Normalization of the generalized K Mittag-Leffler function and ratio to its sequence of partial sums

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Normalization of the generalized K Mittag-Leffler function ratio to its sequence of partial sums H. Rehman, M. Darus J. Salah Abstract. In this article we introduce an operator L k,α (β, δ)(f)(z) associated with generalized K Mittag-Leffler function in the unit disk U= z : z < 1}. Further the ratio of normalized K Mittag-Leffer function Q (z) to its sequence of partial sums Q( ) m(z) are calculated. M.S.C. 2010: 30C45. Key words: Mittag-Leffler function; analytic functions; fractional calculus; Hadamard product; sequence of partial sums. 1 Introduction The (M-L) function was introduced by the Swedish Mathematician Mittag-Leffler [13, 14]. This function may be a classical function dealing with problems in Complex Analysis so it is important for obtaining solutions of fractional differential integral equations which are associated e.g., with the kinetic equation, rom walks, Levy flights super diffusive transport problems. Moreover, from its exponential behavior, the deviations of physical phenomena could also be described by physical laws through Mittag-Leffler functions. Many authors have studied on (M-L) functions for its properties, generalization, applications extension, such as [12], [11], [15]. 2 Preliminaries definitions The one-parameter (M-L) function E α (z) : (z) C see [13] [14], (2.1) E α (z) := z n Γ(α + 1) =: E α,1(z), its two-parameters extension E α,β (z) was studied by Wiman [10], (2.2) E α,β (z) := z n Γ(αn + β) BSG Proceedings, vol. 25, 2018, pp. 79-95. c Balkan Society of Geometers, Geometry Balkan Press 2018. (α 0),

80 H. Rehman, M. Darus J. Salah where α, β C, R(α) > 0 R(β) > 0. E γ α,β Further, in 1971, Prabhakar [8] proposed another general form of (M-L) function (z) as: (2.3) E γ α,β (z) := (γ) n Γ(αn + β)n! zn, for which α, β, γ C, R(α) > 0, R(β) > 0 R(γ) > 0. where (γ) n is the Pochhammar symbol: Γ(γ + n) 1, n = 0 (γ) n = = Γ(γ) γ(γ + 1)...(γ + n 1) Note that (t) n = t(t + 1) n 1, (t) n t n, n N n N Srivastava Tomovski [5] proved that the function E γ α,β (z) defined by 2.3 is an entire function in the complex z-plane. Another useful generalization of the Mittag-Leffler function called as K Mittag- Leffler function E γ k,α,β (z), introduced in [3] as: (2.4) E γ k,α,β (z) := (γ) n,k Γk(αn + β)n! zn, where (γ) n,k is the k Pochhammer symbol defined as: (2.5) (γ) n,k = γ(γ + k)(γ + 2k)...(γ + (n 1)k) (γ C, k R, n N). The following extension is due to A. K. Shukla J. C. Prajapati [17], (2.6) E α,β (z) := (γ) nq Γk(αn + β)n! zn, Remark 2.1. In case q N then (γ) nq = q qn q r=1 Further extension of K Mittag-Leffler function GE studied by K. S Gehlot [2] as for q (0, 1) N, ( ) γ + r 1 q k,α,β (2.7) GE k,α,β (z) := (γ) nq,k Γk(αn + β)n! zn, n (z) took place which was where (γ) nq,k is defined as (2.5) the generalized pochhammer symbol is defined in [1] under condition if q N. (2.8) (γ) nq = Γ(γ + nq), Γ(γ)

The generalized K M L function ratio to its sequence of partial sums 81 Due to the high interest of researchers in (M-L) functions another parameter δ C was inserted by Salim [18] which has the generalized form of: E k,α (β, δ)(z): (2.9) E (z) = (γ) nq,k z n, Γk(αn + β)(δ) n the imposition on parameters are α, β, γ C, R(α) > 0, R(β) > 0, k R, δ is non-negative real number nq is a positive integer. Let M represents the class of the normalized functions of the form: (2.10) f(z) = z + which are analytic in the open unit disk a n z n U = z C : z < 1}. Since the Mittag-Leffler function in (2.1) does not belong to the class M therefore, for (M-L) functions to be the member of class M, Srivastava his co-authors [16] have considered some normalization on the E α,β as: (2.11) E α,β (z) = Γ(β)zE α,β (z) Γ(β) = z + Γ(αn + β) zn+1, the above equality can also be written as where E α,β (z) = z + Γ(β) Γ(α(n 1) + β) zn, (z, α, β C; R(α) > 0) (β 0, 1, 2,...). The normalized Mittag-Leffler function E α,β contains some well-known functions for particular values belonging to real numbers of α, β z U. E 2,1 = zcosh( z), E 2,2 = zsinh( z), E 2,3 = 2[cosh( z) 1], E 2,4 = 6[sinh( z) z] z. Definition 2.2. For a function f M given by (2.1) g M given by g(z) = z + b n z n, we define the Hadamard product (or convolution) of f g by (2.12) (f g)(z) = z + a n b n z n, (a n 0, z U).

82 H. Rehman, M. Darus J. Salah Salah Darus [15] generalization of Mittag-Leffler functions defined by Srivastava Tomovski [5] is given by, (2.13) mf α,δ (z) = m i=1 (γ i ) q n i (δ i ) αi n n! zn, Remark 2.3. Note that if m = 1 then m F α,δ (z) = Γ(β)E α,δ (z) Definition 2.4. (Taylor Series). The Taylor series of a function f(z) about z = a is (2.14) f(z) = f(a) + f (a)(z a) +... = f n (a) (z a) n, n! Remark 2.5. The equality between f(z) its Taylor series is only valid if the series converges. Remark 2.6. We choose a geometric series f(z) = 1 1 z = 1 + z2 + z 3 +... = z n, which is Taylor series about z = 0. Note that the function f(z) = 1 exists is 1 z infinitely differentiable everywhere except at z = 1 while the series exists in the unit disc z < 1 hence analytic. Now we introduce a function φ(z) = the form (2.15) φ(z) = z + z 1 z = z + z2 + z 3 +... = which is analytic in the open unit disk U = z C : z < 1}. z n z n+1 M of Definition 2.7. The generalized Libera integral operator J c for a function f(z) belonging to the class A, we define the generalized Libera integral operator J c [20] by (2.16) J c (f) = c + 1 z c z 0 t c 1 f(t)dt = z k=n+1 ( ) c + 1 a k z k, (c 0) n + 1 (2.17) J 1 (f) = 2 z z 0 f(t)dt = z k=n+1 ( ) 2 a k z k. n + 1 The operator J c, when c = 1, 2, 3,...} was introduced by Bernardi [19]. In particular, the operator J 1, was studied earlier by Libera [20] Livingston [21]. Subsequent to our studies of [4] [16] we impose some normalization over the most generalized Mittag-Leffler function E (z) which is defined in 2.9.

The generalized K M L function ratio to its sequence of partial sums 83 3 Main Results Theorem 3.1. If f(z) belongs to M such that z U then M class of function f(z) convolution of the generalized K Mittag-Leffler function GE (z) is (3.1) L (f)(z) = z + (γ) nq,k Γk(α + β)γ(δ + 1) (γ) q,k Γk(αn + β)γ(δ + n) a nz n, if the following conditions hold 1. α, β, γ C, R(α) > 0, R(β) > 0 R(γ) > 0, k R q (0, 1) N. 2. f(z) is analytic in the open unit disk, U= z : z < 1}. 3. R(α i ), R(β i ), R(γ i ), R(δ i ) > max0, R(q i ) 1} q (0, 1) N, R(q i ) > 0, γ 0. 4. (γ) nq,k is generalized pochhammer symbol as defined in (2.5). Proof. The Generalized Mittag-Leffler function [18] E (z) = (γ) nq,k z n, Γk(αn + β)(δ) n where α, β, γ C, R(α) > 0, R(β) > 0, k R, δ is non-negative real number, nq is a positive integer q (0, 1) N. (3.2) E Γ(γ + k) (z) = Γ(γ)Γk(β) + The above equation can also be written as (3.3) ( Γk(α + β)γ(δ) (E (γ) ) (γ) ) k q,k Γk(β) (γ) q,k Γk(α + β)γ(δ) z + = z + (γ) nq,k Γk(αn + β)(δ) n z n. (γ) nq,k Γk(α + β)γ(δ + 1) (γ) q,k Γk(αn + β)γ(δ + n) zn. Now we define the function Q (z) by ( (3.4) Q Γk(α + β)γ(δ) (z) = (E (γ) ) (γ) ) k. q,k Γk(β) Then equation (3.4) implies (3.5) Q (z) = z + (γ) nq,k Γk(β)Γ(δ + 1) (γ) q,k Γk(αn + β)γ(δ + n) zn+1. (3.6) Q (z) = z + (γ) (n 1)q,k Γk(α + β)γ(δ + 1) (γ) q,k Γk(α(n 1) + β)γ(δ + n 1) zn.

84 H. Rehman, M. Darus J. Salah Let f(z) M. Denote L k,αβ,δ (f)(z) : M M the operator is defined by (3.7) L (f)(z) = Q (z) f(z), where the symbol (*) sts for Hadamard product (or convolution). Now applying Hadamard product using the equations (2.10), (3.6) (3.7) we obtain the desired result. Corollary 3.2. If we put γ = q = k = β = δ = 1 α = 0 in equation (3.1). Let the condition of Theorem (3.1) be satisfied, then we get the following results, L 1,1 1,0,1,1 (f)(z) = z + a n z n = f(z) Corollary 3.3. If we set γ = 2, q = k = β = δ = 1 α = 0 in equation (3.1). Let the condition of Theorem (3.1) be satisfied, then the reduced form is, L 2,1 1,0,1,1 (f)(z) = z + ( n + 1 2 ) a n z n = 1 2 f(z) + zf (z)} Corollary 3.4. If we set out the values of γ = q = k = β = 1, δ = α = 0 in equation (3.1). Let the condition of Theorem (3.1) be satisfied, then the reduced form is, L 1,1 1,0,1,0 (f)(z) = z + na n z n = zf (z) Corollary 3.5. If we keep γ = q = k = β = 1, δ = 2 α = 0 in equation (3.1). Let the condition of Theorem (3.1) be satisfied, then the reduced form is, L 1,1 1,0,1,2 (f)(z) = z + 2 ( n + 1 )a nz n = 2 z z 0 f(t)dt. Corollary 3.6. Note that corollary (3.5) is Bernardi type of integral [19]. Particularly, the operator J 1 defined in (2.7), was studied earlier by Libera [20] Livingston [21]. Theorem 3.7. If f(z) belongs to M such that z U then M class of function φ(z) convolution of the generalized K Mittag-Leffler function GE (z) is (3.8) L (f)(z) = z + (γ) nq,k Γk(α + β)γ(δ + 1) (γ) q,k Γk(αn + β)γ(δ + n) zn, if the following conditions hold 1. α, β, γ C, R(α) > 0, R(β) > 0 R(γ) > 0, k R q (0, 1) N. 2. f(z) is analytic in the open unit disk, U= z : z < 1}. 3. R(α i ), R(β i ), R(γ i ), R(δ i ) > max0, R(q i ) 1} q (0, 1) N, R(q i ) > 0, γ 0.

The generalized K M L function ratio to its sequence of partial sums 85 4. (γ) nq,k is generalized pochhammer symbol as defined in (2.5). Proof. The generalized Mittag-Leffler function [18] E (z) = (γ) nq,k z n, Γk(αn + β)(δ) n where α, β, γ C, R(α) > 0, R(β) > 0, k R, δ is non-negative real number, nq is a positive integer q (0, 1) N. (3.9) E (z) = (γ) k Γk(β) + (γ) q,k Γk(α + β)(δ) z + (γ) nq,k Γk(αn + β)(δ) n z n, The above equation can also be written as ( Γk(α + β)(δ) (3.10) (E (γ) ) (γ) ) k (γ) nq,k Γk(α + β)γ(δ + 1) = z + q,k Γk(β) (γ) q,k Γk(αn + β)γ(δ + n) zn. Now we define the function Q,δ k,α,β (z) by (3.11) Q Γk(α + β)(δ) (z) = (γ) q,k Then equation (3.11) implies ( (E ) (γ) ) k. Γk(β) (3.12) Q,δ k,α,β (z) = z + (γ) nq,k Γk(α + β)γ(δ + 1) (γ) q,k Γk(αn + β)γ(δ + n) zn. z Let φ(z) = ( ) M. Denote L k,αβ,δ (φ)(z) : M M the operator is defined 1 z by (3.13) L (φ)(z) = Q,δ k,α,β (z) φ(z), where the symbol (*) sts for Hadamard product (or convolution). Now applying Hadamard product using the equations (2.10), (3.12) (3.13) we obtained the desired result. Remark 3.1. Note that, Q,δ Γk(β) k,α,β (z) = ze (γ) (z), k (z U). Corollary 3.8. If we set the values of γ = q = k = β = δ = 1 α = 1 in equation (3.8). Let the condition of Theorem (3.7) be satisfied, then the reduced form is, L 1,1 1,1,1,1 (φ)(z) = z + 1 n! zn = e z 1 Corollary 3.9. If we keep γ = q = k = β = 1, δ = 2 α = 0 in equation (3.8). Let the condition of Theorem (3.7) be satisfied, then the reduced form is, L 1,1 1,0,1,2 (φ)(z) = z + 2 2log(1 z) ( n + 1 )zn = 2 z

86 H. Rehman, M. Darus J. Salah Corollary 3.10. If we put γ = k = β = 1 q = 0, δ = α = 0 in equation (3.8). Let the condition of Theorem (3.7) be satisfied, then the reduced form is, L 1,0 1,0,1,0 (φ)(z) = z + 1 Γ(n) zn = ze z Corollary 3.11. If we put γ = k = q = β = 1, δ = α = 0 in equation (3.8). Let the condition of Theorem (3.7) be satisfied, then the reduced form is, L 1,1 1,0,1,0 (φ)(z) = z + nz n (z 2) = z (z 1) 2 z2 Motivated by the work of Bansal Prajapat [7] also following the results of Raducanu [6], we investigate the ratio of K Mittaq-Leffler function Q (z) defined by (3.5) to its sequence of partial sums (Q ) 0(z) = z (Q ) m(z) = z + z n+1, m N, where = (γ) nq,kγk(β)γ(δ + 1), (α, β, δ > 0). (γ) q,k Γk(αn + β)γ(δ + n) The lower bounds we obtained on ratio like Q R (z) } (Q (Q )m(z), R )m(z) } Q (z), R Q γ,q (z) } (Q (Q, R ) m(z) ) m(z) (Q γ,q )m(z) }. 4 Ratio of normalized K Mittag-Leffler function In order to verify our results we require the following Lemma. Lemma 4.1. Let α 1, γ 1, δ 1. Then the function Q the two inequalities enlisted below; (4.1) (4.2) Q (z) β 2 δ + β 2 + 2βδ βγ + β + δ + 1 β 2 δ + β 2, z U + βδ βγ Q (z) (β 2 δ + β 2 βγ + 4βδ + 3β γ + 3δ + 2) β 2 δ + β 2, z U + βδ βγ (z) satisfies Proof. By using hypothesis that, Γ(αn + β) Γk(αn + β) so we can write, (4.3) (γ) nq,k Γk(β)Γ(δ + 1) (γ) q,k Γk(αn + β)γ(δ + n) (γ) nq,kγk(β)γ(δ + 1) (γ) q,k Γk(n + β)γ(δ + n) = (γ) n(δ) (γ)(β) n (δ) n, n N,

The generalized K M L function ratio to its sequence of partial sums 87 therefore, for z U picking equation (3.5) using (4.3) a note followed by equation (2.3) we have, (4.4) Q (z) = z + (γ) nq,k Γk(β)Γ(δ + 1) (γ) q,k Γk(αn + β)γ(δ + n) zn+1 (γ) nq,k Γk(β)Γ(δ + 1) 1 + (γ) q,k Γk(αn + β)γ(δ + n) 1 + (γ) n (δ) (γ)(β) n (δ) n 1 + δ (γ) n γ (β) n (δ) n = 1 + 1 (γ + 1) n 1 β (β + 1) n 1 (δ + 1) n 1 1 + 1 (γ + 1) n 1 β (β + 1) n 1 (δ + 1) n 1 = 1 + 1 } n (γ + 1), for (γ + 1) β (β + 1)(δ + 1) (β + 1)(δ + 1) < 1 1 + 1 ( ) (β + 1)(δ + 1) β βδ + β + δ γ + 2 β2 δ + β 2 + 2βδ βγ + β + δ + 1 β 2 δ + β 2 + βδ βγ hence the inequality in (4.1) is proved. Using the derivative of equation (3.5) once more the triangle inequality, for z U, we obtain Q (z) = 1 + (n + 1)(γ) nq,k Γk(β)Γ(δ + 1) (γ) q,k Γk(αn + β)γ(δ + n) zn n(γ) nq,k Γk(β)Γ(γ + 1) (4.5) 1 + (γ) q,k Γk(αn + β)γ(δ + n) + (γ) nq,k Γk(β)Γ(γ + 1) (γ) q,k Γk(αn + β)γ(δ + n). For β 1, δ 1 γ 1 we obtain (4.6) n(γ) n Γ(β)(δ) = n(γ) n(δ) (γ)γ(n + β)(δ) n γ(β) n (δ) n n(γ + 1) n 1 = β(β + 1) n 1 (δ + 1) n 1 n(γ + 1) n 2 (γ + n 1) = β(β + 1) n 2 (β + n 1)(δ + 1) n 2 (δ + n 1) (γ + 1) n 2. β(β + 1) n 2 (δ + 1) n 2 Taking into account, inequalities (4.6), (4.7) a note followed by equation (2.3) we

88 H. Rehman, M. Darus J. Salah have, (4.7) Q (z) = 1 + 1 + n(γ) n Γ(β)Γ(δ + 1) (γ)γ(n + β)γ(δ + n) + (γ) n Γ(β)Γ(δ + 1) (γ)γ(n + β)γ(δ + n) (γ) n (δ) γ(β) n (δ) n n(γ) n (δ) γ(β) n (δ) n + 1 + 1 β + 1 (γ + 1) n 2 + 1 (γ + 1) n 1 β (β + 1) n 2 (δ + 1) n 2 β (β + 1) n 1 (δ + 1) n 1 1 + 1 β + 1 ( ) n (γ + 1) + 1 ( ) n (γ + 1) β (β + 1)(δ + 1) β (β + 1)(δ + 1) 1 + 1 β + 2 ( ) (β + 1)(δ + 1) β δβ + β + δ + γ + 2 (β2 δ + β 2 βγ + 4βδ + 3β γ + 3δ + 2) β 2 δ + β 2 + βδ βγ hence the inequality in (4.2) is proved. ( ) 1 + u(z) In the sequel we involve a well-known result R > 0, z U if only 1 u(z) if u(z) < 1 u(z) be analytic function in U. We noted in the paper of Silverman [9, page 223, theorem.1] to set so that, u(z) = (A(z) B(z)) (2 + A(z) + B(z)). (1 + A(z)) (1 + u(z)) = (1 + B(z)) (1 u(z)), Theorem 4.2. Let α, q, k, δ} 1 β (γ + 1) + ( γ 1) 2 + 4(δ + 1) 2. Then 2(δ + 1) Q (4.8) R (z) } (Q ) β2 δ + β 2 βγ β δ 1 m(z) β 2 δ + β 2 + βδ βγ (Q (4.9) R ) } m(z) β 2 δ + β 2 βγ + βδ Q (z) β 2 δ + β 2 βγ + 2βδ + β + δ + 1 Proof. Using equation (4.1) of Lemma (4.1) we can write where 1 + β2 δ + β 2 + 2βδ βγ + β + δ + 1 β 2 δ + β 2, + βδ βγ = (γ) nq,kγk(β)γ(δ + 1), (α, β, δ > 0). (γ) q,k Γk(αn + β)γ(δ + n)

The generalized K M L function ratio to its sequence of partial sums 89 The above inequality is equivalent to β 2 δ + β 2 + βδ βγ βδ + β + δ + 1 1. In order to prove our result inequality (4.8), we consider u(z) defined by β 2 δ + β 2 + βδ βγ (Q )(z) } βδ + β + δ + 1 (Q ) β2 δ + β 2 βγ β δ 1 (1 + u(z)) = m(z) βδ + β + δ + 1 (1 u(z)) For the sake of simplicity let ψ(β, δ, γ) = β2 δ + β 2 + βδ βγ βδ + β + δ + 1 (4.10) ξ(β, δ, γ) = β2 δ + β 2 βγ β δ 1 βδ + β + δ + 1 (1 + u(z)) (1 u(z)) = 1 + z n + ψ(β, δ, γ) 1 + z n, z n where the value of, ψ(β, δ, γ) u(z) = 2 + 2 z n + ψ(β, δ, γ) ψ(β, δ, γ) u(z) < 2 2 ψ(β, δ, γ) z n. The inequality u(z) < 1 holds if only if 2ψ(β, δ, γ) 2 2, which is equivalent to (4.11) + ψ(β, δ, γ) 1.

90 H. Rehman, M. Darus J. Salah To verify (4.11) it is sufficient to show that its left-h side is bounded above by which is equivalent to ψ(β, δ, γ) ξ(β, δ, γ) 0. The last inequality holds true for β (γ + 1) + ( γ 1) 2 + 4(δ + 1) 2 ; δ 1. 2(δ + 1) In a similar method we prove the second inequality (4.9) of our theorem. Consider the function u(z) given by β 2 δ + β 2 + 2βδ βγ + β + δ + 1 (Q ) } m(z) βδ + β + δ + 1 (Q )(z) β2 δ + β 2 βγ + βδ βδ + β + δ + 1 Again for the sake of simplicity we put, = (1 + u(z)) (1 u(z)) Θ(β, δ, γ) = β2 δ + β 2 + 2βδ βγ + β + δ + 1, βδ + β + δ + 1 (β, δ, γ) = β2 δ + β 2 βγ + βδ βδ + β + δ + 1 (4.12) where the value of, (1 + u(z)) (1 u(z)) = u(z) = 2 + 2 1 + z n + Θ(β, δ, γ) 1 + Θ(β, δ, γ) z n, z n Θ(β, δ, γ) z n z n Θ(β, δ, γ) u(z) < 2 2 Θ(β, δ, γ).

The generalized K M L function ratio to its sequence of partial sums 91 The inequality u(z) < 1 holds if only if (4.13) + Θ(β, δ, γ) Since the left-h side of (4.13) is bounded above by, which is equivalent to Θ(β, δ, γ) (4.14) (β, δ, γ), 0. 1 And hence the inequality (4.9) holds true for β (γ + 1) + ( γ 1) 2 + 4(δ + 1) 2 ; 2(δ + 1) if α, q, k, δ} 1. Corollary 4.3. If we put γ 1, δ 1 β 1 + 5, then the inequalities in 2 (4.8) (4.9) holds true which is in fact the result given by Raducanu [6, page 3, theorem.2.1]. Theorem 4.4. Let α 1, q 1, k 1, β H(γ, δ) where H(γ, δ) = (γ + 2δ + 3) + ( (γ + 2δ + 3)) 2 4(δ + 1)(γ 3δ 2) ; δ 1, 2δ + 2 Then (4.15) R Q, (z) } (Q β2 δ + β 2 βγ 2βδ 3β + γ 3δ 2 ) m(z) β 2 δ + β 2 + βδ βγ } (Q (4.16) R ) m(z) β 2 δ + β 2 βγ + βδ Q, (z) β 2 δ + β 2 βγ + 4βδ + 3β γ + 3δ + 2 Proof. From (4.2) making the use of (4.5) we can write where 1 + (β2 δ + β 2 βγ + 4βδ + 3β γ + 3δ + 2) β 2 δ + β 2, + βδ βγ = (γ) nq,kγk(β)γ(δ + 1), (α, β, δ > 0). (γ) q,k Γk(αn + β)γ(δ + n) The above inequality is equivalent to β 2 δ + β 2 + βδ βγ 3βδ + 3β + 3δ γ + 2 1

92 H. Rehman, M. Darus J. Salah In order to prove our result inequality (4.15), define a function u(z) by β 2 δ + β 2 + βδ βγ 3βδ + 3β + 3δ γ + 2 For the sake of convenience suppose which produces (Q )(z) } (Q ) β2 δ + β 2 βγ 2βδ 3β + γ 3δ 2 m(z) 3βδ + 3β + 3δ γ + 2 Λ(β, δ, γ) = = (1 + u(z)) (1 u(z)) β2 δ + β 2 + βδ βγ 3βδ + 3β + 3δ γ + 2 Υ(β, δ, γ) = β2 δ + β 2 βγ 2βδ 3β + γ 3δ 2 3βδ + 3β + 3δ γ + 2 (4.17) (1 + u(z)) (1 u(z)) = 1 + z n + Λ(β, δ, γ) 1 + z n, z n where the value of, Λ(β, δ, γ) u(z) = 2 + 2 z n + Λ(β, δ, γ) Λ(β, δ, γ) u(z) = 2 2 z n Λ(β, δ, γ) the provision u(z) < 1 is valid if only if z n z n (4.18) (n + 1) + Λ(α, β) (n + 1) 1. The left-h side of the (4.18) is bounded above by Λ(β, δ, γ) (n + 1),

The generalized K M L function ratio to its sequence of partial sums 93 if which holds true for Υ(β, δ, γ) (n + 1) 0 β (γ + 2δ + 3) + ( (γ + 2δ + 3)) 2 4(δ + 1)(γ 3δ 2) ; δ 1. 2δ + 2 The proof of (4.16) follows the same pattern. For this purpose consider the function u(z) given by where, where the value of, Ω(β, δ, γ) Q, (z) } (1 + u(z)) (Q Φ(β, δ, γ) = ) m(z) (1 u(z)) Ω(β, δγ) = β2 δ + β 2 βγ + 4βδ + 3β γ + 3δ + 2 3βδ + 3β γ 3δ + 2 u(z) = u(z) < Φ(β, δ, γ) = 2 + 2 β2 δ + β 2 βγ + βδ 3βδ + 3β γ 3δ + 2 Ω(β, δ, γ) z n Ω(β, δ, γ) 2 2 Ω(β, δ, γ) Ω(β, δ, γ) The inequality u(z) < 1 holds if only if z n. (4.19) + Ω(β, δ, γ) 1. Since the left-h side of (4.19) is bounded above by, Ω(β, δ, γ), which is equivalent to Φ(β, δ, γ) 0,

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