Hindawi Publishing Corporation Journal of Inequalities and Applications Volume 2008, Article ID 259205, 11 pages doi:10.1155/2008/259205 Research Article On Meromorphic Harmonic Functions with Respect to k-Symmetric Points K. Al-Shaqsi and M. Darus School of Mathematical Sciences, Faculty of Science and Technology, Universiti Kebangsaan Malaysia, Bangi, Selangor D. Ehsan 43600, Malaysia Correspondence should be addressed to M. Darus, maslina@ukm.my Received 22 May 2008; Revised 20 July 2008; Accepted 23 August 2008 Recommended by Ramm Mohapatra In our previous work in this journal in 2008, we introduced the generalized derivative operator j Dm for f ∈ SH . In this paper, we introduce a class of meromorphic harmonic function with j respect to k-symmetric points defined by Dm . Coefficient bounds, distortion theorems, extreme points, convolution conditions, and convex combinations for the functions belonging to this class are obtained. Copyright q 2008 K. Al-Shaqsi and M. Darus. 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 A continuous function f u iv is a complex valued harmonic function in a domain D ⊂ C if both u and v are real harmonic in D. In any simply connected domain, we write f h g where h and g are analytic in D. A necessary and sufficient condition for f to be locally univalent and orientation preserving in D is that |h | > |g | in D see 1. Hengartner and {z : |z| > 1}. Schober 2 investigated functions harmonic in the exterior of the unit disk U They showed that complex valued, harmonic, sense preserving, univalent mapping f must admit the representation fz hz gz A log |z|, 1.1 where hz and gz are defined by hz αz ∞ n1 for 0 ≤ |β| < |α|, A ∈ C and z ∈ U. an z−n , gz βz ∞ bn z−n , n1 1.2 2 Journal of Inequalities and Applications For z ∈ U \ {0}, let MH denote the class of functions: fz hz gz ∞ ∞ 1 an zn bn zn , z n1 n1 1.3 which are harmonic in the punctured unit disk U \ {0}, where hz and gz are analytic in U \ {0} and U, respectively, and hz has a simple pole at the origin with residue 1 here. j In 3, the authors introduced the operator Dm for f ∈ SH which is the class of functions f h g that are harmonic univalent and sense-preserving in the unit disk U {z : |z| < 1} for which f0 h0 fz 0 − 1 0. For more details about the operator j Dm , see 4. j Now, we define Dm for f h g given by 1.3 as j j j Dm fz Dm hz −1j Dm gz, j, m ∈ N0 N ∪ {0}; z ∈ U \ {0}, 1.4 where j Dm hz j Dm gz ∞ −1j nj Cm, nan zn , z n1 ∞ nj Cm, nbn zn , 1.5 n1 Cm, n nm−1 m n m − 1! . m!n − 1! A function f ∈ MH is said to be in the subclass MS∗H of meromorphically harmonic starlike functions in U \ {0} if it satisfies the condition zh z − zg z > 0, Re − hz gz z ∈ U \ {0}. 1.6 Note that the class of harmonic meromorphic starlike functions has been studied by Jahangiri and Silverman 5, and Jahangiri 6. Now, we have the following definition. k Definition 1.1. For j, m ∈ N0 , 0 ≤ α < 1 and k ≥ 1, let MHSs j, m, α denote the class of meromorphic harmonic functions f of the form 1.3 such that j1 Dm fz Re − j > 0, Dm fk z z ∈ U \ {0}, 1.7 where j j j Dm fk z Dm hk −1j Dm gk j, m ∈ N0 , k ≥ 1, ∞ ∞ −1j hk z an Φn zn , gk z Φn zn , z n1 n1 k−1 1 2πi . εn−1ν , k ≥ 1; ε exp Φn k ν0 k 1.8 1.9 1.10 K. Al-Shaqsi and M. Darus 3 For more details about harmonic functions with respect to k-symmetric points, see papers 7, 8 given by the authors. 2 Also, note that MHSs j, 0, α ⊂ MHS∗S n, α was introduced by Bostancı and Öztürk 9. k k Finally, let MHSs j, m, α denote the subclass of MHSs j, m, α consist of harmonic functions fj hj gj such that hj and gj are of the form ∞ −1j |an |zn , z n1 hj z gj z −1j ∞ |bn |zn . 1.11 n1 Also, let fkj hkj gkj where hkj and gkj are of the form hkj z ∞ −1j Φn |an |zn , z n1 gkj z −1j ∞ Φn |bn |zn , 1.12 n1 where Φn is given by 1.10. In this paper, we will give a sufficient condition for functions f h g, where h and k g given by 1.3 to be in the class MHSs j, m, α. Indeed, it is shown that this coefficient k condition is also necessary for functions to be in the class MHSs j, m, α. Also, we obtain k distortion bounds and characterize the extreme points for functions in MHSs j, m, α. Convolution and closure theorems are also obtained. 2. Coefficient bounds First, we prove a sufficient coefficient bound. Theorem 2.1. Let f h g be of the form 1.3 and fk hk gk where hk and gk are given by 1.9. If ∞ j n − 1k 1 α|an−1k1 | n − 1k 1 − α|bn−1k1 |Ωm n, k n1 ∞ j1 n 2.1 Cm, n|an | |bn | ≤ 1 − α, n2 n/ lk1 j where j, m ∈ N0 , 0 ≤ α < 1, k ≥ 1 and Ωm n, k n − 1k 1j Cm, nk 1, then f is harmonic k univalent, sense preserving in U \ {0} and f ∈ MHSs j, m, α. Proof. For 0 < |z1 | ≤ |z2 | < 1, we have f z1 − f z2 ≥ h z1 − h z2 − g z1 − g z2 ∞ z1 − z2 an bn zn−1 · · · zn−1 ≥ − z1 − z2 2 1 z1 z2 n1 ∞ z1 − z2 2 > 1 − z2 n an bn z1 z2 n1 4 Journal of Inequalities and Applications ∞ ∞ z1 − z2 2 n − 1k 1 an−1k1 bn−1k1 n an bn > 1 − z2 z1 z2 n1 n1 ∞ z1 − z2 j > 1 − n − 1k 1 α an−1k1 − n − 1k 1 − α bn−1k1 Ωm n, k z1 z2 n1 − ∞ nj1 Cm, n an bn . n2 n/ lk1 2.2 This last expression is nonnegative by 2.1, and so f is univalent in U \ {0}. To show that f is sense preserving in U \ {0}, we need to show that |h z| ≥ |g z| in U \ {0}. We have |h z| ≥ ∞ 1 − n|an ||z|n−1 |z|2 n1 ∞ ∞ 1 n−1 − n|a |r > 1 − n|an | n r 2 n1 n1 ≥1− ∞ ∞ j n − 1k 1 α|an−1k1 |Ωm n, k − nj1 Cm, n|an | n2 n/ lk1 n1 ≥ ∞ n − 1k 1 − j α|bn−1k1 |Ωm n, k ∞ 2n|b2n | n1 > ∞ j1 n 2.3 Cm, n|bn | n2 n/ lk1 n1 ≥ ∞ ∞ 2n − 1|b2n−1 | n1 n|bn |r n−1 n1 ∞ n|bn ||z|n−1 ≥ |g z|. n1 k Now, we will show that f ∈ MHSs j, m, α. According to 1.4 and 1.7, for 0 ≤ α < 1, we have ⎧ ⎫ j1 ⎨ Dj1 hz − −1j Dj1 gz ⎬ Dm fz m m ≥ α. 2.4 Re − Re − j ⎩ ⎭ j j j Dm fk z Dm hk z −1 Dm gk z Using the fact that Re{w} ≥ α if and only if |1 − α w| ≥ |1 α − w|, it suffices to show that j1 j1 1 − α − Dm fz ≥ 1 α Dm fz , j j Dm fk z Dm fk z 2.5 j1 j Dm fz − 1 − αDjm fk z − Dj1 m fz 1 αDm fk z ≥ 0. 2.6 which is equivalent to K. Al-Shaqsi and M. Darus j 5 j1 j Substituting Dm fz, Dm fz, and Dm fk z in 2.6 yields j1 j1 j j j Dm hz − −1j Dm gz − 1 − α Dm hk z −1 Dm gk z j1 j1 j j − Dm hz − −1j Dm gz 1 α Dm hk z −1j Dm gk z ∞ ∞ −1j − nj1 Cm, nan zn −1j nj1 Cm, nbn zn z n1 n1 ∞ ∞ −1j nj Cm, nΦn an zn −1j nj Cm, nΦn bn zn 1 − α z n1 n1 ∞ ∞ −1j − − nj1 Cm, nan zn −1j nj1 Cm, nbn zn z n1 n1 ∞ ∞ −1j nj Cm, nΦn an zn −1j nj Cm, nΦn bn zn − 1 α z n1 n1 ∞ ∞ 2 − α−1j j j n j n − n Cm, nn−1−αΦn an z −1 n Cm, nn1−αΦn bn z z n1 n1 ∞ ∞ α−1j j j n j − − n Cm, nn 1 αΦn an z −1 n Cm, nn − 1 αΦn bn zn z n1 n1 ≥ ∞ ∞ 2 − α − nj Cm, nn − 1 − αΦn |an ||zn | − nj Cm, nn 1 − αΦn |bn ||zn | |z| n1 n1 − ∞ ∞ α − nj Cm, nn 1 αΦn |an ||zn | − nj Cm, nn − 1 αΦn |bn ||zn | |z| n1 n1 ∞ j ∞ j n1 n1 n Cm, nn αΦn n Cm, nn − αΦ 21 − α n 1− |an |z − |bn |z |z| 1−α 1−α n1 n1 ≥ 21 − α 1 − ∞ j n Cm, nn αΦn n1 1−α |an | − ∞ j n Cm, nn − αΦn n1 1−α |bn | . 2.7 From the definition of Φn , we know that Φn ⎧ ⎨1, n lk 1, ⎩ 0, n/ lk 1, n ≥ 2, k, l ≥ 1. 2.8 6 Journal of Inequalities and Applications Substituting 2.8 in 2.7, then 2.7 is equivalent to j1 j Dm fz − 1 − αDjm fk z − Dj1 m fz 1 αDm fk z ∞ nk 1j Cm, nk 1nk 1 α |ank1 | ≥ 21 − α 1 − 1−α n1 − ∞ nk 1j Cm, nk 1nk 1 − α 1−α n1 − ∞ nj Cm, n 1α |bn | − |a1 | − |b1 | 1 − α 1−α n2 ∞ nj Cm, n |an | 1−α n2 n / lk1 n/ lk1 21 − α 1 − ∞ n − 1k 1 α n1 − |bnk1 | − 1−α n − 1k 1 − α j |an−1k1 | − |bn−1k1 | Ωm n, k 1−α ∞ nj1 Cm, n |an | |bn | 1−α n2 ≥ 0, by 2.6. n / lk1 2.9 Thus, this completes the proof of the theorem. k We next show that condition 2.1 is also necessary for functions in MHSs j, m, α. Theorem 2.2. Let fj hj gj , where hj and gj are given by 1.11, and fkj hkj gkj where hkj k and gkj are given by 1.12. Then, fj ∈ MHSs j, m, α, if and only if the inequality 2.1 holds for the coefficient of fj hj gj and fkj hkj gkj . k ∈MHSs j, m, α if condition Proof. In view of Theorem 2.1, we need only to show that fj / k 2.1 does not hold. We note that for fj ∈ MHSs j, m, α, then by 1.7 the condition 2.4 must be satisfied for all values of z in U \ {0}. Substituting for hj , gj , hkj , and gkj given by 1.11 and 1.12, respectively, in 2.4 and choosing 0 < z r < 1, we are required to have Re{Ψz/Υz} ≥ 0, where j1 j1 j j Ψz −Dm hj z −1n Dm gj z − αDm hkj z − α−1j Dm gkj z ∞ ∞ 1−α − nj Cm, nn αΦn |an |zn nj Cm, nn − αΦn |bn |zn , z n1 n1 j j 2.10 Υz Dm hkj z −1j Dm gkj z ∞ ∞ 1 nj Cm, nΦn |an |zn nj Cm, nΦn |bn |zn . z n1 n1 Then, the required condition Re{Ψz/Υz} ≥ 0 is equivalent to ∞ j j n n 1 − α/z − ∞ n1 n Cm, nn αΦn |an |r n1 n Cm, nn − αΦn |bn |r . ∞ j ∞ j 1/z n1 n Cm, nΦn |an |r n n1 n Cm, nΦn |bn |r n 2.11 K. Al-Shaqsi and M. Darus 7 By using 2.8, and if condition 2.1 does not hold, then the numerator of 2.11 is negative for r sufficiently close to 1. Thus, there exists a z0 r0 in 0, 1 for which the quotient in 2.11 k is negative. This contradicts the required condition for fj ∈ MHSs j, m, α and so the proof is complete. 3. Distortion bounds and extreme points k In this section, we will obtain distortion bounds for functions fj ∈ MHSs j, m, α and also k provide extreme points for the class MHSs j, m, α. k Theorem 3.1. If fj hj gj ∈ MHSs j, m, α and 0 < |z| r < 1, then 1−α 1−α 1 1 − j r ≤ |fj z| ≤ j r. r 2 m 12 − α r 2 m 12 − α 3.1 Proof. We will prove the left side of the inequality. The argument for the right side of the inequality is similar to the left side, and thus the details will be omitted. Let fj hj gj ∈ k MHSs j, m, α. Taking the absolute value of f, we obtain ∞ ∞ −1j n n n an z −1 bn z |fj | z n1 n1 ≥ ∞ 1 − |an | |bn |r n r n1 ≥ ∞ 1 − |an | |bn |r r n1 ∞ j 1−α 2 m 12 − αΦ2 1 |an | |bn |r ≥ − j r 2 m 12 − αΦ2 n1 1−α 3.2 ∞ j 1−α nj Cm, nn − αΦn n Cm, nn αΦn 1 |an | |bn | r ≥ − j r 2 m 12 − α n1 1−α 1−α ≥ 1−α 1 − r, r 2j m 12 − α by 2.7. The bounds given in Theorem 3.1 hold for functions fj h gj of the form 1.11. And it is also discovered that the bounds hold for functions of the form 1.3, if the coefficient condition 2.1 is satisfied. The following covering result follows from the left-hand side of the inequality in Theorem 3.1. k Corollary 3.2. If fj ∈ MHSs j, m, α, then 2j m 12 − α − 1 − α fj U \ {0} ⊂ w : |w| < . 2j m 12 − α 3.3 8 Journal of Inequalities and Applications k Next, we determine the extreme points of closed convex hulls of MHSs j, m, α k denoted by clcoMHSs j, m, α. k Theorem 3.3. Let fj hj gj where hj and gj are given by 1.11. Then, fj ∈ MHSs j, m, α if and only if fj,n z ∞ xn hjn z yn gjn z, 3.4 n0 where hj,0 gj,0 z −1j /z, hj,n z −1j /z 1 − α/nj Cm, nn αΦn zn n 1, 2, 3, . . ., gj,n z −1j /z −1j 1 − α/nj Cm, nn − αΦn zk n 1, 2, 3, . . ., ∞ n0 xn k yn 1, xn ≥ 0, yn ≥ 0. In particular, the extreme points of MHSs j, m, α are {hj,n } and {gj,n }. Proof. For functions fj hj gj , where hj and gj are given by 1.11, we have fj,n z ∞ xn hj,n z yn gj,n z n0 ∞ ∞ 1−α −1j xn zn xn yn j z n Cm, nn αΦ n n0 n1 −1j 3.5 ∞ 1−α y zk . j Cm, nn − αΦ n n n n1 Now, the first part of the proof is complete, and Theorem 2.2 gives ∞ 1−α nj Cm, nn αΦn xn j 1−α n1 n Cm, nn αΦn ∞ 1−α n1 nj Cm, nn nj Cm, nn − αΦn yn 1−α − αΦn 3.6 ∞ xn yn − x0 y0 1 − x0 y0 ≤ 1. n0 k Conversely, suppose that fj ∈ clcoMHSs j, m, α. For n 1, 2, 3, . . ., set nj Cm, nn αΦn |an | 1−α 0 ≤ xn ≤ 1, nj Cm, nn − αΦn yn |bn | 1−α 0 ≤ yn ≤ 1, xn 3.7 K. Al-Shaqsi and M. Darus x0 1 − ∞ n1 xn fj,n z 9 yn . Therefore, f can be written as ∞ ∞ −1j |an |zn −1j |bn |zn z n1 n1 ∞ ∞ 1 − αyn 1 − αxn −1j j n z −1 zn j j z n Cm, nn αΦ n Cm, nn − αΦ n n n1 n1 ∞ ∞ −1j −1j −1j xn yn hj,n z − gj,n z − z z z n1 n1 3.8 ∞ ∞ ∞ ∞ −1j hj,n zxn gj,n zyn 1 − xn − yn z n1 n1 n1 n1 ∞ hj,n zxn gj,n zyn , as required. n0 4. Convolution and convex combination k In this section, we show that the class MHSs j, m, α is invariant under convolution and convex combination of its member. n j ∞ n For harmonic functions fj z −1j /z ∞ n1 |an |z −1 n1 |bn |z and Fj z n j ∞ n −1j /z ∞ n1 |An |z −1 n1 |Bn |z , the convolution of fj and Fj is given by fj ∗Fj z fj z∗Fj z ∞ ∞ −1j |an ||An |zn −1j |bn ||Bn |zn . z n1 n1 k 4.1 k Theorem 4.1. For 0 ≤ β ≤ α < 1, let fj ∈ MHSs j, m, α and Fj ∈ MHSs j, m, β. Then, k k fj ∗Fj ∈ MHSs j, m, α ⊂ MHSs j, m, β. Proof. We wish to show that the coefficients of fj ∗Fj satisfy the required condition given in k Theorem 2.2. For Fj ∈ MHSs j, m, β, we note that |An | ≤ 1 and |Bn | ≤ 1. Now, for the convolution function fj ∗Fj , we obtain ∞ j n Cm, nn βΦn 1−β n1 ≤ 1−β 1−β 1−α |an | |an | 1−β ∞ j n Cm, nn − αΦn n1 k |bn ||Bn | ∞ j n Cm, nn − βΦn n1 ∞ j n Cm, nn − αΦn n1 ∞ j n Cm, nn − βΦn n1 ∞ j n Cm, nn βΦn n1 ≤ |an ||An | 1−α |bn | 4.2 |bn | ≤ 1, k since 0 ≤ β ≤ α < 1 and fj ∈ MHSs j, m, α. Therefore fj ∗Fj ∈ MHSs j, m, α ⊂ k MHSs j, m, β. 10 Journal of Inequalities and Applications k We now examine the convex combination of MHSs j, m, α. Let the functions fj,t be defined, for t 1, 2, . . . , ρ, by ∞ ∞ −1j |an,t |zn −1j |bn,t |zn . z n1 n1 fj,t z 4.3 k Theorem 4.2. Let the functions fj,t defined by 4.3 be in the class MHSs j, m, α for every t 1, 2, . . . , ρ. Then, the functions ξt z defined by ξt z ρ ct fjn z, 0 ≤ ct ≤ 1, 4.4 t1 k are also in the class MHSs j, m, α, where ρ t1 ct 1. Proof. According to the definition of ξt , we can write ρ ρ ∞ ∞ −1j j n ξt z ct an,t z −1 ct bn,t zn . z n1 t1 n1 t1 4.5 k Further, since fj,t z are in MHSs j, m, α for every t 1, 2, . . . , ρ. Then by 2.7, we have ρ ρ ∞ j n αΦn ct |an,t | n − αΦn ct |bn,t | n Cm, n n1 t1 t1 ρ ∞ j ct n αΦn |an,t | n − αΦn |bn,t |n Cm, n t1 ≤ 4.6 n1 ρ ct 1 − α ≤ 1 − α. t1 Hence, the theorem follows. k Corollary 4.3. The class MHSs j, m, α is close under convex linear combination. k Proof. Let the functions fj,t z t 1, 2 defined by 4.3 be in the class MHSs j, m, α. Then, the function ψz defined by ψz μfj,1 z 1 − μfj,2 z, 0 ≤ μ ≤ 1, 4.7 k is in the class MHSs j, m, α. Also, by taking ρ 2, ξ1 μ, and ξ2 1 − μ in Theorem 4.2, we have the corollary. Acknowledgment The work here was fully supported by Fundamental Research Grant SAGA: STGL-012-2006, Academy of Sciences, Malaysia. K. Al-Shaqsi and M. Darus 11 References 1 J. Clunie and T. Sheil-Small, “Harmonic univalent functions,” Annales Academiae Scientiarum Fennicae. Series A I. Mathematica, vol. 9, pp. 3–25, 1984. 2 W. Hengartner and G. Schober, “Univalent harmonic functions,” Transactions of the American Mathematical Society, vol. 299, no. 1, pp. 1–31, 1987. 3 K. Al-Shaqsi and M. Darus, “On harmonic functions defined by derivative operator,” Journal of Inequalities and Applications, vol. 2008, Article ID 263413, 10 pages, 2008. 4 K. Al-Shaqsi and M. Darus, “An operator defined by convolution involving the polylogarithms functions,” Journal of Mathematics and Statistics, vol. 4, no. 1, pp. 46–50, 2008. 5 J. M. Jahangiri and H. Silverman, “Meromorphic univalent harmonic functions with negative coefficients,” Bulletin of the Korean Mathematical Society, vol. 36, no. 4, pp. 763–770, 1999. 6 J. M. Jahangiri, “Harmonic meromorphic starlike functions,” Bulletin of the Korean Mathematical Society, vol. 37, no. 2, pp. 291–301, 2000. 7 K. Al-Shaqsi and M. Darus, “On subclass of harmonic starlike functions with respect to K-symmetric points,” International Mathematical Forum, vol. 2, no. 57–60, pp. 2799–2805, 2007. 8 K. Al-Shaqsi and M. Darus, “On harmonic univalent functions with respect to k-symmetric points,” International Journal of Contemporary Mathematical Sciences, vol. 3, no. 1–4, pp. 111–118, 2008. 9 H. Bostancı and M. Öztürk, “New classes of Salagean type meromorphic harmonic functions,” International Journal of Mathematics Sciences, vol. 2, no. 1, pp. 52–57, 2008.