Processing math: 100%
Research article

Infinite growth of solutions of second order complex differential equations with meromorphic coefficients

  • Received: 25 December 2021 Revised: 18 January 2022 Accepted: 19 January 2022 Published: 26 January 2022
  • MSC : 30D35, 34M10, 37F10

  • This paper is devoted to studying the growth of solutions of f+A(z)f+B(z)f=0, where A(z) and B(z) are meromorphic functions. With some additional conditions, we show that every non-trivial solution f of the above equation has infinite order. In addition, we also obtain the lower bound of measure of the angular domain, in which the radial order of f is infinite.

    Citation: Zheng Wang, Zhi Gang Huang. Infinite growth of solutions of second order complex differential equations with meromorphic coefficients[J]. AIMS Mathematics, 2022, 7(4): 6807-6819. doi: 10.3934/math.2022379

    Related Papers:

    [1] Zhuo Wang, Weichuan Lin . The uniqueness of meromorphic function shared values with meromorphic solutions of a class of q-difference equations. AIMS Mathematics, 2024, 9(3): 5501-5522. doi: 10.3934/math.2024267
    [2] Dan-Gui Yao, Zhi-Bo Huang, Ran-Ran Zhang . Uniqueness for meromorphic solutions of Schwarzian differential equation. AIMS Mathematics, 2021, 6(11): 12619-12631. doi: 10.3934/math.2021727
    [3] Erhan Deniz, Hatice Tuǧba Yolcu . Faber polynomial coefficients for meromorphic bi-subordinate functions of complex order. AIMS Mathematics, 2020, 5(1): 640-649. doi: 10.3934/math.2020043
    [4] Linkui Gao, Junyang Gao . Meromorphic solutions of fn+Pd(f)=p1eα1z+p2eα2z+p3eα3z. AIMS Mathematics, 2022, 7(10): 18297-18310. doi: 10.3934/math.20221007
    [5] Pan Gong, Hong Yan Xu . Oscillation of arbitrary-order derivatives of solutions to the higher order non-homogeneous linear differential equations taking small functions in the unit disc. AIMS Mathematics, 2021, 6(12): 13746-13757. doi: 10.3934/math.2021798
    [6] Yongxiang Zhu, Min Zhu . Well-posedness and order preservation for neutral type stochastic differential equations of infinite delay with jumps. AIMS Mathematics, 2024, 9(5): 11537-11559. doi: 10.3934/math.2024566
    [7] Cai-Mei Yan, Jin-Lin Liu . On second-order differential subordination for certain meromorphically multivalent functions. AIMS Mathematics, 2020, 5(5): 4995-5003. doi: 10.3934/math.2020320
    [8] Rana M. S. Alyoubi, Abdelhalim Ebaid, Essam R. El-Zahar, Mona D. Aljoufi . A novel analytical treatment for the Ambartsumian delay differential equation with a variable coefficient. AIMS Mathematics, 2024, 9(12): 35743-35758. doi: 10.3934/math.20241696
    [9] Chunmei Song, Qihuai Liu, Guirong Jiang . Harmonic and subharmonic solutions of quadratic Liénard type systems with sublinearity. AIMS Mathematics, 2021, 6(11): 12913-12928. doi: 10.3934/math.2021747
    [10] Yongyi Gu, Najva Aminakbari . Two different systematic methods for constructing meromorphic exact solutions to the KdV-Sawada-Kotera equation. AIMS Mathematics, 2020, 5(4): 3990-4010. doi: 10.3934/math.2020257
  • This paper is devoted to studying the growth of solutions of f+A(z)f+B(z)f=0, where A(z) and B(z) are meromorphic functions. With some additional conditions, we show that every non-trivial solution f of the above equation has infinite order. In addition, we also obtain the lower bound of measure of the angular domain, in which the radial order of f is infinite.



    Throughout this paper, we assume that the reader is familar with the fundamental results and the standard notations of Nevanlinna's value distribution theory (see [9,14,28]). In addition, we use ρ(f) and μ(f) to denote the order and lower order of a meromorphic function f(z) respectively, which are defined as

    ρ(f)=lim suprlog+T(r,f)logr,μ(f)=lim infrlog+T(r,f)logr.

    The second order linear differential equation

    f+A(z)f+B(z)f=0, (1.1)

    where A(z) and B(z) are meromorphic functions, is the focus of this paper. To begin, we look for the conditions of coefficients that guarantee that every non-trivial meromorphic solution of Eq (1.1) has infinite order. Every non-trivial solution of Eq (1.1) must be an entire function, if A(z) and B(z) are entire functions, as is widely known. When A(z) and B(z) are entire functions, a lot of progress has been made, see Gundersen [5], Hellerstein, Miles and Rossi [10], and Ozawa [19]. The following is a summary of their work.

    Theorem A. Suppose that A(z) and B(z) are entire functions satisfying any one of the following additional hypotheses:

    (1) ρ(A)<ρ(B), see [5];

    (2) A(z) is a polynomial and B(z) is transcendental, see [10];

    (3) ρ(B)<ρ(A)12, see [19].

    Then, every non-trivial solution f of Eq (1.1) is of infinite order.

    One may ask a question based on Theorem A.

    Question 1: If ρ(A)=ρ(B), or if ρ(A)>ρ(B) and ρ(A)>12, is every non-trivial solution f of Eq (1.1) is of infinite order?

    In general, the answer to Question 1 is negative.

    Example 1.1. Let Q(z) be any non-constant polynomial, let B(z)0 be any entire function with ρ(B)<deg(Q), let f be any antiderivative of eQ(z) that satisfies ρ(f)=deg(Q), and set A(z)=QB(z)feQ. Then ρ(B)<ρ(A)=deg(Q)=ρ(f), and f+A(z)f+B(z)f=0. This shows that it is possible to have a finite order non-trivial solution f of Eq (1.1) where ρ(B)<ρ(A) and ρ(A) may be any positive integer.

    Example 1.2 Let Q(z) be any non-constant polynomial, let A(z)0 be any entire function, and set B(z)=Q(Q)2A(z)Q. Then ρ(A)=ρ(B) and it can be verifies that f(z)=eQ(z) satisfies the equation f+A(z)f+B(z)f=0. This shows that it is possible to have a finite order non-trivial solution f of Eq (1.1) where ρ(A)=ρ(B).

    In some special cases, however, an entire solution of Eq (1.1) can have infinite order, see, for example, [3,13,15,16,22,23]. Gundersen [8] took into account a special case in which the coefficient A(z) of Eq (1.1) is an exponential function.

    Theorem B. [8] Let A(z)=ez and B(z) is a transcendental entire function with order ρ(B)1. Then every non-trivial solution f of Eq (1.1) has infinite order.

    When ρ(B)=1, the entire solution of Eq (1.1) may be finite order, according to Theorem B. What conditions can guarantee that every non-trivial solution f of Eq (1.1) has infinite order if ρ(B)=1? Chen [3] considered this question and proved the following result.

    Theorem C. [3] Suppose that Aj(z)(j=0,1) are entire functions with ρ(Aj)<, a and b are complex constants with ab0 and a=cb(c>1). Let A(z)=A1(z)eaz, B(z)=A2(z)ebz. Then every non-trivial solution f of Eq (1.1) has infinite order.

    Remark 1.1. Because ρ(A)=1 and ρ(B)1 in Theorem B, ρ(A)>ρ(B) and ρ(A)>12 can occur, whereas ρ(A)=ρ(B)=1 in Theorem C. As a result, Theorems B and C partially answer Question 1 as well.

    Question 1 was recently studied by several scholars who assumed that A(z) is a nontrivial solution of a second order differential equation. We have the following collection theorem.

    Theorem D. Let A(z) be a nontrivial solution of w+P(z)w=0, where P(z) is a nonconstant polynomials with deg(P)=n, and satisfying any one of the following additional hypotheses:

    (1) ρ(B)<12, see [24];

    (2) B(z) is an entire function with Fabry gaps, see [16]; Here, an entire function f(z)=n=0anzλn is said to have Fabry gaps if λnn as n.

    (3) T(r,B)logM(r,B) as r outside a set of finite logarithmic measure such that ρ(A)ρ(B), see [29]. Then every nontrivial solution of Eq (1.1) is of infinite order.

    Remark 1.2. We know that ρ(A)=n+22 based on Theorem D's assumptions. Clearly, Theorem D partially answers Question 1 because ρ(A)=ρ(B) or ρ(A)>ρ(B) with ρ(A)>12 can occur if B(z) meets one of the conditions (1)-(3) in Theorem D. We also find that the proof of three cases of Theorem D is based on the observation that if A(z) is a nontrivial solution of w+P(z)w=0, then the whole plane may be divided into n+2 sectors Sj(j=0,1,,n+1) in which A(z) either blows up or decays to zero exponentially.

    We will continue to study Question 1 in this paper. We consider a more general case in which A(z) in some angular domains either blows up or decays to zero rapidly. The coefficients of Eq (1.1) in particular, are meromorphic rather than entire.

    Theorem 1.1. Let {ϕk} be a finite set of real numbers satisfying ϕ1<ϕ2<...<ϕ2n<ϕ2n+1 with ϕ2n+1=ϕ1+2π, and set

    v=max1k2n(ϕk+1ϕk).

    Suppose that A(z) and B(z) are meromorphic functions such that for some constant α0 and a set H[0,2π) of linear measure zero,

    |A(z)|=O(|z|α)

    as z in argz(ϕ2k1,ϕ2k)H for k=1,...,n, and where B(z) is transcendental with a deficient value and

    μ(B)<4arcsinδ(,B)2v.

    Then every non-trivial meromorphic solution f of Eq (1.1) has infinite order.

    Remark 1.3. We can use a specific example to illustrate our point. If A(z)=eP(z), where P(z) is a polynomial with deg(P)=n, and B(z) is an entire function with μ(B)<n, then the example meets Theorem 1.1's criteria.

    Corollary 1.1. Suppose that A(z)=h1(z)ep1(z)+h2(z)ep2(z)+p3(z), where p3(z) is a polynomial, pi(z)=aizn+...(i=1,2) are two non-constant polynomials of degree n with arga1arga2±π, and hi(z)(i=1,2) are meromorphic functions of order less than n. Let B(z) be given as Theorem 1.1. Then every non-trivial solution f of Eq (1.1) has infinite order.

    Remark 1.4. For p1(z) and p2(z), from remark 2.1, there exist Ωk(p1) and Ωk(p2) such that when k is odd, δ(p1,θ)<0 if θΩk(p1) and δ(p2,θ)<0 if θΩk(p2). Since arga1arga2±π, Ωk(p1)Ωk(p2). Then we can redivide the plane into 2n open angles Sj(j=0,1,...,2n1) such that for θSj, δ(p1,θ)<0 and δ(p2,θ)<0 if j is odd, while δ(p1,θ)0 or δ(p2,θ)0 if j is even. Suppose that deg(p3)=m. By Lemma 2.3, we know |A(reiθ)|=O(rm) in Sj outside a set of linear measure zero when j is odd. By Theorem 1.1, Corollary 1.1 holds.

    Corollary 1.2. Suppose A(z)=h1(z)ep1(z)+h2(z)ep2(z)+p3(z), where p3 is a polynomial, pi(i=1,2) are two non-constant polynomials with deg(p1)deg(p2), and hi(z)(i=1,2) are meromorphic functions of order less than deg(pi). Let B(z) be given as Theorem 1.1. Then every non-trivial solution f of Eq (1.1) has infinite order.

    Remark 1.5. Let p1(z)=anzn+...+a0, p2(z)=btzt+...+b0. Similarly as remark 1.4, we also can redivide the plane into 2s open angles Sj(j=0,1,...,2s1) where s may be different from n and t, and depends on deg(pi)(i=1,2), an and bt, such that for θSj, δ(p1,θ)<0 and δ(p2,θ)<0 if j is odd; while j is even, δ(p1,θ)0 or δ(p2,θ)0. Then Corollary 1.2 holds.

    Next, we consider the lower bound estimate of the measure of the angular domain, in which the radial order of every non-trivial solution of (1.1) is infinite. The following notations and notions are provided to further illustrate our concerns.

    Assuming 0α<β2π, we denote

    Ω(α,β)={zC:argz(α,β)},

    and use ¯Ω(α,β) to denote the closure of Ω(α,β). Similarly, we denote

    Ω(r,α,β)={zC:argz(α,β),|z|>r}.

    Suppose that f(z) is an analytic function in ¯Ω(α,β), we use ρα,β to denote the order of growth of f on Ω(α,β), that is

    ρα,β(f)=lim suprlog+log+M(r,Ω(α,β),f)logr,

    where M(r,Ω(α,β),f)=supαθβ|f(reiθ)|. Furthermore, we denote the radial order of f(z) by

    ρθ(f)=limε0lim suprlog+log+M(r,Ω(θε,θ+ε),f)logr.

    In recent years, some progress in the angular distribution of entire solutions of linear differential equations have been obtained by several researchers, see [12,20,21,24,25,26,27]. In particular, Huang and Wang [11] considered the following question. We know that for a transcendental entire function f(z) of infinite order, at least one ray argz=θ exists with the radial order ρθ(f)=. However, for any angular domain Ω(α,β), ρ(f)= cannot ensure ρα,β(f)=, f(z)=eez, for example, satisfies ρ(f)=, whereas ρπ/2,3π/2(f)=0. Motivated by this fact, we raise an interesting question: how wide are such Ω(α,β) with ρα,β(f)=? Let

    I(f)={θ[0,2π):ρθ(f)=}.

    Clearly, I(f) is closed and measurable. In 2015, Huang and Wang [11] proved the following result.

    Theorem E. Suppose that A(z), B(z) are entire function with ρ(A)<μ(B). If f(z) is a non-trivial solution of Eq (1.1), then mesI(f)min{2π,π/μ(B)}.

    Inspired by Theorem E, we consider the lower bound of measure of the set of infinite radial order solutions of Eq (1.1). As a result, we have the following.

    Theorem 1.2. Let A(z) be an entire function of finite order having a finite Borel exceptional value, and B(z) be a transcendental entire function with μ(B)<ρ(A). Then, every non-trivial solution f of Eq (1.1) is of infinite order and satisfies mes(I(f))min{k1,k2}, where k1:=π, k2:={[ρ(A)/μ(B)]2πρ(A),if[ρ(A)μ(B)]is evenπμ(B)[ρ(A)/μ(B)]+12πρ(A),if[ρ(A)μ(B)]is odd.

    Remark 1.6. In Theorem 1.2, we use [x] to denote the largest integer not exceeding the real number x, for example, [1.2]=1.

    Remark 1.7. Under the assumptions of Corollary 1.1, we know every non-trivial solution f of Eq (1.1) is an entire function with infinite order. Hence, from the proof of Theorem 1.2, we obtain that mes(I(f))k1 if μ(B)[0,12), while mes(I(f))k2 if μ(B)[12,ρ(A)).

    Lemma 2.1. [17] Let f be an entire function of finite order having a finite Borel exceptional value c. Then

    f(z)=h(z)eQ(z)+c,

    where h(z) is an entire function with ρ(h)<ρ(f), Q(z) is a polynomial of degree deg(Q)=ρ(f).

    Lemma 2.2. [6] Let g(z) be a transcendental meromorphic function of order ρ(g)=ρ<. Then there exists a set E[0,2π) of linear measure zero such that, for any θ[0,2π)E, there exists a positive constant R0=R0(θ)>1 such that, for all z satisfying argz=θ and |z|>R0,

    |g(k)(z)g(z)||z|k(ρ(g)1+ε),

    where k=1,2 and ε is given positive real constant.

    Remark 2.1. For the polynomial p(z) with degree n, set p(z)=(α+iβ)zn+pn1(z) with α,β real, and denote δ(p,θ):=αcosnθβcosnθ. The rays

    argz=θk=arctanαβ+kπn,k=0,1,2,...,2n1

    satisfying δ(p,θk)=0 can split the complex domain into 2n equal angles. We denote these angle domains as

    Ωk(p)={θ:arctanαβn+(2k1)π2n<θ<arctanαβn+(2k+1)π2n},k=0,1,...,2n1.

    And we know that for θΩk(p), δ(p,θ)>0 if k is even, while δ(p,θ)<0 if k is odd.

    Lemma 2.3. [4,Lemma 1.20] Let p(z) be a polynomial of degree n1. Suppose that h(z)0 is a meromorphic function and ρ(h)<n. Consider the function g(z):=h(z)ep(z), there exists a set H1[0,2π) of linear measure zero, for every θ[0,2π)(H1H2) and r>r0(θ)>0, we have

    (1) If δ(p,θ)>0,

    |g(reiθ)|exp{12δ(p.θ)rn}

    holds here;

    (1) If δ(p,θ)<0,

    |g(reiθ)|exp{12δ(p.θ)rn}

    holds here, where H2={θ:δ(p,θ)=0,0θ<2π} is a finite set.

    The following lemma due to Markushevich [18].

    Lemma 2.4. [18] Suppose f(z)=eP(z), where P(z) is a polynomial of degree n:

    P(z)=bnzn+bn1zn1+...+b0(bn0,n1).

    We know that f(z) is a function of order n. Let bn=αneiθn, αn>0, θn[0,2π) and z=reiθ, we now divide the plane into 2n equal open angles

    Sj={θ:θnn+(2j1)π2n<θ<θnn+(2j+1)π2n},

    where j=0,1,2,...,2n1. We also introduce 2n closed angles

    Sj(ε)={θ:θnn+(2j1)π2n+εnθθnn+(2j+1)π2nεn},j=0,1,2,...,2n1,

    where 0<ε<π/2 and Sj(ε)Sj. Then there exists a positive number R=R(ε) such that for |z|=r>R,

    |f(z)|>exp{αn(1ε)sin(nε)rn}

    if argzSj(ε) when j is even; While

    |f(z)|<exp{αn(1ε)sin(nε)rn}

    if argzSj(ε) when j is odd.

    Remark 2.2. Clearly, for any argzSj, we always find an ε, ε(0,π/2) and a positive number R=R(ε) such that argzSj(ε), and for |z|=r>R,

    |f(z)|>exp{αn(1ε)sin(nε)rn}

    if j is even; While

    |f(z)|<exp{αn(1ε)sin(nε)rn}

    if j is odd.

    Lemma 2.5. [1] Suppose that g(z) is an entire function with μ(g)[0,1). Then, for every α(μ(g),1), there exists a set E[0,) such that ¯logdensE1μ(g)α, where E={r[0,):m(r)>M(r)cosπα}, m(r)=inf|z|=rlog|g(z)| and M(r)=sup|z|=rlog|g(z)|.

    Lemma 2.6. [22] Suppose that f is an entire function and lower order μ(f)[12,+). Then, there exists an domain Ω(α,β), where α,β satisfy βαπμ(f) and 0αβ2π, such that

    limsuprloglog|f(reiψ)|logrμ(f)

    for all ψ(α,β).

    Lemma 2.7. [7] Let z=rexp(iψ),r0+1<r and αψβ, where 0<βα2π. Suppose that n(2) is an integer, and that g(z) is analytic in Ω(r0,α,β) with ρα,β<. Choose α<α1<β1<β. Then, for every ε(0,βjαj2)(j=1,2,...,n1) outside a set of linear measure zero with

    αj=α+j1s=1εsandβj=β+j1s=1εs,j=2,3,...,n1,

    there exist K>0 and M>0 only depending g, ε1,...,εn1 and Ω(αn1,βn1), and not depend on z such that

    |g(z)g(z)|KrM(sink(ψα))2

    and

    |g(n)(z)g(z)|KrM(sink(ψα)n1j=1sinkj(ψαj))2

    for all zΩ(αn1,βn1) outside an R-set D, where k=π/(βα) and kεj=π/(βjαj(j=1,2,...,n1)).

    Lemma 2.8. [2] Let f(z) be a transcendental meromorphic function of finite lower order μ, and have one deficient value a. Let Λ(r) be a positive function with Λ(r)=o(T(r,f)) as r. Then for any fixed sequence of Pólya peaks {rn} of order μ, we have

    lim infnmesDΛ(rn,a)min{2π,4μarcsinδ(a,f)2},

    where DΛ(r,a) is defined by

    DΛ(r,)={θ[0,2π):|f(reiθ)|>eΛ(r)},

    and for finite a,

    DΛ(r,a)={θ[0,2π):|f(reiθ)a|<eΛ(r)}.

    Suppose on the contrary to the assertion that there exists a non-trivial solution f with ρ(f)<. We aim for a contradiction. Let {ϕk} be a finite collection of real numbers satisfying ϕ1<ϕ2<...<ϕ2n<ϕ2n+1 with ϕ2n+1=ϕ1+2π, and set

    v=max1k2n(ϕk+1ϕk).

    Suppose that A(z) is a meromorphic function such that for some constant α0 and a set H[0,2π) of linear measure zero,

    |A(z)|=O(|z|α) (3.1)

    as z in argz(ϕ2k1,ϕ2k)H for k=1,...,n. From Eq (1.1), we get the following inequality

    |B(z)||f(z)f(z)|+|f(z)f(z)||A(z)|. (3.2)

    From Lemma 2.2, we can obtain that there exists a set E[0,2π) of linear measure zero and a positive constant R0>1 such that

    |f(reiθ)f(reiθ)|rρ(f),|f(reiθ)f(reiθ)|r2ρ(f), (3.3)

    for any θ[0,2π)E and r>R0.

    Let B(z) be a transcendental meromorphic function having a deficient value and μ(B)<4arcsinδ(,B)2/v. Then we have

    4μ(B)arcsinδ(,B)2>v. (3.4)

    Next, we define

    Λ(r)=T(r,B)logr.

    It is clear that Λ(r)=o(T(r,B)) and Λ(r)/logr as r since B(z) is a transcendental meromorphic function. Applying Lemma 2.8 to B(z) gives the existence of the Pólya peaks {rj} of order μ(B) such that for sufficiently large j,

    mesDΛ(rj,)min{2π,4μ(B)arcsinδ(,B)2},

    where DΛ(rj,) is defined by

    DΛ(rj,)={θ[0,2π):|B(rjeiθ)|>eΛ(rj)}.

    From (3.4), there exists at least one sector (ϕ2k1,ϕ2k) such that

    mes((ϕ2k1,ϕ2k)DΛ(rj,))>0,

    where k=1,...,n.

    Let Fj:=(ϕ2k1,ϕ2k)DΛ(rj,). On the one hand, for any θFj and sufficiently large j, we have

    |B(rjeiθ)|>exp{Λ(rj)}.

    Since Λ(r)/logr as r,

    limjlog|B(rjeiθ)|logrj=. (3.5)

    Substituting (3.1) and (3.3) into (3.2), for any θFj(EH) and sufficiently large j, we have

    |B(rjeiθ)|<O(r2ρ(f)+αj), (3.6)

    where α0 is a constant. Coupling (3.5)and (3.6) yields a contradiction. Thus, every non-trivial solution f of Eq (1.1) is of infinite order.

    We assume the contrary to the assertion that m(I(f))<k, where k=k1 or k2. Then t:=kmesI(f)>0. Our goal is to obtain a contradiction. Since I(f) is closed, H:=(0,2π)I(f) is open. So it consists of at most countably many open intervals. We can choose finitely many open intervals Ii=(αi,βi)(i=1,2,...,m) in H such that

    mes(Hmi=1Ii)<t4. (4.1)

    It easy to see that IiI(f)=, and hence ραi,βi(f)< for each i=1,2,...,m. Apply Lemma 2.7 to f, for sufficiently small ξ>0, there exist two constants M>0 and K>0 such that

    |f(s)(z)f(z)|KrM,(s=1,2) (4.2)

    for all zmi=1Ω(rj,αi+ξ,βiξ) outside an R-set D.

    Suppose that A(z) is an entire function of finite order having a finite Borel exceptional value a. By Lemma 2.1, we have

    A(z)=h(z)eQ(z)+a,

    where h(z) is an entire function with ρ(h)<ρ(A), Q(z) is a polynomial of degree deg(Q)=ρ(A). Let Q(z)=bdzd+bd1zd1+...+b0, where d is a positive integer and bd=αdeiθd, αd>0 and θd[0,2π). We now divide the plane into 2d equal open angles

    Sj={θ:θdd+(2j1)π2d<θ<θdd+(2j+1)π2d},

    where j=0,1,2,...,2d1. We also introduce 2d closed angles

    Sj(ε)={θ:θdd+(2j1)π2d+εdθθdd+(2j+1)π2dεd},j=0,1,2,...,2d1,

    where 0<ε<π/4 and Sj(ε)Sj. According to Lemma 2.4, for z=reiθ, if θSj(ε) and j is odd, there exists a positive number R(ε), such that

    |eQ(z)|<exp{αd(1ε)sin(dε)rd}

    for r>R(ε). Then for any given ε(0,π/4), ρ(h)<d=ρ(A) and θSj(ε)(j is odd), we have

    |A(reiθ)a|<exp{C(ε)rd},

    for all sufficiently large r, where C(ε) is a positive only constant depending on αd, ε and ρ(A). Therefore, for any θSj(j is odd), we can find an ε and a positive constant C(ε) such that θSj(ε) and

    |A(reiθ)||A(reiθ)a|+|a|<exp{C(ε)rd}+|a| (4.3)

    for all sufficiently large r. From Eq (1.1), we have

    |B(z)||f(z)f(z)|+|f(z)f(z)||A(z)|. (4.4)

    In the following, we consider three cases.

    Case 1. Suppose μ(B)=0. Then k=k1. Define

    S:=di=1S2i1.

    Clearly, mes S=π. Thus,

    mes(SH)=mes(S(I(f)S))mes(S)mes(I(f))>3t4.

    Hence

    mes((mi=1Ii)S)=mes(SH)mes((Hmi=1Ii)S)>3t4t4=t2.

    Then we can conclude that exists at least one open interval Ii0=(α0,β0) such that

    mes(S(α0,β0))>t2m>0,

    and there exists at least one sector Sj(j is odd) such that

    mes(Sj(α0,β0))>t2md>0.

    We can find an ε>0 such that mes(Sj(ε)(α0,β0))>0. So D(ε):=Sj(ε)(α0+ξ,β0ξ), where 0<ξ<mes(Sj(ε)(α0,β0))/4. Applying Lemma 2.5 to B(z), we can choose α=14 and there is a set E[0,) such that ¯logdensE=1 such that, for all rE,

    log|B(reiθ)|>22logM(r,B),θ[0,2π) (4.5)

    where M(r,B)=sup|z|=r|B(z)|. By substituting (4.5), (4.3) and (4.2) into (4.4), for any θD(ε) and rE outside an R-set D, we have

    M(r,B)22<KrM(1+exp{C(ε)rd}+|a|) (4.6)

    for all sufficiently large r. Since B(z) is a transcendental entire function, we know that

    lim infrlogM(r,B)logr=+. (4.7)

    From (4.6) and (4.7), we can deduce a contradiction. Therefore, mes(I(f))k1.

    Case 2. Suppose 0<μ(B)<12. So k=k1. Similarly as in Case 1, we have a sector D(ε):=Sj(ε)(α0+ξ,β0ξ). According to Lemma 2.5, for any given α(μ(B),12), there exists a set E[0,) such that ¯logdensE1μ(B)α, where E={r[0,):m(r)>M(r)cosπα}, m(r)=inf|z|=rlog|B(z)| and M(r)=sup|z|=rlog|B(z)|. Thus, there exists a constant R1>0 such that, for arbitrarily small η>0 and all rE[0,R1],

    |B(reiθ)|exp{rμ(B)η},θ[0,2π). (4.8)

    Taking (4.8), (4.3) and (4.2) into (4.4), for any θD(ε) and rE[0,R1] outside an R-set D, we deduce

    exp{rμ(B)η}<KrM(1+exp{Crd}+|a|) (4.9)

    for all sufficiently large r. This is a contradiction. Therefore, mes(I(f))k1.

    Case 3. Suppose 12μ(B)<ρ(A). So k=k2. By using Lemma 2.6 to B(z), we can get a sector Ω(α,β) with βαπμ(B)>πρ(A)=πd, which satisfies

    lim suprloglog|B(reiθ)|logrμ(B)

    for all θ(α,β). That is, there exist a sequence {rn} such that, for arbitrarily small η>0,

    |B(rneiθ)|exp{rμ(B)ηn},θ(α,β). (4.10)

    Let

    G:=S(α,β).

    Clearly, mes(G)k2. By using the similar method in Case 1, we have at least one open interval Ii1=(α1,β1) such that

    mes(G(α1,β1))>t2m>0.

    Then there exists at least one sector Sj(j is odd) such that

    mes(Sj(α0,β0))>t2md>0.

    We can find an ε>0 such that mes (Sj(ε)(α1,β1))>0. So F(ε):=Sj(ε)(α1+ξ,β1ξ). Substituting (4.10), (4.3) and (4.2) into (4.4), for any argz=θF(ε) and {rn} outside an R-set D, we have

    exp{rμ(B)ηn}<KrMn(1+exp{Crdn}+|a|) (4.11)

    for all sufficiently large n. A contradiction. Therefore, mes(I(f))k2.

    All authors declare no conflicts of interest in this paper.



    [1] P. D. Barry, Some theorems related to the cosπρ theorem, Proc. Lond. Math. Soc., 21 (1970), 334–360. https://doi.org/10.1112/plms/s3-21.2.334 doi: 10.1112/plms/s3-21.2.334
    [2] A. Baernstein, Proof of Edreis spread conjecture, Proc. Lond. Math. Soc., 26 (1973), 418–434. https://doi.org/10.1112/plms/s3-26.3.418 doi: 10.1112/plms/s3-26.3.418
    [3] Z. X. Chen, The growth of solutions of the differential equation f+ezf+Q(z)f=0, Sci. China Ser. A, 45 (2002), 290–300. https://doi.org/10.1360/02ye9035 doi: 10.1360/02ye9035
    [4] S. A. Gao, Z. X. Chen, T. W. Chen, Complex Oscillation Theory of Linear Differential Equations, Wuhan: Huazhong University of Science and Technology Press, 1998 (Chinese).
    [5] G. G. Gundersen, Finite order solutions of second order linear differential equations, Trans. Amer. Math. Soc., 305 (1988), 415–429. https://doi.org/10.1090/S0002-9947-1988-0920167-5 doi: 10.1090/S0002-9947-1988-0920167-5
    [6] G. G. Gundersen, Estimates for the logarithmic derivative of a meromorphic function, plus similar estimates, J. Lond. Math. Soc., 37 (1998), 88–104.
    [7] G. G. Gundersen, On the real zeros of solutions of f+A(z)f=0, where A(z) is entire, Ann. Acad. Sci. Fenn. Math., 11 (1986), 275–294. https://doi.org/10.5186/aasfm.1986/1105 doi: 10.5186/aasfm.1986/1105
    [8] G. G. Gundersen, On the question of whether f+ezf+Q(z)=0 can admit a solution f0 of finite order, Pro. Roy. Soc. Edinburgh Sect. A, 102 (1986), 9–17. https://doi.org/10.1017/S0308210500014451 doi: 10.1017/S0308210500014451
    [9] W. K. Hayman, Meromorphic Functions, Clarendon Press, Oxford, 1964.
    [10] S. Hellerstein, J. Miles, J. Rossi, On the growth of solutions of f+gf+hf=0, Trans. Amer. Math. Soc., 324 (1991), 693–705. https://doi.org/10.1056/NEJM199103073241027 doi: 10.1056/NEJM199103073241027
    [11] Z. G. Huang, J. Wang, The radial oscillation of entire solutions of complex differential equations, J. Math. Anal. Appl., 431 (2015), no. 2,988–999.
    [12] Z.B.Huang, Z.X.Chen, Angular distribution with hyper-order in complex oscillation theory, Acta Math Sinica, 50 (2007), 601–614. https://doi.org/10.1080/00140130601154954 doi: 10.1080/00140130601154954
    [13] I. Laine, P. C. Wu, Growth of solutions of second order linear differential equations, Proc. Amer. Math. Soc., 128 (2000), 2693–2703. https://doi.org/10.1090/S0002-9939-00-05350-8 doi: 10.1090/S0002-9939-00-05350-8
    [14] I. Laine, Nevanlinna Theory and Complex Differential Equations, Walter de Gruyter, Berlin, 1993. https://doi.org/10.1515/9783110863147
    [15] S. T. Lan, Z. X. Chen, On the growth of meromorphic solutions of difference equations, Ukrainian Mathematical Journal, 68 (2017), 1561–1570.
    [16] J. R. Long, Growth of solutions of second order linear differential equations with extremal functions for Denjoy's conjecture as coeffcients, Tamkang J. Math., 47 (2016), 237–247. https://doi.org/10.5556/j.tkjm.47.2016.1914 doi: 10.5556/j.tkjm.47.2016.1914
    [17] J. R. Long, Growth of solutions of second order complex linear differential equations with entire coefficients, Filomat, 32 (2018), 275–284. https://doi.org/10.2298/FIL1801275L doi: 10.2298/FIL1801275L
    [18] A. I. Markushevich, Theory of Functions of a Complex Variable, Vol.II, Revised English Edition Translated and Edited by Richard A. Silverman. Prentice-Hall, Inc., Englewood Cliffs, N. J., 1965.
    [19] M. Ozawa, On a solution of w+ezw+(az+b)w=0, Kodai Math. J., 3 (1980), 295–309.
    [20] L. Qiu, S. J. Wu, Radial distributions of Julia sets of meromorphic functions, J. Aust. Math. Soc., 81 (2006), 363–368. https://doi.org/10.1017/S1446788700014361 doi: 10.1017/S1446788700014361
    [21] L. Qiu, Z. X. Xuan, Y. Zhao, Radial distribution of Julia sets of some entire functions with infinite lower order, Chinese Ann. Math. Ser. A, 40 (2019), 325–334.
    [22] X. B. Wu, J. R. Long, J. Heittokangas, K. E. Qiu, Second-order complex linear differential equations with special functions or extremal functions as coefficients, Electronic J. Differential Equa., 143 (2015), 1–15. https://doi.org/10.5089/9781513546261.002 doi: 10.5089/9781513546261.002
    [23] P. C. Wu, J. Zhu, On the growth of solutions of the complex differential equation f+Af+Bf=0, Sci. China Ser. A, 54 (2011), 939–947. https://doi.org/10.1007/s11425-010-4153-x doi: 10.1007/s11425-010-4153-x
    [24] S. J. Wu, Angular distribution in complex oscillation theory, Sci. China Math, 48 (2005), 107–114. https://doi.org/10.1360/03YS0159 doi: 10.1360/03YS0159
    [25] S. J. Wu, On the growth of solution of second order linear differential equations in an angle, Complex. Var. Elliptic, 24 (1994), 241–248. https://doi.org/10.1080/17476939408814716 doi: 10.1080/17476939408814716
    [26] N. Wu, Growth of solutions to linear complex differential equations in an angular region, Electron. J. Diff. Equ, 183 (2013), 1–8.
    [27] J. F. Xu, H. X. Yi, Solutions of higher order linear differential equation in an angle, Appl. Math. Lett, 22 (2009), 484–489.
    [28] L. Yang, Value Distribution Theory, Springer, Berlin, 1993.
    [29] G. W. Zhang, L. Z. Yang, Infinite growth of solutions of second order complex differential equations with entire coefficient having dynamical property, Appl. Math. Lett., 112 (2021), 1–8.
  • Reader Comments
  • © 2022 the Author(s), licensee AIMS Press. This is an open access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/4.0)
通讯作者: 陈斌, bchen63@163.com
  • 1. 

    沈阳化工大学材料科学与工程学院 沈阳 110142

  1. 本站搜索
  2. 百度学术搜索
  3. 万方数据库搜索
  4. CNKI搜索

Metrics

Article views(2460) PDF downloads(79) Cited by(0)

Other Articles By Authors

/

DownLoad:  Full-Size Img  PowerPoint
Return
Return

Catalog