Hindawi Publishing Corporation Abstract and Applied Analysis Volume 2012, Article ID 837913, 10 pages doi:10.1155/2012/837913 Research Article On Certain Sufficiency Criteria for p-Valent Meromorphic Spiralike Functions Muhammad Arif Department of Mathematics, Abdul Wali Khan University Mardan, Mardan, Pakistan Correspondence should be addressed to Muhammad Arif, marifmaths@yahoo.com Received 10 June 2012; Accepted 6 August 2012 Academic Editor: Allan Peterson Copyright q 2012 Muhammad Arif. 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. We consider some subclasses of meromorphic multivalent functions and obtain certain simple sufficiency criteria for the functions belonging to these classes. We also study the mapping properties of these classes under an integral operator. 1. Introduction Let p, n denote the class of functions fz of the form fz z−p ∞ ak zk−p1 p∈N , 1.1 kn which are analytic and p-valent in the punctured unit disk U {z : 0 < |z| < 1}. Also let ∗ λ p, n consisting of all functions fz c p, n, α denote the subclasses of λ p, n, α and which are defined, respectively, by z > α cos λ z ∈ U, Re −e fz zf z iλ > α cos λ z ∈ U. Re −e f z of iλ zf 1.2 We note that for λ 0 and n 1, the above classes reduce to the well-known subclasses p consisting of meromorphic multivalent functions which are, respectively, starlike 2 Abstract and Applied Analysis and convex of order α 0 ≤ α < p. For the detail on the subject of meromorphic spiral-like functions and related topics, we refer the work of Liu and Srivastava 1, Goyal and Prajapat 2, Raina and Srivastava 3, Xu and Yang 4, and Spacek 5 and Robertson 6. Analogous to the subclass of 1, 1 for meromorphic univalent functions studied by Wang et al. 7 and Nehari and Netanyahu 8, we define a subclass λN p, n, α of p, n consisting of functions fz satisfying − Re e zf z f z iλ α > p, z ∈ U . < α cos λ 1.3 For more details of the above classes see also 9, 10. Motivated from the work of Frasin 11, we introduce the following integral operator of multivalent meromorphic functions p Hm,p z 1 z m zp1 0 j1 up fj u αj du. 1.4 For p 1, 1.4 reduces to the integral operator introduced and studied by Mohammed and Darus 12, 13. Similar integral operators for different classes of analytic, univalent, and multivalent functons in the open unit disk are studied by various authors, see 14–19. ∗ In this paper, first, we find sufficient conditions for the classes λ p, n, α and λ c p, n, α and then study some mapping properties of the integral operator given by 1.4. We will assume throughout our discussion, unless otherwise stated, that λ is real with |λ| < π/2, 0 ≤ α < p, p, n ∈ N, αj > 0 for j ∈ {1, . . . m}. To obtain our main results, we need the following Lemmas. Lemma 1.1 see 20. If qz ∈ 1, n with n ≥ 1 and satisfies the condition n 2 z q z 1 < √ n2 1 z ∈ U, 1.5 then qz ∈ ∗ 1, n, 0. 1.6 0 Lemma 1.2 see 21. Let Ω be a set in the complex plane C and suppose that Ψ is a mapping from C2 × U to C which satisfies Ψix, y, z ∈ / Ω for z ∈ U, and for all real x, y such that y ≤ −n/21 x2 . If hz 1 cn zn · · · is analytic in U and Ψhz, zh z, z ∈ Ω for all z ∈ U, then Re hz > 0. Abstract and Applied Analysis 3 2. Some Properties of the Classes Theorem 2.1. If fz ∈ ∗ λ p, n, α and λ c p, n, α p, n satisfies p iλ z fz e /p−α cos λ eiλ zf z α cos λ ip sin λ p − α cos λ fz n <√ n2 1 then fz ∈ p − α cos λ 2.1 z ∈ U, ∗ λ p, n, α. Proof. Let us set a function hz by hz eiλ /p−α cos λ 1 eiλ an 1 p zn · · · z fz z z p − α cos λ 2.2 for fz ∈ p, n. Then clearly 2.2 shows that hz ∈ 1, n. Differentiating 2.2 logarithmically, we have f z p eiλ 1 h z − hz fz z z p − α cos λ 2.3 which gives 2 z h z 1 eiλ /p−α cos λ 1 p iλ zf z e z fz α cos λ ip sin λ 1. fz p − α cos λ 2.4 Thus using 2.1, we have n 2 z h z 1 ≤ √ n2 1 Hence, using Lemma 1.1, we have hz From 2.3, we can write 1 zh z hz p − α cos λ Since hz ∈ ∗ 0 1, n, 0, eiλ z ∈ U. ∗ 0 1, n, 0. zf z α cos λ ip sin λ . fz 2.6 it implies that Re−zh z/hz > 0. Therefore, we get 1 zh z iλ zf z − α cos λ Re − >0 Re −e fz hz p − α cos λ 2.5 2.7 4 Abstract and Applied Analysis or eiλ Re − zf z fz 2.8 > α cos λ, and this implies that fz ∈ ∗λ p, n, α. If we take λ 0, we obtain the following result. Corollary 2.2. If fz ∈ p, n satisfies p z fz 1/p−α eiλ zf z α p − α < √1 p − α fz 2 then fz ∈ ∗ z ∈ U, p, n, α. Theorem 2.3. If fz ∈ p, n satisfies eiλ /p−α cos λ zp1 f z zf z iλ 1 α cos λ ip sin λ p − α cos λ e −p f z n 1 p − α cos λ < n 12 1 then fz ∈ 2.9 2.10 z ∈ U, λ c p, n, α. Proof. Let us set hz − z 0 1 t2 −tp1 f t p eiλ /p−α cos λ dt eiλ an 1 n−p1 zn · · · . z np p − α cos λ 2.11 Also let 1 gz −zh z z −zp1 f z p eiλ /p−α cos λ Then clearly hz and gz ∈ 1 gz z eiλ an 1 p−n−1 zn · · · . 2.12 z p p − α cos λ 1, n. Now −zp1 f z p eiλ /p−α cos λ . 2.13 Abstract and Applied Analysis 5 Differentiating logarithmically and then simple computation gives us 2 z g z 1 ei λ/p−α cos λ zp1 f z zf z 1 1 α cos λ ip sin λ 1 eiλ −p f z p − α cos λ <√ n n2 1 . 2.14 Therefore, by using Lemma 1.1, we have gz −zh z ∈ ∗ 1, n, 0 2.15 0 which implies that hz ∈ 1 0 c 1, n, 0. Since zf z zh z eiλ p 1 − 1, h z p − α cos λ f z 2.16 therefore zh z 1 Re 1 Re eiλ 1 h z p − α cos λ 1 iλ Re e 1 p − α cos λ Since hz ∈ 0 c 1, n, 0, zf z f z zf z f z peiλ − p − α cos λ α cos λ . 2.17 so zf z −1 α cos λ > 0, Re eiλ 1 f z p − α cos λ 2.18 or zf z − Re eiλ 1 > α cos λ. f z It follows that fz ∈ Theorem 2.4. If fz ∈ 2.19 λ c p, n, α. p, n satisfies zf z M2 iλ zf z α N Re e −1 > fz f z 4L z ∈ U, 2.20 6 Abstract and Applied Analysis then fz ∈ ∗ λ p, n, β, where 0 ≤ α ≤ 1, 0 ≤ β < p and n β − p cos 2λ cos λ, Lα p−β 2 M α β − p 1 − β cos λ sin 2λ cos λ, n N α β2 cos2 λ sin2 λ − β − p cos λ 1 αβ cos λ. 2 2.21 Proof. Let us set eiλ zf z β − p hz − β cos λ − i sin λ. fz 2.22 Then hz is analytic in U with p0 1. Taking logarithmic differentiation of 2.22 and then by simple computation, we obtain eiλ zf z zf z α − 1 Azh z Bh2 z Chz D fz f z Ψ hz, zh z, z 2.23 with A β − p α cos λ, 2 B αe−iλ β − p cos2 λ, C p − β αe−iλ 2βcos2 λ i sin 2λ 1 αe−iλ cos λ , 2.24 D αe−iλ β2 cos2 λ − sin2 λ iβ sin 2λ 1 α β cos λ − i sin λ . Now for all real x and y satisfying y ≤ −n/21 x2 , we have Ψ ix, y, z Ay − Bx2 Cix D. 2.25 Reputing the values of A, B, C, and D and then taking real part, we obtain Re Ψ ix, y, z ≤ −Lx2 Mx N − < where L, M, and N are given in 2.21. √ M Lx − √ 2 L M2 N, 4L 2 M2 N 4L 2.26 Abstract and Applied Analysis 7 / Ω, Let Ω {w : Re w > M2 /4L N}. Then Ψhz, zh z, z ∈ Ω and Ψix, y, z ∈ for all real x and y satisfying y ≤ −n/21 x2 , z ∈ U. By using Lemma 1.2, we have Re hz > 0, that is fz ∈ ∗λ p, n, β. If we put λ 0, we obtain the following result. Corollary 2.5. If fz ∈ p, n satisfies zf z zf z n α − 1 > α β2 − Re β − p 1 αβ fz f z 2 then fz ∗ z ∈ U, 2.27 p, n, β, where 0 ≤ α ≤ 1, 0 ≤ β < p. Theorem 2.6. For j ∈ {1, . . . m}, let fj z ∈ p, n and satisfy 2.9. If m αj < j1 then Hm,p z ∈ N p, n, ζ, p1 , p−β 2.28 where ζ > p. Proof. From 1.4, we obtain m α p zp1 Hm,p z fj z j . z p 1 zp Hm,p z 2.29 j1 Differentiating again logarithmically and then by simple computation, we get ⎤ ⎡ m Hm,p z zfj z H z m,p ⎣ αj 1 p2 − 1 2p 1 p 1 p − 1⎦, fj z Hm,p zHm,p zHm,p z z z j1 zHm,p z 2.30 or, equivalently we can write − zHm,p z Hm,p z 1 ⎛ ⎞ ⎡ ⎤ m zfj z 2 ⎣ p 1 ⎝ αj − − p 1⎠ p − 1 ⎦ fj z zHm,p z j1 Hm,p z m j1 αj − zfj z fj z −p 1 2p . 2.31 8 Abstract and Applied Analysis Now taking real part on both sides, we obtain − Re zHm,p z Hm,p z 1 ⎞ ⎛ ⎡ ⎤ m zfj z 2 ⎣ p 1 ⎝ αj − − p 1⎠ p − 1 ⎦ Re fj z zHm,p z j1 Hm,p z m αj − Re zfj z j1 fj z −p 1 2p . 2.32 This further implies that − Re zHm,p z Hm,p z 1 ⎛ ⎞ ⎡ ⎤ m zfj z Hm,p z 2 ⎣ p 1 ⎝ αj − ≤ − p 1⎠ p − 1 ⎦ fj z zHm,p z j1 m αj − Re j1 zfj z fj z −p 1 2p . 2.33 Let ⎛ ⎞ ⎡ ⎤ m zfj z Hm,p z ⎣ p 1 ⎝ αj − ζ − p 1⎠ p2 − 1 ⎦ fj z zHm,p z j1 ⎡ ⎤ m zfj z ⎣ αj − Re − p 1 2p ⎦. fj z j1 2.34 Clearly we have ⎡ ⎤ m zfj z ζ > ⎣ αj − Re − p 1 2p ⎦. fj z j1 2.35 Then by using 2.28 and Corollary 2.2, we obtain ζ> m αj β − p 1 2p > p. j1 Therefore Hm,p z ∈ N p, n, ζ with ζ > p. 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