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Research article

The existence and forms of solutions for some Fermat-type differential-difference equations

  • Received: 07 October 2019 Accepted: 11 December 2019 Published: 19 December 2019
  • MSC : 30D35, 39A13, 39B72

  • The main aim of this article is to investigate the existence and the forms of solutions for several complex differential-difference equations of Fermat-type. Our results about the existence and the forms of solutions for these Fermat type equations are great improvement of the previous theorems given by Liu, Yang, Cao, Zhang. Moreover, it is a very satisfactory fact that in some examples explicit solutions are given.

    Citation: Hua Wang, Hong Yan Xu, Jin Tu. The existence and forms of solutions for some Fermat-type differential-difference equations[J]. AIMS Mathematics, 2020, 5(1): 685-700. doi: 10.3934/math.2020046

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  • The main aim of this article is to investigate the existence and the forms of solutions for several complex differential-difference equations of Fermat-type. Our results about the existence and the forms of solutions for these Fermat type equations are great improvement of the previous theorems given by Liu, Yang, Cao, Zhang. Moreover, it is a very satisfactory fact that in some examples explicit solutions are given.


    The main purpose of this article is to deal with the existence of solutions for several complex differential-difference equations of Fermat type. The basic results and the standard symbols of Nevanlinna theory will be used in this paper (see [8,28,30]). A. Wiles and R. Taylor [23,24] in 1995 pointed out: The Fermat equation xm+ym=1 does not admit nontrivial solutions in rational numbers as m3, and this equation possesses nontrivial rational solutions as m=2. About sixty years ago, Gross [4] investigated the existence of solutions for the Fermat-type functional equation fm+gm=1, and obtained: For m=2, the entire solutions are f=cosa(z),g=sina(z), where a(z) is an entire function; for m>2, there are no nonconstant entire solutions.

    In the last twenty years, Nevanlinna theory (especially the difference analogues such as logarithmic derivative lemma, Tumura-Clunie theorem, etc.) has played an important role in studying the properties of solutions for complex difference equations, complex differential-difference equations, and there were a number of results about the existence and the form of solutions for some equations (including [1,2,3,5,6,7,9,10,11,12,13,17,18,19,20,21,22,25,26,27]). In 2009, Liu [14] proved that the Fermat type equation f(z)2+[f(z+c)f(z)]2=a2 has no nonconstant entire solutions of finite order, where a is a nonzero constant. In 2012, Liu et al. [15] pointed out that equation f(z)2+f(z+c)2=1 has a transcendental entire solution of finite order. Furthermore, they also obtained that equation f(z)2+[f(z+c)f(z)]2=1 admits the finite order transcendental entire solutions with the form f(z)=1/2sin(2z+Bi), where c=(2k+1)π, and B is a constant (see [15]).

    In 2018, Zhang [31] further discussed the existence of solutions for some Fermat type differential-difference equations, which forms are more general than those given by Liu [14], Liu etal. [15], and obtained

    Theorem A (see [31,Theorem 1.3]). Let f be a transcendental meromorphic function with finitely many poles and σ(f)<. Then f can not be a solution of the difference equation

    f(z)2+[f(z+c)f(z)]2=R,

    where R is a nonzero rational function and c is a nonzero constant.

    Theorem B (see [31,Theorem 1.4]). Let f be a transcendental meromorphic function with finitely many poles and σ(f)<. If f is a solution of the differential-difference equation

    f(z)2+[f(z+c)f(z)]2=R,

    where R is a nonzero rational function and c is a nonzero constant, then R is a nonzero constant and f is of form

    f(z)=c1e2iz+c2e2iz+b,c=kπ+π/2,

    where c1,c2 are two nonzero constants such that 16c1c2=R, b is a constant and k is an integer.

    In this paper, we proceed to study the existence and the form of the solutions for some differential-difference equations with more general form than the previous form given by Liu, Liu et al. and Zhang [14,15,31]. Our results are listed as follows.

    Theorem 1.1. Let c be a nonzero constant, R be a nonzero rational function, and α,βC satisfy α2β21. Then the following difference equation of Fermat type

    f(z)2+[αf(z+c)βf(z)]2=R(z), (1.1)

    has no finite order transcendental meromorphic solutions with finitely many poles.

    Theorem 1.2. Let c(0),α(0),βC and P(z),Q(z) be nonzero polynomials satisfying one of two following cases

    (i) degzR1 or degzQ1;

    (ii) P,Q are two constants and P2(α2β2)1. Then the following Fermat-type difference equation

    f(z)2+P(z)2[αf(z+c)βf(z)]2=Q(z), (1.2)

    has no transcendental entire solutions with finite order.

    Theorem 1.3. Let α(0),βC, and k is an integer. Let f be a transcendental meromorphic solution of difference-differential equation of Fermat type

    f(z)2+[αf(z+c)βf(z)]2=R(z) (1.3)

    where R(z) is a nonzero rational function and c is a nonzero constant. If f is of finite order and has finitely many poles, then iαc=±1 and R(z) is a nonconstant polynomial with degzR2 or R(z) is a nonzero constant. Furthermore,

    (i) If R(z) is a nonconstant polynomial and degzR2, then f is of the form

    f(z)=s1(z)eaz+b+s2(z)e(az+b)2,

    where R(z)=(as1(z)+m1)(as2(z)+m2), a0,bC, and a,b,c,α,β satisfy α±β, a=i(α+β), c=(2k+1)πai, iαc=1 or a=i(αβ), c=2kπai, iαc=1, where sj(z)=mjz+nj, mj,njC(j=1,2);

    (ii) If R(z) is a nonzero constant, then f is of the form

    f(z)=n1eaz+b+n2e(az+b)2+d,

    R=a2n1n2, a0,bC, and a,b,c,α,β satisfy the following cases:

    (ii1) if α=β, then a=2αi, c=(2k+1)πai and dC;

    (ii2) if α=β, then a=2αi, c=2kπai and d=0;

    (ii3) if α±β, then d=0 and a=i(α+β), c=(2k+1)πai or a=i(αβ), c=2kπai.

    Next, we give some examples to explain the existence of solutions for Eq. (1.3) in the above cases.

    ● For Case (ⅰ), let s1(z)=1, s2=z+1, c=πi, a=1 and bC. That is

    f(z)=ez+b+(z+1)e(z+b)2.

    Thus, f(z) satisfies Eq. (1.3) with c=πi, α=1π, β=i1π and R(z)=z;

    Let s1(z)=z+1, s2=z1, a=1 and bC. That is

    f(z)=(z+1)ez+b+(z1)e(z+b)2.

    Thus, f(z) satisfies Eq. (1.3) with c=πi, α=1π, β=i1π and R(z)=z(z+2);

    ● For Case (ii1), let n1(z)=1, n2=2, a=1 and b,dC. That is

    f(z)=ez+b+2e(z+b)2+d.

    Thus, f(z) satisfies Eq. (1.3) with c=πi, α=i2, β=i2 and R(z)=2;

    For Case (ii2), let n1(z)=1, n2=1, a=2 and bC. That is

    f(z)=e2z+b+e(2z+b)2.

    Thus, f(z) satisfies Eq. (1.3) with c=πi, α=i, β=i and R(z)=4;

    For Case (ii3), let n1(z)=2, n2=1, a=1 and bC. That is

    f(z)=2ez+b+e(z+b)2.

    Thus, f(z) satisfies Eq. (1.3) with c=2πi, α=1, β=1+i and R(z)=2.

    Theorem 1.4. Let α(0),βC, and k is an integer. Let f be a transcendental meromorphic solution of difference-differential equation of Fermat type

    f(z)2+[αf(z+c)βf(z)]2=R(z) (1.4)

    where R(z) is a nonzero rational function and c is a nonzero constant.

    (i) If α=±β, then Eq. (1.4) has no finite order transcendental meromorphic solutions with finitely many poles;

    (ii) If α±β, and Eq. (1.4) has a finite order transcendental meromorphic solution f with finitely many poles, then R(z) must be a nonzero polynomial with degzR1. Furthermore,

    (ii1) if R(z) is a nonzero polynomial of degree one, then f(z) is of the form

    f(z)=s1(z)eaz+b+n2e(az+b)2,

    where a4=α2β2, bC, c=loga2+iβiα+2kπia, eac=2aiαc±1 and R=a3n2[as1(z)+2m1], s1(z)=m1z+n1, or f(z) is of the form

    f(z)=n1eaz+b+s2(z)e(az+b)2,

    where a4=α2β2, bC, c=loga2+iβiα+(2k+1)πia, eac=iαc2a±1 and R=a3n1[as2(z)2m2], s2(z)=m2z+n2;

    (ii2) if R(z) is a nonzero constant, then f(z) is of the form

    f(z)=c1eaz+b+c2e(az+b)2,

    where a,b,c,α,β,c1,c2,R satisfy a4=α2β2, bC, c=loga2+iβiα+2kπia and R=a4c1c2;

    The following examples show that the existence of solutions for complex differential-difference equation of Theorem 1.4 (ii1) and (ii2).

    Example 1.1. Let s1(z)=z, n2=1, a=1 and bC. And let c0 be a solution of equation e2c(1c)=1, α=2ic0ec0, and β=2c0ic0. Then it follows that iαec0iβ=1, iαec0iβ=1, α2β2=1, and iαc0ec0=2. Thus, we can deduce that

    f(z)=zez+b+e(z+b)2

    satisfies the following equation

    f(z)2+[αf(z+c)βf(z)]2=z+2.

    Example 1.2. Let c1=1, c2=1, ec=52, a=1,bC, α=i2, and β=52i. Thus

    f(z)=c1ez+b+c2e(z+b)2

    satisfies the following equation

    f(z)2+[i2f(z+c)52if(z)]2=1.

    To prove our theorems, we require the following lemmas.

    Lemma 2.1. ([31,Lemma 2.1]). If f is a nonconstant rational function and it satisfies the following differential-difference equation

    f=ηΔcf=η[f(z+c)f(z)],

    where η and c are two nonzero constants, then ηc=1 and f is a polynomial of degree one.

    Lemma 2.2. Let c,a,α be three nonzero constants satisfying ηcn1 and n1 be an integer. If f is a nonconstant rational solution of the following differential-difference equation

    iαΔcf(z)=f(n)(z)+(n1)ηf(n1)(z)++(nj)ηjf(nj)(z)++(nn1)ηn1f(z). (2.1)

    Then iαc=nηn1 and f is a polynomial of degree one.

    Proof. We firstly prove that f(z) has no poles. On the contrary, suppose that z0 is a pole of f. Since (2.1) can be rewritten (2.1) in the following form

    iαf(z+c)=[f(n)(z)+nηf(n1)(z)++(nj)ηjf(nj)(z)++nηn1f(z)]+iαf(z). (2.2)

    It is easy to see that z0+c is also a pole of f(z) by comparing the order of pole z0 on both sides of Eq. (2.2). By the cyclic utilization of this operation, we can get that a sequence poles of f(z) are z0+2c, z0+3c, , z0+tc, , this is impossible since f(z) is a nonconstant rational function. Hence, f(z) is a polynomial.

    Let f(z) be a polynomial of the form f(z)=akzk+ak1zk1++a0, where k1 and ak(0),ak1,,a0 are constants. Then

    f(z)=kakzk1+(k1)ak1zk2+,f(z)=k(k1)akzk2+(k1)(k2)ak1zk3+,, (2.3)

    and

    Δcf(z)=ak[(z+c)kzk]+ak1[(z+c)k1zk1]++a1c=ak(kczk1+(k2)c2zk2+)+ak1[(k1)czk2+]++a1c=akkczk1+[ak(k2)c2+ak1(k1)c]zk2++a1c. (2.4)

    Substituting (2.3), (2.4) into Eq. (2.2), we obtain

    {iαakkc=nηn1kak,iα[ak(k2)c2+ak1(k11)c]=nηn1(k1)ak1+(n2)ηn2k(k1)ak,

    which means {iαc=nηn1,12akk(k1)ηn2(ηcn+1)=0. In view of ηcn1, thus it follows that iαc=nηn1 and k=1.

    Noting that f(z) is a polynomial of degree one if k=1, then the conclusions of this lemma are proved.

    Therefore, this completes the proof of this lemma.

    Lemma 2.3. Let α,a,c be three nonzero constants. If R1,R2 are two nonconstant rational functions satisfying the following differential-difference equations

    {iαeac[R1(z+c)R1(z)]=R1(z)+2aR1(z),iαeac[R2(z+c)R2(z)]=R2(z)+2aR2(z), (2.5)

    Then eac=±1 and R1,R2 are two polynomials of degree one.

    Proof. Firstly, (2.5) can be written in the following form

    {R1(z+c)=1iαeac[R1(z)+2aR1(z)]+R1(z),R2(z+c)=1iαeac[R2(z)+2aR2(z)]+R2(z). (2.6)

    Similar to the argument in Lemma 2.2, we can prove that R1,R2 are two nonconstant polynomials. Let

    R1(z)=akzk+ak1zk1++a1z+a0,R2(z)=btzt+bt1zt1++b1z+b0,

    where aj,bjC, ak0,bt0, k1 and t1. Substituting R1(z),R2(z) into (2.5), and comparing the coefficients of zk1,zk2,zt1 and zt2 both sides of such two equations, it yields

    {iαeacakkc=2aakk,iαeacbttc=2aatt,iαeac[ak(k2)c2+ak1(k1)c]=2a(k1)ak1+k(k1)ak,iαeac[bt(t2)c2+bt1(t1)c]=2a(t1)bt1t(t1)bt,

    which means

    {eac=±1,k(k1)(ac1)=0,t(t1)(ac+1)=0. (2.7)

    Since k1 and t1, it follows eac=±1 and k=1,s=1. Therefore, this completes the proof of Lemma 2.3

    Lemma 2.4. Let R be a nonconstant rational function and p(z)=az+b (a0). Denote A1=R+Rp, An=An1+An1p, B1=RRp, Bn=Bn1+Bn1(p). Then

    lim|z|AnR=0,lim|z|AnR=an,lim|z|BnR=0,lim|z|BnR=(a)n.

    Proof. We use the mathematical induction to prove it. When k=1, since R is a nonconstant rational function and p=a, then lim|z|A1R=lim|z|R+RaR=0 and lim|z|A1R=lim|z|R+RpR=a.

    Suppose that lim|z|AkR=0,lim|z|AkR=ak. Thus, lim|z|Ak+1R=lim|z|Ak+AkaR=0 and lim|z|Ak+1R=lim|z|Ak+AkpR=ak+1. Hence, we have lim|z|AnR=0 and lim|z|AnR=an.

    Similar to the above argument, we can prove that lim|z|BnR=0 and lim|z|BnR=(a)n.

    Therefore, this completes the proof of Lemma 2.4.

    Lemma 2.5. ([30,Theorem 1.51]). Suppose that f1,f2,,fn(n2) are meromorphic functions and g1,g2,, gn are entire functions satisfying the following conditions

    (i) nj=1fjegj0;

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

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

    Then fj0 (j=1,2,,n).

    Lemma 2.6. (see [30,Theorem 2.7]). Let f be a meromorphic function of finite order ρ(f). Write

    f(z)=ckzk+ck+1zk+1+,(ck0)

    near z=0 and let {a1,a2,} and {b1,b2,} be the zeros and poles of f in C{0}, respectively. Then

    f(z)=zkeQ(z)P1(z)P2(z),

    where P1(z) and P2(z) are the canonical products of f formed with the non-null zeros and poles of f, respectively, and Q(z) is a polynomial of degree ρ(f).

    Proof. Suppose that Eq. (1.1) admits a finite order transcendental meromorphic solution f(z) with finitely many poles. We can rewrite Eq. (1.1) as

    [f(z)+i(αf(z+c)βf(z))][f(z)i(αf(z+c)βf(z))]=R(z). (3.1)

    Since f(z) has finitely many poles and R is a nonzero rational function, then f(z)+i(αf(z+c)βf(z)) and f(z)i(αf(z+c)βf(z)) both have finitely many poles and zeros. Thus, in view of Lemma 2.6, (3.1) can be written as

    {f(z)+i(αf(z+c)βf(z))=R1ep(z),f(z)i(αf(z+c)βf(z))=R2ep(z), (3.2)

    where R1,R2 are two nonzero rational functions such that R1R2=R and p(z) is a nonconstant polynomial. By solving the above equations system, we have

    {f(z)=R1ep(z)+R2ep(z)2,αf(z+c)βf(z)=R1ep(z)R2ep(z)2i. (3.3)

    Substituting the first equation of system (3.3) into the second equation of system (3.3), we get

    ep(z)[iαR1(z+c)ep(z+c)p(z)iβR1(z)R1(z)]+ep(z)[iαR2(z+c)ep(z+c)+p(z)iβR2(z)+R2(z)]=0. (3.4)

    By Lemma 2.5, it yields from (3.4) that

    {iαR1(z+c)ep(z+c)p(z)iβR1(z)R1(z)=0,iαR2(z+c)ep(z+c)+p(z)iβR2(z)+R2(z)=0. (3.5)

    Since R1,R2 are two nonzero rational functions and f is of finite order, we obtain that p(z) is a polynomial of degree one. Otherwise, assume that degzp(z)2. Thus, in view of (3.5), we have

    ep(z+c)p(z)=iβR1(z)+R1(z)iαR1(z+c),ep(z+c)+p(z)=iβR2(z)R2(z)iαR2(z+c),

    which imply 1=ρ(ep(z+c)p(z))=ρ(iβR1(z)+R1(z)iαR1(z+c))=0, a contradiction. Hence, degzp(z)=1. Let p(z)=az+b, a0,bC. Substituting this into (3.5), we can deduce

    lim|z|i(R1(z+c)R1(z)ep(z+c)p(z)β)=i(αeacβ)=1,lim|z|i(R2(z+c)R2(z)ep(z+c)p(z)β)=i(αeacβ)=1.

    Thus, it yields that α2β2=1, a contradiction.

    Therefore, this completes the proof of Theorem 1.1.

    Proof. Suppose that f(z) is a transcendental entire solution with finite order of Eq. (1.2). Similar to the above argument as in the proof of Theorem 1.1, it follows that

    {f(z)=Q1ep(z)+Q2ep(z)2,αf(z+c)βf(z)=Q1ep(z)Q2ep(z)2iP(z), (4.1)

    where p(z) is a nonconstant polynomial and Q1(z)Q2(z)=Q(z), Q1(z),Q2(z) are nonzero polynomials. In view of (4.1), it yields that

    ep(z)[iαP(z)Q1(z+c)ep(z+c)p(z)iβP(z)Q1(z)Q1(z)]+ep(z)[iαP(z)Q2(z+c)ep(z+c)+p(z)iβP(z)Q2(z)+Q2(z)]=0. (4.2)

    Since p(z) is a nonconstant polynomial, then by Lemma 2.5, we conclude that

    {iαP(z)Q1(z+c)ep(z+c)p(z)iβP(z)Q1(z)Q1(z)=0,iαP(z)Q2(z+c)ep(z+c)+p(z)iβP(z)Q2(z)+Q2(z)=0, (4.3)

    which implies that p(z) is a polynomial of degree one. Set p(z)=az+b, a0,bC. Thus, it follows from (4.3) that

    {iαP(z)Q1(z+c)eac=(iβP(z)+1)Q1(z),iαP(z)Q2(z+c)eac=(iβP(z)1)Q2(z),

    which means that

    α2P(z)2Q1(z+c)Q2(z+c)=(β2P(z)2+1)Q1(z)Q2(z).

    Hence, it yields

    P(z)2[α2Q(z+c)β2Q(z)]=Q(z). (4.4)

    Set degzP=p and degzQ=q, then p0, q0 and p,qN+.

    Case 1. p1 and α=±β. If q1. Since α0, thus, by comparing the order both sides of Eq. (4.4), it follows 2p+q1=q, that is, p=12, a contradiction. If q=0, that is, Q(z) is a constant. Thus, we can conclude from (4.4) that Q(z)0, a contradiction.

    Case 2. p1 and α±β. If q1. Since α0, thus, by comparing the order both sides of Eq. (4.4), it follows 2p+q=q, that is, p=0, a contradiction. If q=0, that is, Q(z) is a constant. Thus, we can conclude from (4.4) that P(z) is a constant, a contradiction with p1.

    Case 3. p=0 and α=±β. Thus, P(z)=K(0). If q1. Since α0, thus, by comparing the order both sides of Eq. (4.4), it follows q1=q, a contradiction. If q=0, it follows Q(z)0, a contradiction.

    Case 4. p=0 and α±β. If q1, set P(z)=K(0), Q(z)=bqzq+bq1zq1++b0, bq0,bq1,,b0 are constants. By comparing the coefficients of zq,zq1 both sides of (4.4), it yields that

    K2[α2β2]=1,K2[α2qcaq+(α2β2)aq1]=aq1, (4.5)

    which implies that α2qcaq=0, a contradiction. If q=0, then K2(α2β2)=1, a contradiction.

    Therefore, this completes the proof of Theorem 1.2.

    Proof. Suppose that Eq. (1.3) admits a finite order transcendental meromorphic solution f(z) with finitely many poles. We can rewrite Eq. (1.3) in the following form

    [f(z)+i(αf(z+c)βf(z))][f(z)i(αf(z+c)βf(z))]=R(z). (5.1)

    Since f(z) has finitely many poles and R is a nonzero rational function, then f(z)+i(αf(z+c)βf(z)) and f(z)i(αf(z+c)βf(z)) both have finitely many poles and zeros. Thus, in view of Lemma 2.6, (5.1) can be written as

    {f(z)+i(αf(z+c)βf(z))=R1ep(z),f(z)i(αf(z+c)βf(z))=R2ep(z), (5.2)

    where R1,R2 are two nonzero rational functions such that R1R2=R, and p(z) is a nonconstant polynomial. By solving the above equations system, we have

    {f(z)=R1ep(z)+R2ep(z)2,αf(z+c)βf(z)=R1ep(z)R2ep(z)2i. (5.3)

    In view of the second equation of (5.3), it follows that

    αf(z+c)βf(z)=A1ep(z)B1ep(z)2i, (5.4)

    where A1=R1+R1p and B1=R2R2p. Substituting the first equation of system (5.3) into (5.4), it yields that

    ep(z)[iαR1(z+c)ep(z+c)p(z)iβR1(z)A1(z)]+ep(z)[iαR2(z+c)ep(z+c)+p(z)iβR2(z)+B1(z)]=0. (5.5)

    By Lemma 2.5, it yields from (5.5) that

    {iαR1(z+c)ep(z+c)p(z)iβR1(z)A1(z)=0,iαR2(z+c)ep(z+c)+p(z)iβR2(z)+B1(z)=0. (5.6)

    Since R1,R2 are two nonzero rational functions and f is of finite order, similar to argument as in the proof of Theorem 1.1, it follows that p(z) is a polynomial of degree one. Let p(z)=az+b, a0,bC. Substituting p(z),A1,B1 into (5.6), and let z, thus we can conclude from Lemma 2.4 that

    lim|z|i(R1(z+c)R1(z)ep(z+c)p(z)β)=i(αeacβ)=R1(z)R1(z)+a=a,lim|z|i(R2(z+c)R2(z)ep(z+c)p(z)β)=i(αeacβ)=R2(z)R2(z)+a=a,

    which means that

    i(αeacβ)=a,i(αeacβ)=a. (5.7)

    Hence, it yields eac=±1.

    If eac=1, then a=iαiβ. Thus, we can rewrite (5.6) in the following form

    {iα[R1(z+c)R1(z)]=R1(z),iα[R2(z+c)R2(z)]=R2(z). (5.8)

    If R1,R2 are nonzero constants, then (5.8) holds and R=R1R2 is a constant.

    If Rj(j=1,2) is a nonzero rational function, then in view of Lemma 2.1, it follows that iαc=1 and Rj(j=1,2) is a polynomial of degzRj=1. In view of R=R1R2, thus R is a nonconstant polynomial with degzR2.

    If eac=1, then a=iαiβ. Thus, we can rewrite (5.6) in the following form

    {iα[R1(z+c)R1(z)]=R1(z),iα[R2(z+c)R2(z)]=R2(z). (5.9)

    Like in the previous case, we can obtain that iαc=±1 and R(z) is a nonconstant polynomial with degzR2 or R(z) is a nonzero constant.

    Hence, we can conclude that R is a nonconstant polynomial with degzR2 or R is a nonzero constant.

    (ⅰ) Suppose that R(z) is a nonconstant polynomial with degzR2, then in view of the first equation of (5.3), it follows that f(z) is of the form

    f(z)=s1(z)eaz+b+s2(z)e(az+b)2+γ, (5.10)

    where sj(z)=mjz+nj,mj,njC (j=1,2) and γC.

    Case 1. If degzR=2, then it follows that mj0(j=1,2). Substituting (5.10) into (5.3), it follows that R(z)=(as1(z)+m1)(as2(z)+m2), iαc=1 and a=i(αβ) or iαc=1 and a=i(α+β).

    If iαc=1 and a=i(αβ), then eac=1, i.e., c=2kπia. Obviously, αβ as a0. If α=β, then a=2iα. Thus, since α0 and from (5.7), it follows 1=eac=e2iαc=e2, a contradiction. Hence, α±β. Thus, substituting (5.10) into the second equation of (5.3), it follows γ0.

    If iαc=1 and a=i(α+β), then eac=1, i.e., c=(2k+1)πia. Obviously, αβ as a0. If α=β, then a=2iα. Thus, since α0 and from (5.7), it follows 1=eac=e2iαc=e2, a contradiction. Hence, α±β.

    Case 2. If degzR=1, then one of m1,m2 is zero, without loss of generality, assuming that m1=0. Substituting (5.10) into (5.3), it follows that R1 is a constant and R2 is a polynomial of degree one, and iαc=1 and a=i(αβ) or iαc=1 and a=i(α+β). Similar to the argument as in Case 1, it is easy to prove that α±β and γ0.

    Therefore, f(z) is of the form

    f(z)=s1(z)eaz+b+s2(z)e(az+b)2,

    where R(z)=(as1(z)+m1)(as2(z)+m2), a0,bC, and a,b,c,α,β satisfy α±β, a=i(α+β), c=(2k+1)πai, iαc=1 or a=i(αβ), c=2kπai, iαc=1.

    (ⅱ) If R(z) is a nonzero constant, then in view of the first equation of (5.3), it follows that f(z) is of the form

    f(z)=n1eaz+b+n2e(az+b)2+d, (5.11)

    where n1,n2C and γC. Substituting (5.11) into the first equation of (5.3), it yields R=a2n1n2. For the sake of brevity and readability, we give the proof of Theorem 1.3 (ii1)-(ii3) in Appendix A.

    Therefore, this completes the proof of Theorem 1.3.

    Proof. Suppose that Eq. (1.4) admits a finite order transcendental meromorphic solution f(z) with finitely many poles. We can rewrite Eq. (1.4) as

    [f(z)+i(αf(z+c)βf(z))][f(z)i(αf(z+c)βf(z))]=R(z). (6.1)

    Since f(z) has finitely many poles and R is a nonzero rational function, then f(z)+i(αf(z+c)βf(z)) and f(z)i(αf(z+c)βf(z)) both have finitely many poles and zeros. Thus, (6.1) can be written as

    {f(z)+i(αf(z+c)βf(z))=R1ep(z),f(z)i(αf(z+c)βf(z))=R2ep(z), (6.2)

    where R1,R2 are two nonzero rational functions such that R1R2=R and p(z) is a nonconstant polynomial. By solving the above equations system, we have

    {f(z)=R1ep(z)+R2ep(z)2,αf(z+c)βf(z)=R1ep(z)R2ep(z)2i. (6.3)

    In view of the second equation of (6.3), it follows that

    αf(z+c)βf(z)=A2ep(z)B2ep(z)2i, (6.4)

    where A2=A1+A1p and B2=B1B1p. Substituting the first equation of system (6.3) into (6.4), it yields

    ep(z)[iαR1(z+c)ep(z+c)p(z)iβR1(z)A2(z)]+ep(z)[iαR2(z+c)ep(z+c)+p(z)iβR2(z)+B2(z)]=0. (6.5)

    By Lemma 2.5, it yields from (6.5) that

    {iαR1(z+c)ep(z+c)p(z)iβR1(z)A2(z)=0,iαR2(z+c)ep(z+c)+p(z)iβR2(z)+B2(z)=0. (6.6)

    Since R1,R2 are two nonzero rational functions and f is of finite order, we obtain that p(z) is a polynomial of degree one. Let p(z)=az+b, a0,bC. Substituting p(z),A2,B2 into (6.6), and let z, thus we can conclude from Lemma 2.4 that

    lim|z|i(R1(z+c)R1(z)ep(z+c)p(z)β)=i(αeacβ)=A1(z)R1(z)+a2=a2,lim|z|i(R2(z+c)R2(z)ep(z+c)p(z)β)=i(αeacβ)=B1(z)R2(z)a2=a2,

    which means that

    i(αeacβ)=a2,i(αeacβ)=a2. (6.7)

    Hence, it follows a4=α2β2.

    (ⅰ) If α=±β, this is a contradiction with a4=α2β2. Therefore, this proves the conclusion of Theorem 1.3 (ⅰ).

    (ⅱ) If α±β. Substituting p(z)=az+b and (6.7) into (6.6), it yields

    {iαeac[R1(z+c)R1(z)]=R1(z)+2aR1(z),iαeac[R2(z+c)R2(z)]=R2(z)+2aR2(z). (6.8)

    Suppose that R1,R2 are nonconstant rational functions, in view of Lemma 2.3 and (6.8), we can conclude that eac=±1 and R1,R2 are nonconstant polynomials of degree one. Set degzR1=k and degzR2=s.

    If k=1 and s=1, in view of Lemma 2.3, we obtain (2.7). If eac=1, then from (6.7), it follows that iαiβ=a2 and iαiβ=a2, a contradiction. If eac=1, then from (6.7), it follows that iαiβ=a2 and iαiβ=a2, a contradiction. Hence, there is at most a polynomial of degree one in R1 and R2. For the sake of brevity and readability, we give the proof of Theorem 1.4 (ii1) and (ii2) in Appendix B.

    Therefore, this completes the proof of Theorem 1.4.

    We thank the referee(s) for reading the manuscript very carefully and making a number of valuable and kind comments which improved the presentation.

    This work was supported by the National Natural Science Foundation of China (11561033, 11561031), the Natural Science Foundation of Jiangxi Province in China (20181BAB201001), and the Foundation of Education Department of Jiangxi (GJJ180734) of China.

    The authors declare that none of the authors have any competing interests in the manuscript.



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