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On meromorphic solutions of certain differential-difference equations

  • 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 [19].

    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 [19].



    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,βC satisfy α2β21. 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), βC, 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(α2β2)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, aC{0}, ϱiC(i=1,2,,m), R(z) be a nonzero rational function, and mi=1ϱi(expaci+expaci)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, aC{0}, ϱiC(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[mi=1ϱiexpacimi=1ϱiexpaci]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, aC{0}, ϱiC(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 mj=1cj2ϱjexpacjmj=1cj2ϱjexpacj0, then R(z) is a nonconstant polynomial with degzR(z)2, and mj=1cjϱjexpacjmj=1cjϱjexpacj=1. Furthermore,

    (i) If R(z) is a nonconstant polynomial with degzR(z)2, and mi=1ϱi0, then we have

    l(z)=s1(z)expaz+b+s2(z)exp(az+b)2,

    where R(z)=(m1+as1(z))(m2as2(z)),a0,bC and a,b,cj,ϱi satisfy i(ϱ1expac1++ϱmexpacm)=a and i(ϱ1expac1++ϱmexpacm)=a, where sj(z)=mjz+nj,mj,njC(j=1,2).

    (ii) If R(z) is a nonzero constant, and mi=1ϱi0, then

    l(z)=n1expaz+b+n2exp(az+b)2,

    where R(z)=a2n1n2,a0,bC.

    Theorem 1.4. Let cj(j=1,2,,m) be distinct constants, aC{0}, ϱiC(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 mi=1ϱiexpaci+mi=1ϱiexpaci0, then (1.4) has no finite order transcendental meromorphic solution with finitely many poles.

    (ii) If mj=1icjϱjexpacj2a, mj=1icjϱjexpacj2a, and (1.4) has a finite order transcendental meromorphic solution l(z) with finitely many poles, then R(z) is a constant. Furthermore if mi=1ϱi0, then we have

    l(z)=t1expaz+b+t2exp(az+b)2,

    where a,b,t1,t2,ϱi,cj satisfy mi=1ϱiexpaci+mi=1ϱiexpaci=0, R(z)=a4t1t2, bC.

    The following two lemmas play an important role in the proof of our results.

    Lemma 2.1. ([22]) Suppose that f1,f2,,fn(n2) are meromorphic functions and g1,g2,,gn are entire functions satisfying the following conditions:

    (i) nj=1fjexpgj0;

    (ii) gjgk are not constants for 1j<kn;

    (iii) For 1jn,1h<kn, T(r,fj)=o{T(r,expghgk)}(r,rE), where E is a set of r(0,) with finite linear measure.

    Then fj0(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+,(ck0),

    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)expp(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)expp(z)2, (3.4)

    and

    ϱ1l(z+c1)+ϱ2l(z+c2)++ϱml(z+cm)=R1(z)expp(z)R2(z)expp(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))+expp(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,a0,bC. 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(ϱ1expac1++ϱmexpacm)=1.

    Thus, it yields that mi=1ϱi(expaci+expaci)=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)expp(z)2, (4.1)

    and

    ϱ1l(z+c1)+ϱ2l(z+c2)++ϱml(z+cm)=Q1(z)expp(z)Q2(z)expp(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))+expp(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,a0,bC. (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)expac1ac2++ϱ1ϱmQ1(z+c1)Q2(z+cm)expac1acm+ϱ2ϱ1Q1(z+c2)Q2(z+c1)expac2ac1++ϱ2ϱmQ1(z+c2)Q2(z+cm)expac2acm++ϱmϱm1Q1(z+cm1)Q2(z+cm)expacmacm1]=Q(z). (4.6)

    Set degzP(z)=p and degzQ(z)=q, then p0,q0 and p,qN+. Next we divided the following proof into four cases:

    Case 1. p1 and mi=1ϱiexpacimi=1ϱiexpaci=0. If q1, by comparing the order both sides of (4.6), we have 2p+q1q, that is, p12, 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. p1 and mi=1ϱiexpacimi=1ϱiexpaci0. If q1, 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 mi=1ϱiexpacimi=1ϱiexpaci=0. That is, P(z)=K(0). If q1, we have q1=q, this is impossible. If q=0, we have Q(z)0. A contradiction.

    Case 4. p=0 and mi=1ϱiexpacimi=1ϱiexpaci0. If q1, set P(z)=K(0), Q(z)=bqzq+bq1zq1++b0,bq0,bq1,,b0 are constants. By comparing the coefficients of zq both sides of (4.6), we have

    K2[mi=1ϱiexpacimi=1ϱiexpaci]=1. (4.7)

    This is a contradiction with the condition of Theorem 1.2. If q=0, then K2[mi=1ϱiexpacimi=1ϱiexpaci]=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)expp(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)expp(z)2, (5.4)

    and

    ϱ1l(z+c1)+ϱ2l(z+c2)++ϱml(z+cm)=R1(z)expp(z)R2(z)expp(z)2i. (5.5)

    (5.5) implies that

    ϱ1l(z+c1)+ϱ2l(z+c2)++ϱml(z+cm)=A1(z)expp(z)B1(z)expp(z)2i, (5.6)

    where A1(z)=R1+R1(z)p and B1(z)=R2R2(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))+expp(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,a0,bC. 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)=R1(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(ϱ1expac1++ϱmexpacm)=R2(z)R2(z)+a=a.

    That is

    i(ϱ1expac1++ϱmexpacm)=a,i(ϱ1expac1++ϱmexpacm)=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

    iϱ1expac1(R2(z+c1)R2(z))+iϱ2expac2(R2(z+c2)R2(z))++iϱmexpacm(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+an1zn1++a0, then

    Ri(z)=nanzn1+(n1)an1zn2+, (5.13)
    Ri(z+cm)Ri(z)=nancmzn1+(anC2nc2m+(n1)an1cm)zn2+, (5.14)

    where i=1,2. Substituting (5.13) and (5.14) into (5.11) and (5.12), comparing the coefficients of zn1, zn2, we have mj=1icjϱjexpacj=1, mj=1cj2ϱjexpacj=0 and mj=1icjϱjexpacj=1, mj=1cj2ϱjexpacj=0, a contradiction with mj=1cj2ϱjexpacjmj=1cj2ϱjexpacj0. 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,njC,(j=1,2) and ϑC;

    Case 1. If degzR(z)=2, then mj0,j=1,2. If mi=1ϱi0, substituting (5.15) into (5.5), we have ϑ0, R(z)=(m1+as1(z))(m2as2(z)). Hence, we have

    l(z)=s1(z)expaz+b+s2(z)exp(az+b)2,

    R(z)=(m1+as1(z))(m2as2(z)),a0,bC.

    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 ϑ0. Hence, we obtain that

    l(z)=s1(z)expaz+b+s2(z)exp(az+b)2,

    R(z)=(m1+as1(z))(m2as2(z)),a0,bC.

    (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,n2C and dC. 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)expp(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)expp(z)2, (6.4)

    and

    ϱ1l(z+c1)+ϱ2l(z+c2)++ϱml(z+cm)=R1(z)expp(z)R2(z)expp(z)2i. (6.5)

    (6.5) implies that

    ϱ1l(z+c1)+ϱ2l(z+c2)++ϱml(z+cm)=A2(z)expp(z)B2(z)expp(z)2i, (6.6)

    where A2(z)=A1+A1(z)p and B2(z)=B1B1(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))+expp(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,a0,bC. 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(ϱ1expac1++ϱmexpacm)=B1(z)R2(z)a2=a2,

    that is

    i(ϱ1expac1++ϱmexpacm)=a2,i(ϱ1expac1++ϱmexpacm)=a2. (6.10)

    So, we have mi=1ϱiexpaci+mi=1ϱiexpaci=0.

    (i) If mi=1ϱiexpaci+mi=1ϱiexpaci0, this is a contradiction with mi=1ϱiexpaci+mi=1ϱiexpaci=0. Hence, Theorem 1.4 (i) holds.

    (ii) If mj=1icjϱjexpacj2a and mj=1icjϱjexpacj2a. 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

    iϱ1expac1(R2(z+c1)R2(z))+iϱ2expac2(R2(z+c2)R2(z))++iϱmexpacm(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+an1zn1++a0, then

    Ri(z)=nanzn1+(n1)an1zn2+,Ri(z)=n(n1)anzn2+(n1)(n2)an1zn3+,Ri(z+cm)Ri(z)=nancmzn1+(anC2nc2m+(n1)an1cm)zn2+(anC3nc3m+an1C2n1c2m+(n2)an2cm)zn3+, (6.13)

    where i=1,2. Substituting (6.13) into (6.11) and (6.12), comparing the coefficients of zn1, zn2, we have mj=1icjϱjexpacj=2a, mj=1cj2ϱjexpacj=2 and mj=1icjϱjexpacj=2a, mj=1cj2ϱjexpacj=2, a contradiction. Hence, degzRi(z)1.

    If degzRi(z)=1, then (6.11) and (6.12) imply that mj=1icjϱjexpacj=2a and mj=1icjϱjexpacj=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 a0, bC, t1, t2C{0} and P(z) is a polynomial of degree one. Since mi=1ϱi0, then by (6.5), we have P(z)0. So, we have

    l(z)=t1expaz+b+t2exp(az+b)2, (6.14)

    where mi=1ϱiexpaci+mi=1ϱiexpaci=0, bC, 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.



    [1] G. G. Gundersen, J. Heittokangas, I. Laine, J. Rieppo, D. Yang, Meromorphic solutions of generalized Schröder equations, Aequat. Math., 63 (2002), 110–135. doi: 10.1007/s00010-002-8010-z
    [2] R. G. Halburd, R. Korhonen, Finite-order meromorphic solutions and the discrete Painlevˊe equations, Proc. London. Math. Soc., 94 (2007), 443–474. doi: 10.1112/plms/pdl012
    [3] R. G. Halburd, R. J. Korhonen, Nevanlinna theory for the difference operator, Ann. Acad. Sci. Fenn. Math., 31 (2006), 463–478.
    [4] W. K. Hayman, Meromorphic solutions, Oxford: The Clarendon Press, 1964.
    [5] J. Heittokangas, R. Korhonen, I. Laine, J. Rieppo, K. Tohge, Complex difference equations of Malmquist type, Comput. Methods. Funct. Theory, 1 (2001), 27–39. doi: 10.1007/BF03320974
    [6] I. Laine, Nevanlinna theory and complex differential equations, Berlin: Walter de Gruyter, 1993.
    [7] Z. Latreuch, On the existence of entire solutions of certain class of nonlinear difference equations, Mediterr. J. Math., 14 (2017), 115. doi: 10.1007/s00009-017-0914-x
    [8] H. C. Li, On the existence of differential-difference equations, Math. Method. Appl. Sci., 39 (2016), 144–151. doi: 10.1002/mma.3465
    [9] K. Liu, T. B. Cao, X. L. Liu, The properties of differential-difference polynomials, Ukr. Math. J., 69 (2017), 85–100. doi: 10.1007/s11253-017-1348-0
    [10] K. Liu, Meromorphic functions sharing a set with applications to difference equations, J. Math. Anal. Appl., 359 (2009), 384–393. doi: 10.1016/j.jmaa.2009.05.061
    [11] K. Liu, T. B. Cao, H. Z. Cao, Entire solutions of Fermat-type differential-difference equations, Arch. Math., 99 (2012), 147–155. doi: 10.1007/s00013-012-0408-9
    [12] K. Liu, L. Z. Yang, On of some differential-difference equations, Comput. Methods. Funct. Theory., 13 (2013), 433–447. doi: 10.1007/s40315-013-0030-2
    [13] K. Liu, T. B. Cao, Entire solutions of Fermat-type differential-difference equations, Electron. J. Differ. Eq., 2013 (2013), 1–10. doi: 10.1186/1687-1847-2013-1
    [14] K. Liu, C. J. Song, Meromorphic solutions of complex differential-difference equations, Results Math., 72 (2017), 1759–1771. doi: 10.1007/s00025-017-0736-y
    [15] X. G. Qi, L. Z. Yang, Properties of meromorphic solutions to certain differential-difference equations, Electron. J. Differ. Eq., 2013 (2013), 1–9. doi: 10.1186/1687-1847-2013-1
    [16] J. Rieppo, On a class of complex functional equations, Ann. Acad. Sci. Fenn. Math., 32 (2007), 151–170.
    [17] A. J. Wiles, Modular elliptic curves and Fermat's Last Theorem, Ann. Math., 141 (1995), 443–551. doi: 10.2307/2118559
    [18] H. Wang, H. Y. Xu, J. Tu, The existence and forms of solutions for some Fermat-type differential-difference equations, AIMS Mathematics, 5 (2020), 685–700. doi: 10.3934/math.2020046
    [19] H. Y. Xu, S. Y. Liu, Q. P. Li, Entire solutions of several systems of nonlinear difference and partial differential-difference equations of Fermat-type, J. Math. Anal. Appl., 483 (2020), 123641. doi: 10.1016/j.jmaa.2019.123641
    [20] H. Y. Xu, S. Y. Liu, Q. P. Li, The existence and growth of solutions for several systems of complex nonlinear difference equations, Mediterr. J. Math., 16 (2019), 8. doi: 10.1007/s00009-018-1296-4
    [21] H. Y. Xu, J. Tu, Growth of solutions to systems of q-difference differential equations, Electron. J. Differ. Eq., 2016 (2016), 1–14. doi: 10.1186/s13662-015-0739-5
    [22] C. C. Yang, H. X. Yi, Uniqueness theroy of meromorphic functions, Dordrecht: Kluwer Academic Publishers, 2003.
    [23] J. Zhang, On some spcial difference equations of Malmquist type, Bull. Korean Math. Soc., 55 (2018), 51–61.
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