In this article, we mainly use Nevanlinna theory to investigate some differential-difference equations. Our results about the existence and the forms of solutions for these differential-difference equations extend the previous theorems given by Wang, Xu and Tu [
Citation: Yong Liu, Chaofeng Gao, Shuai Jiang. On meromorphic solutions of certain differential-difference equations[J]. AIMS Mathematics, 2021, 6(9): 10343-10354. doi: 10.3934/math.2021599
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In this article, we mainly use Nevanlinna theory to investigate some differential-difference equations. Our results about the existence and the forms of solutions for these differential-difference equations extend the previous theorems given by Wang, Xu and Tu [
We assume that the reader is familiar with the basic notions of Nevanlinna theory (see [4,6,22]). Recently, a number of papers (including [1,2,3,5,7,8,9,10,11,12,13,14,15,16,17,18,19,20,21,23]) have focused on solvability and existence of meromorphic solutions of difference equations or differential-difference equations in complex plane. In 2009, Liu [10] obtianed the Fermat type equation l(z)2+[l(z+c)−l(z)]2=1 has a nonconstant entire solution of finite order. In 2012, Liu et al. [11] proved that l(z)2+l(z+c)2=1 has a transcendental entire solution of finite order. In 2018, Zhang [23] obtained the difference equations l(z)2+[l(z+c)−l(z)]2=R(z) has no finite order transcendental meromorphic solutions with finitely many poles. In 2020, Wang et al. [18] further discussed the existence and the forms of the solutions for some differential-difference equations, they obtained
Theorem A. Let c be a nonzero constant, R(z) be a nonzero rational function, and α,β∈C satisfy α2−β2≠1. Then the following difference equation of Fermat-type
l(z)2+[αl(z+c)−βl(z)]2=R(z), |
has no finite order transcendental meromorphic solutions with finitely many poles.
Theorem B. Let c(≠0), α(≠0), β∈C, and P(z), Q(z) be nonzero polynomials satisfying one of two following cases:
(i) degzP(z)≥1, degzQ(z)≥1;
(ii) P(z), Q(z) are two constants and P2(α2−β2)≠1. Then the following Fermat-type difference equation
l(z)2+P2(z)[αl(z+c)−βl(z)]2=Q(z), |
has no transcendental entire solutions with finite order.
For further study, we continue to discuss the existence and the forms of solutions for certain differential-difference equations with more general forms than the previous forms by Liu et al. [10,11,18,23] and obtain the following results.
Theorem 1.1. Let cj(j=1,2,⋯,m) be distinct constants, a∈C∖{0}, ϱi∈C(i=1,2,⋯,m), R(z) be a nonzero rational function, and m∑i=1ϱi(expaci+exp−aci)≠0. Then the following difference equation
l(z)2+[ϱ1l(z+c1)+ϱ2l(z+c2)+⋯+ϱml(z+cm)]2=R(z) | (1.1) |
has no finite order transcendental meromorphic solutions with finitely many poles.
Theorem 1.2. Let cj(j=1,2,⋯,m) be distinct constants, a∈C∖{0}, ϱi∈C(i=1,2,⋯,m), and P(z), Q(z) be nonzero polynomials satisfying one of two following cases:
(i) degzP(z)≥1;
(ii) P is a constant and P2[m∑i=1ϱiexpacim∑i=1ϱiexp−aci]≠1. Then the following difference equation
l(z)2+P(z)2[ϱ1l(z+c1)+ϱ2l(z+c2)+⋯+ϱml(z+cm)]2=Q(z) | (1.2) |
has no transcendental entire solutions with finite order.
Theorem 1.3. Let cj(j=1,2,⋯,m) be distinct constants, a∈C∖{0}, ϱi∈C(i=1,2,⋯,m). Let l(z) be a transcendental finite order meromorphic solution of difference-differential equation
l′(z)2+[ϱ1l(z+c1)+ϱ2l(z+c2)+⋯+ϱml(z+cm)]2=R(z), | (1.3) |
where R(z) is a nonzero rational function. If l(z) has finitely many poles, and m∑j=1cj2ϱjexpacjm∑j=1cj2ϱjexp−acj≠0, then R(z) is a nonconstant polynomial with degzR(z)⩽2, and m∑j=1cjϱjexpacjm∑j=1cjϱjexp−acj=1. Furthermore,
(i) If R(z) is a nonconstant polynomial with degzR(z)⩽2, and m∑i=1ϱi≠0, then we have
l(z)=s1(z)expaz+b+s2(z)exp−(az+b)2, |
where R(z)=(m1+as1(z))(m2−as2(z)),a≠0,b∈C and a,b,cj,ϱi satisfy i(ϱ1expac1+⋯+ϱmexpacm)=a and i(ϱ1exp−ac1+⋯+ϱmexp−acm)=a, where sj(z)=mjz+nj,mj,nj∈C(j=1,2).
(ii) If R(z) is a nonzero constant, and m∑i=1ϱi≠0, then
l(z)=n1expaz+b+n2exp−(az+b)2, |
where R(z)=−a2n1n2,a≠0,b∈C.
Theorem 1.4. Let cj(j=1,2,⋯,m) be distinct constants, a∈C∖{0}, ϱi∈C(i=1,2,⋯,m). Let l(z) be a transcendental meromorphic solution of the following difference-differential equation
l″(z)2+[ϱ1l(z+c1)+ϱ2l(z+c2)+⋯+ϱml(z+cm)]2=R(z), | (1.4) |
where R(z) is a nonzero rational function.
(i) If m∑i=1ϱiexpaci+m∑i=1ϱiexp−aci≠0, then (1.4) has no finite order transcendental meromorphic solution with finitely many poles.
(ii) If m∑j=1icjϱjexpacj≠2a, m∑j=1icjϱjexp−acj≠2a, and (1.4) has a finite order transcendental meromorphic solution l(z) with finitely many poles, then R(z) is a constant. Furthermore if m∑i=1ϱi≠0, then we have
l(z)=t1expaz+b+t2exp−(az+b)2, |
where a,b,t1,t2,ϱi,cj satisfy m∑i=1ϱiexpaci+m∑i=1ϱiexp−aci=0, R(z)=a4t1t2, b∈C.
The following two lemmas play an important role in the proof of our results.
Lemma 2.1. ([22]) Suppose that f1,f2,⋯,fn(n≥2) are meromorphic functions and g1,g2,⋯,gn are entire functions satisfying the following conditions:
(i) n∑j=1fjexpgj≡0;
(ii) gj−gk are not constants for 1≤j<k≤n;
(iii) For 1≤j≤n,1≤h<k≤n, T(r,fj)=o{T(r,expgh−gk)}(r→∞,r∉E), where E is a set of r∈(0,∞) with finite linear measure.
Then fj≡0(j=1,2,⋯,m).
Lemma 2.2. ([22]) Let l(z) be a meromorphic function of finite order ρ(l). Write
l(z)=ckzk+ck+1zk+1+⋯,(ck≠0), |
near z=0 and let {a1,a2,⋯} and {b1,b2,⋯} be the zeros and poles of l in C∖{0}, respectively. Then
l(z)=zkexpQ(z)P1(z)P2(z), |
where P1(z) and P2(z) are the canonical products of l formed with the non-null zeros and poles of l, respectively, and Q(z) is a polynomial of degree ⩽ρ(l).
Suppose that (1.1) has a finite order transcendental meromorphic solution l(z) with finitely many poles. Rewriting (1.1) as follows
(l(z)+i(ϱ1l(z+c1)+ϱ2l(z+c2)+⋯+ϱml(z+cm)))(l(z)−i(ϱ1l(z+c1)+ϱ2l(z+c2)+⋯+ϱml(z+cm)))=R(z). | (3.1) |
Since l(z) has finitely many poles, R(z) is a nonzero rational function, then l(z)+i(ϱ1l(z+c1)+ϱ2l(z+c2)+⋯+ϱml(z+cm)) and l(z)−i(ϱ1l(z+c1)+ϱ2l(z+c2)+⋯+ϱml(z+cm)) both have finitely many poles and zeros. Together Lemma 2.2 with (3.1), we obtain that
l(z)+i(ϱ1l(z+c1)+ϱ2l(z+c2)+⋯+ϱml(z+cm))=R1(z)expp(z), | (3.2) |
and
l(z)−i(ϱ1l(z+c1)+ϱ2l(z+c2)+⋯+ϱml(z+cm))=R2(z)exp−p(z), | (3.3) |
where R1(z),R2(z) are two nonzero rational functions such that R1(z)R2(z)=R(z), and p(z) is a nonconstant polynomial. (3.2) and (3.3) imply that
l(z)=R1(z)expp(z)+R2(z)exp−p(z)2, | (3.4) |
and
ϱ1l(z+c1)+ϱ2l(z+c2)+⋯+ϱml(z+cm)=R1(z)expp(z)−R2(z)exp−p(z)2i. | (3.5) |
Substituting (3.4) into (3.5), we have
expp(z)(iϱ1R1(z+c1)expp(z+c1)−p(z)+iϱ2R1(z+c2)expp(z+c2)−p(z)+⋯+iϱmR1(z+cm)expp(z+cm)−p(z)−R1(z))+exp−p(z)(iϱ1R2(z+c1)expp(z)−p(z+c1)+iϱ2R2(z+c2)expp(z)−p(z+c2)+⋯+iϱmR2(z+cm)expp(z)−p(z+cm)+R2(z))=0. | (3.6) |
By Lemma 2.1 and (3.6), we have
iϱ1R1(z+c1)expp(z+c1)−p(z)+iϱ2R1(z+c2)expp(z+c2)−p(z)+⋯+iϱmR1(z+cm)expp(z+cm)−p(z)−R1(z)=0, | (3.7) |
and
iϱ1R2(z+c1)expp(z)−p(z+c1)+iϱ2R2(z+c2)expp(z)−p(z+c2)+⋯+iϱmR2(z+cm)expp(z)−p(z+cm)+R2(z)=0. | (3.8) |
Since R1(z),R2(z) are two nonzero rational functions and that l(z) is of finite order, we obtain that p(z) is a polynomial of degree one. If degzp(z)≥2, then we obtain that degz[p(z+cj)−p(z+ci)]≥1. Hence, we have T(r,iϱjRj(z+cj))=S(r,expp(z+ci)−p(z+cj)), Lemma 2.1 and (3.7) imply that R1(z)≡0. This is impossible. By the similar method as above, we also have R2(z)≡0, a contradiction. So we have degzp(z)=1. Set p(z)=az+b,a≠0,b∈C. By (3.7) and (3.8), we have
lim|z|→∞i(ϱ1R1(z+c1)R1(z)expp(z+c1)−p(z)+⋯+ϱmR1(z+cm)R1(z)expp(z+cm)−p(z))=i(ϱ1expac1+⋯+ϱmexpacm)=1, |
and
lim|z|→∞i(ϱ1R2(z+c1)R2(z)expp(z)−p(z+c1)+⋯+ϱmR2(z+cm)R2(z)expp(z)−p(z+cm))=i(ϱ1exp−ac1+⋯+ϱmexp−acm)=−1. |
Thus, it yields that m∑i=1ϱi(expaci+exp−aci)=0, this is a contradiction with the assumption of Theorem 1.1. Hence, Theorem 1.1 holds.
If l(z) is a transcendental entire solution with finite order of (1.2), then by the similar method as the proof of Theorem 1.1, we have
l(z)=Q1(z)expp(z)+Q2(z)exp−p(z)2, | (4.1) |
and
ϱ1l(z+c1)+ϱ2l(z+c2)+⋯+ϱml(z+cm)=Q1(z)expp(z)−Q2(z)exp−p(z)2iP(z), | (4.2) |
where p(z) is a nonconstant polynomial and Q1(z)Q2(z)=Q(z), Q1(z), Q2(z) are nonzero polynomials. Together (4.1) with (4.2), we have
expp(z)(iϱ1P(z)Q1(z+c1)expp(z+c1)−p(z)+iϱ2P(z)Q1(z+c2)expp(z+c2)−p(z)+⋯+iϱmP(z)Q1(z+cm)expp(z+cm)−p(z)−Q1(z))+exp−p(z)(iϱ1P(z)Q2(z+c1)expp(z)−p(z+c1)+iϱ2P(z)Q2(z+c2)expp(z)−p(z+c2)+⋯+iϱmP(z)Q2(z+cm)expp(z)−p(z+cm)+Q2(z))=0. | (4.3) |
By Lemma 2.1 and p(z) is a nonconstant polynomial, we have
iϱ1P(z)Q1(z+c1)expp(z+c1)−p(z)+iϱ2P(z)Q1(z+c2)expp(z+c2)−p(z)+⋯+iϱmP(z)Q1(z+cm)expp(z+cm)−p(z)−Q1(z)=0, | (4.4) |
and
iϱ1P(z)Q2(z+c1)expp(z)−p(z+c1)+iϱ2P(z)Q2(z+c2)expp(z)−p(z+c2)+⋯+iϱmP(z)Q2(z+cm)expp(z)−p(z+cm)+Q2(z)=0. | (4.5) |
If degzp(z)≥2, then we have that degz[p(z+cj)−p(z+ci)]≥1. Hence, we have T(r,iϱjP(z)Q1(z+cj))=S(r,expp(z+ci)−p(z+cj)), Lemma 2.1 and (4.4) imply that Q1(z)≡0. A contradiction. By the similar method as above, we also obtain that Q2(z)≡0, this is also impossible. Hence, degzp(z)=1. Let p(z)=az+b,a≠0,b∈C. (4.4) and (4.5) imply that
iϱ1P(z)Q1(z+c1)expp(z+c1)−p(z)+iϱ2P(z)Q1(z+c2)expp(z+c2)−p(z)+⋯+iϱmP(z)Q1(z+cm)expp(z+cm)−p(z)=Q1(z), |
and
iϱ1P(z)Q2(z+c1)expp(z)−p(z+c1)+iϱ2P(z)Q2(z+c2)expp(z)−p(z+c2)+⋯+iϱmP(z)Q2(z+cm)expp(z)−p(z+cm)=−Q2(z). |
By this, we have
P(z)2[ϱ12Q(z+c1)+ϱ22Q(z+c1)+⋯+ϱm2Q(z+cm)+ϱ1ϱ2Q1(z+c1)Q2(z+c2)expac1−ac2+⋯+ϱ1ϱmQ1(z+c1)Q2(z+cm)expac1−acm+ϱ2ϱ1Q1(z+c2)Q2(z+c1)expac2−ac1+⋯+ϱ2ϱmQ1(z+c2)Q2(z+cm)expac2−acm+⋯+ϱmϱm−1Q1(z+cm−1)Q2(z+cm)expacm−acm−1]=Q(z). | (4.6) |
Set degzP(z)=p and degzQ(z)=q, then p≥0,q≥0 and p,q∈N+. Next we divided the following proof into four cases:
Case 1. p≥1 and m∑i=1ϱiexpacim∑i=1ϱiexp−aci=0. If q≥1, by comparing the order both sides of (4.6), we have 2p+q−1⩽q, that is, p⩽12, this is impossible. If q=0, that is, Q(z) is a constant. Hence, by (4.6), we have Q(z)=0, a contradiction.
Case 2. p≥1 and m∑i=1ϱiexpacim∑i=1ϱiexp−aci≠0. If q≥1, by comparing the order both sides of (4.6), we have 2p+q=q, that is, p=0, a contradiction. If q=0, that is, Q(z) is a constant. Hence, by (4.6), we have P(z) is a constant, this is impossible.
Case 3. p=0 and m∑i=1ϱiexpacim∑i=1ϱiexp−aci=0. That is, P(z)=K(≠0). If q≥1, we have q−1=q, this is impossible. If q=0, we have Q(z)≡0. A contradiction.
Case 4. p=0 and m∑i=1ϱiexpacim∑i=1ϱiexp−aci≠0. If q≥1, set P(z)=K(≠0), Q(z)=bqzq+bq−1zq−1+⋯+b0,bq≠0,bq−1,⋯,b0 are constants. By comparing the coefficients of zq both sides of (4.6), we have
K2[m∑i=1ϱiexpacim∑i=1ϱiexp−aci]=1. | (4.7) |
This is a contradiction with the condition of Theorem 1.2. If q=0, then K2[m∑i=1ϱiexpacim∑i=1ϱiexp−aci]=1, this is impossible.
Hecne, Theorem 1.2 holds.
Suppose that (1.3) has a finite order transcendental meromorphic solution l(z) with finitely many poles. Rewriting (1.3) as follows
(l′(z)+i(ϱ1l(z+c1)+ϱ2l(z+c2)+⋯+ϱml(z+cm)))(l′(z)−i(ϱ1l(z+c1)+ϱ2l(z+c2)+⋯+ϱml(z+cm)))=R(z). | (5.1) |
Since l(z) has finitely many poles, and R(z) is a nonzero rational function, then l′(z)+i(ϱ1l(z+c1)+ϱ2l(z+c2)+⋯+ϱml(z+cm)) and l′(z)−i(ϱ1l(z+c1)+ϱ2l(z+c2)+⋯+ϱml(z+cm)) both have finitely many poles and zeros. Hence, by Lemma 2.2, (5.1) can be written as
l′(z)+i(ϱ1l(z+c1)+ϱ2l(z+c2)+⋯+ϱml(z+cm))=R1(z)expp(z), | (5.2) |
and
l′(z)−i(ϱ1l(z+c1)+ϱ2l(z+c2)+⋯+ϱml(z+cm))=R2(z)exp−p(z), | (5.3) |
where R1(z),R2(z) are two nonzero rational functions such that R1(z)R2(z)=R(z), and p(z) is a nonconstant polynomial. (5.2) and (5.3) imply that
l′(z)=R1(z)expp(z)+R2(z)exp−p(z)2, | (5.4) |
and
ϱ1l(z+c1)+ϱ2l(z+c2)+⋯+ϱml(z+cm)=R1(z)expp(z)−R2(z)exp−p(z)2i. | (5.5) |
(5.5) implies that
ϱ1l′(z+c1)+ϱ2l′(z+c2)+⋯+ϱml′(z+cm)=A1(z)expp(z)−B1(z)exp−p(z)2i, | (5.6) |
where A1(z)=R′1+R1(z)p′ and B1(z)=R′2−R2(z)p′. Substituting (5.4) into (5.6), we have
expp(z)(iϱ1R1(z+c1)expp(z+c1)−p(z)+iϱ2R1(z+c2)expp(z+c2)−p(z)+⋯+iϱmR1(z+cm)expp(z+cm)−p(z)−A1(z))+exp−p(z)(iϱ1R2(z+c1)expp(z)−p(z+c1)+iϱ2R2(z+c2)expp(z)−p(z+c2)+⋯+iϱmR2(z+cm)expp(z)−p(z+cm)+B1(z))=0. | (5.7) |
Together Lemma 2.1 with (5.7), we have
iϱ1R1(z+c1)expp(z+c1)−p(z)+iϱ2R1(z+c2)expp(z+c2)−p(z)+⋯+iϱmR1(z+cm)expp(z+cm)−p(z)−A1(z)=0, | (5.8) |
and
iϱ1R2(z+c1)expp(z)−p(z+c1)+iϱ2R2(z+c2)expp(z)−p(z+c2)+⋯+iϱmR2(z+cm)expp(z)−p(z+cm)+B1(z)=0. | (5.9) |
Since R1(z),R2(z) are two nonzero rational functions and l(z) is of finite order, by the similar method as the proof of Theorem 1.1, we have degzp(z)=1. Let p(z)=az+b,a≠0,b∈C. Substituting p(z), A1(z), B1(z) into (5.8) and (5.9), as z⟶∞, we have
lim|z|→∞i(ϱ1R1(z+c1)R1(z)expp(z+c1)−p(z)+⋯+ϱmR1(z+cm)R1(z)expp(z+cm)−p(z))=i(ϱ1expac1+⋯+ϱmexpacm)=R′1(z)R1(z)+a=a, |
and
lim|z|→∞i(ϱ1R2(z+c1)R2(z)expp(z)−p(z+c1)+⋯+ϱmR2(z+cm)R2(z)expp(z)−p(z+cm))=i(ϱ1exp−ac1+⋯+ϱmexp−acm)=−R′2(z)R2(z)+a=a. |
That is
i(ϱ1expac1+⋯+ϱmexpacm)=a,i(ϱ1exp−ac1+⋯+ϱmexp−acm)=a. | (5.10) |
According to (5.8), (5.9) and (5.10), we have
iϱ1expac1(R1(z+c1)−R1(z))+iϱ2expac2(R1(z+c2)−R1(z))+⋯+iϱmexpacm(R1(z+cm)−R1(z))=R1′(z), | (5.11) |
and
iϱ1exp−ac1(R2(z+c1)−R2(z))+iϱ2exp−ac2(R2(z+c2)−R2(z))+⋯+iϱmexp−acm(R2(z+cm)−R2(z))=−R2′(z). | (5.12) |
If R1(z),R2(z) are two nonzero constants, then (5.11) and (5.12) hold and R1(z)R2(z)=R(z) is a constant.
We next consider the case that R1(z),R2(z) are two nonzero rational functions. If R1(z) has a pole of multiplicity v at z0, by (5.11), we know that there exists at least on index l1∈{1,2,⋯,m} such that z0+cl1 is a pole of R1(z) of multiplicity v+1, following the above step, we know R1(z) has a sequence of poles
{τn=z0+cl1+⋯+cln:n=1,2,⋯}. |
Hence, we have λ(1R1(z))≥1, this is impossible. So R1(z) is a polynomial. Using the same method as above, we know that R2(z) is also a polynomial. If Ri(z) is a nonconstant polynomial with degzRi(z)≥2. Let Ri(z)=anzn+an−1zn−1+⋯+a0, then
R′i(z)=nanzn−1+(n−1)an−1zn−2+⋯, | (5.13) |
Ri(z+cm)−Ri(z)=nancmzn−1+(anC2nc2m+(n−1)an−1cm)zn−2+⋯, | (5.14) |
where i=1,2. Substituting (5.13) and (5.14) into (5.11) and (5.12), comparing the coefficients of zn−1, zn−2, we have m∑j=1icjϱjexpacj=1, m∑j=1cj2ϱjexpacj=0 and m∑j=1icjϱjexp−acj=−1, m∑j=1cj2ϱjexp−acj=0, a contradiction with m∑j=1cj2ϱjexpacjm∑j=1cj2ϱjexp−acj≠0. Hence, degzRi(z)≤1. So degzR(z)=degzR1(z)R2(z)≤2.
(i) If R(z) is a nonconstant polynomial with degzR(z)⩽2, then by (5.4), we have
l(z)=s1(z)expaz+b+s2(z)exp−(az+b)2+ϑ, | (5.15) |
where sj(z)=mjz+nj,mj,nj∈C,(j=1,2) and ϑ∈C;
Case 1. If degzR(z)=2, then mj≠0,j=1,2. If m∑i=1ϱi≠0, substituting (5.15) into (5.5), we have ϑ≡0, R(z)=(m1+as1(z))(m2−as2(z)). Hence, we have
l(z)=s1(z)expaz+b+s2(z)exp−(az+b)2, |
R(z)=(m1+as1(z))(m2−as2(z)),a≠0,b∈C.
Case 2. If degzR(z)=1, then one of m1,m2 is zero, we can assume that m1=0. Substituting (5.15) into (5.5), we have R1(z) is a constant and R2(z) is a polynomial of degree one. Using the same method as case 1, we have ϑ≡0. Hence, we obtain that
l(z)=s1(z)expaz+b+s2(z)exp−(az+b)2, |
R(z)=(m1+as1(z))(m2−as2(z)),a≠0,b∈C.
(ii) If R(z) is a nonzero constant, by (5.4), we have
l(z)=n1expaz+b+n2exp−(az+b)2+d, | (5.16) |
where n1,n2∈C and d∈C. Substituting (5.16) into (5.5), we have d=0, R(z)=−a2n1n2. Hence, Theorem 1.3 holds.
Suppose that (1.4) has a finite order transcendental meromorphic solution l(z) with finitely many poles. Rewriting (1.4) as follows
(l″(z)+i(ϱ1l(z+c1)+ϱ2l(z+c2)+⋯+ϱml(z+cm)))(l″(z)−i(ϱ1l(z+c1)+ϱ2l(z+c2)+⋯+ϱml(z+cm)))=R(z). | (6.1) |
Since l(z) has finitely many poles, R(z) is a nonzero rational function, then l″(z)+i(ϱ1l(z+c1)+ϱ2l(z+c2)+⋯+ϱml(z+cm)) and l″(z)−i(ϱ1l(z+c1)+ϱ2l(z+c2)+⋯+ϱml(z+cm)) both have finitely many poles and zeros. Hence, we can rewrite (6.1) as follows
l″(z)+i(ϱ1l(z+c1)+ϱ2l(z+c2)+⋯+ϱml(z+cm))=R1(z)expp(z), | (6.2) |
and
l″(z)−i(ϱ1l(z+c1)+ϱ2l(z+c2)+⋯+ϱml(z+cm))=R2(z)exp−p(z), | (6.3) |
where R1(z),R2(z) are two nonzero rational functions such that R1(z)R2(z)=R(z), and p(z) is a nonconstant polynomial. By (6.2) and (6.3), we obtain
l″(z)=R1(z)expp(z)+R2(z)exp−p(z)2, | (6.4) |
and
ϱ1l(z+c1)+ϱ2l(z+c2)+⋯+ϱml(z+cm)=R1(z)expp(z)−R2(z)exp−p(z)2i. | (6.5) |
(6.5) implies that
ϱ1l″(z+c1)+ϱ2l″(z+c2)+⋯+ϱml″(z+cm)=A2(z)expp(z)−B2(z)exp−p(z)2i, | (6.6) |
where A2(z)=A′1+A1(z)p′ and B2(z)=B′1−B1(z)p′. Together (6.4) with (6.6), we obtain that
expp(z)(iϱ1R1(z+c1)expp(z+c1)−p(z)+iϱ2R1(z+c2)expp(z+c2)−p(z)+⋯+iϱmR1(z+cm)expp(z+cm)−p(z)−A2(z))+exp−p(z)(iϱ1R2(z+c1)expp(z)−p(z+c1)+iϱ2R2(z+c2)expp(z)−p(z+c2)+⋯+iϱmR2(z+cm)expp(z)−p(z+cm)+B2(z))=0. | (6.7) |
Lemma 2.1 and (6.7) imply that
iϱ1R1(z+c1)expp(z+c1)−p(z)+iϱ2R1(z+c2)expp(z+c2)−p(z)+⋯+iϱmR1(z+cm)expp(z+cm)−p(z)−A2(z)=0, | (6.8) |
and
iϱ1R2(z+c1)expp(z)−p(z+c1)+iϱ2R2(z+c2)expp(z)−p(z+c2)+⋯+iϱmR2(z+cm)expp(z)−p(z+cm)+B2(z)=0. | (6.9) |
Since R1(z),R2(z) are two nonzero rational functions and l(z) is of finite order, using the similar method as the proof of Theorem 1.1, we know that p(z) is a polynomial of degree one. Let p(z)=az+b,a≠0,b∈C. Substituting p(z),A2(z),B2(z) into (6.8) and (6.9), and as z⟶∞, we have
lim|z|→∞i(ϱ1R1(z+c1)R1(z)expp(z+c1)−p(z)+⋯+ϱmR1(z+cm)R1(z)expp(z+cm)−p(z))=i(ϱ1expac1+⋯+ϱmexpacm)=A1′(z)R1(z)+a2=a2, |
and
lim|z|→∞i(ϱ1R2(z+c1)R2(z)expp(z)−p(z+c1)+⋯+ϱmR2(z+cm)R2(z)expp(z)−p(z+cm))=i(ϱ1exp−ac1+⋯+ϱmexp−acm)=−B1′(z)R2(z)−a2=−a2, |
that is
i(ϱ1expac1+⋯+ϱmexpacm)=a2,i(ϱ1exp−ac1+⋯+ϱmexp−acm)=−a2. | (6.10) |
So, we have m∑i=1ϱiexpaci+m∑i=1ϱiexp−aci=0.
(i) If m∑i=1ϱiexpaci+m∑i=1ϱiexp−aci≠0, this is a contradiction with m∑i=1ϱiexpaci+m∑i=1ϱiexp−aci=0. Hence, Theorem 1.4 (i) holds.
(ii) If m∑j=1icjϱjexpacj≠2a and m∑j=1icjϱjexp−acj≠2a. By (6.8)–(6.10), we have
iϱ1expac1(R1(z+c1)−R1(z))+iϱ2expac2(R1(z+c2)−R1(z))+⋯+iϱmexpacm(R1(z+cm)−R1(z))=R1″(z)+2aR1′(z), | (6.11) |
and
iϱ1exp−ac1(R2(z+c1)−R2(z))+iϱ2exp−ac2(R2(z+c2)−R2(z))+⋯+iϱmexp−acm(R2(z+cm)−R2(z))=−R2″(z)+2aR2′(z). | (6.12) |
If R1(z),R2(z) are two nonzero rational functions, using the similar method as the proof of Theorem 1.3, we know that Ri(z) is a polynomial. If degzRi(z)≥2. Let Ri(z)=anzn+an−1zn−1+⋯+a0, then
R′i(z)=nanzn−1+(n−1)an−1zn−2+⋯,R″i(z)=n(n−1)anzn−2+(n−1)(n−2)an−1zn−3+⋯,Ri(z+cm)−Ri(z)=nancmzn−1+(anC2nc2m+(n−1)an−1cm)zn−2+(anC3nc3m+an−1C2n−1c2m+(n−2)an−2cm)zn−3+⋯, | (6.13) |
where i=1,2. Substituting (6.13) into (6.11) and (6.12), comparing the coefficients of zn−1, zn−2, we have m∑j=1icjϱjexpacj=2a, m∑j=1cj2ϱjexpacj=2 and m∑j=1icjϱjexp−acj=2a, m∑j=1cj2ϱjexp−acj=−2, a contradiction. Hence, degzRi(z)≤1.
If degzRi(z)=1, then (6.11) and (6.12) imply that m∑j=1icjϱjexpacj=2a and m∑j=1icjϱjexp−acj=2a, a contradiction. Hence, R1(z), R2(z) are two nonzero constants, R(z)=R1(z)R2(z) is a constant. By (6.5), we have
l(z)=t1expaz+b+t2exp−(az+b)2+P(z), |
where a≠0, b∈C, t1, t2∈C∖{0} and P(z) is a polynomial of degree one. Since m∑i=1ϱi≠0, then by (6.5), we have P(z)≡0. So, we have
l(z)=t1expaz+b+t2exp−(az+b)2, | (6.14) |
where m∑i=1ϱiexpaci+m∑i=1ϱiexp−aci=0, b∈C, R(z)=a4t1t2. Hence, Theorem 1.4 holds.
We thank the referee(s) for reading the manuscript very carefully and making a number of valuable and kind comments which improved the presentation. The work was supported by the NNSF of China (No.10771121, 11401387), the NSF of Zhejiang Province, China (No. LQ14A010007), the NSFC Tianyuan Mathematics Youth Fund (No. 11226094), the NSF of Shandong Province, China (No. ZR2012AQ020 and No. ZR2010AM030) and the Fund of Doctoral Program Research of Shaoxing College of Art and Science (20135018).
The authors declare that none of the authors have any competing interests in the manuscript.
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1. | Guowei Zhang, The exact transcendental entire solutions of complex equations with three quadratic terms, 2023, 8, 2473-6988, 27414, 10.3934/math.20231403 |