Study on Starlike and Convex Properties
A. O. Mostafa vol. 10, iss. 3, art. 87, 2009
Title Page
Contents
JJ II
J I
Page1of 16 Go Back Full Screen
Close
A STUDY ON STARLIKE AND CONVEX
PROPERTIES FOR HYPERGEOMETRIC FUNCTIONS
A. O. MOSTAFA
Department of Mathematics Faculty of Science
Mansoura University Mansoura 35516, Egypt EMail:adelaeg254@yahoo.com
Received: 07 May, 2008
Accepted: 21 August, 2009
Communicated by: S.S. Dragomir 2000 AMS Sub. Class.: 30C45.
Key words: Starlike, Convex, Hypergeometric function, Integral operator.
Abstract: The objective of the present paper is to give some characterizations for a (Gaus- sian) hypergeometric function to be in various subclasses of starlike and convex functions. We also consider an integral operator related to the hypergeometric function.
Study on Starlike and Convex Properties
A. O. Mostafa vol. 10, iss. 3, art. 87, 2009
Title Page Contents
JJ II
J I
Page2of 16 Go Back Full Screen
Close
Contents
1 Introduction 3
2 Main Results 5
3 An Integral Operator 13
Study on Starlike and Convex Properties
A. O. Mostafa vol. 10, iss. 3, art. 87, 2009
Title Page Contents
JJ II
J I
Page3of 16 Go Back Full Screen
Close
1. Introduction
LetT be the class consisting of functions of the form:
(1.1) f(z) = z−
∞
X
n=2
anzn (an>0),
which are analytic and univalent in the open unit discU ={z :|z|<1}.LetT(λ, α) be the subclass ofT consisting of functions which satisfy the condition:
(1.2) Re
zf0(z)
λzf0(z) + (1−λ)f(z)
> α, for someα(0≤α <1), λ(0≤λ <1)and for allz∈U.
Also, letC(λ, α)denote the subclass of T consisting of functions which satisfy the condition:
(1.3) Re
f0(z) +zf00(z) f0(z) +λzf00(z)
> α, for someα(0≤α <1), λ(0≤λ <1)and for allz∈U.
From(1.2)and(1.3), we have
(1.4) f(z)∈C(λ, α)⇔zf0(z)∈T(λ, α).
We note thatT(0, α) =T∗(α),the class of starlike functions of orderα (0≤α <1) and C(0, α) = C(α), the class of convex functions of orderα (0 ≤ α < 1) (see Silverman [6]).
LetF(a, b;c;z)be the (Gaussian ) hypergeometric function defined by
(1.5) F(a, b;c;z) =
∞
X
n=0
(a)n(b)n
(c)n(1)nzn,
Study on Starlike and Convex Properties
A. O. Mostafa vol. 10, iss. 3, art. 87, 2009
Title Page Contents
JJ II
J I
Page4of 16 Go Back Full Screen
Close
wherec6= 0,−1,−2, ...,and(θ)nis the Pochhammer symbol defined by (θ)n =
( 1, n= 0
θ(θ+ 1)· · ·(θ+n−1) n∈N ={1,2, ...}.
We note that F(a, b;c; 1) converges for Re(c− a −b) > 0 and is related to the Gamma function by
(1.6) F(a, b;c; 1) = Γ(c)Γ(c−a−b) Γ(c−a)Γ(c−b).
Silverman [7] gave necessary and sufficient conditions forzF(a, b;c;z)to be in T∗(α)and C(α), also examining a linear operator acting on hypergeometric func- tions. For other interesting developments onzF(a, b;c;z)in connection with various subclasses of univalent functions, the reader can refer the to works of Carlson and Shaffer [2], Merkes and Scott [4], Ruscheweyh and Singh [5] and Cho et al. [3].
Study on Starlike and Convex Properties
A. O. Mostafa vol. 10, iss. 3, art. 87, 2009
Title Page Contents
JJ II
J I
Page5of 16 Go Back Full Screen
Close
2. Main Results
To establish our main results, we need the following lemma due to Altintas and Owa [1].
Lemma 2.1.
(i) A functionf(z)defined by(1.1)is in the classT(λ, α)if and only if (2.1)
∞
X
n=2
(n−λαn−α+λα)an ≤1−α.
(ii) A functionf(z)defined by(1.1)is in the classC(λ, α)if and only if (2.2)
∞
X
n=2
n(n−λαn−α+λα)an≤1−α.
Theorem A.
(i) Ifa, b >−1, c > 0andab <0,thenzF(a, b;c;z)is inT(λ, α)if and only if (2.3) c > a+b+ 1− (1−λα)ab
1−α .
(ii) If a, b > 0 andc > a+b+ 1, thenF1(a, b;c;z) = z[2−F(a, b;c;z)] is in T(λ, α)if and only if
(2.4) Γ(c)Γ(c−a−b) Γ(c−a)Γ(c−b)
1 + (1−λα)ab (1−α)(c−a−b−1)
≤2.
Study on Starlike and Convex Properties
A. O. Mostafa vol. 10, iss. 3, art. 87, 2009
Title Page Contents
JJ II
J I
Page6of 16 Go Back Full Screen
Close
Proof. (i)Since
zF(a, b;c;z) =z+ ab c
∞
X
n=2
(a+ 1)n−2(b+ 1)n−2
(c+ 1)n−2(1)n−1
zn (2.5)
=z−
ab c
∞
X
n=2
(a+ 1)n−2(b+ 1)n−2
(c+ 1)n−2(1)n−1
zn,
according to(i)of Lemma2.1, we must show that (2.6)
∞
X
n=2
(n−λαn−α+λα)(a+ 1)n−2(b+ 1)n−2
(c+ 1)n−2(1)n−1
≤
c ab
(1−α). Note that the left side of(2.6)diverges ifc < a+b+ 1. Now
∞
X
n=2
(n−λαn−α+λα)(a+ 1)n−2(b+ 1)n−2 (c+ 1)n−2(1)n−1
= (1−λα)
∞
X
n=0
(n+ 1)(a+ 1)n(b+ 1)n (c+ 1)n(1)n+1
+ (1−α)
∞
X
n=0
(a+ 1)n(b+ 1)n (c+ 1)n(1)n+1
= (1−λα)
∞
X
n=0
(a+ 1)n(b+ 1)n
(c+ 1)n(1)n +(1−α)c ab
∞
X
n=1
(a)n(b)n (c)n(1)n
= (1−λα)Γ(c+ 1)Γ(c−a−b−1)
Γ(c−a)Γ(c−b) +(1−α)c ab
Γ(c)Γ(c−a−b) Γ(c−a)Γ(c−b)−1
.
Study on Starlike and Convex Properties
A. O. Mostafa vol. 10, iss. 3, art. 87, 2009
Title Page Contents
JJ II
J I
Page7of 16 Go Back Full Screen
Close
Hence,(2.6)is equivalent to (2.7) Γ(c+ 1)Γ(c−a−b−1)
Γ(c−a)Γ(c−b)
(1−λα) + (1−α)(c−a−b−1) ab
≤(1−α)h
c ab
+ c
ab i
= 0.
Thus,(2.7)is valid if and only if
(1−λα) + (1−α)(c−a−b−1)
ab ≤0,
or equivalently,
c>a+b+ 1− (1−λα)ab 1−α . (ii)Since
F1(a, b;c;z) =z−
∞
X
n=2
(a)n−1(b)n−1
(c)n−1(1)n−1
zn, by(i)of Lemma2.1, we need only to show that
∞
X
n=2
(n−λαn−α+λα)(a)n−1(b)n−1
(c)n−1(1)n−1
≤1−α.
Now,
∞
X
n=2
(n−λαn−α+λα)(a)n−1(b)n−1
(c)n−1(1)n−1
(2.8)
=
∞
X
n=2
[(n−1)(1−λα) + (1−α)](a)n−1(b)n−1
(c)n−1(1)n−1
Study on Starlike and Convex Properties
A. O. Mostafa vol. 10, iss. 3, art. 87, 2009
Title Page Contents
JJ II
J I
Page8of 16 Go Back Full Screen
Close
= (1−λα)
∞
X
n=1
n(a)n(b)n
(c)n(1)n + (1−α)
∞
X
n=1
(a)n(b)n (c)n(1)n
= (1−λα)
∞
X
n=1
(a)n(b)n (c)n(1)n−1
+ (1−α)
∞
X
n=1
(a)n(b)n (c)n(1)n. Noting that(θ)n=θ((θ+ 1)n−1then,(2.8)may be expressed as
(1−λα)ab c
∞
X
n=1
(a+ 1)n−1(b+ 1)n−1
(c+ 1)n−1(1)n−1 + (1−α)
∞
X
n=1
(a)n(b)n (c)n(1)n
= (1−λα)ab c
∞
X
n=0
(a+ 1)n(b+ 1)n
(c+ 1)n(1)n + (1−α)
" ∞ X
n=0
(a)n(b)n (c)n(1)n −1
#
= (1−λα)ab c
Γ(c+ 1)Γ(c−a−b−1)
Γ(c−a)Γ(c−b) + (1−α)
Γ(c)Γ(c−a−b) Γ(c−a)Γ(c−b)−1
= Γ(c)Γ(c−a−b) Γ(c−a)Γ(c−b)
(1−α) + ab(1−λα) (c−a−b−1)
−(1−α).
But this last expression is bounded above by1−αif and only if(2.4)holds.
Theorem B.
(i) Ifa, b >−1,ab < 0,andc > a+b+ 2,thenzF(a, b;c;z)is inC(λ, α)if and only if
(2.9) (1−λα)(a)2(b)2 + (3−2λα−α)ab(c−a−b−2)
+ (1−α)(c−a−b−2)2 >0.
Study on Starlike and Convex Properties
A. O. Mostafa vol. 10, iss. 3, art. 87, 2009
Title Page Contents
JJ II
J I
Page9of 16 Go Back Full Screen
Close
(ii) If a, b > 0 and c > a+b+ 2, thenF1(a, b;c;z) = z[2−F(a, b;c;z)] is in C(λ, α)if and only if
(2.10) Γ(c)Γ(c−a−b) Γ(c−a)Γ(c−b)
1 + (1−λα)(a)2(b)2 (1−α)(c−a−b−2)2 +
3−2λα−α 1−α
ab c−a−b−1
≤2.
Proof. (i) SincezF(a, b;c;z)has the form (2.5), we see from(ii) of Lemma 2.1, that our conclusion is equivalent to
(2.11)
∞
X
n=2
n(n−λαn−α+λα)(a+ 1)n−2(b+ 1)n−2
(c+ 1)n−2(1)n−1
≤
c ab
(1−α). Note that forc > a+b+ 2, the left side of(2.11)converges. Writing
(n+ 2)[(n+ 2)(1−λα)−α(1−λ)]
= (n+ 1)2(1−λα) + (n+ 1)(2−α−λα) + (1−α), we see that
∞
X
n=0
(n+ 2)[(n+ 2)(1−λα)−α(1−λ)](a+ 1)n(b+ 1)n (c+ 1)n(1)n+1
= (1−λα)
∞
X
n=0
(n+ 1)2(a+ 1)n(b+ 1)n (c+ 1)n(1)n+1 + (2−α−λα)
∞
X
n=0
(n+ 1)(a+ 1)n(b+ 1)n
(c+ 1)n(1)n+1 + (1−α)
∞
X
n=0
(a+ 1)n(b+ 1)n
(c+ 1)n(1)n+1
Study on Starlike and Convex Properties
A. O. Mostafa vol. 10, iss. 3, art. 87, 2009
Title Page Contents
JJ II
J I
Page10of 16 Go Back Full Screen
Close
= (1−λα)
∞
X
n=0
(n+ 1)(a+ 1)n(b+ 1)n (c+ 1)n(1)n + (2−α−λα)
∞
X
n=0
(a+ 1)n(b+ 1)n
(c+ 1)n(1)n + (1−α)
∞
X
n=0
(a+ 1)n(b+ 1)n (c+ 1)n(1)n+1
= (1−λα)
∞
X
n=0
n(a+ 1)n(b+ 1)n (c+ 1)n(1)n
+ (3−α−2λα)
∞
X
n=0
(a+ 1)n(b+ 1)n (c+ 1)n(1)n
+ (1−α)
∞
X
n=1
(a+ 1)n−1(b+ 1)n−1
(c+ 1)n−1(1)n
= (1−λα)(a+ 1)(b+ 1) (c+ 1)
∞
X
n=0
(a+ 2)n(b+ 2)n (c+ 2)n(1)n + (3−α−2λα)
∞
X
n=0
(a+ 1)n(b+ 1)n
(c+ 1)n(1)n + (1−α) c ab
∞
X
n=1
(a)n(b)n (c)n(1)n
= Γ(c+ 1)Γ(c−a−b−2) Γ(c−a)Γ(c−b)
−(1−λα)(a+ 1)(b+ 1) +(3−α−2λα)(c−a−b−2) + (1−α)
ab (c−a−b−2)2
− (1−α)c ab . This last expression is bounded above by
abc
(1−α)if and only if (1−λα)(a+1)(b+1)+(3−α−2λα)(c−a−b−2)+(1−α)
ab (c−a−b−2)2 ≤0, which is equivalent to(2.9).
Study on Starlike and Convex Properties
A. O. Mostafa vol. 10, iss. 3, art. 87, 2009
Title Page Contents
JJ II
J I
Page11of 16 Go Back Full Screen
Close
(ii)In view of(ii)of Lemma2.1, we need to show that
∞
X
n=2
n(n−λαn−α+λα)(a)n−1(b)n−1
(c)n−1(1)n−1
≤(1−α). Now
∞
X
n=2
n(n−λαn−α+λα)(a)n−1(b)n−1
(c)n−1(1)n−1
(2.12)
=
∞
X
n=0
(n+ 2)[(n+ 2)(1−λα)−α(1−λ)](a)n+1(b)n+1 (c)n+1(1)n+1
= (1−λα)
∞
X
n=0
(n+2)2(a)n+1(b)n+1
(c)n+1(1)n+1−α(1−λ)
∞
X
n=0
(n+2)(a)n+1(b)n+1 (c)n+1(1)n+1. Writing(n+ 2) = (n+ 1) + 1,we have
∞
X
n=0
(n+ 2)(a)n+1(b)n+1 (c)n+1(1)n+1 =
∞
X
n=0
(n+ 1)(a)n+1(b)n+1 (c)n+1(1)n+1 +
∞
X
n=0
(a)n+1(b)n+1 (c)n+1(1)n+1 (2.13)
=
∞
X
n=0
(a)n+1(b)n+1 (c)n+1(1)n +
∞
X
n=0
(a)n+1(b)n+1 (c)n+1(1)n+1 and
∞
X
n=0
(n+ 2)2(a)n+1(b)n+1 (c)n+1(1)n+1 (2.14)
=
∞
X
n=0
(n+ 1)(a)n+1(b)n+1
(c)n+1(1)n + 2
∞
X
n=0
(a)n+1(b)n+1
(c)n+1(1)n +
∞
X
n=0
(a)n+1(b)n+1
(c)n+1(1)n+1
Study on Starlike and Convex Properties
A. O. Mostafa vol. 10, iss. 3, art. 87, 2009
Title Page Contents
JJ II
J I
Page12of 16 Go Back Full Screen
Close
=
∞
X
n=1
(a)n+1(b)n+1 (c)n+1(1)n−1
+ 3
∞
X
n=0
(a)n+1(b)n+1 (c)n+1(1)n +
∞
X
n=1
(a)n(b)n (c)n(1)n. Substituting(2.13)and(2.14)into the right side of(2.12), yields (2.15) (1−λα)
∞
X
n=0
(a)n+2(b)n+2
(c)n+2(1)n + (3−2λα−α)
∞
X
n=0
(a)n+1(b)n+1 (c)n+1(1)n + (1−α)
∞
X
n=1
(a)n(b)n (c)n(1)n. Since(a)n+k= (a)k(a+k)n,we may write(2.15)as
Γ(c)Γ(c−a−b) Γ(c−a)Γ(c−b)
(1−λα)(a)2(b)2
(c−a−b−2)2 +(3−2λα−α)ab
(c−a−b−1) + (1−α)
−(1−α).
By a simplification, we see that the last expression is bounded above by(1−α)if and only if(2.10)holds.
Puttingλ= 0in(i)of TheoremB, we have:
Corollary 2.2. If a, b > −1, ab < 0, and c > a+b + 2,then zF(a, b;c;z) is in C(α)if and only if
(a)2(b)2+ (3−α)ab(c−a−b−2) + (1−α)(c−a−b−2)2 >0.
Remark 1. Corollary2.2, corrects the result obtained by Silverman [7, Theorem 4].
Study on Starlike and Convex Properties
A. O. Mostafa vol. 10, iss. 3, art. 87, 2009
Title Page Contents
JJ II
J I
Page13of 16 Go Back Full Screen
Close
3. An Integral Operator
In the theorems below, we obtain similar results in connection with a particular inte- gral operatorG(a, b;c;z)acting onF(a, b;c;z)as follows:
(3.1) G(a, b;c;z) =
Z z
0
F(a, b;c;t)dt.
Theorem C. Let a, b > −1, ab < 0 and c > max{0, a +b}. Then G(a, b;c;z) defined by(3.1)is inT(λ, α)if and only if
(3.2) Γ(c+ 1)Γ(c−a−b) Γ(c−a)Γ(c−b)
(1−λα)
ab − α(1−λ)(c−a−b) (a−1)2(b−1)2
+α(1−λ)(c−1)2 (a−1)2(b−1)2 ≤0.
Proof. Since
G(a, b;c;z) = z−
ab c
∞
X
n=2
(a+ 1)n−2(b+ 1)n−2
(c+ 1)n−2(1)n
zn,
by(i)of Lemma2.1, we need only to show that
∞
X
n=2
(n−λαn−α+λα)(a+ 1)n−2(b+ 1)n−2
(c+ 1)n−2(1)n ≤
c ab
(1−α).
Study on Starlike and Convex Properties
A. O. Mostafa vol. 10, iss. 3, art. 87, 2009
Title Page Contents
JJ II
J I
Page14of 16 Go Back Full Screen
Close
Now
∞
X
n=2
[n(1−λα)−α(1−λ)](a+ 1)n−2(b+ 1)n−2 (c+ 1)n−2(1)n
= (1−λα)
∞
X
n=0
(n+ 2)(a+ 1)n(b+ 1)n (c+ 1)n(1)n+2
−α(1−λ)
∞
X
n=0
(a+ 1)n(b+ 1)n (c+ 1)n(1)n+2
= (1−λα)
∞
X
n=0
(a+ 1)n(b+ 1)n
(c+ 1)n(1)n+1 −α(1−λ)
∞
X
n=1
(a+ 1)n−1(b+ 1)n−1
(c+ 1)n−1(1)n+1
= (1−λα)
∞
X
n=1
(a+ 1)n−1(b+ 1)n−1
(c+ 1)n−1(1)n −α(1−λ) c ab
∞
X
n=1
(a)n(b)n (c)n(1)n+1
= (1−λα) c ab
∞
X
n=1
(a)n(b)n
(c)n(1)n −α(1−λ) c ab
∞
X
n=1
(a)n(b)n (c)n(1)n+1
= (1−λα) c ab
" ∞ X
n=0
(a)n(b)n (c)n(1)n
−1
#
−α(1−λ) (c−1)2 (a−1)2(b−1)2
∞
X
n=2
(a−1)n(b−1)n (c−1)n(1)n
= Γ(c+ 1)Γ(c−a−b) Γ(c−a)Γ(c−b)
(1−λα)
ab − α(1−λ)(c−a−b) (a−1)2(b−1)2
+ α(1−λ)(c−1)2
(a−1)2(b−1)2 − (1−α)c ab , which is bounded above by(1−α)
abc
if and only if(3.2)holds.
Now, we observe that G(a, b;c;z) ∈ C(λ, α) if and only if zF(a, b;c;z) ∈
Study on Starlike and Convex Properties
A. O. Mostafa vol. 10, iss. 3, art. 87, 2009
Title Page Contents
JJ II
J I
Page15of 16 Go Back Full Screen
Close
T(λ, α).Thus any result of functions belonging to the classT(λ, α)aboutzF(a, b;c;z) leads to that of functions belonging to the class C(λ, α).Hence we obtain the fol- lowing analogous result to TheoremA.
Theorem 3.1. Leta, b > −1, ab < 0andc > a+b+ 2.ThenG(a, b;c;z)defined by(3.1)is inC(λ, α)if and only if
c > a+b+ 1−(1−λα)ab 1−α .
Remark 2. Puttingλ= 0in the above results, we obtain the results of Silverman [7].
Study on Starlike and Convex Properties
A. O. Mostafa vol. 10, iss. 3, art. 87, 2009
Title Page Contents
JJ II
J I
Page16of 16 Go Back Full Screen
Close
References
[1] O. ALTINTASANDS. OWA, On subclasses of univalent functions with negative coefficients, Pusan Ky˘ongnam Math. J., 4 (1988), 41–56.
[2] B.C. CARLSONANDD.B. SHAFFER, Starlike and prestarlike hypergeometric functions, J. Math. Anal. Appl., 15 (1984), 737–745.
[3] N.E. CHO, S.Y. WOOANDS. OWA, Uniform convexity properties for hyperge- ometric functions, Fract. Calculus Appl. Anal., 5(3) (2002), 303–313.
[4] E. MERKESANDB.T. SCOTT, Starlike hypergeometric functions, Proc. Amer.
Math. Soc., 12 (1961), 885–888.
[5] St. RUSCHEWEYHANDV. SINGH, On the order of starlikeness of hypergeo- metric functions, J. Math. Anal. Appl., 113 (1986), 1–11.
[6] H. SILVERMAN, Univalent functions with negative coefficients, Proc. Amer.
Math. Soc., 51 (1975), 109–116.
[7] H. SILVERMAN, Starlike and convexity properties for hypergeometric func- tions, J. Math. Anal. Appl., 172 (1993), 574–581.