299 International Journal of Advanced Research and Development
ISSN: 2455-4030, Impact Factor: RJIF 5.24 www.advancedjournal.com
Volume 2; Issue 4; July 2017; Page No. 299-304
New subclass of univalent function associated with a fractional calculus operators
1 Pawan Chanchal, 2 AK Arora, 3 Jyoti Taneja
1 Departmentof Mathematics, Government College Kekri, Ajmer, Rajasthan, India
2 Department of Mathematics, Government College of Ajmer, Ajmer, Rajasthan, India
3 Department of Mathematics, Bhag Singh Khalsa College for Women, Abohar, Punjab, India Abstract
In this paper, by making use of generalized hypergeometric function we define a new class π(a, b, c; Ξ², Ξ΄, k) of univalent functions in the open unit disk. We derived coefficient estimate, distortion theorems, extreme points and application to fractional calculus operator for the function belonging to this class.
Keywords: hadamard product, generalized hypergeometric functions, fractional integral operator, coefficient estimate, distortion theorem
1. Introduction
Let β¦ be the class of analytic and univalent function in the open unit disk π = { π§ β πΆ βΆ |π§| < 1} is of the form
f(z) = z + ββπ=2πΌππ§π (1)
Let f β¦ given by (1) and g β¦ given by
g(z) = z + ββk=2Ξ²kzk (2)
We define the convolution product (or Hadamard) of f and g by
(f β g)(z) = z + ββk=2Ξ±kΞ²kzk= (g β f) (z); (z β π°), (3) Let β is subclass of β¦ consisting of the functions of the form:
f(z) = z - ββπ=2πΌππ§π (4)
Definition 1:- The generalized hypergeometric function 2R1 (a, b, c; k; z) [1] is defined by
2R1 (a, b, c; k; z) = Ξ(c)
Ξ(b)β (a)nΞ(b+kn)zn
Ξ(c+kn) (n)!
βn=0 , k β R, k > 0, |z| < 1, (5)
Where Re(c-a-b)>0 and (a)n Pochhammer symbol is given by (π)π= Ξ(a+n)
Ξ(a) .
Definition 2:- Let f(z) be in form (4), by using (3) we define a operator Ξ¦(a, b, c; k): ββ β by
Β΅(a, b, c; k)f(z) = ( z 2R1 (a, b, c; k; z)) β f(z) = (z (Ξ(c)
Ξ(b)β(a)nΞ(b + kn)zn Ξ(c + kn) (n)!
β
n=0
)) β (z β β πΌππ§π
β
π=2
)
Β΅(a, b, c; k)f(z) = z βΞ(c)
Ξ(b)β (a)nβ1Ξ(b+k(nβ1))πΌπzn Ξ(c+k(nβ1)) (nβ1)!
βn=0 π, π, π β π; π§ β π, π > 0 (6)
Definition 3:- Let f(z) be in the form (4) is said to be in subclass X (a, b, c; Ξ², Ξ΄, k) if and only if
|π§(Β΅(a,b,c;k)f(z))β²β²β²βΞ΄(Β΅(a,b,c;k)f(z))β²β²
(Β΅(a,b,c;k)f(z))β²β²+2(1βΞ΄) | < π½, π§ β π, 0 β€ πΏ β€ 1, 0 < π½ β€ 1, (7)
300 2. Coefficient Estimate
Theorem 1:- Let the function f(z) defined by (4). Then π(π§) β π(a, b, c; Ξ², Ξ΄, k) if and only if
ββπ=2π(π β 1)(π β 2 + πΏ + π½)Ξ(c)(a)nβ1Ξ(b+k(nβ1))πΌπ
Ξ(b)Ξ(c+k(nβ1)) (nβ1)! β€ 2Ξ²(1 β Ξ΄) (8)
above result is sharp for the function of the form
π(π§) = π§ β 2Ξ²(1βΞ΄)
π(πβ1)(πβ2+πΏ+π½)Ξ(c)(a)nβ1Ξ(b+k(nβ1)) Ξ(b)Ξ(c+k(nβ1)) (nβ1)!
π§π, π β₯ 2 (9)
Proof:- Suppose that the inequalities (8) holds true then we obtain
|π§(Β΅(a, b, c; k)f(z))β²β²β²β Ξ΄(Β΅(a, b, c; k)f(z))β²β²| β π½|(Β΅(a, b, c; k)f(z))β²β²+ 2(1 β Ξ΄)|
= |β β π(π β 1)(π β 2) Ξ(c)(a)nβ1Ξ(b + k(n β 1))
Ξ(b)Ξ(c + k(n β 1)) (n β 1)!πΌπznβ2
β
π=2
+ πΏ β π(π β 1) Ξ(c)(a)nβ1Ξ(b + k(n β 1))
Ξ(b)Ξ(c + k(n β 1)) (n β 1)!πΌπznβ2
β
π=2
|
βπ½ |2(1 β πΏ) β β π(π β 1) Ξ(c)(a)nβ1Ξ(b + k(n β 1))
Ξ(b)Ξ(c + k(n β 1)) (n β 1)!πΌπznβ2
β
π=2
|
β€ β π(π β 1)(π β 2 + πΏ + π½) Ξ(c)(a)nβ1Ξ(b + k(n β 1)) Ξ(b)Ξ(c + k(n β 1)) (n β 1)!πΌπ
β
π=2
β 2π½(1 β πΏ) β€ 0.
Hence by maximum modulus principle, π(π§) β π(a, b, c; Ξ², Ξ΄, k) Conversely:- Suppose π(π§) β π(a, b, c; Ξ², Ξ΄, k) then
|π§(Β΅(a,b,c;k)f(z))β²β²β²βΞ΄(Β΅(a,b,c;k)f(z))β²β²
(Β΅(a,b,c;k)f(z))β²β²+2(1βΞ΄) | < π½, π§ β π then
|π§(Β΅(a, b, c; k)f(z))β²β²β²β Ξ΄(Β΅(a, b, c; k)f(z))β²β²| < π½|(Β΅(a, b, c; k)f(z))β²β²+ 2(1 β Ξ΄)|
we get
|β β π(π β 1)(π β 2) Ξ(c)(a)nβ1Ξ(b + k(n β 1))
Ξ(b)Ξ(c + k(n β 1)) (n β 1)!πΌπznβ2
β
π=2
+ πΏ β π(π β 1) Ξ(c)(a)nβ1Ξ(b + k(n β 1))
Ξ(b)Ξ(c + k(n β 1)) (n β 1)!πΌπznβ2
β
π=2
|
< π½ |2(1 β πΏ) β β π(π β 1) Ξ(c)(a)nβ1Ξ(b + k(n β 1))
Ξ(b)Ξ(c + k(n β 1)) (n β 1)!πΌπznβ2
β
π=2
| thus
ββπ=2π(π β 1)(π β 2 + πΏ + π½)Ξ(c)(a)nβ1Ξ(b+k(nβ1))πΌπ
Ξ(b)Ξ(c+k(nβ1)) (nβ1)! β€ 2Ξ²(1 β Ξ΄) finally we can see sharpness follows for the function defined in (9).
3. Distortion Bounds
Theorem 2:- Let the function f (z) defined by (4) be in the class π(a, b, c; Ξ², Ξ΄, k) then we have
|π§| βΞ²(1βΞ΄)(πΏ+π½). Ξ(b)Ξ(c+k)
a Ξ(c)Ξ(b+k) |π§|2β€ |π(π§)| β€ |π§| + Ξ²(1βπΏ)
(πΏ+π½). Ξ(b)Ξ(c+k)
a Ξ(c)Ξ(b+k) |π§|2, (10)
Furthermore
301 1 β 2Ξ²(1βπΏ)
(πΏ+π½) . Ξ(b)Ξ(c+k)
a Ξ(c)Ξ(b+k) |π§| β€ |πβ²(π§)| β€ 1 + 2Ξ²(1βπΏ)
(πΏ+π½) . Ξ(b)Ξ(c+k)
a Ξ(c)Ξ(b+k) |π§|, (11)
the result is sharp for the function defined by
π(π§) = π§ βΞ²(1βπΏ)
(πΏ+π½). Ξ(b)Ξ(c+k)
a Ξ(c)Ξ(b+k) π§2 (12)
Proof :- It is easy to see from theorem1 that
2(πΏ + π½)a Ξ(c)Ξ(b + k) Ξ(b)Ξ(c + k) β πΌπ
β
π=2
β€ β π(π β 1)(π β 2 + πΏ + π½)
β
π=2
Ξ(c)(a)nβ1Ξ(b + k(n β 1))πΌπ Ξ(b)Ξ(c + k(n β 1)) (n β 1)!
β€ 2Ξ²(1 β πΏ) Then
ββπ=2πΌπβ€ Ξ²(1βπΏ)
(πΏ+π½). Ξ(b)Ξ(c+k)
a Ξ(c)Ξ(b+k) (13)
by using (13), we have
|π(π§)| β₯ |π§| β |π§|2ββπ=2πΌπ β₯ |π§| β Ξ²(1βπΏ)
(πΏ+π½). Ξ(b)Ξ(c+k)
a Ξ(c)Ξ(b+k) |π§|2, and
|π(π§)| β€ |π§| + |π§|2ββπ=2πΌπ β€ |π§| + Ξ²(1βπΏ)
(πΏ+π½). Ξ(b)Ξ(c+k)
a Ξ(c)Ξ(b+k) |π§|2, Which proves the assertion (10)
from (13) and theorem1, it follows also that
ββπ=2ππΌπβ€ 2Ξ²(1βπΏ)(πΏ+π½) . Ξ(b)Ξ(c+k)
a Ξ(c)Ξ(b+k)
consequently, we have
|πβ²(π§)| β₯ 1 β |π§| ββπ=2ππΌπ β₯ 1 β 2Ξ²(1βπΏ)
(πΏ+π½) . Ξ(b)Ξ(c+k)
a Ξ(c)Ξ(b+k) |π§|, and
|πβ²(π§)| β€ 1 + |π§| ββπ=2ππΌπ β€ 1 + 2Ξ²(1βπΏ)
(πΏ+π½) . Ξ(b)Ξ(c+k)
a Ξ(c)Ξ(b+k) |π§|,
This proves the assertion (11). Since each of equalities in (10) and (11) is satisfied by the function f(z) given by (12), which proves our theorem.
4. Extreme Points
Theorem 3:- Let π1(π§) = π§ πππ ππ(π§) = π§ β 2Ξ²(1βπΏ)
π(πβ1)(πβ2+πΏ+π½)Ξ(c)(a)nβ1Ξ(b+k(nβ1)) Ξ(b)Ξ(c+k(nβ1)) (nβ1)!
π§π, n=2,3,.. Then π(π§) β π(a, b, c; Ξ², πΏ, k) iff it can be expressed in the form π(π§) = ββπ=1ππππ(π§) Where bn β₯ 0 and ββπ=1ππ= 1.
Proof:- Firstly, let
π(π§) = β ππππ(π§)
β
π=1
= π1π§ + β ππ[π§ β 2Ξ²(1 β πΏ)
π(π β 1)(π β 2 + πΏ + π½)Ξ(c)(a)nβ1Ξ(b+k(nβ1)) Ξ(b)Ξ(c+k(nβ1)) (nβ1)!
π§π]
β
π=2
= π§ (π1+ β ππ
β
π=2
) β β 2Ξ²(1 β πΏ)
π(π β 1)(π β 2 + πΏ + π½)Ξ(c)(a)nβ1Ξ(b+k(nβ1)) Ξ(b)Ξ(c+k(nβ1)) (nβ1)!
π§π
β
π=2
= π§ β β 2Ξ²(1 β πΏ)
π(π β 1)(π β 2 + πΏ + π½)Ξ(c)(a)nβ1Ξ(b+k(nβ1)) Ξ(b)Ξ(c+k(nβ1)) (nβ1)!
π§π
β
π=2
302 Therefore, (π§) β π(a, b, c; Ξ², πΏ, k), since
β 2Ξ²(1 β πΏ)
π(π β 1)(π β 2 + πΏ + π½)Ξ(c)(a)nβ1Ξ(b+k(nβ1)) Ξ(b)Ξ(c+k(nβ1)) (nβ1)!
.
π(π β 1)(π β 2 + πΏ + π½)Ξ(c)(a)nβ1Ξ(b+k(nβ1)) Ξ(b)Ξ(c+k(nβ1)) (nβ1)!
2Ξ²(1 β πΏ)
β
π=2
= β ππ
β
π=2
= 1 β π1< 1
Conversely:- Assume that π(π§) β π(a, b, c; Ξ², πΏ, k), then by (8) we may set
ππ=
π(π β 1)(π β 2 + πΏ + π½)Ξ(c)(a)nβ1Ξ(b+k(nβ1)) Ξ(b)Ξ(c+k(nβ1)) (nβ1)!
2Ξ²(1 β πΏ) πΌπ, π β₯ 2 πππ 1 β β ππ
β
π=2
= π1
Thus
π(π§) = π§ β β πΌππ§π
β
π=2
= π§ β β 2Ξ²(1 β πΏ)bn
π(π β 1)(π β 2 + πΏ + π½)Ξ(c)(a)nβ1Ξ(b+k(nβ1)) Ξ(b)Ξ(c+k(nβ1)) (nβ1)!
β
π=2
π§π
= π§ β β ππ(π§ β ππ(π§)) = π§
β
π=2
(1 β β ππ
β
π=2
) + β ππππ(π§)
β
π=2
= π1π§ + β ππππ(π§)
β
π=2
= β ππππ(π§)
β
π=1
This proves the theorem.
5. Application to the Fractional Calculus
Many definitions of fractional calculus are given in the literature ([2, 3, 5]) i.e. fractional derivatives and fractional integrals. We here recall the following definition which is used by Owa [6] and by Srivastava and Owa [4].
Definition 4:- The fractional integral of order ΞΌ is defined for a function f (z), by π·π§βππ(π§) = 1
Ξ(π)β«0π§(π§βπ‘)π(π‘)1βπ ππ‘ (π > 0),
Where f(z) is an analytic function in a simply-connected region of the complex z-plane containing the origin and the multiplicity of (z-t)ΞΌ-1 is removed by requiring log(z-t) to the real when z-t > 0.
Definition 5:- The fractional derivative of order ΞΌ is defined, for a function f(z), by π·π§ππ(π§) = 1
Ξ(1βπ) π
ππ§β«0π§(π§βπ‘)π(π‘)π ππ‘ (0 β€ π < 1),
Where f(z) is an analytic function in a simply-connected region of the complex z-plane containing the origin and the multiplicity of (z-t)-ΞΌ is removed by requiring log(z-t) to the real when z-t > 0.
Definition6:- under the hypotheses of definition5, the fractional derivative of order n+ΞΌ is defined by π·π§π+ππ(π§) = ππ
ππ§ππ·π§ππ(π§) (0 β€ π < 1; π β β0) Now, we state the definition of fractional integral operator given by [7].
Definition7:- for real number Ξ± > 0, Ξ· and Ξ΄, the fractional operator, Ξ0,π§πΌ,π,πΏ is defined by Ξ0,π§πΌ,π,πΏπ(π§) =π§βπΌβπ
Ξ(πΌ) β« (π§ β π‘)πΌβ1πΉ (πΌ + π, βπΏ; πΌ; 1 βπ‘
π§) π(π‘)ππ‘,
π§
0 (13)
Where f(z) is analytic function ina simply connected region containing the origin with order π(π§) = Ξ(|π§|π), π§ β 0, π€βπππ π > max(0, π β πΏ) β 1,
303 πΉ(π, π, π; π§) = β (π)π(π)π
(π)π(1)π
βπ=0 π§π
and (a)n is the Pochhammer symbol defined by (π)π=Ξ(π+π)
Ξ(π) = { 1 π = 0
π(π + 1) β¦ β¦ (π + π β 1) π β π
and the multiplicity of (z-t)Ξ±-1 is removed by requiring log(z-t) to the real when z-t > 0. To prove our result we need lemma given by Srivastava [7].
Lemma1:- Let Ξ± > 0 and n > Ξ· β Ξ΄ -1. Then
Ξ0,π§πΌ,π,πΏπ(π§) = Ξ(π+1)Ξ(πβπ+πΏ+1) Ξ(πβπ+1)Ξ(π+πΌ+πΏ+1)π§πβπ making use of lemma1. We prove the following theorem.
Theorem4:- let Ξ· < 2, Ξ± >0, Ξ·(Ξ± + Ξ») β€ 3 Ξ± and Ξ± + Ξ» > -2. If f(z) be defined by the function (4) is in the class π(a, b, c; Ξ², πΏ, k) then
|Ξ0,π§πΌ,π,ππ(π§)| β₯ Ξ(2βπ+π)
Ξ(2βπ)Ξ(2+πΌ+π)(1 β2π½(2βπ+π)(1βπΏ)Ξ(π)Ξ(π+π)
π(2βπ)(2+πΌ+π)Ξ(π)Ξ(π+π)|π§|) (14)
And
|Ξ0,π§πΌ,π,ππ(π§)| β€ Ξ(2βπ+π)
Ξ(2βπ)Ξ(2+πΌ+π)(1 +2π½(2βπ+π)(1βπΏ)Ξ(π)Ξ(π+π)
π(2βπ)(2+πΌ+π)Ξ(π)Ξ(π+π)|π§|) (15)
for π§ β π0 where
π0= { π π β€ 1 π β {0} π > 1 The result is sharp for the function given by
π(π§) = π§ βΞ²(1βΞ΄)
(πΏ+π½). Ξ(b)Ξ(c+k)
a Ξ(c)Ξ(b+k)π§2 Proof:- By using above lemma, we have
Ξ0,π§πΌ,π,ππ(π§) = Ξ(2βπ+π)
Ξ(2βπ)Ξ(2+πΌ+π)π§1βπβ β Ξ(π+1)Ξ(πβπ+π+1)
Ξ(πβπ+1)Ξ(π+πΌ+π+1)πΌππ§πβπ
βπ=2 (16)
taking
π»(π§) =Ξ(2βπ)Ξ(2+πΌ+π)
Ξ(2βπ+π) π§πΞ0,π§πΌ,π,ππ(π§) = π§ β ββπ=2β(π)πΌππ§π where
β(π) = (2βπ+π)πβ1(1)π
(2βπ)πβ1(2+πΌ+π)πβ1, ( π β₯ 2) (17)
it can be easily seen that h(n) is non-increasing for n β₯ 2 and thus we have 0 < β(π) β€ β(2) = 2(2βπ+π)
(2βπ)(2+πΌ+π) (18)
now by using theorem1 and (18), we have
|π»(π§)| β₯ |π§| β β(2)|π§|2β πΌπ
β
π=2
β₯ |π§| β2π½(2 β π + π)(1 β πΏ)Ξ(π)Ξ(π + π) π(2 β π)(2 + πΌ + π)Ξ(π)Ξ(π + π) |π§|2,
304 and
|π»(π§)| β€ |π§| + β(2)|π§|2β πΌπ
β
π=2
β€ |π§| +2π½(2 β π + π)(1 β πΏ)Ξ(π)Ξ(π + π) π(2 β π)(2 + πΌ + π)Ξ(π)Ξ(π + π) |π§|2, This proves (14) and (15).
6. References
1. Virchenko N, Kalla SL, Al-Zamel A. Some results on generalized hypergeometric function, Integral Transforms and Special Funcion. 2001; 12(1):89-100.
2. Aouf MK. On fractional derivatives and fractional integrals of certain subclasses of starlike and convex functionsβ Math. Japon.
1990; 35(5):831-837.
3. Srivastava HM, Owa S. An application of the fractional derivative, Math. Japon. 1984; 29:383-389.
4. Srivastava HM, Owa S. Univalent functions, Fractional calculus and their applicationsβ Halsted press, John Wiley and Sons, New York, Chichester, Brisbane and Toronto, 1989.
5. Srivastava HM, Aouf MK. A Certain fractional derivative operator and its applications to a new class of analytic and multivalent functions with negative coefficient I and II J. Math. Anal. Appl. 1992; 171:973-986.
6. Owa S. On the Distortion Theorems, I, Kyungpook Math J. 1978; 18:53-59.
7. Srivastava HM, Siago M, Owa S. A class of distortion theorem of fractional calculus J Math Anal. Appl. 1988; 131:412-420.