Hindawi Publishing Corporation Journal of Applied Mathematics Volume 2013, Article ID 312387, 8 pages http://dx.doi.org/10.1155/2013/312387 Research Article On Certain Subclass of Analytic Functions with Fixed Point T. Al-Hawary,1 B. A. Frasin,2 and M. Darus1 1 School of Mathematical Sciences, Faculty of Science and Technology, Universiti Kebangsaan Malaysia, 43600 Bangi, Selangor, Malaysia 2 Department of Mathematics, Faculty of Science, Al al-Bayt University, Mafraq 130095, Jordan Correspondence should be addressed to M. Darus; maslina@ukm.my Received 14 October 2012; Revised 27 December 2012; Accepted 27 December 2012 Academic Editor: Yongkun Li Copyright © 2013 T. Al-Hawary et al. 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. π ∗ π(π§) and a subclass ππ,π€ (πΌ, π½, πΎ, πΏ, π) are introduced for functions of the form π(π§) = A new certain differential operator ππΌ,π½,πΏ,π ∞ π (π§ − π€) − ∑π=2 ππ (π§ − π€) which are univalent in the unit disc π = {π§ ∈ C : |π§| < 1}. In this paper, we obtain coefficient inequalities, ∗ (πΌ, π½, πΎ, πΏ, π). distortion theorem, closure theorems, and class preserving integral operators of functions belonging to the class ππ,π€ 1. Introduction Let π»(π) be the set of functions which are regular in the unit disc π = {π§ ∈ C : |π§| < 1}, π΄ = {π ∈ π»(π) : π(0) = πσΈ (0) − 1 = 0} and π = {π ∈ π΄ : π is univalent in π}. We recall here the definitions of the well-known classes of starlike and convex functions: π∗ = {π ∈ π΄ : Re ( π§πσΈ (π§) ) > 0, π§ ∈ π} , π (π§) π§πσΈ σΈ (π§) ) > 0, π§ ∈ π} . π = {π ∈ π΄ : Re (1 + σΈ π (π§) (1) π Let π€ be a fixed point in π and π΄(π€) = {π ∈ π»(π) : π(π€) = πσΈ (π€) − 1 = 0}. In [1], Kanas and Rønning introduced the following classes: ππ€ = {π ∈ π΄ (π€) : π is univalent in π} , ∗ = {π ∈ ππ€ : Re ( πππ€ = ππ€ (π§ − π€) πσΈ (π§) ) > 0, π§ ∈ π} , π (π§) π πππ€ = ππ€ = {π ∈ ππ€ : 1+Re ( (π§−π€) πσΈ σΈ (π§) ) > 0, π§ ∈ π} . πσΈ (π§) (2) These classes are extensively studied by Acu and Owa [2]. ∗ is defined by geometric property that the The class ππ€ image of any circular arc centered at π€ is starlike with respect π is defined by the to π(π€) and the corresponding class ππ€ property that the image of any circular arc centered at π€ is convex. We observe that the definitions are somewhat similar to the ones for uniformly starlike and convex functions introduced by Goodman in [3, 4], except that in this case the point π€ is fixed. In fact, several subclasses of π have been introduced by a fixed geometric property of the image domain. It is interesting to note that these subclasses play an important role in other branches of mathematics. For example, starlike functions and convex functions play an important role in the solution of certain differential equations (see Robertson [5], Saitoh [6], Owa et al. [7], Reade and Silverman [8], and SokoΜΕ and WisΜniowska-Wajnryb [9]). One of the important problems in geometric function theory are the extremal problems, which pose an effective method for establishing the existence of analytic functions with certain natural properties. Extremal problems (supremum Re{π}) play an important role in geometric function theory, for finding sharp estimates, coefficient bounds, and an extremal function. The results we obtained here may have potential application in other branches of mathematics, both pure and applied. For example the extremal problems are closely connected to Hele-Shaw flow of fluid mechanics [10], exterior inverse problems in potential theory, and many others. 2 Journal of Applied Mathematics Now let us begin with our definitions as follows. The function π(π§) in ππ€ is said to be starlike functions of order πΎ if and only if Re { (π§ − π€) πσΈ (π§) }>πΎ π (π§) (π§ ∈ π) (3) for some πΎ (0 ≤ πΎ < 1). We denote by πππ€ (πΎ) the class of all starlike functions of order πΎ. Similarly, a function π(π§) in ππ€ is said to be convex of order πΎ if and only if Re {1 + (π§ − π€) πσΈ σΈ (π§) }>πΎ πσΈ (π§) (π§ ∈ π) (4) for some πΎ (0 ≤ πΎ < 1). We denote by πππ€ (πΎ) the class of all convex functions of order πΎ. It is easy to see that ππ€ denoting the subclass of π΄(π€) has the series of expansion: Remark 1. (i) When π€ = πΏ = 0, we have the operator introduced and studied by Darus and Ibrahim (see [11]). (ii) When π€ = πΌ = πΏ = 0 and π½ = 1, we have the operator introduced and studied by Al-Oboudi (see [12]). (iii) When πΌ = πΏ = 0 and π = π½ = 1, we have the operator introduced and studied by Acu and Owa (see [2]). (iv) And when πΌ = πΏ = π€ = 0 and π = π½ = 1, we have the Μ operator introduced and studied by SalΜ agean (see [13]). π , we With the help of the differential operator ππΌ,π½,πΏ,π define the class ππ,π€ (πΌ, π½, πΎ, πΏ, π) as follows. Definition 2. A function π(π§) ∈ ππ€ is said to be a member of the class ππ,π€ (πΌ, π½, πΎ, πΏ, π) if it satisfies σ΅¨σ΅¨ σ΅¨σ΅¨ σΈ π σ΅¨σ΅¨ (π§ − π€) (ππΌ,π½,πΏ,π σ΅¨σ΅¨ π (π§)) σ΅¨σ΅¨ σ΅¨ − 1σ΅¨σ΅¨σ΅¨ σ΅¨σ΅¨ π σ΅¨σ΅¨ σ΅¨σ΅¨ π π (π§) πΌ,π½,πΏ,π σ΅¨σ΅¨ σ΅¨σ΅¨ σ΅¨σ΅¨ σ΅¨σ΅¨ σΈ π σ΅¨σ΅¨ (π§ − π€) (ππΌ,π½,πΏ,π σ΅¨σ΅¨ π (π§)) σ΅¨σ΅¨ σ΅¨ < σ΅¨σ΅¨ + 1 − 2πΎσ΅¨σ΅¨σ΅¨ π σ΅¨σ΅¨ σ΅¨σ΅¨ π π (π§) πΌ,π½,πΏ,π σ΅¨σ΅¨ σ΅¨σ΅¨ ∞ π (π§) = (π§ − π€) + ∑ ππ (π§ − π€)π . (5) π=2 For the function π(π§) in the class ππ€ , we define the following new differential operator: 0 π π (π§) = π (π§) , 1 ππΌ,π½,πΏ,π π (π§) = (1 − π½ (π − πΌ)) π (π§) + π½ (π − πΌ) (π§ − π€) πσΈ (π§) + πΏ(π§ − π€)2 πσΈ σΈ (π§) , 2 1 π (π§) = (1 − π½ (π − πΌ)) (ππΌ,π½,πΏ,π π (π§)) ππΌ,π½,πΏ,π for some 0 ≤ πΎ < 1, πΌ ≥ 0, π½ ≥ 0, πΏ ≥ 0, π ≥ 0, and π ∈ N0 and for all π§ ∈ π. It is easy to check that π0,0 (0, 1, πΎ, 0, 1) is the class of starlike functions of order πΎ and π0,0 (0, 1, 0, 0, 1) gives the all class of starlike functions. Let ππ€ denote the subclass of π΄(π€) consisting of functions of the following form: ∞ π (π§) = (π§ − π€) − ∑ ππ (π§ − π€)π , σΈ 1 π (π§)) + π½ (π − πΌ) (π§ − π€) (ππΌ,π½,πΏ,π ππ ≥ 0. π=2 σΈ σΈ 1 + πΏ(π§ − π€)2 (ππΌ,π½,πΏ,π π (π§)) , (9) (10) ∗ Further, we define the class ππ,π€ (πΌ, π½, πΎ, πΏ, π) by (6) and for π = 1, 2, 3, . . .. (11) In this paper, coefficient inequalities, distortion theorem, and closure theorems of functions belonging to the class ∗ ππ,π€ (πΌ, π½, πΎ, πΏ, π) are obtained. Finally, the class preserving integral operators of the form π π−1 ππΌ,π½,πΏ,π π (π§) = (1 − π½ (π − πΌ)) (ππΌ,π½,πΏ,π π (π§)) σΈ π−1 π (π§)) + π½ (π − πΌ) (π§ − π€) (ππΌ,π½,πΏ,π σΈ σΈ π−1 + πΏ(π§ − π€)2 (ππΌ,π½,πΏ,π π (π§)) ∞ ∗ ππ,π€ (πΌ, π½, πΎ, πΏ, π) = ππ,π€ (πΌ, π½, πΎ, πΏ, π) ∩ ππ€ . πΉ (π§) = = (π§ − π€) + ∑ [1 + (π − 1) (π½ (π − πΌ) + ππΏ)] π π§ π+1 π−1 π (π‘) ππ‘ π ∫ (π‘ − π€) (π§ − π€) π€ (π > −1) (12) ∗ (πΌ, π½, πΎ, πΏ, π) is considered. for the class ππ,π€ π=2 2. Coefficient Inequalities × ππ (π§ − π€)π , (7) for πΌ ≥ 0, π½ ≥ 0, πΏ ≥ 0, π ≥ 0, and π ∈ N0 = N ∪ {0}. It easily verified from (7) that π½ (π − πΌ) (π§ − Theorem 3. A function π(π§) being defined by (10) is in ∗ (πΌ, π½, πΎ, πΏ, π) if and only if ππ,π€ σΈ π π (π§)) π€) (ππΌ,π½,πΏ,π π+1 π = ππΌ,π½,πΏ,π π (π§) − (1 − π½ (π − πΌ)) ππΌ,π½,πΏ,π π (π§) 2 − πΏ(π§ − π€) σΈ σΈ π (ππΌ,π½,πΏ,π π (π§)) . Our first result provides a sufficient condition for a function, ∗ (πΌ, π½, πΎ, πΏ, π). regular in π, to be in ππ,π€ ∞ (8) π ∑ (π − πΎ) [1 + (π − 1) π½ ((π − πΌ) + ππΏ)] ππ ≤ 1 − πΎ π=2 (π ∈ N0 ) , (13) Journal of Applied Mathematics 3 where 0 ≤ πΎ < 1. The result (13) is sharp for functions of the following form: ππ (π§) = (π§ − π€) − 1−πΎ π (14) π (π§−π€) (π−πΎ) [1+(π−1) π½ ((π−πΌ)+ππΏ)] (π ≥ 2; π ∈ N0 ) . Proof. Suppose that (13) holds true for 0 ≤ πΎ < 1. consider the expression σΈ π (π, π ) σ΅¨σ΅¨ σ΅¨σ΅¨ σΈ π π π (π§)) − (ππΌ,π½,πΏ,π π (π§))σ΅¨σ΅¨σ΅¨ = σ΅¨σ΅¨σ΅¨(π§ − π€) (ππΌ,π½,πΏ,π σ΅¨ σ΅¨ σ΅¨σ΅¨ σ΅¨σ΅¨ σΈ π π − σ΅¨σ΅¨σ΅¨(π§ − π€) (ππΌ,π½,πΏ,π π (π§)) + (1 − 2πΎ) (ππΌ,π½,πΏ,π π (π§))σ΅¨σ΅¨σ΅¨ . σ΅¨ σ΅¨ (15) For the converse, assume that σ΅¨σ΅¨ σ΅¨σ΅¨ σΈ π σ΅¨σ΅¨ σ΅¨σ΅¨ (π§ − π€) (ππΌ,π½,πΏ,π π (π§)) σ΅¨ σ΅¨σ΅¨ − 1σ΅¨σ΅¨σ΅¨ σ΅¨σ΅¨ π σ΅¨σ΅¨ σ΅¨σ΅¨ π π (π§) πΌ,π½,πΏ,π σ΅¨σ΅¨ σ΅¨σ΅¨ σ΅¨σ΅¨ σ΅¨σ΅¨ σΈ π σ΅¨σ΅¨ (π§ − π€) (ππΌ,π½,πΏ,π σ΅¨σ΅¨ π (π§)) σ΅¨σ΅¨ σ΅¨σ΅¨ / σ΅¨σ΅¨ + 1 − 2πΎ σ΅¨σ΅¨ π σ΅¨σ΅¨ σ΅¨σ΅¨ π π (π§) πΌ,π½,πΏ,π σ΅¨σ΅¨ σ΅¨σ΅¨ σ΅¨σ΅¨ ∞ σ΅¨σ΅¨ π = σ΅¨σ΅¨σ΅¨ (− ∑ (π − 1) [1 + (π − 1) π½ ((π − πΌ) + ππΏ)] σ΅¨σ΅¨ π=2 σ΅¨ × ππ (π§ − π€)π ) (17) × (2 (1 − πΎ) (π§ − π€) Then for |π§ − π€| = π < 1, we have ∞ − ∑ (π−2πΎ+1) [1+(π−1) π½ ((π−πΌ)+ππΏ)] σΈ π (π, π ) π=2 σ΅¨σ΅¨ ∞ σ΅¨σ΅¨ π = σ΅¨σ΅¨σ΅¨ ∑ (π − 1) [1 + (π − 1) π½ ((π − πΌ) + ππΏ)] σ΅¨σ΅¨π=2 σ΅¨ σ΅¨σ΅¨ σ΅¨σ΅¨ × ππ (π§ − π€)π σ΅¨σ΅¨σ΅¨ σ΅¨σ΅¨ σ΅¨ σ΅¨σ΅¨ σ΅¨σ΅¨ − σ΅¨σ΅¨σ΅¨ 2 (1 − πΎ) (π§ − π€) σ΅¨σ΅¨ σ΅¨ ∞ − ∑ (π−2πΎ+1) [1+(π−1) π½ ((π−πΌ)+ππΏ)] −1 σ΅¨σ΅¨ σ΅¨σ΅¨ × ππ (π§ − π€) ) σ΅¨σ΅¨σ΅¨ σ΅¨σ΅¨ σ΅¨ π < 1. Since Re(π§ − π€) ≤ |π§ − π€| for all (π§ − π€), it follows from (17) that π π=2 π (π, πσΈ ) π ∞ σ΅¨σ΅¨ σ΅¨σ΅¨ × ππ (π§ − π€)π σ΅¨σ΅¨σ΅¨ , σ΅¨σ΅¨ σ΅¨ Re { ( ∑ (π − 1) [1 + (π − 1) π½ ((π − πΌ) + ππΏ)] π π=2 × ππ (π§ − π€)π ) ∞ ≤ ∑ (π − 1) × (2 (1 − πΎ) (π§ − π€) π=2 π × [1 + (π − 1) π½ ((π − πΌ) + ππΏ)] ππ ππ ∞ − ∑ (π − 2πΎ + 1) [1+(π−1) π½ ((π−πΌ)+ππΏ)] ∞ − 2 (1 − πΎ) + ∑ (π + 2πΎ − 1) π=2 π=2 π π ≤ ∑ 2 (π − πΎ) [1 + (π − 1) π½ ((π − πΌ) + ππΏ)] −1 × ππ (π§ − π€) ) } π × [1 + π (π + π − 2)] ππ π ∞ π π < 1. (18) π=2 × ππ − 2 (1 − πΎ) ≤ 0. (16) ∗ (πΌ, π½, πΎ, πΏ, π). So that π(π§) ∈ ππ,π€ Choose values of (π§ − π€) on the real axis so that π π (π§ − π€)(ππΌ,π½,πΏ,π π(π§))σΈ /ππΌ,π½,πΏ,π π(π§) is real. Upon clearing the 4 Journal of Applied Mathematics denominator in (18) and letting π → 1− through real values, we obtain ∞ Thus, for |π§ − π€| = π < 1, and making use of (22), we have ∞ σ΅¨ σ΅¨σ΅¨ π σ΅¨σ΅¨π (π§)σ΅¨σ΅¨σ΅¨ ≤ |π§ − π€| + ∑ ππ |π§ − π€| π=2 π ∑ (π − 1) [1 + (π − 1) π½ ((π − πΌ) + ππΏ)] ππ ∞ π=2 ≤ π + π2 ∑ ππ < 2 (1 − πΎ) π=2 ∞ ≤π+ π − ∑ (π − 2πΎ + 1) [1 + (π − 1) π½ ((π − πΌ) + ππΏ)] ππ . π=2 (19) 1−πΎ 2 ππ , (2 − πΎ) [1 + π½ ((π − πΌ) + 2πΏ)] ∞ (23) σ΅¨ σ΅¨σ΅¨ π σ΅¨σ΅¨π (π§)σ΅¨σ΅¨σ΅¨ ≥ |π§ − π€| − ∑ ππ |π§ − π€| π=2 This gives the required condition. Hence the theorem follows. ∞ ≥ π − π2 ∑ ππ π=2 Corollary 4. Let the function π(π§) be defined by (10) and ∗ (πΌ, π½, πΎ, πΏ, π), then π(π§) ∈ ππ€ . If π ∈ ππ,π€ ππ ≤ 1−πΎ π, (π − πΎ) [1 + (π − 1)π½((π − πΌ) + ππΏ)] ≥π− 1−πΎ 2 ππ . (2 − πΎ) [1 + π½ ((π − πΌ) + 2πΏ)] Also from Theorem 3, it follows that π ≥ 2. (20) π (2 − πΎ) [1 + π½ ((π − πΌ) + 2πΏ)] ∞ ∑ πππ 2 π=2 ∞ The result (20) is sharp for functions ππ (π§) given by (14). π ≤ ∑ (π − πΎ) [1 + (π − 1) π½ ((π − πΌ) + ππΏ)] ππ (24) π=2 ≤ 1 − πΎ. 3. Distortion Theorem A distortion property for functions in the class π ∗ (πΌ, π½, πΎ, πΏ, π) is contained in ππ,π€ ∈ Theorem 5. Let the function π(π§) one has defined by (10) be ∗ (πΌ, π½, πΎ, πΏ, π). Then for |π§ − π€| = π < 1, we in the class π ∈ ππ,π€ have Hence σ΅¨σ΅¨ σΈ σ΅¨σ΅¨ σ΅¨σ΅¨π (π§)σ΅¨σ΅¨ σ΅¨ σ΅¨ ∞ ≤ 1 + ∑ πππ |π§ − π€|π−1 π=2 ∞ ≤ 1 + π ∑ πππ 1−πΎ 2 π− ππ (2 − πΎ) [1 + π½ ((π − πΌ) + 2πΏ)] σ΅¨ σ΅¨ ≤ σ΅¨σ΅¨σ΅¨π (π§)σ΅¨σ΅¨σ΅¨ ≤π+ 1− π=2 ≤1+ 1−πΎ 2 ππ , (2 − πΎ) [1 + π½ ((π − πΌ) + 2πΏ)] 2 (1 − πΎ) (21) ππ (25) ∞ ≥ 1 − ∑ πππ |π§ − π€|π−1 π=2 ∞ ≥ 1 − π ∑ πππ π=2 2 (1 − πΎ) π π. (2 − πΎ) [1 + π½ ((π − πΌ) + 2πΏ)] ≥1− ∗ Proof. Since π ∈ ππ,π€ (πΌ, π½, πΎ, πΏ, π), Theorem 3 readily yields the inequality 2 (1 − πΎ) (2 − πΎ) [1 + π½ ((π − πΌ) + 2πΏ)] π π. This completes the proof of Theorem 5. 4. Radii of Starlikeness and Convexity ∞ 1−πΎ ∑ ππ ≤ π. (2 − πΎ) [1 + π½((π − πΌ) + 2πΏ)] π=2 π π, σ΅¨σ΅¨ σΈ σ΅¨σ΅¨ σ΅¨σ΅¨π (π§)σ΅¨σ΅¨ σ΅¨ σ΅¨ (2 − πΎ) [1 + π½ ((π − πΌ) + 2πΏ)] σ΅¨ σ΅¨ ≤ σ΅¨σ΅¨σ΅¨σ΅¨πσΈ (π§)σ΅¨σ΅¨σ΅¨σ΅¨ ≤1+ 2 (1 − πΎ) (2 − πΎ) [1 + π½ ((π − πΌ) + 2πΏ)] (22) The radii of starlikeness and convexity for the class ∗ (πΌ, π½, πΎ, πΏ, π) is given by the following theorems. ππ,π€ Journal of Applied Mathematics 5 Theorem 6. If the function π(π§) defined by (10) is in the class ∗ (πΌ, π½, πΎ, πΏ, π), then π(π§) is of order π(0 ≤ π < 1) in |π§ − ππ,π€ π€| < π1 , where Theorem 7. If the function π(π§) defined by (10) is in the class ∗ (πΌ, π½, πΎ, πΏ, π), then π(π§) is convex of order π (0 ≤ π < 1) ππ,π€ in |π§ − π€| < π2 , where 1/π π (1 − π) (π − πΎ) [1 + (π − 1) π½ ((π − πΌ) + ππΏ)] π1 = inf { } . π≥2 (π − π) (1 − πΎ) (26) π (1−π)(π−πΎ)[1+(π−1)π½((π−πΌ)+ππΏ)] π2 = inf { } π≥2 π(π+π−2)(1−πΎ) 1/(π−1) (π ≥ 2) . (33) The result is sharp for the functions ππ (π§) given by (14). Proof. It suffices to prove that The result is sharp for the functions ππ (π§) given by (14). σ΅¨σ΅¨ σ΅¨σ΅¨ σ΅¨σ΅¨ σ΅¨σ΅¨ (π§ − π€) πσΈ (π§) σ΅¨σ΅¨ ≤ 1 − π, σ΅¨σ΅¨ − 1 σ΅¨σ΅¨ σ΅¨σ΅¨ π (π§) σ΅¨ σ΅¨ (27) for |π§ − π€| < π1 . We have σ΅¨ σ΅¨σ΅¨ σ΅¨σ΅¨ (π§ − π€) πσΈ σΈ (π§) σ΅¨σ΅¨σ΅¨ σ΅¨σ΅¨ ≤ 1 − π, σ΅¨σ΅¨ σ΅¨σ΅¨ πσΈ (π§) σ΅¨σ΅¨σ΅¨ σ΅¨ σ΅¨σ΅¨ σ΅¨σ΅¨ σ΅¨σ΅¨ σ΅¨σ΅¨ (π§ − π€) πσΈ (π§) σ΅¨σ΅¨ σ΅¨σ΅¨ − 1 σ΅¨σ΅¨ σ΅¨σ΅¨ π (π§) σ΅¨ σ΅¨ σ΅¨σ΅¨ − ∑∞ (π − 1) π (π§ − π€)π σ΅¨σ΅¨ σ΅¨ σ΅¨σ΅¨ π π=2 σ΅¨ = σ΅¨σ΅¨σ΅¨σ΅¨ ∞ π σ΅¨σ΅¨ σ΅¨σ΅¨ (π§ − π€) − ∑π=2 ππ (π§ − π€) σ΅¨σ΅¨ ≤ Proof. By using the technique employed in the proof of Theorem 6, we can show that (28) π ∑∞ π=2 (π − 1) ππ |π§ − π€| ∞ π . 1 − ∑π=2 ππ |π§ − π€| (34) for |π§ − π€| < π2 , with the aid of Theorem 3. Thus we have the assertion of Theorem 7. 5. Closure Theorems Let the functions ππ (π§), π = 1, 2, . . . , π, be defined by Hence (28) holds true if ∞ ∑ (π − 1) ππ |π§ − π€|π ∞ π=2 (29) ∞ ≤ (1 − π) (1 − ∑ ππ |π§ − π€|π ) π=2 ππ (π§) = (π§ − π€) − ∑ ππ,π (π§ − π€)π , π=2 (ππ,π ≥ 0) (35) for π§ ∈ π. or ∞ π−π ππ |π§ − π€|π ≤ 1 ∑ 1 − π π=2 (30) Theorem 8. Let the functions ππ (π§) be defined by (35) in ∗ the class ππ,π€ (πΌ, π½, πΎ, πΏ, π) for every π = 1, 2, . . . , π. Then the function πΊ(π§) defined by with the aid of (13), (30) is true if ∞ πΊ (π§) = (π§ − π€) − ∑ ππ (π§ − π€)π , π−π |π§ − π€|π 1−π π=2 (31) π (π − πΎ) [1 + (π − 1) π½ ((π − πΌ) + ππΏ)] ≤ . 1−πΎ ππ = |π§ − π€| π 1/π (π ≥ 2) . Proof. Since ππ (π§) Theorem 3 that ∞ (32) (36) ∗ (πΌ, π½, πΎ, πΏ, π), where is a member of the class ππ,π€ Solving (31) for |π§ − π€|, we obtain (1 −π) (π −πΎ) [1 + (π −1) π½ ((π−πΌ)+ππΏ)] } ≤{ (π−π) (1−πΎ) (ππ ≥ 0) ∈ 1 π ∑π π π=1 π,π (π ≥ 2) . (37) ∗ ππ,π€ (πΌ, π½, πΎ, πΏ, π), it follows from π ∑ (π − πΎ) [1 + (π − 1) π½ ((π − πΌ) + ππΏ)] ππ,π ≤ 1 − πΎ π=2 This completes the proof of Theorem 6. (38) 6 Journal of Applied Mathematics for every π = 1, 2, . . . , π. Hence, Theorem 10. Let ∞ π0 (π§) = π§ − π€, π ∑ (π − πΎ) [1 + (π − 1) π½ ((π − πΌ) + ππΏ)] ππ ππ (π§) = (π§ − π€) π=2 ∞ = ∑ (π − πΎ) [1 + (π − 1) π½ ((π − πΌ) + ππΏ)] π π=2 (π ≥ 2; π ∈ N0 ) . (43) } {1 π × { ∑ ππ,π } π } { π=1 = π ∗ Then π(π§) ∈ ππ,π€ (πΌ, π½, πΎ, πΏ, π) if and only if it can be expressed in the form ∞ 1 ∑ ( ∑ (π − πΎ) π π=1 π=2 ∞ π (π§) = ∑ π π ππ (π§) , π where π π ≥ 0 and ∑∞ π=1 π π = 1. Proof. Suppose that 1 π ∑ (1 − πΎ) = 1 − πΎ π π=1 ∞ π (π§) = ∑ π π ππ (π§) , (39) which (in view of Theorem 5) implies that πΊ(π§) ∗ ππ,π€ (πΌ, π½, πΎ, πΏ, π). ∈ where π π ≥ 0 (π ≥ 1) and ∑∞ π=1 π π = 1. Then π (π§) = ∑ π π ππ (π§) π=1 ∞ Proof. Suppose that the functions ππ (π§) (π = 1, 2) defined by ∗ (35) be in the class ππ,π€ (πΌ, π½, πΎ, πΏ, π), it is sufficient to prove that the function π» (π§) = ππ1 (π§) + (1 − π) π2 (π§) is also in the class (0 ≤ π ≤ 1) = π 1 π1 (π§) + ∑ π π ππ (π§) π=2 (40) ∞ 1−πΎ π π=2 (π − πΎ) [1 + (π − 1) π½ ((π − πΌ) + ππΏ)] −∑ Since, for 0 ≤ π ≤ 1, ∞ π=2 (46) = (π§ − π€) × π π (π§ − π€)π . π» (π§) = (π§ − π€) − ∑ {πππ,1 + (1 − π) ππ,2 } (π§ − π€)π , (41) Since we observe that ∞ ∞ ∑ (π − πΎ) [1 + (π − 1) π½ ((π − πΌ) + ππΏ)] (45) π=1 ∞ ∗ Theorem 9. The class ππ,π€ (πΌ, π½, πΎ, πΏ, π) is closed under convex linear combination. ∗ (πΌ, π½, πΎ, πΏ, π). ππ,π€ (44) π=1 × [1 + (π − 1) π½ ((π − πΌ) + ππΏ)] ππ,π ) ≤ 1−πΎ π π (π§ − π€) (π − πΎ) [1 + (π − 1) π½ ((π − πΌ) + ππΏ)] − ∑ (π − πΎ) [1 + (π − 1) π½ ((π − πΌ) + ππΏ)] π π=2 π=2 ⋅ × {πππ,1 + (1 − π) ππ,2 } ∞ π 1−πΎ π ππ (π − πΎ) [1 + (π − 1) π½ ((π − πΌ) + ππΏ)] (47) ∞ π = (1 − πΎ) ∑ π π = π ∑ (π − πΎ) [1 + (π − 1) π½ ((π − πΌ) + ππΏ)] ππ,1 π=2 π=2 ∞ = (1 − πΎ) (1 − π 0 ) ≤ 1 − πΎ, + (1 − π) ∑ (π − πΎ) π=2 π × [1 + (π − 1) π½ ((π − πΌ) + ππΏ)] ππ,2 ≤ π (1 − πΎ) + (1 − π) (1 − πΎ) = (1 − πΎ) . (42) ∗ Hence π»(π§) ∈ ππ,π€ (πΌ, π½, πΎ, πΏ, π). This completes the proof of Theorem 9. it follows from Theorem 3 that the function π(π§) ∈ ∗ (πΌ, π½, πΎ, πΏ, π). Conversely, let us suppose that π(π§) ∈ ππ,π€ ∗ (πΌ, π½, πΎ, πΏ, π). Since ππ,π€ ππ ≤ 1−πΎ π (π − πΎ) [1 + (π − 1) π½ ((π − πΌ) + ππΏ)] (π ≥ 2; π ∈ N0 ) . (48) Journal of Applied Mathematics 7 Setting Since ∞ ∑ (π − πΎ) [1 + (π − 1) π½ ((π − πΌ) + ππΏ)] π (π − πΎ) [1 + (π − 1) π½ ((π − πΌ) + ππΏ)] ππ = ππ , 1−πΎ (π ≥ 2; π ∈ N0 ) , π=2 1−πΎ π ππ (π − πΎ) [1 + (π − 1) π½ ((π − πΌ) + ππΏ)] ⋅ (49) ∞ (54) ∞ π1 = 1 − ∑ ππ, = (1 − πΎ) ∑ π π π=2 π=2 ∗ it follows that π(π§) = ππ,π€ (πΌ, π½, πΎ, πΏ, π). This completes the proof of the theorem. 6. Extreme Points = (1 − πΎ) (1 − π 0 ) ≤ 1 − πΎ, it follows from Theorem 3 that the function π(π§) ∈ ∗ (πΌ, π½, πΎ, πΏ, π). Conversely, let us suppose that π(π§) ∈ ππ,π€ ∗ (πΌ, π½, πΎ, πΏ, π). Since ππ,π€ ππ ≤ Theorem 11. Let 1−πΎ π (π − πΎ) [1 + (π − 1) π½ ((π − πΌ) + ππΏ)] (55) (π ≥ 2; π ∈ N0 ) . π0 (π§) = π§ − π€, Setting ππ (π§) = (π§ − π€) 1−πΎ − π (π − πΎ) [1 + (π − 1) π½ ((π − πΌ) + ππΏ)] × (π§ − π€)π Then π(π§) ∈ in the form π (50) π ππ = (π − πΎ) [1 + (π − 1) π½ ((π − πΌ) + ππΏ)] ππ , 1−πΎ (π ≥ 2; π ∈ N0 ) , (π ≥ 2; π ∈ N0 ) . ∞ π1 = 1 − ∑ ππ, ∗ (πΌ, π½, πΎ, πΏ, π) if and only if it can be expressed ππ,π€ π=2 it follows that π(π§) = proof of theorem. ∞ π (π§) = ∑ π π ππ (π§) , (51) π=1 ∗ (πΌ, π½, πΎ, πΏ, π). ππ,π€ Proof. Suppose that 7. Integral Operators πΉ (π§) = ∞ (52) π=1 π§ π+1 π−1 π (π‘) ππ‘ π ∫ (π‘ − π€) (π§ − π€) π€ ∗ also belongs to the class ππ,π€ (πΌ, π½, πΎ, πΏ, π). ∞ π ∑ (π − πΎ) [1 + (π − 1)π½((π − πΌ) + ππΏ)] ππ ∞ π (π§) = ∑ π π ππ (π§) π=2 π=1 ∞ = ∑ (π − πΎ) [1 + (π − 1) π½ ((π − πΌ) + ππΏ)] ∞ = π 1 π1 (π§) + ∑ π π ππ (π§) (53) ∞ 1 −πΎ π π=2 (π −πΎ) [1 +(π −1) π½ ((π −πΌ) +ππΏ)] × π π (π§ − π€)π . π π=2 π=2 −∑ (57) Proof. From (57), it follows that πΉ(π§) = (π§ − π€) − π ∑∞ π=2 ππ (π§ − π€) , where ππ = ((π + 1)/(π + π))ππ . Therefore where π π ≥ 0 (π ≥ 1) and ∑∞ π=1 π π = 1. Then = (π§ − π€) This completes the Theorem 12. If the function π(π§) defined by (10) is in the class ∗ (πΌ, π½, πΎ, πΏ, π), and let π be a real number such that π > −1. ππ,π€ Then the function πΉ(π§) defined by where π π ≥ 0 and ∑∞ π=1 π π = 1. π (π§) = ∑ π π ππ (π§) , (56) ×( ∞ π+1 )π π+π π (58) π ≤ ∑ (π − πΎ) [1 + (π − 1) π½ ((π − πΌ) + ππΏ)] ππ π=2 ≤ 1 − πΎ, 8 Journal of Applied Mathematics ∗ since π(π§) ∈ ππ,π€ (πΌ, π½, πΎ, πΏ, π). Hence by Theorem 3, πΉ(π§) ∈ ∗ ππ,π€ (πΌ, π½, πΎ, πΏ, π). Acknowledgment The work here was fully supported by LRGS/TD/2011/ UKM/ICT/03/02 and UKM-DLP-2011-050. References [1] S. Kanas and F. Rønning, “Uniformly starlike and convex functions and other related classes of univalent functions,” Annales Universitatis Mariae Curie-SkΕodowska A, vol. 53, pp. 95–105, 1999. [2] M. Acu and S. Owa, “On a subclass of n-starlike functions,” International Journal of Mathematics and Mathematical Sciences, vol. 2005, no. 17, pp. 2841–2846, 2005. [3] A. W. Goodman, “On uniformly starlike functions,” Journal of Mathematical Analysis and Applications, vol. 155, no. 2, pp. 364– 370, 1991. [4] A. W. Goodman, “On uniformly convex functions,” Annales Polonici Mathematici, vol. 56, no. 1, pp. 87–92, 1991. [5] M. S. Robertson, “Extremal problems for analytic functions with positive real part and applications,” Transactions of the American Mathematical Society, vol. 106, pp. 236–253, 1963. σΈ σΈ [6] H. Saitoh, “Univalence and starlikeness of solutions of π + ππσΈ + ππ = 0,” Annales Universitatis Mariae Curie-SkΕodowska A, vol. 53, pp. 209–216, 1999. [7] S. Owa, H. Saitoh, H. M. Srivastava, and R. Yamakawa, “Geometric properties of solutions of a class of differential equations,” Computers & Mathematics with Applications, vol. 47, no. 10-11, pp. 1689–1696, 2004. [8] M. O. Reade and H. Silverman, “Radii problems for linear properties of univalent functions,” Houston Journal of Mathematics, vol. 17, no. 2, pp. 227–235, 1991. [9] J. SokoΜΕ and A. WisΜniowska-Wajnryb, “On certain problem in the class of k-starlike functions,” Computers & Mathematics with Applications, vol. 62, no. 12, pp. 4733–4741, 2011. [10] P. Curt and D. Fericean, “A special class of univalent functions in Hele-Shaw flow problems,” Abstract and Applied Analysis, vol. 2011, Article ID 948236, 10 pages, 2011. [11] M. Darus and R. W. Ibrahim, “On subclasses for generalized operators of complex order,” Far East Journal of Mathematical Sciences, vol. 33, no. 3, pp. 299–308, 2009. [12] F. M. Al-Oboudi, “On univalent functions defined by a generalized SaΜlaΜgean operator,” International Journal of Mathematics and Mathematical Sciences, vol. 2004, no. 27, pp. 1429–1436, 2004. [13] G. SaΜlaΜgean, “Subclasses of univalent functions,” in Lecture Notes in Mathematics, pp. 362–372, Springer, Heidelberg, Germany, 1983. Advances in Operations Research Hindawi Publishing Corporation http://www.hindawi.com Volume 2014 Advances in Decision Sciences Hindawi Publishing Corporation http://www.hindawi.com Volume 2014 Mathematical Problems in Engineering Hindawi Publishing Corporation http://www.hindawi.com Volume 2014 Journal of Algebra Hindawi Publishing Corporation http://www.hindawi.com Probability and Statistics Volume 2014 The Scientific World Journal Hindawi Publishing Corporation http://www.hindawi.com Hindawi Publishing Corporation http://www.hindawi.com Volume 2014 International Journal of Differential Equations Hindawi Publishing Corporation http://www.hindawi.com Volume 2014 Volume 2014 Submit your manuscripts at http://www.hindawi.com International Journal of Advances in Combinatorics Hindawi Publishing Corporation http://www.hindawi.com Mathematical Physics Hindawi Publishing Corporation http://www.hindawi.com Volume 2014 Journal of Complex Analysis Hindawi Publishing Corporation http://www.hindawi.com Volume 2014 International Journal of Mathematics and Mathematical Sciences Journal of Hindawi Publishing Corporation http://www.hindawi.com Stochastic Analysis Abstract and Applied Analysis Hindawi Publishing Corporation http://www.hindawi.com Hindawi Publishing Corporation http://www.hindawi.com International Journal of Mathematics Volume 2014 Volume 2014 Discrete Dynamics in Nature and Society Volume 2014 Volume 2014 Journal of Journal of Discrete Mathematics Journal of Volume 2014 Hindawi Publishing Corporation http://www.hindawi.com Applied Mathematics Journal of Function Spaces Hindawi Publishing Corporation http://www.hindawi.com Volume 2014 Hindawi Publishing Corporation http://www.hindawi.com Volume 2014 Hindawi Publishing Corporation http://www.hindawi.com Volume 2014 Optimization Hindawi Publishing Corporation http://www.hindawi.com Volume 2014 Hindawi Publishing Corporation http://www.hindawi.com Volume 2014