International Journal of Analysis and Applications ISSN 2291-8639 Volume 4, Number 2 (2014), 159-173 http://www.etamaths.com PROPERTIES OF SOLUTIONS OF COMPLEX DIFFERENTIAL EQUATIONS IN THE UNIT DISC ZINELÂABIDINE LATREUCH AND BENHARRAT BELAÏDI∗ Abstract. In this paper, we investigate the growth and oscillation of higher order differential polynomial with meromorphic coefficients in the unit disc ∆ = {z : |z| < 1} generated by solutions of the linear differential equation f(k) + A (z) f = 0 (k ≥ 2) , where A (z) is a meromorphic function of finite iterated p−order in ∆. 1. Introduction and main results Throughout this paper, we assume that the reader is familiar with the fundamental results and the standard notations of the Nevanlinna’s value distribution theory on the complex plane and in the unit disc ∆ = {z : |z| < 1} (see [14] , [15] , [18] , [20] , [22]). We need to give some definitions and discussions. Firstly, let us give two defini- tions about the degree of small growth order of functions in ∆ as polynomials on the complex plane C. There are many types of definitions of small growth order of functions in ∆ (see [11] , [12]) . Definition 1.1 Let f be a meromorphic function in ∆, and D (f) := lim sup r→1− T (r,f) log 1 1−r = b. If b < ∞, we say that f is of finite b degree (or is non-admissible). If b = ∞, we say that f is of infinite degree (or is admissible), both defined by characteristic function T(r,f). Definition 1.2 Let f be an analytic function in ∆, and DM (f) := lim sup r→1− log+ M (r,f) log 1 1−r = a < ∞ (or a = ∞) , then we say that f is a function of finite a degree (or of infinite degree) defined by maximum modulus function M(r,f) = max |z|=r |f (z)| . Now we give the definitions of iterated order and growth index to classify generally the functions of fast growth in ∆ as those in C (see [5] , [17] , [18]). Let us define 2010 Mathematics Subject Classification. 34M10, 30D35. Key words and phrases. Iterated p−order, Linear differential equations, Iterated exponent of convergence of the sequence of distinct zeros, Unit disc, Differential polynomials. c©2014 Authors retain the copyrights of their papers, and all open access articles are distributed under the terms of the Creative Commons Attribution License. 159 160 LATREUCH AND BELAÏDI inductively, for r ∈ [0, 1) , exp1 r = er and expp+1 r = exp ( expp r ) , p ∈ N. We also define for all r sufficiently large in (0, 1) , log1 r = log r and logp+1 r = log ( logp r ) , p ∈ N. Moreover, we denote by exp0 r = r, log0 r = r, exp−1 r = log1 r, log−1 r = exp1 r. Definition 1.3 [6] The iterated p−order of a meromorphic function f in ∆ is defined as ρp (f) = lim sup r→1− log+p T (r,f) log 1 1−r (p ≥ 1) . For an analytic function f in ∆, we also define ρM,p (f) = lim sup r→1− log+p+1 M (r,f) log 1 1−r (p ≥ 1) . Remark 1.1 It follows by M. Tsuji in [22] that if f is an analytic function in ∆, then ρ1 (f) ≤ ρM,1 (f) ≤ ρ1 (f) + 1. However, it follows by Proposition 2.2.2 in [18] ρM,p (f) = ρp (f) (p ≥ 2) . Definition 1.4 [6] The growth index of the iterated order of a meromorphic func- tion f(z) in ∆ is defined as i (f) =   0, if f is non-admissible, min{j ∈ N : ρj (f) < ∞} , if f is admissible and ρj (f) < ∞ for some j ∈ N, +∞, if ρj (f) = ∞ for all j ∈ N. For an analytic function f in ∆, we also define iM (f) =   0, if f is of finite degree, min{j ∈ N : ρM,j (f) < ∞} , if f is of infinite degree and ρM,j (f) < ∞ for some j ∈ N, +∞, if ρM,j (f) = ∞ for all j ∈ N. Definition 1.5 ([13] , [16]) The iterated p−type of a meromorphic function f of iterated p−order ρp (f) (0 < ρp (f) < ∞) in ∆ is defined as τp (f) = lim sup r→1− (1 −r)ρp(f) log+p−1 T (r,f) . Definition 1.6 [7] Let f be a meromorphic function in ∆. Then the iterated exponent of convergence of the sequence of zeros of f (z) is defined as λp (f) = lim sup r→1− log+p N ( r, 1 f ) log 1 1−r , where N ( r, 1 f ) is the counting function of zeros of f (z) in {z ∈ C : |z| < r} . Simi- larly, the iterated exponent of convergence of the sequence of distinct zeros of f (z) is defined as λp (f) = lim sup r→1− log+p N ( r, 1 f ) log 1 1−r , PROPERTIES OF SOLUTIONS OF COMPLEX DIFFERENTIAL EQUATIONS 161 where N ( r, 1 f ) is the counting function of distinct zeros of f (z) in {z ∈ C : |z| < r}. Definition 1.7 [7] The growth index of the convergence exponent of the sequence of zeros of a meromorphic f(z) in ∆ is defined as iλ (f) =   0, if N ( r, 1 f ) = O ( log 1 1−r ) , min{j ∈ N : λj (f) < ∞} , if some j ∈ N with λj (f) < ∞ exists, +∞, if λj (f) = ∞ for all j ∈ N. Remark 1.2 Similarly, we can define the finiteness degree iλ (f) of λp(f). Consider for k ≥ 2 the complex differential equation (1.1) f(k) + A (z) f = 0 and the differential polynomial (1.2) gf = dkf (k) + dk−1f (k−1) + · · · + d1f′ + d0f, where A and dj (j = 0, 1, · · · ,k) are meromorphic functions in ∆. Let L(G) denote a differential subfield of the field M(G) of meromorphic functions in a domain G ⊂ C. Throughout this paper, we simply denote L instead of L(∆) . Special case of such differential subfield Lp+1,ρ={g meromorphic in ∆: ρp+1 (g) < ρ} , where ρ is a positive constant. Recently, T. B. Cao, H. Y. Xu and C. X. Zhu [8], T. B. Cao, L. M. Li, J. Tu and H. Y. Xu [10] have studied the complex oscillation of differential polynomial generated by meromorphic and analytic solutions of second order linear differential equations with meromorphic coefficients and obtained the following results. Theorem A [10] Let A (z) be an analytic function of infinite degree and of finite iterated order ρM,p (A) = ρ > 0 in the unit disc ∆, and let f 6≡ 0 be a solution of the equation (1.3) f′′ + A (z) f = 0. Moreover, let (1.4) P [f] = P ( f,f′, · · · ,f(m) ) = m∑ j=0 pjf (j) be a linear differential polynomial with analytic coefficients pj ∈ Lp+1,ρ, assuming that at least one of the coefficients pj does vanish identically. If ϕ (z) ∈ Lp+1,ρ is a non-zero analytic function in ∆, and neither P [f] nor P [f] − ϕ vanishes identically, then we have iλ (P [f] −ϕ) = i (f) = p + 1 and λp+1 (P [f] −ϕ) = ρM,p+1 (f) = ρM,p (A) = ρ. Theorem B [8] Let A be an admissible meromorphic function of finite iterat- ed order ρp (A) = ρ > 0 (1 ≤ p < ∞) in the unit disc ∆ such that δ (∞,A) = 162 LATREUCH AND BELAÏDI lim inf r→1− m(r,A) T(r,A) = δ > 0, and let f be a non-zero meromorphic solution of equation (1.3) such that δ (∞,f) > 0. Moreover, let be a linear differential polynomial (1.4) with meromorphic coefficients pj ∈ Lp+1,ρ, assuming that at least one of the coef- ficients pj does not vanish identically. If ϕ ∈ Lp+1,ρ is a non-zero meromorphic function in ∆, and neither P [f] nor P [f] −ϕ vanishes identically, then we have i (f) = iλ (P [f] −ϕ) = p + 1 and λp (P [f] −ϕ) = ρp+1 (f) = ρp (A) = ρ if p > 1, while ρp (A) ≤ λp (P [f] −ϕ) ≤ ρp+1 (f) ≤ ρp (A) + 1 if p = 1. Remark 1.3 The idea of the proofs of Theorems A-B is borrowed from the paper of Laine, Rieppo [19] with the modifications reflecting the change from the complex plane C to the unit disc ∆. Before we state our results, we define the sequence of meromorphic functions αi,j (j = 0, · · · ,k − 1) in ∆ by (1.5) αi,j = { α′i,j−1 + αi−1,j−1, for all i = 1, · · · ,k − 1, α′0,j−1 −Aαk−1,j−1, for i = 0 and (1.6) αi,0 = { di, for all i = 1, · · · ,k − 1, d0 −dkA, for i = 0. We define also h and ψ (z) by (1.7) h = ∣∣∣∣∣∣∣∣∣∣ α0,0 α1,0 . . αk−1,0 α0,1 α1,1 . . αk−1,1 . . . . . . . . . . α0,k−1 α1,k−1 . . αk−1,k−1 ∣∣∣∣∣∣∣∣∣∣ , (1.8) ψ (z) = C0ϕ + C1ϕ ′ + · · · + Ck−1ϕ(k−1), where Cj (j = 0, · · · ,k − 1) are finite iterated p−order meromorphic functions in ∆ depending on αi,j and ϕ 6≡ 0 is a meromorphic function in ∆ with ρp (ϕ) < ∞. The main purpose of this paper is to study the growth and oscillation of differential polynomial (1.2) generated by meromorphic solutions of equation (1.1) in the unit disc ∆. Theorem 1.1 Suppose that A (z) is a meromorphic function of finite iterated p−order in ∆ and that dj (z) (j = 0, 1, · · · ,k) are finite iterated p−order meromor- phic functions in ∆ that are not all vanishing identically such that h 6≡ 0. If f (z) is an infinite iterated p−order meromorphic solution of (1.1) with ρp+1 (f) = ρ, then the differential polynomial (1.2) satisfies ρp (gf ) = ρp (f) = ∞ PROPERTIES OF SOLUTIONS OF COMPLEX DIFFERENTIAL EQUATIONS 163 and ρp+1 (gf ) = ρp+1 (f) = ρ. Furthermore, if f is a finite iterated p−order meromorphic solution of (1.1) such that (1.9) ρp (f) > max{ρp (A) ,ρp (dj) (j = 0, 1, · · · ,k)} , then ρp (gf ) = ρp (f) . Remark 1.4 In Theorem 1.1, if we do not have the condition h 6≡ 0, then the conclusions of Theorem 1.1 cannot hold. For example, if we take dk = 1,d0 = A and dj ≡ 0 (j = 1, · · · ,k − 1) , then h ≡ 0. It follows that gf ≡ 0 and ρp (gf ) = 0. So, if f (z) is an infinite iterated p−order meromorphic solution of (1.1) , then ρp (gf ) = 0 < ρp (f) = ∞, and if f is a finite iterated p−order meromorphic solution of (1.1) such that (1.9) holds, then ρp (gf ) = 0 < ρp (f). Corollary 1.1 Suppose that A (z) is admissible meromorphic function in ∆ such that i (A) = p (1 ≤ p < ∞) and δ (∞,A) = δ > 0. Let dj (z) (j = 0, 1, · · · ,k) be finite iterated p−order meromorphic functions in ∆ that are not all vanishing identically such that h 6≡ 0, and let f be a nonzero meromorphic solution of (1.1) . If δ (∞,f) > 0, then the differential polynomial gf satisfies i (gf ) = p + 1 and ρp+1 (gf ) = ρp+1 (f) = ρp (A) if p > 1, while ρp (A) ≤ ρp+1 (gf ) = ρp+1 (f) ≤ ρp (A) + 1 if p = 1. Theorem 1.2 Under the assumptions of Theorem 1.1, let ϕ (z) 6≡ 0 be a meromor- phic function with finite iterated p−order in ∆ such that ψ (z) is not a solution of (1.1) . If f (z) is an infinite iterated p−order meromorphic solution of (1.1) with ρp+1 (f) = ρ, then the differential polynomial (1.2) satisfies λp (gf −ϕ) = λp (gf −ϕ) = ρp (f) = ∞ and λp+1 (gf −ϕ) = λp+1 (gf −ϕ) = ρp+1 (f) = ρ. Furthermore, if f is a finite iterated p−order meromorphic solution of (1.1) such that (1.10) ρp (f) > max{ρp (A) ,ρp (ϕ) ,ρp (dj) (j = 0, 1, · · · ,k)} , then λp (gf −ϕ) = λp (gf −ϕ) = ρp (f) . Corollary 1.2 Under the assumptions of Corollary 1.1, let ϕ (z) 6≡ 0 be a mero- morphic function with finite iterated p−order in ∆ such that ψ (z) 6≡ 0. Then the differential polynomial (1.2) satisfies λp+1 (gf −ϕ) = λp+1 (gf −ϕ) = ρp+1 (f) = ρp (A) if p > 1, while ρp (A) ≤ λp+1 (gf −ϕ) = λp+1 (gf −ϕ) = ρp+1 (f) ≤ ρp (A) + 1 if p = 1. 164 LATREUCH AND BELAÏDI Remark 1.5 The ideas of the proofs of Theorems 1.1 and 1.2 are from [21] with modification from the complex plane C to the unit disc ∆. For some papers related in the complex plane see [19, 21, 4] . 2. Auxiliary lemmas Lemma 2.1 [9] Let A0, A1, · · · , Ak−1, F 6≡ 0 be meromorphic functions in ∆, and let f be a meromorphic solution of the equation (2.1) f(k) + Ak−1 (z) f (k−1) + · · · + A1 (z) f′ + A0 (z) f = F (z) such that max{ρp (Aj) (j = 0, 1, · · · ,k − 1) ,ρp (F)} < ρp (f) ≤ +∞. Then λp (f) = λp (f) = ρp (f) and λp+1 (f) = λp+1 (f) = ρp+1 (f) . Lemma 2.2 [6] Let p ≥ 1 be an integer, and let A0(z), · · · ,Ak−1(z) be analytic functions in ∆ such that i (A0) = p. If max{i (Aj) : j = 1, · · · ,k − 1} < p or max{ρp (Aj) : j = 1, · · · ,k − 1} < ρp (A0) , then every solution f 6≡ 0 of the equation (2.2) f(k) + Ak−1 (z) f (k−1) + · · · + A1 (z) f′ + A0 (z) f = 0, satisfies i (f) = p + 1 and ρp (f) = ∞, ρp (A0) ≤ ρp+1 (f) = ρM,p+1 (f) ≤ max{ρM,p (Aj) : j = 0, 1, · · · ,k − 1}. Lemma 2.3 [3] Let f and g be meromorphic functions in the unit disc ∆ such that 0 < ρp (f) ,ρp (g) < ∞ and 0 < τp (f) ,τp (g) < ∞. Then we have (i) If ρp (f) > ρp (g) , then we obtain (2.3) τp (f + g) = τp (fg) = τp (f) . (ii) If ρp (f) = ρp (g) and τp (f) 6= τp (g) , then we get (2.4) ρp (f + g) = ρp (fg) = ρp (f) = ρp (g) . Lemma 2.4 [17, 2] Let f be a meromorphic function in the unit disc for which i (f) = p ≥ 1 and ρp (f) = β < ∞, and let k ∈ N. Then for any ε > 0, (2.5) m ( r, f(k) f ) = O ( expp−2 ( log 1 1 −r )β+ε) for all r outside a set E ⊂ [0, 1) with ∫ E dr 1−r < ∞. Lemma 2.5 [8] Let A (z) be an admissible meromorphic function in ∆ such that i (A) = p (1 ≤ p < ∞) and δ (∞,A) = δ > 0, and let f be a nonzero meromorphic PROPERTIES OF SOLUTIONS OF COMPLEX DIFFERENTIAL EQUATIONS 165 solution of (1.1) . If δ (∞,f) > 0, then i (f) = p + 1 and ρp+1 (f) = ρp (A) if p > 1, while ρp (A) ≤ ρp+1 (f) ≤ ρp (A) + 1 if p = 1. Lemma 2.6 [1] Let g : (0, 1) → R and h : (0, 1) → R be monotone increasing functions such that g (r) ≤ h (r) holds outside of an exceptional set E1 ⊂ [0, 1) for which ∫ E1 dr 1−r < ∞. Then there exists a constant d ∈ (0, 1) such that if s (r) = 1 −d (1 −r) , then g (r) ≤ h (s (r)) for all r ∈ [0, 1). 3. Proofs of the Theorems and the Corollaries Proof of Theorem 1.1 Suppose that f is an infinite iterated p−order meromor- phic solution of (1.1) with ρp+1 (f) = ρ. By (1.1) we have (3.1) f(k) = −Af which implies gf = dkf (k) + dk−1f (k−1) + · · · + d0f (3.2) = dk−1f (k−1) + · · · + (d0 −dkA) f. We can rewrite (3.2) as (3.3) gf = k−1∑ i=0 αi,0f (i), where αi,0 are defined in (1.6) . Differentiating both sides of equation (3.3) and replacing f(k) with f(k) = −Af, we obtain g′f = k−1∑ i=0 α′i,0f (i) + k−1∑ i=0 αi,0f (i+1) = k−1∑ i=0 α′i,0f (i) + k∑ i=1 αi−1,0f (i) = α′0,0f + k−1∑ i=1 α′i,0f (i) + k−1∑ i=1 αi−1,0f (i) + αk−1,0f (k) = α′0,0f + k−1∑ i=1 ( α′i,0 + αi−1,0 ) f(i) −αk−1,0Af (3.4) = k−1∑ i=1 ( α′i,0 + αi−1,0 ) f(i) + ( α′0,0 −αk−1,0A ) f. We can rewrite (3.4) as (3.5) g′f = k−1∑ i=0 αi,1f (i), where (3.6) αi,1 = { α′i,0 + αi−1,0, for all i = 1, · · · ,k − 1, α′0,0 −Aαk−1,0, for i = 0. 166 LATREUCH AND BELAÏDI Differentiating both sides of equation (3.5) and replacing f(k) with f(k) = −Af, we obtain g′′f = k−1∑ i=0 α′i,1f (i) + k−1∑ i=0 αi,1f (i+1) = k−1∑ i=0 α′i,1f (i) + k∑ i=1 αi−1,1f (i) = α′0,1f + k−1∑ i=1 α′i,1f (i) + k−1∑ i=1 αi−1,1f (i) + αk−1,1f (k) = α′0,1f + k−1∑ i=1 ( α′i,1 + αi−1,1 ) f(i) −αk−1,1Af (3.7) = k−1∑ i=1 ( α′i,1 + αi−1,1 ) f(i) + ( α′0,1 −αk−1,1A ) f which implies that (3.8) g′′f = k−1∑ i=0 αi,2f (i), where (3.9) αi,2 = { α′i,1 + αi−1,1, for all i = 1, · · · ,k − 1, α′0,1 −Aαk−1,1, for i = 0. By using the same method as above we can easily deduce that (3.10) g (j) f = k−1∑ i=0 αi,jf (i), j = 0, 1, · · · ,k − 1, where (3.11) αi,j = { α′i,j−1 + αi−1,j−1, for all i = 1, · · · ,k − 1, α′0,j−1 −Aαk−1,j−1, for i = 0 and (3.12) αi,0 = { di, for all i = 1, · · · ,k − 1, d0 −dkA, for i = 0. By (3.3) − (3.12) we obtain the system of equations (3.13)   gf = α0,0f + α1,0f ′ + · · · + αk−1,0f(k−1), g′f = α0,1f + α1,1f ′ + · · · + αk−1,1f(k−1), g′′f = α0,2f + α1,2f ′ + · · · + αk−1,2f(k−1), · · · g (k−1) f = α0,k−1f + α1,k−1f ′ + · · · + αk−1,k−1f(k−1). By Cramer’s rule, and since h 6≡ 0 we have (3.14) f = ∣∣∣∣∣∣∣∣∣∣ gf α1,0 . . αk−1,0 g′f α1,1 . . αk−1,1 . . . . . . . . . . g (k−1) f α1,k−1 . . αk−1,k−1 ∣∣∣∣∣∣∣∣∣∣ h . PROPERTIES OF SOLUTIONS OF COMPLEX DIFFERENTIAL EQUATIONS 167 So, we obtain (3.15) f = C0gf + C1g ′ f + · · · + Ck−1g (k−1) f , where Cj are finite iterated p−order meromorphic functions in ∆ depending on αi,j, where αi,j are defined in (3.11) and (3.12) . If ρp (gf ) < +∞, then by (3.15) we obtain ρp (f) < +∞, and this is a contra- diction. Hence ρp (gf ) = ρp (f) = +∞. Now, we prove that ρp+1 (gf ) = ρp+1 (f) = ρ. By (3.2), we get ρp+1 (gf ) ≤ ρp+1 (f) and by (3.15) we have ρp+1 (f) ≤ ρp+1 (gf ). This yield ρp+1 (gf ) = ρp+1 (f) = ρ. Furthermore, if f is a finite iterated p−order meromorphic solution of equation (1.1) such that (3.16) ρp (f) > max{ρp (A) ,ρp (dj) (j = 0, 1, · · · ,k)} , then (3.17) ρp (f) > max{ρp (αi,j) : i = 0, · · · ,k − 1,j = 0, · · · ,k − 1} . By (3.2) and (3.16) we have ρp (gf ) ≤ ρp (f) . Now, we prove ρp (gf ) = ρp (f) . If ρp (gf ) < ρp (f) , then by (3.15) and (3.17) we get ρp (f) ≤ max{ρp (Cj) (j = 0, · · · ,k − 1) ,ρp (gf )} < ρp (f) and this is a contradiction. Hence ρp (gf ) = ρp (f) . Remark 3.1 From (3.15) , it follows that the condition h 6≡ 0 is equivalent to that gf,g ′ f,g ′′ f , ...,g (k−1) f are linearly independent over the field of meromorphic functions of finite iterated p−order in ∆. Proof of Corollary 1.1 Suppose f 6≡ 0 is a meromorphic solution of (1.1) . Then, by Lemma 2.5, we have i (f) = p + 1 and ρp+1 (f) = ρp (A) if p > 1, while ρp (A) ≤ ρp+1 (f) ≤ ρp (A) + 1 if p = 1. Thus, by Theorem 1.1 we obtain that the differential polynomial gf satisfies i (gf ) = p + 1 and ρp+1 (gf ) = ρp+1 (f) = ρp (A) if p > 1, while ρp (A) ≤ ρp+1 (gf ) = ρp+1 (f) ≤ ρp (A) + 1 if p = 1. Proof of Theorem 1.2 Suppose that f is an infinite iterated p−order meromorphic solution of equation (1.1) with ρp+1 (f) = ρ. Set w (z) = gf −ϕ. Since ρp (ϕ) < ∞, then by Theorem 1.1 we have ρp (w) = ρp (gf ) = ∞ and ρp+1 (w) = ρp+1 (gf ) = ρ. To prove λp (gf −ϕ) = λp (gf −ϕ) = ∞ and λp+1 (gf −ϕ) = λp+1 (gf −ϕ) = ρ we need to prove λp (w) = λp (w) = ∞ and λp+1 (w) = λp+1 (w) = ρ. By gf = w + ϕ and (3.15) , we get (3.18) f = C0w + C1w ′ + · · · + Ck−1w(k−1) + ψ (z) , where (3.19) ψ (z) = C0ϕ + C1ϕ ′ + · · · + Ck−1ϕ(k−1). 168 LATREUCH AND BELAÏDI Substituting (3.18) into (1.1) , we obtain (3.20) Ck−1w (2k−1) + 2k−2∑ i=0 φiw (i) = − ( ψ(k) + A (z) ψ ) = H, where φi (i = 0, · · · , 2k − 2) are meromorphic functions in ∆ with finite iterated p−order. Since ψ (z) is not a solution of (1.1) , it follows that H 6≡ 0. Then by Lemma 2.1, we obtain λp (w) = λp (w) = ∞ and λp+1 (w) = λp+1 (w) = ρ, i. e., λp (gf −ϕ) = λp (gf −ϕ) = ∞ and λp+1 (gf −ϕ) = λp+1 (gf −ϕ) = ρ. Suppose that f is a finite iterated p−order meromorphic solution of equation (1.1) such that (1.10) holds. Set w (z) = gf −ϕ. Since ρp (ϕ) < ρp (f) , then by The- orem 1.1 we have ρp (w) = ρp (gf ) = ρp (f) . To prove λp (gf −ϕ) = λp (gf −ϕ) = ρp (f) we need to prove λp (w) = λp (w) = ρp (f) . Using the same reasoning as above, we get Ck−1w (2k−1) + 2k−2∑ i=0 φiw (i) = − ( ψ(k) + A (z) ψ ) = F, where Ck−1, φi (i = 0, · · · , 2k − 2) are meromorphic functions in ∆ with finite it- erated p−order ρp (Ck−1) < ρp (w) , ρp (φi) < ρp (w) (i = 0, · · · , 2k − 2) and ψ (z) = C0ϕ + C1ϕ ′ + · · · + Ck−1ϕ(k−1), ρp (F) < ρp (w) . Since ψ (z) is not a solution of (1.1) , it follows that F 6≡ 0. Then by Lemma 2.1, we obtain λp (w) = λp (w) = ρp (f) , i. e., λp (gf −ϕ) = λp (gf −ϕ) = ρp (f) . Proof of Corollary 1.2 Suppose that f 6≡ 0 is a meromorphic solution of (1.1) . Then, by Lemma 2.5, we have i (f) = p + 1 and ρp+1 (f) = ρp (A) if p > 1, while ρp (A) ≤ ρp+1 (f) ≤ ρp (A) + 1 if p = 1. Since ψ 6≡ 0 and ρp (ψ) < ∞, then ψ cannot be a solution of equation (1.1) . Thus, by Theorem 1.2 we obtain that the differential polynomial gf satisfies λp+1 (gf −ϕ) = λp+1 (gf −ϕ) = ρp+1 (f) = ρp (A) if p > 1, while ρp (A) ≤ λp+1 (gf −ϕ) = λp+1 (gf −ϕ) = ρp+1 (f) ≤ ρp (A) + 1 if p = 1. 4. Discussions and applications In this section, we consider the differential equation (4.1) f′′′ + A (z) f = 0, where A (z) is a meromorphic function of finite iterated p−order in ∆. It is clear that the difficulty of the study of the differential polynomial generated by solutions lies in the calculation of the coefficients αi,j. We explain here that by using our method, the calculation of the coefficients αi,j can be deduced easily. We study for example the growth of the differential polynomial (4.2) gf = f ′′′ + f′′ + f′ + f. PROPERTIES OF SOLUTIONS OF COMPLEX DIFFERENTIAL EQUATIONS 169 We have (4.3)   gf = α0,0f + α1,0f ′ + α2,0f ′′, g′f = α0,1f + α1,1f ′ + α2,1f ′′, g′′f = α0,2f + α1,2f ′ + α2,2f ′′. By (1.6) we obtain (4.4) αi,0 = { 1, for all i = 1, 2, 1 −A, for i = 0. Now, by (3.6) we get αi,1 = { α′i,0 + αi−1,0, for all i = 1, 2 α′0,0 −Aα2,0, for i = 0. Hence (4.5)   α0,1 = α ′ 0,0 −Aα2,0 = −A′ −A, α1,1 = α ′ 1,0 + α0,0 = 1 −A, α2,1 = α ′ 2,0 + α1,0 = 1. Finally, by (3.11) we have αi,2 = { α′i,1 + αi−1,1, for all i = 1, 2, α′0,1 −Aα2,1, for i = 0. So, we obtain (4.6)   α0,2 = α ′ 0,1 −Aα2,1 = −A′′ −A′ −A, α1,2 = α ′ 1,1 + α0,1 = −2A′ −A, α2,2 = α ′ 2,1 + α1,1 = 1 −A. Hence (4.7)   gf = (1 −A) f + f′ + f′′, g′f = (−A ′ −A) f + (1 −A) f′ + f′′, g′′f = (−A ′′ −A′ −A) f + (−2A′ −A) f′ + (1 −A) f′′ and h = ∣∣∣∣∣∣ 1 −A 1 1 −A′ −A 1 −A 1 −A′′ −A′ −A −2A′ −A 1 −A ∣∣∣∣∣∣ (4.8) = 3A′ −A−AA′ −AA′′ + A2 −A3 + 2(A′)2 + 1. Suppose that h 6≡ 0, by simple calculations we have (4.9) f = Ag′′f + (−1 − 2A ′) g′f + ( 1 −A + 2A′ + A2 ) gf h and by different conditions on the solution f we can ensure that ρp (f ′′′ + f′′ + f′ + f) = ρp (f) . Turning now to the problem of oscillation, for that we consider a meromorphic function ϕ (z) 6≡ 0 of finite iterated p−order in ∆. From (4.9) we get (4.10) f = Aw′′ + (−1 − 2A′) w′ + ( 1 −A + 2A′ + A2 ) w h + ψ (z) , 170 LATREUCH AND BELAÏDI where w = gf −ϕ and (4.11) ψ (z) = Aϕ′′ + (−1 − 2A′) ϕ′ + ( 1 −A + 2A′ + A2 ) ϕ h . Hence (4.12) f = A h w′′ + C1w ′ + C0w + ψ, where C1 = − 1 + 2A′ h , C0 = 1 −A + 2A′ + A2 h . Substituting (4.12) into (4.1) , we obtain A h w(5) + 4∑ i=0 φiw (i) = − ( ψ(3) + A (z) ψ ) , where φi (i = 0, · · · , 4) are meromorphic functions in ∆ with finite iterated p−order. Suppose that all meromorphic solutions f 6≡ 0 of (4.1) are of infinite iterated p−order and ρp+1 (f) = ρ. If ψ 6≡ 0, then by Lemma 2.1 we obtain (4.13) λp (gf −ϕ) = λp (gf −ϕ) = ρp (f) = +∞ and (4.14) λp+1 (gf −ϕ) = λp+1 (gf −ϕ) = ρp+1 (f) = ρ. Suppose that f is a meromorphic solution of (4.1) of finite iterated p−order such that ρp (f) > max{ρp (A) ,ρp (ϕ)} . If ψ(3) + A (z) ψ 6≡ 0, then by Lemma 2.1 we obtain λp (gf −ϕ) = λp (gf −ϕ) = ρp (f) . Finally, we can state the following two results without the additional conditions h 6≡ 0 and ψ is not a solution of (4.1). Theorem 4.1 Suppose that A (z) is analytic function in ∆ of finite iterated p−order 0 < ρp (A) < ∞ and 0 < τp (A) < ∞, and that dj (z) (j = 0, 1, 2, 3) are finite it- erated p−order analytic functions in ∆ that are not all vanishing identically such that max{ρp (dj) (j = 0, 1, 2, 3)} < ρp (A) . If f is a nontrivial solution of (4.1), then the differential polynomial (4.15) gf = d3f (3) + d2f ′′ + d1f ′ + d0f satisfies ρp (gf ) = ρp (f) = ∞ and ρp (A) ≤ ρp+1 (gf ) = ρp+1 (f) ≤ ρM,p (A) . Theorem 4.2 Under the assumptions of Theorem 4.1, let ϕ (z) 6≡ 0 be an analytic function in ∆ with finite iterated p−order. If f is a nontrivial solution of (4.1) , then the differential polynomial gf = d3f (3) + d2f ′′ + d1f ′ + d0f (d3 6≡ 0) satisfies (4.16) λp (gf −ϕ) = λp (gf −ϕ) = ρp (f) = ∞ PROPERTIES OF SOLUTIONS OF COMPLEX DIFFERENTIAL EQUATIONS 171 and (4.17) ρp (A) ≤ λp+1 (gf −ϕ) = λp+1 (gf −ϕ) = ρp+1 (f) ≤ ρM,p (A) . Remark 4.1 The results obtained in Theorems 4.1 and 4.2 and refinement of Corollaries 1.1 and 1.2 respectively. Proof of Theorem 4.1 Suppose that f is a nontrivial solution of (4.1). Then by Lemma 2.2, we have ρp (f) = ∞, ρp (A) ≤ ρp+1 (f) ≤ ρM,p (A) . First, we suppose that d3 6≡ 0. By the same reasoning as before we obtain that h = ∣∣∣∣∣∣ H0 H1 H2 H3 H4 H5 H6 H7 H8 ∣∣∣∣∣∣ , where H0 = d0 − d3A, H1 = d1, H2 = d2,H3 = d′0 − (d2 + d′3) A − d3A′, H4 = d0 + d ′ 1 −d3A, H5 = d1 + d′2,H6 = d′′0 − (d1 + 2d′2 + d′′3 ) A− (d2 + 2d′3) A′ −d3A′′, H7 = 2d ′ 0 + d ′′ 1 − (d2 + 2d′3) A− 2d3A′, H8 = d0 + 2d′1 + d′′2 −d3A. Then h = (3d0d1d2 + 3d0d1d ′ 3 + 3d0d2d ′ 2 − 6d0d3d ′ 1 + 3d1d2d ′ 1 + 3d1d3d ′ 0 +d0d2d ′′ 3 − 2d0d3d ′′ 2 + d1d2d ′′ 2 + d1d3d ′′ 1 + d2d3d ′′ 0 + 2d0d ′ 2d ′ 3 + 2d1d ′ 1d ′ 3 − 4d2d ′ 0d ′ 3 +2d2d ′ 1d ′ 2 + 2d3d ′ 0d ′ 2 −d1d ′ 2d ′′ 3 + d1d ′ 3d ′′ 2 + d2d ′ 1d ′′ 3 −d2d ′′ 1d ′ 3 −d3d ′ 1d ′′ 2 +d3d ′ 2d ′′ 1 −d 3 1 − 3d 2 0d3 − 2d1(d ′ 2) 2 − 3d21d ′ 2 −2d3(d ′ 1) 2 −d22d ′′ 1 −d 2 1d ′′ 3 − 3d 2 2d ′ 0 ) A + (2d0d2d ′ 3 + 2d0d3d ′ 2 −d1d2d ′ 2 + 2d1d3d ′ 1 − 4d2d3d ′ 0 + d1d3d ′′ 2 −d2d3d′′1 − 2d1d ′ 2d ′ 3 + 2d2d ′ 1d ′ 3 + 3d0d1d3 + d0d 2 2 −d 2 1d2 + d 2 2d ′ 1 − 2d 2 1d ′ 3 ) A′ +(d2d3d ′ 1 + d0d2d3 −d1d3d ′ 2 −d 2 1d3)A ′′ + (2d2d3d ′ 3 − 3d1d 2 3 + 2d 2 2d3 − 2d 2 3d ′ 2)AA ′ + ( d32 − 3d1d2d3 − 3d1d3d ′ 3 − 3d2d3d ′ 2 −d2d3d ′′ 3 − 2d3d ′ 2d ′ 3 +3d0d 2 3 + 3d 2 3d ′ 1 + 2d2(d ′ 3) 2 + 3d22d ′ 3 + d 2 3d ′′ 2 ) A2 −d33A 3 + 2d2d 2 3(A ′)2 −d2d23AA ′′ − 3d0d1d′0 −d0d1d ′′ 1 −d0d2d ′′ 0 − 2d0d ′ 0d ′ 2 +d1d ′′ 0d ′ 2 + d2d ′ 0d ′′ 1 −d2d ′ 1d ′′ 0 + d 3 0 + 2d0(d ′ 1) 2 + 3d20d ′ 1 + 2d2(d ′ 0) 2 +d21d ′′ 0 + d 2 0d ′′ 2 − 2d1d ′ 0d ′ 1 + d0d ′ 1d ′′ 2 −d0d ′ 2d ′′ 1 −d1d ′ 0d ′′ 2. By d3 6≡ 0, A 6≡ 0 and Lemma 2.3, we have ρp (h) = ρp (A), hence h 6≡ 0. For the cases (i) d3 ≡ 0, d2 6≡ 0; (ii) d3 ≡ 0,d2 ≡ 0 and d1 6≡ 0 by using a similar reasoning as above we get h 6≡ 0. Finally, if d3 ≡ 0, d2 ≡ 0, d1 ≡ 0 and d0 6≡ 0, then we have h = d30 6≡ 0. Hence h 6≡ 0. By h 6≡ 0, we obtain f = 1 h ∣∣∣∣∣∣ gf d1 d2 g′f d0 + d ′ 1 −d3A d1 + d′2 g′′f 2d ′ 0 + d ′′ 1 − (d2 + 2d′3) A− 2d3A′ d0 + 2d′1 + d′′2 −d3A ∣∣∣∣∣∣ , which we can write (4.18) f = 1 h ( D0gf + D1g ′ f + D2g ′′ f ) , where D0 = (d1d2 − 2d0d3 + 2d1d′3 + d2d ′ 2 − 3d3d ′ 1 −d3d ′′ 2 + 2d ′ 2d ′ 3) A + (2d1d3 + 2d3d ′ 2) A ′ + A2d23 + 3d0d ′ 1 − 2d1d ′ 0 + d0d ′′ 2 −d1d ′′ 1 172 LATREUCH AND BELAÏDI −2d′0d ′ 2 + d ′ 1d ′′ 2 −d ′ 2d ′′ 1 + d 2 0 + 2(d ′ 1) 2, D1 = ( d1d3 − 2d2d′3 −d 2 2 ) A + d2d ′′ 1 −d0d1 − 2d1d ′ 1 + 2d2d ′ 0 −d1d ′′ 2, D2 = d2d3A + d 2 1 −d2d ′ 1 + d1d ′ 2 −d0d2. If ρp (gf ) < +∞, then by (4.18) we obtain ρp (f) < +∞, and this is a contradiction. Hence ρp (gf ) = ρp (f) = +∞. Now, we prove that ρp+1 (gf ) = ρp+1 (f) . By (4.15), we get ρp+1 (gf ) ≤ ρp+1 (f) and by (4.18) we have ρp+1 (f) ≤ ρp+1 (gf ). This yield ρp (A) ≤ ρp+1 (gf ) = ρp+1 (f) ≤ ρM,p (A) . Proof of Theorem 4.2 By setting w = gf −ϕ in (4.18) , we have (4.19) f = 1 h (D0w + D1w ′ + D2w ′′) + ψ, where (4.20) ψ = D2ϕ ′′ + D1ϕ ′ + D0ϕ h . Since d3 6≡ 0, then h 6≡ 0. It follows by Theorem 4.1 that gf is of infinite iterated p−order analytic function and ρp (A) ≤ ρp+1 (gf ) ≤ ρM,p (A) . Since ρp (ϕ) < ∞, then we have ρp (w) = ρp (gf ) = ρp (f) = ∞ and ρp (A) ≤ ρp+1 (w) = ρp+1 (gf ) = ρp+1 (f) ≤ ρM,p (A) . Substituting (4.19) into (4.1) , we obtain D2 h w(5) + 4∑ i=0 φiw (i) = − ( ψ(3) + A (z) ψ ) , where φi (i = 0, · · · , 4) are meromorphic functions in ∆ with finite iterated p−order. We prove first that ψ 6≡ 0. Suppose that ψ ≡ 0, then (4.20) can be rewritten as (4.21) D2ϕ ′′ + D1ϕ ′ + D0ϕ = 0 and by Lemma 2.3, we have (4.22) ρ (D0) > max{ρ (D1) ,ρ (D2)} . By (4.21) we obtain D0 = − ( D2 ϕ′′ ϕ + D1 ϕ′ ϕ ) . Since ρp (ϕ) = β < ∞, then by Lemma 2.4 we have T (r,D0) ≤ T (r,D1) + T (r,D2) + O ( expp−2 ( log 1 1 −r )β+ε) , r /∈ E, where E ⊂ [0, 1) is a set with ∫ E dr 1−r < ∞. Then, by using Lemma 2.6, we get ρp (D0) ≤ max{ρp (D1) ,ρp (D2)} , which is a contradiction. It is clear now that ψ 6≡ 0 cannot be a solution of (4.1) because ρp (ψ) < ∞. Then, by Lemma 2.1 we obtain λp (w) = λp (w) = λp (gf −ϕ) = λp (gf −ϕ) = ρp (f) = ∞ and ρp (A) ≤ λp+1 (w) = λp+1 (w) = λp+1 (gf −ϕ) = λp+1 (gf −ϕ) = ρp+1 (f) ≤ ρM,p (A) . PROPERTIES OF SOLUTIONS OF COMPLEX DIFFERENTIAL EQUATIONS 173 References [1] S. Bank, General theorem concerning the growth of solutions of first-order algebraic differ- ential equations, Compositio Math. 25 (1972), 61-70. [2] B. Beläıdi, Oscillation of fast growing solutions of linear differential equations in the unit disc, Acta Univ. Sapientiae Math. 2 (2010), no. 1, 25–38. [3] B. Beläıdi, A. El Farissi, Fixed points and iterated order of differential polynomial generated by solutions of linear differential equations in the unit disc, J. Adv. Res. Pure Math. 3 (2011), no. 1, 161–172. [4] B. Beläıdi and Z. Latreuch, Relation between small functions with differential polynomials generated by meromorphic solutions of higher order linear differential equations, Submitted. [5] L. G. Bernal, On growth k-order of solutions of a complex homogeneous linear differential equation, Proc. Amer. Math. Soc. 101 (1987), no. 2, 317–322. [6] T. B. Cao and H. X. Yi, The growth of solutions of linear differential equations with coeffi- cients of iterated order in the unit disc, J. Math. Anal. Appl. 319 (2006), no. 1, 278–294. [7] T. B. Cao, The growth, oscillation and fixed points of solutions of complex linear differential equations in the unit disc, J. Math. Anal. Appl. 352 (2009), no. 2, 739-748. [8] T. B. Cao, H. Y. Xu and C. X. Zhu, On the complex oscillation of differential polynomials generated by meromorphic solutions of differential equations in the unit disc, Proc. Indian Acad. Sci. Math. Sci. 120 (2010), no. 4, 481–493. [9] T. B. Cao and Z. S. Deng, Solutions of non-homogeneous linear differential equations in the unit disc, Ann. Polo. Math. 97(2010), no. 1, 51-61. [10] T. B. Cao, L. M. Li, J. Tu and H. Y. Xu, Complex oscillation of differential polynomials generated by analytic solutions of differential equations in the unit disc, Math. Commun. 16 (2011), no. 1, 205–214. [11] Z. X. Chen and K. H. Shon, The growth of solutions of differential equations with coefficients of small growth in the disc, J. Math. Anal. Appl. 297 (2004), no. 1, 285–304. [12] I. E. Chyzhykov, G. G. Gundersen and J. Heittokangas, Linear differential equations and logarithmic derivative estimates, Proc. London Math. Soc. (3) 86 (2003), no. 3, 735–754. [13] A. El Farissi, B. Beläıdi and Z. Latreuch, Growth and oscillation of differential polynomials in the unit disc, Electron. J. Diff. Equ., Vol. 2010(2010), No. 87, 1-7. [14] W. K. Hayman, Meromorphic functions, Oxford Mathematical Monographs Clarendon Press, Oxford, 1964. [15] J. Heittokangas, On complex differential equations in the unit disc, Ann. Acad. Sci. Fenn. Math. Diss. 122 (2000), 1-54. [16] J. Heittokangas, R. Korhonen and J. Rättyä, Fast growing solutions of linear differential equations in the unit disc, Results Math. 49 (2006), no. 3-4, 265–278. [17] L. Kinnunen, Linear differential equations with solutions of finite iterated order, Southeast Asian Bull. Math. 22 (1998), no. 4, 385-405. [18] I. Laine, Nevanlinna theory and complex differential equations, de Gruyter Studies in Math- ematics, 15. Walter de Gruyter & Co., Berlin-New York, 1993. [19] I. Laine and J. Rieppo, Differential polynomials generated by linear differential equations, Complex Var. Theory Appl. 49 (2004), no. 12, 897–911. [20] I. Laine, Complex differential equations, Handbook of differential equations: ordinary differ- ential equations. Vol. IV, 269–363, Handb. Differ. Equ., Elsevier/North-Holland, Amsterdam, 2008. [21] Z. Latreuch and B. Beläıdi, Growth and oscillation of differential polynomials generated by complex differential equations, Electron. J. Diff. Equ., Vol. 2013 (2013), No. 16, 1-14. [22] M. Tsuji, Potential Theory in Modern Function Theory, Chelsea, New York, (1975), reprint of the 1959 edition. Department of Mathematics, Laboratory of Pure and Applied Mathematics, Univer- sity of Mostaganem (UMAB), B. P. 227 Mostaganem-(Algeria) ∗Corresponding author