Hindawi Publishing Corporation Abstract and Applied Analysis Volume 2013, Article ID 634739, 8 pages http://dx.doi.org/10.1155/2013/634739 Research Article Complex Oscillation of Higher-Order Linear Differential Equations with Coefficients Being Lacunary Series of Finite Iterated Order Jin Tu,1 Hong-Yan Xu,2 Hua-ming Liu,3 and Yong Liu4,5 1 College of Mathematics and Information Science, Jiangxi Normal University, Nanchang 330022, China Department of Informatics and Engineering, Jingdezhen Ceramic Institute, Jingdezhen, Jiangxi 333403, China 3 School of Sciences, Jiangxi Agricultural University, Nanchang 330045, China 4 Department of Mathematics, Shaoxing College of Arts and Sciences, Shaoxing, Zhejiang 312000, China 5 Department of Physics and Mathematics, University of Eastern Finland, P.O. Box 111, 80101 Joensuu, Finland 2 Correspondence should be addressed to Jin Tu; tujin2008@sina.com Received 18 January 2013; Accepted 12 April 2013 Academic Editor: Micah Osilike Copyright © 2013 Jin Tu 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. The authors introduce the lacunary series of finite iterated order and use them to investigate the growth of solutions of higher-order linear differential equations with entire coefficients of finite iterated order and obtain some results which improve and extend some previous results of Belaidi, 2006, Cao and Yi, 2007, Kinnunen, 1998, Laine and Wu, 2000, Tu and Chen, 2009, Tu and Deng, 2008, Tu and Deng, 2010, Tu and Liu, 2009, and Tu and Long, 2009. 1. Definitions and Notations In this paper, we assume that readers are familiar with the fundamental results and standard notations of the Nevanlinna theory of meromorphic functions (see [1–3]). In order to describe the growth of order of entire functions or meromorphic functions more precisely, we first introduce some notations about finite iterated order. Let us define inductively, for π ∈ (0, +∞), exp1 π = ππ and expπ+1 π = exp(expπ π), π ∈ N. For all sufficiently large π, we define log1 π = log π and logπ+1 π = log(logπ π), π ∈ N. We also denote exp0 π = π = log0 π and exp−1 π = log1 π. Moreover, we denote the logarithmic measure of a set πΈ ⊂ (0, +∞) by ππ πΈ = ∫πΈ ππ‘/π‘, and the upper logarithmic density of πΈ ⊂ (0, +∞) is defined by log dens πΈ = lim π→∞ ππ (πΈ β [1, π]) . log π (1) Throughout this paper, we use π to denote a positive integer. In the following, we recall some definitions of entire functions or meromorphic functions of finite iterated order (see [4– 10]). Definition 1. The π-iterated order of a meromorphic function π(π§) is defined by ππ (π) = lim π→∞ logπ π (π, π) log π . (2) Remark 2. If π(π§) is an entire function, then the π-iterated order of π(π§) is defined by ππ (π) = lim logπ π (π, π) π→∞ log π = lim π→∞ logπ+1 π (π, π) log π . (3) If π = 1, the classical growth of order of π(π§) is defined by π (π) = lim π→∞ log π (π, π) log2 π (π, π) = lim . π → ∞ log π log π (4) If π = 2, the hyperorder of π(π§) is defined by π2 (π) = lim π→∞ log3 π (π, π) log2 π (π, π) = lim . π→∞ log π log π (5) 2 Abstract and Applied Analysis Definition 3. If π(π§) is an entire function with 0 < ππ (π) = π < ∞, then the π-iterated type of π(π§) is defined by logπ π (π, π) (6) . ππ Definition 4. The π-iterated lower order of an entire function π(π§) is defined by ππ (π) = lim π→∞ logπ π (π, π) ππ (π) = lim log π π→∞ = lim logπ+1 π (π, π) log π π→∞ . (7) Definition 5. The finiteness degree of the iterated order of a meromorphic function π(π§) is defined by π (π) 0 for π (π§) rational, { { { { { min {π ∈ N : ππ (π) < ∞} { (8) { ={ for π transcendental for which some { { { π ∈ N with ππ (π) < ∞ exists, { { { or π (π§) with ππ (π) = ∞ ∀π ∈ N. {∞ Definition 6. The π-iterated exponent of convergence of πpoint of a meromorphic function π(π§) is defined by π π (π, π) = lim π→∞ logπ π (π, π) logπ π (π, π) = lim log π log π π→∞ . (9) If π = 0, the π-iterated exponent of convergence of zero-sequence and distinct zero-sequence of a meromorphic function π(π§) are defined, respectively, by π π (π) = lim logπ π (π, 1/π) log π π→∞ ππ (π) = lim logπ π (π, 1/π) log π π→∞ = lim logπ π (π, 1/π) log π π→∞ = lim logπ π (π, 1/π) log π π→∞ . The π-iterated lower exponent of convergence of zerosequence and distinct zero-sequence of a meromorphic function π(π§) are defined, respectively, by π→∞ ππ (π) = lim π→∞ logπ π (π, 1/π) log π logπ π (π, 1/π) log π = lim logπ π (π, 1/π) π→∞ = lim log π logπ π (π, 1/π) π→∞ log π Theorem B (see [8]). Let π΄ 0 (π§), . . . , π΄ π−1 (π§) be entire functions and let π(π΄ 0 ) = π. If π(π΄ π ) < π or ππ (π΄ π ) < ππ (π΄ 0 ) for all π = 1, . . . , π − 1, then π(π) = π + 1 and ππ+1 (π) = ππ (π΄ 0 ) hold for all nontrivial solutions of (12). Theorem C (see [4, 12]). Let π΄ 0 (π§), . . . , π΄ π−1 (π§) be entire functions and let π(π΄ 0 ) = π. Assume that max{ππ (π΄ π ) : π = 1, . . . , π − 1} ≤ ππ (π΄ 0 ) (> 0) and max{ππ (π΄ π ) : ππ (π΄ π ) = ππ (π΄ 0 )} < ππ (π΄ 0 ). Then, every solution π(π§) ≡ΜΈ 0 of (12) satisfies π(π) = π + 1 and ππ+1 (π) = ππ (π΄ 0 ). Theorem D (see [10]). Let π΄ 0 (π§), . . . , π΄ π−1 (π§) be entire functions of finite iterated order satisfying π(π΄ 0 ) = π, ππ (π΄ 0 ) = π, and limπ → ∞ (∑π−1 π=1 π(π, π΄ π )/π(π, π΄ 0 )) < 1. Then, every nontrivial solution π(π§) of (12) satisfies ππ+1 (π) = ππ (π΄ 0 ) = π. Theorem E (see [10]). Let π΄ 0 (π§), . . . , π΄ π−1 (π§) be entire functions of finite iterated order satisfying max{ππ (π΄ π ), π =ΜΈ 0} < ππ (π΄ 0 ) = ππ (π΄ 0 ) and limπ → ∞ (∑π−1 π=1 π(π, π΄ π )/π(π, π΄ 0 )) < 1 (π ∉ πΈ), where πΈ is a set of π of finite linear measure, then every nontrivial solution π(π§) of (12) satisfies ππ+1 (π) = ππ (π΄ 0 ) = ππ (π΄ 0 ). Theorem F (see [5]). Let π΄ π (π§) (π = 0, . . . , π − 1) be entire functions of finite iterated order such that there exists one transcendental π΄ π (0 ≤ π ≤ π − 1) satisfying ππ (π΄ π ) ≤ ππ (π΄ π ) < ∞ for all π =ΜΈ π , then (12) has at least one solution π(π§) that satisfies π(π) = π + 1 and ππ+1 (π) = ππ (π΄ π ). , (10) ππ (π) = lim Theorem A (see [8]). Let π΄ 0 (π§), . . . , π΄ π−1 (π§) be entire functions, if π(π΄ π ) ≤ π (π = 0, . . . , π − 1), then π(π) ≤ π + 1 and ππ+1 (π) ≤ max{ππ (π΄ π ), π = 0, . . . , π − 1} hold for all solutions of (12). , . (11) 2. Introductions and Main Results In the past ten years, many authors have investigated the complex oscillation properties of the higher-order linear differential equations π(π) + π΄ π−1 (π§) π(π−1) + ⋅ ⋅ ⋅ + π΄ 0 (π§) π = 0, (12) π(π) + π΄ π−1 (π§) π(π−1) + ⋅ ⋅ ⋅ + π΄ 0 (π§) π = πΉ (π§) (13) with π΄ π (π§) (π = 0, . . . , π − 1), πΉ(π§) being entire functions or meromorphic functions of fast growing (e.g., see [4–12]), and obtained the following results. Remark 7. Theorems B–E are investigating the growth of solutions of (12) when the coefficients are of finite iterated order and π΄ 0 (π§) grows faster than other coefficients in (12). What can we have if there exists one middle coefficient π΄ π (π§) (1 ≤ π ≤ π−1) such that π΄ π (π§) grows faster than other coefficients in (12) or (13)? Many authors have investigated this question when π΄ π (π§) is of finite order and obtained many results (e.g., see [13–15]). Here, our question is that under what conditions can we obtain similar results with Theorems B-C if π΄ π (π§) (1 ≤ π ≤ π − 1) is of finite iterated order and grows faster than other coefficients in (12) or (13). In 2009, Tu and Liu make use of the proposition of lacunary power series to investigate the above question in the case π = 1 and obtain the following result. Theorem G (see [15]). Let π΄ π (π§) (π = 0, . . . , π − 1), πΉ(π§) be entire functions satisfying max{π(π΄ π ), π =ΜΈ π, π(πΉ)} < ππ π(π΄ π ) < ∞ (1 ≤ π ≤ π−1). Suppose that π΄ π (π§) = ∑∞ π=0 ππ π π§ is an entire function of regular growth such that the sequence of exponents {π π } satisfies Fabry gap condition ππ σ³¨→ ∞ π (π σ³¨→ ∞) , (14) Abstract and Applied Analysis 3 then one has (i) if πΉ(π§) ≡ 0, then every transcendental solution π(π§) of (13) satisfies π2 (π) = π(π΄ π ); (ii) if πΉ(π§) ≡ΜΈ 0, then every transcendental solution π(π§) of (13) satisfies π2 (π) = π 2 (π) = π2 (π) = π(π΄ π ). In this paper, we continue our research in this area and obtain the following results. Theorem 8. Let π΄ π (π§) (π = 0, . . . , π − 1), πΉ(π§) be entire functions of finite iterated order and satisfying 0 < max{ππ (π΄ π ), π =ΜΈ π} ≤ ππ (π΄ π ) < ∞ and max{ππ (π΄ π ) : ππ (π΄ π ) = ππ (π΄ π )} < ππ (π΄ π ) (0 ≤ π ≤ π − 1). Suppose ππ that π΄ π (π§) = ∑∞ is an entire function such that the π=0 ππ π π§ sequence of exponents {π π } satisfies ππ 2+π > (log π) π (π > 0, π ∈ N) , (15) for some π > 0, then one has (i) if ππ (πΉ) < ππ (π΄ π ) or ππ (πΉ) = ππ (π΄ π ) and ππ (πΉ) < ππ (π΄ π ), then every transcendental solution π(π§) of (13) satisfies ππ+1 (π) = ππ (π΄ π ); furthermore if πΉ(π§) ≡ΜΈ 0, then every transcendental solution π(π§) of (13) satisfies ππ+1 (π) = π π+1 (π) = ππ+1 (π) = ππ (π΄ π ); (ii) if ππ (πΉ) > ππ (π΄ π ) and ππ+1 (πΉ) ≤ ππ (π΄ π ), then all solutions of (13) satisfy ππ (π) ≥ ππ (πΉ) and ππ+1 (π) ≤ ππ (π΄ π ); (iii) if ππ+1 (πΉ) > ππ (π΄ π ), then all solutions of (13) satisfy ππ+1 (π) = ππ+1 (πΉ), and ππ+1 (π) = π π+1 (π) = ππ+1 (πΉ) holds for all solutions of (13) with at most one exceptional solution π0 satisfying π π+1 (π0 ) < ππ+1 (πΉ). ππ Remark 9. If π(π§) = ∑∞ π=0 ππ π π§ is an entire function of finite order and the sequence of exponents {π π } satisfies (14), then (18) in Lemma 15 holds for π(π§), but for entire functions of infinite order, (14) certainly does not imply (18) in Lemma 15 (see [8]); therefore, we need more stringent gap condition (15) which is sufficient and unnecessary for Theorem 8. Theorem 10. Let π΄ π (π§) (π = 0, . . . , π − 1), πΉ(π§) be entire functions of finite iterated order satisfying max{ππ (π΄ π ), π =ΜΈ π, ππ (πΉ)} < ππ (π΄ π ) = ππ (π΄ π ) = π < ∞ (0 ≤ π ≤ ππ π − 1). Suppose that π΄ π (π§) = ∑∞ π=0 ππ π π§ is an entire function such that the sequence of exponents {π π } satisfies gap condition (15), then every transcendental solution π(π§) of (13) satisfies ππ+1 (π) = ππ+1 (π) = π. Furthermore if πΉ(π§) ≡ΜΈ 0, then every transcendental solution π(π§) of (13) satisfies ππ+1 (π) = ππ+1 (π) = ππ+1 (π) = π π+1 (π) = π. Theorem 11. Let π΄ π (π§) (π = 0, . . . , π − 1), πΉ(π§) be entire functions satisfying max{ππ (π΄ π ), π =ΜΈ π} < ππ (π΄ π ) < ∞ (0 ≤ π ≤ π − 1). Suppose that π(π, π΄ π ) ∼ log π(π, π΄ π ) as π → ∞ outside a set of π of finite logarithmic measure, then one has (i) if ππ (πΉ) < ππ (π΄ π ), then every transcendental solution π(π§) of (13) satisfies ππ+1 (π) = ππ (π΄ π ); furthermore, if πΉ(π§) ≡ΜΈ 0, then every transcendental solution π(π§) of (13) satisfies ππ+1 (π) = π π+1 (π) = ππ+1 (π) = ππ (π΄ π ); (ii) if ππ (πΉ) > ππ (π΄ π ) and ππ+1 (πΉ) ≤ ππ (π΄ π ), then all solutions of (13) satisfy ππ (π) ≥ ππ (πΉ) and ππ+1 (π) ≤ ππ (π΄ π ); (iii) if ππ+1 (πΉ) > ππ (π΄ π ), then all solutions of (13) satisfy ππ+1 (π) = ππ+1 (πΉ), and ππ+1 (π) = π π+1 (π) = ππ+1 (πΉ) holds for all solutions of (13) with at most one exceptional solution π0 satisfying π π+1 (π0 ) < ππ+1 (πΉ); (iv) if ππ (π΄ π ) = ππ (π΄ π ) = π and πΉ(π§) ≡ΜΈ 0 and ππ (πΉ) < π, then every transcendental solution π(π§) of (13) satisfies ππ+1 (π) = ππ+1 (π) = ππ+1 (π) = π π+1 (π) = π. Remark 12. Theorem 10 implies that all the solutions of (13) are of regular growth if π΄ π is of regular growth under some conditions; Theorem 11 is an improvement of the Theorem in [14, page 2694] and Theorems 1-2 in [16, page 624]. In fact, by Lemma 15, the gap condition (15) in Theorem 8 implies that π(π, π΄ π ) ∼ log π(π, π΄ π ) as π → ∞ outside a set of π of finite logarithmic measure; therefore, Theorem 11 is a generalization of Theorem 8 in a sense, but the condition on π΄ π in Theorem 8 is more stringent than that in Theorem 11. In addition, Theorems 8–11 may have polynomial solutions of degree < π if π > 1. 3. Preliminary Lemmas Lemma 13 (see [17]). Let π(π§) be a transcendental meromorphic function, and let πΌ > 1 be a given constant, for any given constant and for any given π > 0, (i) there exist a constant π΅ > 0 and a set πΈ1 ⊂ (0, +∞) having finite logarithmic measure such that for all π§ satisfying |π§| = π ∉ πΈ1 , one has σ΅¨ σ΅¨σ΅¨ (π) σ΅¨σ΅¨ π (π§) σ΅¨σ΅¨σ΅¨ σ΅¨ σ΅¨σ΅¨ σ΅¨σ΅¨ π(π) (π§) σ΅¨σ΅¨σ΅¨ σ΅¨ σ΅¨ ≤ π΅[ π (πΌπ, π) πΌ (log π) log π (πΌπ, π)] π π−π (0 ≤ π < π) . (16) (ii) There exists a set π»1 ⊂ [0, 2π) that has linear measure zero a constant π΅ > 0 that depends only on πΌ, for any π ∈ [0, 2π) \ π»1 , there exists a constant π 0 = π 0 (π) > 1 such that for all π§ satisfying arg π§ = π and |π§| = π > π 0 , one has σ΅¨ σ΅¨σ΅¨ (π) σ΅¨σ΅¨ π (π§) σ΅¨σ΅¨σ΅¨ σ΅¨ σ΅¨σ΅¨ σ΅¨σ΅¨ π(π) (π§) σ΅¨σ΅¨σ΅¨ σ΅¨ σ΅¨ ≤ π΅[π (πΌπ, π) log π (πΌπ, π)] (17) π−π (0 ≤ π < π) . Remark 14. Throughout this paper, we use πΈ1 ⊂ (0, ∞) to denote a set having finite logarithmic measure or finite linear measure, not always the same at each occurrence. 4 Abstract and Applied Analysis ππ Lemma 15 (see [18]). Let π(π§) = ∑∞ be an entire π=0 ππ π π§ function and the sequence of exponents {π π } satisfies the gap condition (15). Then for any given π > 0, log πΏ (π, π) > (1 − π) log π (π, π) (18) holds outside a set of finite logarithmic measure, where π(π, π) = sup|π(π§)|, πΏ(π, π) = inf |π(π§)|. |π§|=π |π§|=π Lemma 16 (see [4]). Let π(π§) be an entire function of finite iterated order satisfying 0 < ππ (π) = π < ∞ and ππ (π) = π > 0, then for any given π½ < π, there exists a set πΈ2 ⊂ (0, +∞) having infinite logarithmic measure such that for all π ∈ πΈ2 , one has π (π, π) > expπ {π½ππ } . (19) ππ be an entire function of Lemma 17. Let π(π§) = ∑∞ π=0 ππ π π§ finite iterated order satisfying 0 < ππ (π) = π < ∞ and ππ (π) = π > 0 such that the sequence of exponents {π π } satisfies the gap condition (15). Then, for any given π½ > π, there exists a set πΈ3 ⊂ (0, +∞) having infinite logarithmic measure such that for all |π§| = π ∈ πΈ3 , one has σ΅¨ σ΅¨σ΅¨ π σ΅¨σ΅¨π (π§)σ΅¨σ΅¨σ΅¨ > expπ {π½π } . (20) Proof. By Lemma 15, for any given π > 0, we have (1−π) σ΅¨ σ΅¨σ΅¨ , σ΅¨σ΅¨π (π§)σ΅¨σ΅¨σ΅¨ ≥ πΏ (π, π) > π(π, π) (π ∉ πΈ1 ) . Lemma 21 (see [2]). Let π : (0, +∞) → π , β : (0, +∞) → π be monotone increasing functions such that (i) π(π) ≤ β(π) outside of an exceptional set of finite linear measure. Then, for any πΌ > 1, there exists π0 > 0 such that π(π) ≤ β(πΌπ) for all π > π0 . (ii) π(π) ≤ β(π) outside of an exceptional set of finite logarithmic measure. Then, for any πΌ > 1, there exists π0 > 0 such that π(π) ≤ β(ππΌ ) for all π > π0 . Lemma 22 (see [19]). Let π(π§) be an entire function of finite iterated order satisfying ππ (π) = π < ∞. Then, for any given π > 0, there exists a set πΈ4 ⊂ (0, +∞) having infinite logarithmic measure such that for all π ∈ πΈ4 , one has π (π, π) < expπ {ππ+π } . (24) Lemma 23 (see [2, 20]). Let π(π§) be a transcendental entire function, let 0 < π1 < 1/4 and π§π a point such that |π§π | = π and that |π(π§π )| > π(π, π)]π (π)−(1/4)+π1 holds. Then, there exists a set πΈ1 ⊂ (0, +∞) of finite logarithmic measure such that π (21) For any given π½ < π, we can choose π½1 and sufficiently small π > 0 such that π½ < π½1 < π and π½ < (1 − π)π½1 < π; by Lemma 16, there exists a set πΈ2 ⊂ (0, +∞) having infinite logarithmic measure such that for all |π§| = π ∈ πΈ2 \ πΈ1 , we have (1−π) σ΅¨ σ΅¨σ΅¨ σ΅¨σ΅¨π (π§)σ΅¨σ΅¨σ΅¨ > π(π, π) (22) (1−π) > (expπ {π½1 ππ }) > expπ {π½ππ } , where πΈ3 = πΈ2\πΈ1 is a set having infinite logarithmic measure. Lemma 18 (see [13]). Let π(π§) be a transcendental entire function. Then, there is a set πΈ1 ⊂ (0, +∞) having finite logarithmic measure such that for all π§ satisfying |π§| = π ∉ πΈ1 and |π(π§)| = π(π, π), one has σ΅¨ σ΅¨σ΅¨ σ΅¨σ΅¨ π (π§) σ΅¨σ΅¨σ΅¨ π σ΅¨ σ΅¨σ΅¨ (23) σ΅¨σ΅¨ π(π) (π§) σ΅¨σ΅¨σ΅¨ ≤ 2π , (π ∈ N) . σ΅¨ σ΅¨ Lemma 19 (see [7, 9, 10]). Let π΄ 0 (π§), . . . , π΄ π−1 (π§), πΉ(π§) ≡ΜΈ 0 be meromorphic functions, and let π(π§) be a meromorphic solution of (13) satisfying one of the following conditions: (i) max{π(πΉ) = π, π(π΄ π )(π = 0, . . . , π − 1)} < π(π) = π + 1 (π, π ∈ N); (ii) π = max{ππ+1 (πΉ), ππ+1 (π΄ π )(π = 0, . . . , π − 1)} < ππ+1 (π), then ππ+1 (π) = π π+1 (π) = ππ+1 (π). Lemma 20 (see [8]). Let π΄ 0 (π§), . . . , π΄ π−1 (π§), πΉ(π§) be entire functions of finite iterated order, if π(π΄ π ) ≤ π, π(πΉ) ≤ π (π = 0, . . . , π − 1). Then ππ+1 (π) ≤ max{ππ (π΄ π ), ππ (πΉ), π = 0, . . . , π − 1} holds for all solutions of (13). ]π (π) π(π) (π§π ) ) (1 + π (1)) =( π§π π (π§π ) (25) holds for all π ∈ N and all π ∉ πΈ1 , where ]π (π) is the central index of π(π§). Lemma 24 (see [7, 9]). Let π(π§) be an entire function of finite iterated order satisfying ππ (π) = π, ππ (π) = π, π, π ∈ N. Then, one has lim π→∞ lim π→∞ logπ ]π (π) log π logπ ]π (π) log π = π, (26) = π. Lemma 25. Let π΄ π (π§) (π = 0, . . . , π − 1), πΉ(π§) be entire functions of finite iterated order satisfying max{ππ (π΄ π ), π =ΜΈ π, ππ (πΉ)} ≤ ππ (π΄ π ) < ∞. Then, every solution π(π§) of (13) satisfies ππ+1 (π) ≤ ππ (π΄ π ). Proof. By (13), we have σ΅¨σ΅¨ (π) σ΅¨σ΅¨ σ΅¨σ΅¨ σ΅¨ π(π−1) σ΅¨σ΅¨σ΅¨ σ΅¨σ΅¨ π σ΅¨σ΅¨ σ΅¨σ΅¨ σ΅¨σ΅¨ σ΅¨σ΅¨ ≤ σ΅¨σ΅¨π΄ π−1 σ΅¨σ΅¨ σ΅¨σ΅¨ π σ΅¨σ΅¨ σ΅¨σ΅¨ π σ΅¨σ΅¨σ΅¨ σ΅¨ σ΅¨ σ΅¨ (27) σ΅¨σ΅¨ σ΅¨ σ΅¨σ΅¨ πσΈ σ΅¨σ΅¨σ΅¨ σ΅¨σ΅¨ σ΅¨σ΅¨ σ΅¨σ΅¨σ΅¨σ΅¨ πΉ (π§) σ΅¨σ΅¨σ΅¨σ΅¨ + ⋅ ⋅ ⋅ + σ΅¨σ΅¨σ΅¨π΄ 1 σ΅¨σ΅¨σ΅¨ + σ΅¨σ΅¨π΄ 0 σ΅¨σ΅¨ + σ΅¨σ΅¨ σ΅¨. σ΅¨σ΅¨ π (π§) σ΅¨σ΅¨σ΅¨ σ΅¨σ΅¨ π σ΅¨σ΅¨ By Lemma 23, there exists a set πΈ1 having finite logarithmic measure such that for all |π§| = π ∉ πΈ1 and |π(π§)| = π(π, π), we have ]π (π) π π(π) (π§) =( ) (1 + π (1)) , π (π§) π§ (π ∈ N) . (28) Abstract and Applied Analysis 5 By Lemma 22, for any given π > 0, there exists a set πΈ4 having infinite logarithmic measure such that for all |π§| = π ∈ πΈ4 and |π(π§)| = π(π, π) > 1, we have σ΅¨ σ΅¨σ΅¨ π (π΄ )+π σ΅¨σ΅¨π΄ π (π§)σ΅¨σ΅¨σ΅¨ ≤ expπ {π π π } , σ΅¨σ΅¨σ΅¨π΄ (π§)σ΅¨σ΅¨σ΅¨ ≤ exp {πππ (π΄ π )+π } , σ΅¨σ΅¨ π σ΅¨σ΅¨ π σ΅¨σ΅¨ πΉ (π§) σ΅¨σ΅¨ ππ (π΄ π )+π σ΅¨σ΅¨ σ΅¨σ΅¨σ΅¨ }. σ΅¨σ΅¨ π (π§) σ΅¨σ΅¨σ΅¨ ≤ |πΉ (π§)| < expπ {π σ΅¨ σ΅¨ ]π (π) π (29) π ≤ (π + 1) ( π π−1 ) (30) (1 + π (1)) expπ {πππ (π΄ π )+π } . By (30) and Lemma 24, we have ππ+1 (π) ≤ Therefore, we complete the proof of Lemma 25. ππ (π΄ π ). Lemma 26. Let π΄ 0 , π΄ 1 , . . . , π΄ π−1 , πΉ ≡ΜΈ 0 be meromorphic functions of finite iterated order; if π is a meromorphic solution of the (13) and satisfies π = max{ππ+1 (πΉ), ππ+1 (π΄ π ), π = 0, . . . , π − 1} < ππ+1 (π), then ππ+1 (π) = ππ+1 (π) = ππ+1 (π). Proof. By (13), we have π(π−1) 1 1 π(π) = ( + π΄ π−1 + ⋅ ⋅ ⋅ + π΄ 0) . π πΉ π π (31) By (31), we get π (π, π−1 1 1 1 ) ≤ ππ (π, ) + π (π, ) + ∑ π (π, π΄ π ) . (32) π π πΉ π=0 (1 − π (1)) π (π, π) ≤ ππ (π, + π {log (ππ (π, π))} (33) 1 1 ) + π (π, ) π πΉ π−1 + ∑ π (π, π΄ π ) + π {log (ππ (π, π))} π=0 = ππ (π, π−1 1 ) + π (π, πΉ) + ∑ π (π, π΄ π ) π π=0 + π {log (ππ (π, π))} , (36) Lemma 27. Let π(π§) be a transcendental entire function, for each sufficiently large |π§| = π, and let π§π = πππππ be a point satisfying |π(π§π )| = π(π, π). Then, there exists a constant πΏπ (> 0) such that for all π§ satisfying |π§| = π ∉ πΈ1 and arg π§ = π ∈ [ππ − πΏπ , ππ + πΏπ ], one has ]π (π) π π(π) (π§) =( ) (1 + π (1)) π (π§) π§ (π ∈ N) . (37) Proof. If π§π = πππππ is a point satisfying |π(π§π )| = π(π, π), since |π(π§)| is continuous in |π§| = π, then there exists a constant πΏπ (> 0) such that for all π§ satisfying |π§| = π (large enough) and arg π§ = π ∈ [ππ − πΏπ , ππ + πΏπ ], we have σ΅¨ σ΅¨ σ΅¨σ΅¨σ΅¨σ΅¨ σ΅¨σ΅¨ σ΅¨σ΅¨σ΅¨σ΅¨π (π§)σ΅¨σ΅¨σ΅¨ − σ΅¨σ΅¨σ΅¨π (π§π )σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨ < π; σ΅¨ 1σ΅¨ σ΅¨ σ΅¨ that is, σ΅¨σ΅¨σ΅¨π (π§)σ΅¨σ΅¨σ΅¨ > σ΅¨σ΅¨σ΅¨π (π§π )σ΅¨σ΅¨σ΅¨ 2 (38) 1 = π (π, π) 2 > π (π, π) ]π (π)−(1/4)+π1 . By Lemma 23, we have (π ∈ N) (39) holds for all π§ satisfying |π§| = π ∉ πΈ1 and arg π§ = π ∈ [ππ − πΏπ , ππ + πΏπ ]. 1 ) + π (1) π ≤ ππ (π, (π ∉ πΈ1 ) . ]π (π) π π(π) (π§) =( ) (1 + π (1)) , π (π§) π§ (π ∉ πΈ1 ) . By (32) and (33), we have π (π, π) = π (π, 1 ), π By Lemma 21 (i) and by (36), we have ππ+1 (π) = ππ+1 (π) = ππ+1 (π). π−1 1 1 ) ≤ π (π, ) + ∑ π (π, π΄ π ) π πΉ π=0 (35) log (ππ (π, π)) = π {π (π, π)} . By the lemma of logarithmic derivative and (31), we have π (π, π = 0, . . . , π − 1, By (34)-(35), we have ) (1 + π (1)) ]π (π) π (π, πΉ) = π {π (π, π)} , π (π, π΄ π ) = π {π (π, π)} , Hence from (27)–(29), for any given π > 0 and for all π§ satisfying |π§| = π ∈ πΈ4 \ πΈ1 and |π(π§)| = π(π, π), we have ( Since max{ππ+1 (πΉ), ππ+1 (π΄ π ), π = 0, 1, . . . , π − 1} < ππ+1 (π), for sufficiently large π, we have (π ∉ πΈ1 ) . (34) Lemma 28. Let π(π§) be a transcendental entire function, for each sufficiently large |π§| = π, and let π§π = πππππ be a point satisfying |π(π§π )| = π(π, π). Then, there exists a constant πΏπ (> 0) such that for all π§ satisfying |π§| = π ∉ πΈ1 and arg π§ = π ∈ [ππ − πΏπ , ππ + πΏπ ], one has σ΅¨σ΅¨ σ΅¨ σ΅¨σ΅¨ π (π§) σ΅¨σ΅¨σ΅¨ π σ΅¨σ΅¨ σ΅¨ σ΅¨σ΅¨ π(π) (π§) σ΅¨σ΅¨σ΅¨ ≤ 2π σ΅¨ σ΅¨ (π ∈ N) . (40) Proof. If π§π = πππππ is a point satisfying |π(π§π )| = π(π, π), then by Lemma 27 there exists a constant πΏπ (> 0) such that for all 6 Abstract and Applied Analysis π§ satisfying |π§| = π∉ πΈ1 and arg π§ = π ∈ [ππ − πΏπ , ππ + πΏπ ], we have ]π (π) π π(π) (π§) =( ) (1 + π (1)) . π (π§) π§ (41) Since π(π§) is transcendental, we have ]π (π) → ∞ (π → ∞). Hence by (41), for all π§ satisfying |π§| = π ∉ πΈ1 and arg π§ = π ∈ [ππ − πΏπ , ππ + πΏπ ], we have σ΅¨ σ΅¨σ΅¨ (π) σ΅¨σ΅¨ π (π§) σ΅¨σ΅¨σ΅¨ 1 −π σ΅¨ σ΅¨σ΅¨ σ΅¨σ΅¨ π (π§) σ΅¨σ΅¨σ΅¨ ≥ 2 π ; σ΅¨ σ΅¨ σ΅¨σ΅¨ σ΅¨ σ΅¨ π (π§) σ΅¨σ΅¨σ΅¨ σ΅¨σ΅¨ ≤ 2ππ that is, σ΅¨σ΅¨σ΅¨σ΅¨ (π) σ΅¨ σ΅¨σ΅¨ π (π§) σ΅¨σ΅¨ (42) (π ∈ N) . Lemma 29. Let π(π§) be an entire function of order 0 < ππ (π) = π < ∞. Then for any given π > 0, there exists a set πΈ5 ⊂ (0, +∞) with positive upper logarithmic density such that for all |π§| = π ∈ πΈ5 , one has π (π, π) > expπ {ππ−π } . (43) Proof. Since 0 < ππ (π) = π < ∞, then for any given π > 0, there exists an increasing sequence {ππ } tending to ∞ such that for π ≥ π4 , we have π (ππ , π) > expπ {πππ−(π/2) } . (44) Since π > 0, we can choose πΌ to satisfy 1 < πΌ < (π−(π/2))/(π− π). Then for all π ∈ [ππ , πππΌ ] (π ≥ π4 ), we have π (π, π) ≥ π (ππ , π) > expπ {πππ−(π/2) } ≥ expπ {π(π−(π/2))/πΌ } > expπ {ππ−π } . Setting πΈ5 = β π=π4 [ππ , πππΌ ], σ΅¨σ΅¨ σ΅¨ σ΅¨σ΅¨π (ππππ )σ΅¨σ΅¨σ΅¨ > π(π, π)1−π σ΅¨ σ΅¨ (π ∉ πΈ1 ) . (45) we have π (πΈ ∩ [1, π]) log dens πΈ5 = lim π 5 π→∞ log π ππ (πΈ5 ∩ [1, πππΌ ]) π→∞ log πππΌ ≥ lim (46) ππ ([ππ , πππΌ ]) πΌ − 1 = > 0. π→∞ log πππΌ πΌ Thus, Lemma 29 is proved. Lemma 30. Let π(π§) be a transcendental entire function satisfying 0 < ππ (π) = π < ∞ and π(π, π) ∼ log π(π, π) as π → ∞ outside a set π of finite logarithmic measure. Then for any given π > 0, there exists a set πΈ6 ⊂ (0, +∞) with positive upper logarithmic density and a set π»2 ⊂ [0, 2π) with linear measure zero such that for all π§ satisfying π ∈ πΈ6 and arg π§ = π ∈ [0, 2π) \ π»2 , one has σ΅¨σ΅¨ σ΅¨ σ΅¨σ΅¨π (ππππ )σ΅¨σ΅¨σ΅¨ > expπ {ππ−π } . σ΅¨ σ΅¨ (47) (49) By (48) and (49), for any given π > 0 and for all π§ satisfying |π§| = π ∈ πΈ6 \ πΈ1 and arg π§ = π ∈ [0, 2π) \ π»2 , we have 1−π σ΅¨σ΅¨ σ΅¨ σ΅¨σ΅¨π (ππππ )σ΅¨σ΅¨σ΅¨ > π(π, π)1−π > (expπ {ππ−(π/2) }) > expπ {ππ−π } . σ΅¨ σ΅¨ (50) Therefore, we complete the proof of Lemma 30. 4. Proofs of Theorems 8–11 Proof of Theorem 8. (i) Assume that π(π§) is a transcendental solution of (13). By (13), we have σ΅¨ (π) σ΅¨ σ΅¨ (π+1) σ΅¨σ΅¨ σ΅¨ σ΅¨ σ΅¨ σ΅¨σ΅¨ π σ΅¨σ΅¨ σ΅¨σ΅¨ σ΅¨σ΅¨σ΅¨σ΅¨ π σ΅¨σ΅¨σ΅¨σ΅¨ σ΅¨σ΅¨π΄ π σ΅¨σ΅¨ ≤ σ΅¨σ΅¨ (π) σ΅¨σ΅¨ + ⋅ ⋅ ⋅ + σ΅¨σ΅¨σ΅¨π΄ π+1 σ΅¨σ΅¨σ΅¨ σ΅¨σ΅¨σ΅¨σ΅¨ (π) σ΅¨σ΅¨σ΅¨σ΅¨ σ΅¨σ΅¨ π σ΅¨σ΅¨ σ΅¨σ΅¨ π σ΅¨σ΅¨ (51) σ΅¨σ΅¨ σ΅¨σ΅¨ (π−1) σ΅¨σ΅¨ σ΅¨ σ΅¨σ΅¨ πΉ σ΅¨σ΅¨ π σ΅¨σ΅¨ π σ΅¨σ΅¨σ΅¨ σ΅¨σ΅¨ σ΅¨ σ΅¨ σ΅¨ σ΅¨ σ΅¨ σ΅¨ σ΅¨ σ΅¨ σ΅¨ σ΅¨σ΅¨ + ⋅ ⋅ ⋅ + σ΅¨σ΅¨σ΅¨π΄ 0 σ΅¨σ΅¨σ΅¨ + σ΅¨σ΅¨σ΅¨ σ΅¨σ΅¨σ΅¨) . + σ΅¨σ΅¨σ΅¨ (π) σ΅¨σ΅¨σ΅¨ (σ΅¨σ΅¨π΄ π−1 σ΅¨σ΅¨σ΅¨ σ΅¨σ΅¨σ΅¨ σ΅¨σ΅¨ π σ΅¨σ΅¨ σ΅¨σ΅¨ π σ΅¨σ΅¨ σ΅¨σ΅¨ π σ΅¨σ΅¨σ΅¨ By Lemma 13 (i), there exists a set πΈ1 ⊂ [1, ∞) having finite logarithmic measure and a constant π΅ > 0 such that σ΅¨ σ΅¨σ΅¨ (π) σ΅¨σ΅¨ π (π§) σ΅¨σ΅¨σ΅¨ 2π σ΅¨ σ΅¨σ΅¨ σ΅¨σ΅¨ π(π) (π§) σ΅¨σ΅¨σ΅¨ ≤ π΅(π (2π, π)) , σ΅¨ σ΅¨ (0 ≤ π < π ≤ π) (52) holds for all |π§| = π ∉ πΈ1 and for sufficiently large π. Since max{ππ (π΄ π ), π =ΜΈ π, ππ (πΉ)} ≤ ππ (π΄ π ) and max{ππ (π΄ π ), ππ (πΉ) : ππ (π΄ π ) = ππ (π΄ π ) = ππ (πΉ)} < ππ (π΄ π ), we choose πΌ1 , π½1 to satisfy max{ππ (π΄ π ), π =ΜΈ π, ππ (πΉ)} < πΌ1 < π½1 < ππ (π΄ π ); by Lemma 17, there exists a set πΈ3 ⊂ (0, +∞) having infinite logarithmic measure such that for all π§ satisfying |π§| = π ∈ πΈ3 and for sufficiently large π, we have σ΅¨ σ΅¨σ΅¨ π (π΄ ) σ΅¨σ΅¨π΄ π (π§)σ΅¨σ΅¨σ΅¨ > expπ {π½1 π π π } , σ΅¨ σ΅¨σ΅¨ σ΅¨σ΅¨π΄ π (π§)σ΅¨σ΅¨σ΅¨ < expπ {πΌ1 πππ (π΄ π ) } , σ΅¨ σ΅¨ ≥ lim (48) By Lemma 29, for any given π > 0, there exists a set πΈ6 ⊂ (0, +∞) with positive upper logarithmic density, we have π (π, π) > expπ {ππ−(π/2) } . Therefore, we complete the proof of Lemma 28. ∞ Proof. Since π(π, π) ∼ log π(π, π) as π → ∞ (π ∉ πΈ1 ), then by the definition of π(π, π), there exists a set π»2 ⊂ [0, 2π) having linear measure zero such that for all π§ satisfying arg π§ = π ∈ [0, 2π) \ π»2 , we have π =ΜΈ π. (53) By Lemma 18, there exists a set πΈ1 ⊂ (0, +∞) having finite logarithmic measure such that for all π§ satisfying |π(π§)| = π(π, π) > 1 and |π§| = π ∉ πΈ1 , we have σ΅¨ σ΅¨σ΅¨ σ΅¨σ΅¨ π (π§) σ΅¨σ΅¨σ΅¨ π σ΅¨ σ΅¨σ΅¨ σ΅¨σ΅¨ π(π) (π§) σ΅¨σ΅¨σ΅¨ ≤ 2π , σ΅¨ σ΅¨ σ΅¨σ΅¨ πΉ (π§) σ΅¨σ΅¨ σ΅¨σ΅¨ σ΅¨σ΅¨ π (π΄ ) σ΅¨σ΅¨ σ΅¨σ΅¨ ≤ |πΉ (π§)| < expπ {πΌ1 π π π } . σ΅¨σ΅¨ π (π§) σ΅¨σ΅¨ (54) Abstract and Applied Analysis 7 Hence from (51)–(54), for all π§ satisfying |π§| = π ∈ πΈ3 \ πΈ1 and |π(π§)| = π(π, π), we have expπ {π½1 πππ (π΄ π ) } 2π ≤ 2π΅ (π + 1) ππ exp {πΌ1 πππ (π΄ π ) } [π (2π, π)] . (55) By (55), we have ππ+1 (π) = lim π→∞ logπ+1 π (π, π) ≥ ππ (π΄ π ) . log π (56) On the other hand, by Lemma 20, we have ππ+1 (π) ≤ ππ (π΄ π ). Therefore, every transcendental solution π(π§) of (13) satisfies ππ+1 (π) = ππ (π΄ π ). Furthermore if πΉ(π§) ≡ΜΈ 0, then by Lemma 19, we have that every transcendental solution π(π§) of (13) satisfies ππ+1 (π) = π π+1 (π) = ππ+1 (π) = ππ (π΄ π ). (ii) We assume that π is a solution of (13). By the elementary theory of differential equations, all the solutions of (13) are entire functions and have the form π = π∗ + πΆ1 π1 + πΆ2 π2 + ⋅ ⋅ ⋅ + πΆπ ππ , (57) where πΆ1 , . . . , πΆπ are complex constants, {π1 , . . . , ππ } is a solution base of (12), and π∗ is a solution of (13) and has the form π∗ = π·1 π1 + π·2 π2 + ⋅ ⋅ ⋅ + π·π ππ , (58) where π·1 , . . . , π·π are certain entire functions satisfying −1 π·πσΈ = πΉ ⋅ πΊπ (π1 , . . . , ππ ) ⋅ π(π1 , . . . , ππ ) (π = 1, . . . , π) , (59) where πΊπ (π1 , . . . , ππ ) are differential polynomials in π1 , . . . , ππ and their derivative with constant coefficients, and π(π1 , . . . , ππ ) is the Wronskian of π1 , . . . , ππ . By Theorem A, we have ππ+1 (ππ ) ≤ ππ (π΄ π ) (π = 1, 2, . . . , π); then by (57)–(59), we get ππ+1 (π) ≤ max {ππ+1 (ππ ) , ππ+1 (πΉ) , π = 1, . . . , π} ≤ ππ (π΄ π ) . (60) Since ππ (πΉ) > ππ (π΄ π ), it is easy to see that ππ (π) ≥ ππ (πΉ) by (13). (iii) Suppose that π is a solution of (13), it is easy to see that ππ+1 (π) ≥ ππ+1 (πΉ) by (13). On the other hand, since ππ+1 (πΉ) > ππ (π΄ π ) and by (57)–(59), we have ππ+1 (π) ≤ max {ππ+1 (ππ ) , ππ+1 (πΉ) , π = 1, . . . , π} ≤ ππ+1 (πΉ) . (61) Therefore, all solutions of (13) satisfy ππ+1 (π) = ππ+1 (πΉ). By the same proof in Theorem 4.2 in [8, page 401], we can obtain that all solutions of (13) satisfying ππ+1 (π) = π π+1 (π) = ππ+1 (πΉ) with at most one exceptional solution π0 satisfying π π+1 (π0 ) < ππ+1 (πΉ). Proof of Theorem 10. Suppose that π(π§) is a transcendental solution of (13), by the same proof in Theorem 8, we have ππ+1 (π) = ππ (π΄ π ) = π. Thus, it remains to show that ππ+1 (π) = ππ (π΄ π ) = π. We choose πΌ2 , π½2 to satisfy max {ππ (π΄ π ) , π =ΜΈ π, ππ (πΉ)} < πΌ2 < π½2 < π. (62) Since the sequence of exponents {π π } of π΄ π satisfies (15) and ππ (π΄ π ) = π, then by Lemma 15, there exists a set πΈ1 having finite logarithmic measure such that for all sufficiently large π ∉ πΈ1 , we have σ΅¨ σ΅¨σ΅¨ π½ σ΅¨σ΅¨π΄ π (π§)σ΅¨σ΅¨σ΅¨ ≥ expπ {π 2 } , σ΅¨σ΅¨ σ΅¨ σ΅¨σ΅¨π΄ π (π§)σ΅¨σ΅¨σ΅¨ ≤ expπ {ππΌ2 } , σ΅¨ σ΅¨ (63) π =ΜΈ π. Hence from (51), (52), (54), and (63), for all π§ satisfying |π§| = π ∉ πΈ1 and |π(π§)| = π(π, π), we have 2π expπ {ππ½2 } ≤ 2π΅ (π + 1) ππ expπ {ππΌ2 } [π (2π, π)] . (64) Since π½2 is arbitrarily close to π, by (64) and Lemma 21 (ii), we have ππ+1 (π) = lim logπ+1 π (π, π) π→∞ log π ≥ π. (65) On the other hand, by Lemma 26, we have ππ+1 (π) ≤ ππ (π΄ π ) = π; therefore, every transcendental solution of (13) satisfies ππ+1 (π) = π. Proof of Theorem 11. (i) By Lemma 20, we know that every solution of (13) satisfies ππ+1 (π) ≤ ππ (π΄ π ). In the following, we show that every transcendental solution π(π§) of (13) satisfies ππ+1 (π) ≥ ππ (π΄ π ). Suppose that π(π§) is a transcendental solution of (13). For each sufficiently large circle |π§| = π, we take a point π§π = πππππ satisfying |π(π§π )| = π(π, π). By Lemma 28, there exist a constant πΏπ > 0 and a set πΈ1 such that for all π§ satisfying |π§| = π ∉ πΈ1 and arg π§ = π ∈ [ππ − πΏπ , ππ + πΏπ ], we have σ΅¨σ΅¨ σ΅¨ σ΅¨σ΅¨ π (π§) σ΅¨σ΅¨σ΅¨ π σ΅¨σ΅¨ σ΅¨ σ΅¨σ΅¨ π(π) (π§) σ΅¨σ΅¨σ΅¨ ≤ 2π . σ΅¨ σ΅¨ (66) By Lemma 13 (ii), there exist a set π»1 ⊂ [0, 2π) having linear measure zero and a constant π΅ > 0 such that for sufficiently large π and for all π§ satisfying arg π§ = π ∈ [ππ − πΏπ , ππ + πΏπ ] \ π»1 , we have σ΅¨ σ΅¨σ΅¨ (π) σ΅¨σ΅¨ π (π§) σ΅¨σ΅¨σ΅¨ 2π σ΅¨ σ΅¨σ΅¨ σ΅¨σ΅¨ π(π) (π§) σ΅¨σ΅¨σ΅¨ ≤ π΅[π (2π, π)] σ΅¨ σ΅¨ (0 ≤ π < π ≤ π) . (67) Setting max{ππ (π΄ π ), ππ (πΉ), π =ΜΈ π} = π < ππ (π΄ π ), for all π§ satisfying |π§| = π ∉ πΈ1 and arg π§ = π ∈ [ππ − πΏπ , ππ + πΏπ ] and for any given π (0 < 2π < ππ (π΄ π ) − π), we have σ΅¨ σ΅¨σ΅¨ σ΅¨σ΅¨π΄ π (π§)σ΅¨σ΅¨σ΅¨ ≤ exp {ππ+π } (π =ΜΈ π) , σ΅¨ σ΅¨ σ΅¨σ΅¨ πΉ (π§) σ΅¨σ΅¨ σ΅¨σ΅¨ σ΅¨σ΅¨ π+π σ΅¨σ΅¨ σ΅¨σ΅¨ ≤ |πΉ (π§)| ≤ exp {π } . σ΅¨σ΅¨ π (π§) σ΅¨σ΅¨ (68) 8 Abstract and Applied Analysis Since π(π, π΄ π ) ∼ log π(π, π΄ π ) as π → ∞ (π ∉ πΈ1 ), by Lemma 30, for any given π > 0, there exists a set πΈ6 ⊂ (0, ∞) with log dens πΈ6 > 0 and a set π»2 ⊂ [0, 2π) with linear measure zero such that for all π§ satisfying |π§| = π ∈ πΈ6 and arg π§ = π ∈ [ππ − πΏπ , ππ + πΏπ ] \ π»2 , we have σ΅¨ σ΅¨σ΅¨ π (π΄ )−π σ΅¨σ΅¨π΄ π (π§)σ΅¨σ΅¨σ΅¨ > expπ {π π π } . (69) Substituting (66)–(69) into (51), for all π§ satisfying |π§| = π ∈ πΈ6 \ πΈ1 and arg π§ = π ∈ [ππ − πΏπ , ππ + πΏπ ] \ (π»1 ∪ π»2 ), we have expπ {πππ (π΄ π )−π } 2π ≤ (π + 1) π΅[π (2π, π)] ⋅ 2ππ ⋅ expπ {ππ+π } . (70) From (70), we have ππ+1 (π) ≥ ππ (π΄ π ). Therefore, every transcendental solution π(π§) of (13) satisfies ππ+1 (π) = ππ (π΄ π ). Furthermore, if πΉ(π§) ≡ΜΈ 0, then every transcendental solution π(π§) of (13) satisfies ππ+1 (π) = π π+1 (π) = ππ+1 (π) = ππ (π΄ π ). (ii)–(iv) By the same proof in Theorems 8 and 10, we can obtain the conclusions (ii)–(iv). Acknowledgments This project was supported by the National Natural Science Foundation of China (Grant nos. 11171119, 11261024, and 61202313), the Natural Science Foundation of Jiangxi Province in China (20122BAB211005, 20114BAB211003, 2010GQS0119, and 20122BAB201016), and the Foundation of Education Bureau of Jiangxi Province in China (Grant no. GJJ12206). References [1] W. K. Hayman, Meromorphic Functions, Clarendon Press, Oxford, UK, 1964. [2] I. Laine, Nevanlinna Theory and Complex Differential Equations, vol. 15, Walter de Gruyter, Berlin, Germany, 1993. [3] C.-C. Yang and H.-X. 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