α/μ1n, then it is easy to see thatφx<0,and soφxattains its maximum value at 0 and
φx≤φ0 nμγ−μ
αn−μ 1−γ, ∀x≥0. 2.14
By puttingγ0 inTheorem 2.1we obtain the following result.
Corollary 2.2. Letnbe the positive integer withn≥2. Also letn1/2n < α≤1andn1−α< μ < αn. Iffz zan1zn1· · · belongs toUα, μ, λ, thenf ∈S∗ whenever0 < λ ≤αn− μ√2α−1/
αn−μ2μ22α−1.
Remark 2.3. Takingα1, μ1 inTheorem 2.1andCorollary 2.2we get results of10. We follow the method ofproof adopted in11.
Theorem 2.4. Letn≥2, a /0, c∈Cwith Re c≥0/cand the functionϕz 1b1zb2z2· · · withbn/0be univalent convex inD. Iffz zan1zn1· · · ∈Uα, μ, λandφa;c;zdefined by1.8satisfy the conditions
z fz
μ
∗φa;c1;z/0 ∀z∈D, φa;c;z≺ϕz,
2.15
then the transformGdefined by1.16has the following: 1G∈Uα, μ, λ|bn||c|/|cn|,
2G∈S∗whenever
0< λ≤ |cn| αn−μ
√
2α−1
|bn||c| αn−μ
2
μ22α−1
. 2.16
Proof. From the definition ofGwe obtain
z Gz
μ
z fz
μ
∗φa;c1;z. 2.17
Differentiatingz/Gzμshows that
z
z Gz
μ
μ
z Gz
μ
−μ
z Gz
μ1
Gz. 2.18
It is easy to see that
z
z fz
μ
∗φa;c1;z z
z fz
μ
∗φa;c1;z
. 2.19
From1.9and2.19we deduce that
z
z fz
μ
∗φa;c1;z
c
z fz
μ
∗φa;c;z−c
z fz
μ
or z z Gz μ c z Gz μ c z fz μ
∗φa;c;z. 2.21
Let us define
pz 1−α z Gz μ α z Gz μ1
Gz:1dnzn· · · , 2.22
thenpzis analytic inD, withp0 1 andp0 · · ·pn−10 0.Combining2.18with
2.21, one can obtain
pz
1αc
μ z Gz μ − αc μ z fz μ
∗φa;c;z. 2.23
Differentiatingpzyields
zpz
1αc
μ z z Gz μ −αc μz z fz μ
∗φa;c;z. 2.24
In view of2.21,2.23, and2.24, we obtain
cpz zpz c
1αc
μ
z Gz
μ
−αc2 μ
z fz
μ
∗φa;c;z
1αc
μ z z Gz μ −αc μ z z fz μ
∗φa;c;z
c
1αc
μ
z fz
μ
∗φa;c;z
−αc2 μ
z fz
μ
∗φa;c;z−αc
μ
z fz
μ
∗φa;c;z
c
z fz
μ
∗φa;c;z−cα
# z fz μ − z fz μ1 fz
$
∗φa;c;z
c
#
1−α z fz μ α z fz μ1 fz
$
∗φa;c;z.
2.25
Hence
pz 1 czp
z
#
1−α z fz μ α z fz μ1 fz
$
Since 1λznandϕz 1b1zb2z2· · · are convex and
1−α
z fz
μ
α
z fz
μ1
fz≺1λzn, φa;c;z≺ϕz, 2.27
by using Lemmas1.2and1.3, from2.26we deduce that
pz 1 czp
z≺1b
nλzn. 2.28
It now follows fromLemma 1.1that
pz≺ψz c zc
z
0
tc−11bnλzndt. 2.29
Therefore
pz≺1 λbnc
cnz
n, 2.30
and the result follows from the last subordination andCorollary 2.2.
It is well-known thatsee,12ifc, a >0 andc≥max{2, a}, thenφa;c;zis univalent convex function in D. So if we take ϕz φa;c;z in the Theorem 2.4, we obtain the following.
Corollary 2.5. Forn ≥2, c, a >0,andc≥ max{2, a}, let the functionfz zanzn1· · · ∈
Uα, μ, λandφa;c;zdefined by1.8satisfy the condition
z fz
μ
∗φa;c1;z/0 ∀z∈D. 2.31
Then the transformGdefined by1.16has the following: 1G∈Uα, μ, λ|an|c/|cn|cn;
2G∈S∗whenever
0< λ≤ cn|cn| αn−μ
√
2α−1
|an|c αn−μ
2
μ22α−1
. 2.32
Corollary 2.6. Forn≥2, c∈Cwith Re c≥0/c, let the functionfz zanzn1· · · ∈Uα, μ, λ
andφa;c;zdefined by1.8satisfy the condition
z fz
μ
∗φa;c1;z/ ∀z∈D. 2.33
Then the transformGdefined by1.16has the following: 1G∈Uα, μ, λ|c|/|cn|;
2G∈S∗whenever
0< λ≤ |cn| αn−μ
√
2α−1
|c| αn−μ2μ22α−1
. 2.34
Remark 2.7. Takingα1 andμ1 onCorollary 2.6, we get a result of11. By puttingc1−Manda2 onTheorem 2.10we obtain the following.
Corollary 2.8. Letn≥2andϕz 1∞k1bkzkwithbn/0be univalent convex function inD.
Also letM∈Cwith ReM <1andfz zan1zn1· · · ∈Uα, μ, λ, satisfy
ΩM
z fz
μ
/
0 z∈D, 2.35
and letGbe the function which is defined by
Gz z
1
ΩM z/fzμ
1/μ
. 2.36
If
φ2; 1−M;z≺ϕz, 2.37
then we have the following:
1G∈Uα, μ, λ|bn||1−M|/|n1−M|;
2G∈S∗whenever
0< λ≤ |1−Mn| αn−μ
√
2α−1
|bn||1−M| αn−μ
2
μ22α−1
. 2.38
In13, Pannusamy and Sahoo have also considered the classUα, μ, λfor the case
α1 withμn.
Theorem 2.10. Form <1, γ /0;Reγ >0, n≥2,letfz zan1zn1· · · ∈Uα, μ, λand ψm, γ, zdefined by1.13satisfy the condition
z fz
μ
∗ψ m, γ, z/0 ∀z∈D. 2.39
Then the transformHdefined by1.17has the following: 1H∈Uα, μ, λ1−m/|1nγ|;
2H∈S∗whenever
0< λ≤ 1nγ αn−μ
√
2α−1
1−m αn−μ2μ22α−1
. 2.40
Proof. Let us define
pz 1−α
z Hz
μ
α
z Hz
μ1
Hz, 2.41
thenpzis analytic inD, withp0 1 andp0 · · ·pn−10 0.Using the same method
as onTheorem 2.4we get
pz γzpz
#
1−α
z fz
μ
α
z fz
μ1 fz
$
∗
1 1−m z
1−z
. 2.42
Since 1λznandhz 1 1−mz/1−zare convex,
1−α
z fz
μ
α
z fz
μ1
fz≺1λzn. 2.43
Using Lemmas1.2and1.3, from2.42it yields
pz γzpz≺1−mλzn. 2.44
It now follows fromLemma 1.1that
pz≺ 1 γz1/γ
z
0
Therefore
pz−1≤ λ 1−m 1nγ|z|
n, 2.46
and the result follows from2.46andCorollary 2.2.
References
1 S. Ponnusamy and P. Vasundhra, “Criteria for univalence, starlikeness and convexity,” Annales Polonici Mathematici, vol. 85, no. 2, pp. 121–133, 2005.
2 M. Obradovi´c, S. Ponnusamy, V. Singh, and P. Vasundhra, “Univalency, starlikeness and convexity applied to certain classes of rational functions,”Analysis, vol. 22, no. 3, pp. 225–242, 2002.
3 S. Owa and H. M. Srivastava, “Univalent and starlike generalized hypergeometric functions,” Canadian Journal of Mathematics, vol. 39, no. 5, pp. 1057–1077, 1987.
4 H. M. Srivastava, A. K. Mishra, and M. K. Das, “A nested class of analytic functions defined by fractional calculus,”Communications in Applied Analysis, vol. 2, no. 3, pp. 321–332, 1998.
5 H. M. Srivastava and A. K. Mishra, “Applications of fractional calculus to parabolic starlike and uniformly convex functions,”Computers & Mathematics with Applications, vol. 39, no. 3-4, pp. 57–69, 2000.
6 S. Y. Trimble, “The convex sum of convex functions,”Mathematische Zeitschrift, vol. 109, pp. 112–114, 1969.
7 M. Obradovi´c, S. Ponnusamy, and P. Vasundhra, “Univalence, strong starlikeness and integral transforms,”Annales Polonici Mathematici, vol. 86, no. 1, pp. 1–13, 2005.
8 St. Ruscheweyh and J. Stankiewicz, “Subordination under convex univalent functions,”Bulletin of the Polish Academy of Sciences, Mathematics, vol. 33, no. 9-10, pp. 499–502, 1985.
9 St. Ruscheweyh and T. Sheil-Small, “Hadamard products of Schlicht functions and the P ¨olya-Schoenberg conjecture,”Commentarii Mathematici Helvetici, vol. 48, pp. 119–135, 1973.
10 S. Ponnusamy and P. Sahoo, “Geometric properties of certain linear integral transforms,”Bulletin of the Belgian Mathematical Society. Simon Stevin, vol. 12, no. 1, pp. 95–108, 2005.
11 M. Obradovi´c and S. Ponnusamy, “Univalence and starlikeness of certain transforms defined by convolution of analytic functions,”Journal of Mathematical Analysis and Applications, vol. 336, no. 2, pp. 758–767, 2007.
12 Y. Ling, F. Liu, and G. Bao, “Some properties of an integral transform,”Applied Mathematics Letters, vol. 19, no. 8, pp. 830–833, 2006.