<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">JAMP</journal-id><journal-title-group><journal-title>Journal of Applied Mathematics and Physics</journal-title></journal-title-group><issn pub-type="epub">2327-4352</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/jamp.2022.109188</article-id><article-id pub-id-type="publisher-id">JAMP-120219</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  On the Meromorphic Solutions of Fermat-Type Differential Equations
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Dengfeng</surname><given-names>Liu</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Biao</surname><given-names>Pan</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>School of Mathematics and Statistics, Fujian Normal University, Fuzhou, China</addr-line></aff><pub-date pub-type="epub"><day>02</day><month>09</month><year>2022</year></pub-date><volume>10</volume><issue>09</issue><fpage>2820</fpage><lpage>2836</lpage><history><date date-type="received"><day>22,</day>	<month>August</month>	<year>2022</year></date><date date-type="rev-recd"><day>27,</day>	<month>September</month>	<year>2022</year>	</date><date date-type="accepted"><day>30,</day>	<month>September</month>	<year>2022</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  In this paper, we investigate the meromorphic solutions of the Fermat-type differential equations 
  <em>f</em>’(
  <em>z</em>)
  <sup><em>n</em></sup> + 
  <em>f</em>(
  <em>z</em>+
  <em>c</em>)
  <sup><em>m</em></sup> = 
  <em>e</em>
  <em><sup>Az</sup></em>
  <sup>+</sup>
  <em style="vertical-align:super;">B</em> (
  <em>c</em> ≠ 0) over the complex plane C for positive integers 
  <em>m</em>, 
  <em>n</em>, and 
  <em>A</em>, 
  <em>B</em>, 
  <em>c</em> are constants. Our results improve and extend some earlier results given by Liu 
  <em>et al</em>. Moreover, some examples are presented to show the preciseness of our results.
 
</p></abstract><kwd-group><kwd>Fermat-Type Equations</kwd><kwd> Differential Equations</kwd><kwd> Nevanlinna Theory</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction and Main Results</title><p>Throughout this paper, we concentrate on such meromorphic functions that are nonconstant and meromorphic in the whole complex plane ℂ . Then it is assumed that the reader is familiar with the fundamental notation and terminology of Nevanlinna’s value distribution theory (see [<xref ref-type="bibr" rid="scirp.120219-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.120219-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.120219-ref3">3</xref>] [<xref ref-type="bibr" rid="scirp.120219-ref4">4</xref>]) and in particular with the most usual of symbols: T ( r , f ) , N ( r , f ) , N &#175; ( r , f ) , m ( r , f ) and the order ρ ( f ) and so on. Meanwhile, we denote by S ( f ) the family of all meromorphic functions α such that T ( α , f ) = o { T ( r , f ) } , where r → + ∞ outside of a possible exceptional set of finite logarithmic measure. Moreover, we also include all constant functions in S ( f ) .</p><p>The following equation</p><p>f n ( z ) + g n ( z ) = 1 (1.1)</p><p>can be regarded as the Fermat diophantine equations x n + y n = 1 over function fields, where n is a positive integer. Montel [<xref ref-type="bibr" rid="scirp.120219-ref5">5</xref>] obtained that Equation (1.1) has no nonconstant entire solutions when n &gt; 2 . Gross [<xref ref-type="bibr" rid="scirp.120219-ref6">6</xref>] proved that Equation (1.1) has no nonconstant meromorphic solutions when n &gt; 3 . For n = 2 , Gross [<xref ref-type="bibr" rid="scirp.120219-ref7">7</xref>] showed that all meromorphic solutions of Equation (1.1) of the form</p><p>f ( z ) = 1 − α 2 ( z ) 1 + α 2 ( z ) and g ( z ) = 2 α ( z ) 1 + α 2 ( z ) , where α ( z ) is a nonconstant meromorphic function. For n = 3 , Baker [<xref ref-type="bibr" rid="scirp.120219-ref8">8</xref>] proved that the only nonconstant meromorphic solutions of Equation (1.1) are the functions f = 1 2 { 1 + ℘ ′ ( u ) 3 } / ℘ ( u ) and g = η 2 { 1 − ℘ ′ ( u ) 3 } / ℘ ( u ) for a nonconstant entire function u and a cubic root η of unity, where ℘ denotes the Weierstrass ℘ function. Further, Yang [<xref ref-type="bibr" rid="scirp.120219-ref9">9</xref>] investigated a generalization of the Fermat-type equation</p><p>f n ( z ) + g m ( z ) = 1 (1.2)</p><p>and obtained that Equation (1.2) has no nonconstant entire solutions when 1 m + 1 n &lt; 1 . For more detail, we refer the reader to the work of Hu, Li and Yang [<xref ref-type="bibr" rid="scirp.120219-ref10">10</xref>].</p><p>As we known, Halburd-Korhonen [<xref ref-type="bibr" rid="scirp.120219-ref11">11</xref>] and Chiang-Feng [<xref ref-type="bibr" rid="scirp.120219-ref12">12</xref>] independently proved the difference analogue of the logarithmic derivative lemma in 2006. Afterwards, a number of papers have focused on entire solutions of complex difference equations and differential-difference equations. For some works related to partial differential equations of Fermat type, see [<xref ref-type="bibr" rid="scirp.120219-ref13">13</xref>] - [<xref ref-type="bibr" rid="scirp.120219-ref18">18</xref>].</p><p>In 2012, Liu et al. [<xref ref-type="bibr" rid="scirp.120219-ref13">13</xref>] investigated the entire solutions of the Fermat-type differential equation of the</p><p>f ′ ( z ) n + f ( z + c ) m = 1 (1.3)</p><p>and obtained the following results.</p><p>Theorem A ( [<xref ref-type="bibr" rid="scirp.120219-ref13">13</xref>]) Equation (1.3) has no transcendental entire solutions with finite order, provided that m ≠ n , where n , m are positive integers, c ( ≠ 0 ) is a constant.</p><p>Theorem B ( [<xref ref-type="bibr" rid="scirp.120219-ref13">13</xref>]) The transcendental entire solutions with finite order of the equation f ′ ( z ) 2 + f ( z + c ) 2 = 1 must satisfy f ( z ) = sin ( z + B i ) , where B is a constant and c = 2 k π or c = ( 2 k + 1 ) π , k is an integer.</p><p>For m = n = 1 , Liu [<xref ref-type="bibr" rid="scirp.120219-ref13">13</xref>] gave examples to illustrate the existence of the solutions of the Equation (1.3).</p><p>Example A f ( z ) = 1 + e z is a solution of the equation f ′ ( z ) + f ( z + c ) = 1 , where e c = − 1 .</p><p>Example B f ( z ) = 1 + sin z is a solution of the equation f ′ ( z ) + f ( z + c ) = 1 , where c = 3 π 2 .</p><p>Since no attempts, till now, have so far been made by any researchers investigating the form of the solution of Equation (1.3) When m = n = 1 . Naturally, we pose the following questions.</p><p>Question 1. Can we get the forms of the solutions of Equation (1.3) when m = n = 1 .</p><p>In addition, we recall the definition of exponential polynomial, an exponential polynomial of order q ≥ 1 , which is an entire function of the form:</p><p>f ( z ) = P 1 ( z ) e Q 1 ( z ) + P 2 ( z ) e Q 2 ( z ) + ⋯ + P k ( z ) e Q k ( z ) , (1.4)</p><p>where P i ( z ) and Q i ( z ) are polynomials in z for 1 ≤ j ≤ k , such that q = max { deg ( Q j ) : 1 ≤ j ≤ k } . Following Steinmetz [<xref ref-type="bibr" rid="scirp.120219-ref19">19</xref>], such a function can be written in the form:</p><p>f ( z ) = H 0 ( z ) + H 1 ( z ) e ω 1 z q + ⋯ + H m ( z ) e ω m z q , (1.5)</p><p>where ω 1 , ω 2 , ⋯ , ω m ( 1 ≤ k ≤ m ) are m distinct finite nonzero complex numbers, while H j ( z ) ≡ 0   ( j = 1 , 2 , ⋯ , m ) is either an exponential polynomial of degree less than q or an ordinary polynomial in z for 0 ≤ m ≤ j .</p><p>In this paper, we pay our attention to the above question and prove the following some theorems that improve and extend Theorem B.</p><p>Theorem 1.1. Let f ( z ) be the exponential polynomial solutions of the equation</p><p>f ′ ( z ) + f ( z + c ) = 1 , (1.6)</p><p>where c ∈ ℂ \ { 0 } , one of the following conclusions hold:</p><p>1) If c = − 1 e , then f ( z ) = 1 + ( a z + b ) e − e z + ∑ i = 1 m     b i e w i z , where a , b , b i ∈ ℂ , w i satisfy e − 1 e w i + w i = 0   ( w i ≠ − e ) .</p><p>2) If c ≠ − 1 e , then f ( z ) = 1 + ∑ i = 1 m     b i e w i z , where b i ∈ ℂ , w i satisfy e w i c + w i = 0 .</p><p>Example 1.1. If c = − 1 e in (1.6), then the exponential polynomial solutions of the following equation</p><p>f ′ ( z ) + f ( z − 1 e ) = 1</p><p>must satisfy f ( z ) = 1 + ( a z + b ) e − e z + ∑ i = 1 m     b i e w i z , where a , b , b i ∈ ℂ , e − 1 e w i + w i = 0   ( w i ≠ − e ) . It is easy to obtain that the above equation has a solution f ( z ) = 1 + ( 1 + z ) e − e z .</p><p>Example 1.2. If c = − π 2 + 2 k π in (1.6), then the exponential polynomial solutions of the following equation</p><p>f ′ ( z ) + f ( z − π 2 + 2 k π ) = 1</p><p>must satisfy f ( z ) = 1 + ∑ i = 1 m     b i e w i z , where b i ∈ ℂ , e − π 2 w i + w i = 0 . It is easy to obtain that the above equation has a solution f ( z ) = 1 + a 1 e i z + a 2 e − i z , where a 1 , a 2 are constants.</p><p>Further, we study the solutions of Fermat-type differential equation</p><p>f ′ ( z ) n + f ( z + c ) m = e A z + B , (1.7)</p><p>where m , n are positive integers, c ∈ ℂ \ { 0 } , A , B , c ∈ ℂ . First of all, one fact needs to be clear. For n = m , the general trivial solutions of Equation (1.7) is f ( z ) = d e A z + B n , where d n ( ( A n ) n + e A c ) = 1 . In this paper, we study the solution of nontrivial solutions and prove the following results.</p><p>Theorem 1.2. Let f ( z ) be the exponential polynomial solutions of the equation</p><p>f ′ ( z ) + f ( z + c ) = e A z + B , (1.8)</p><p>where A , B , c ∈ ℂ and c \ { 0 } , one of the following conclusions hold:</p><p>1) If A + e A c ≠ 0 and c = − 1 e , then f ( z ) = e A z + B ( 1 A + e A c + ( a z + b ) e ( − e − A ) z + ∑ i = 1 m     b i e w i z ) , where a , b , b i ∈ ℂ , w i satisfy e − 1 e ( A + w i ) + A + w i = 0 . If A + e A c ≠ 0 and c ≠ − 1 e , then f ( z ) = e A z + B ( 1 A + e A c + ∑ i = 1 m     b i e w i z ) , where b i ∈ ℂ , w i satisfy e ( A + w i ) c + A + w i = 0 .</p><p>2) If A + e A c = 0 , c = − 1 e and A c ≠ 1 (namely A ≠ − e ), then f ( z ) = e A z + B ( a 0 + 1 1 + c e A c z + ( a z + b ) e ( − e − A ) z + ∑ i = 1 m     b i e w i z ) , where a 0 , a , b , b i ∈ ℂ , w i satisfy e − 1 e ( A + w i ) + A + w i = 0 . If A + e A c = 0 , c ≠ − 1 e and A c ≠ 1 , then f ( z ) = e A z + B ( a 0 + 1 1 + c e A c z + ∑ i = 1 m     b i e w i z ) , where a 0 , b i ∈ ℂ , w i satisfy e ( A + w i ) c + A + w i = 0 .</p><p>3) If A + e A c = 0 , c = − 1 e and A = − e (namely A c = 1 ), then f ( z ) = e A z + B ( a 0 + a 1 z + 1 c 2 e A c z 2 + ∑ i = 1 m     b i e w i z ) , where a 0 , a 1 , b i ∈ ℂ , w i satisfy e − 1 e ( − e + w i ) − e + w i = 0 .</p><p>Example 1.3. If c = π i , A = 2 , B = 1 in (1.8), then the exponential polynomial solutions of the following equation</p><p>f ′ ( z ) + f ( z + π i ) = e 2 z + 1</p><p>must satisfy f ( z ) = e 2 z + 1 ( 1 3 + ∑ i = 1 m     b i e w i z ) , where b i ∈ ℂ , e ( 2 + w i ) π i + 2 + w i = 0 . It is easy to obtain that the above equation has a solution f ( z ) = e 2 z + 1 ( 1 3 + e − z ) .</p><p>Example 1.4. If c = − 1 e , A = 1 , B = − 1 in (1.8), then the exponential polynomial solutions of the following equation</p><p>f ′ ( z ) + f ( z − 1 e ) = e z − 1</p><p>must satisfy f ( z ) = e z − 1 ( 1 1 + e − 1 e + ( a z + b ) e ( − e − 1 ) z + ∑ i = 1 m     b i e w i z ) , where a , b , b i ∈ ℂ , e ( 1 + w i ) ( − 1 e ) + 1 + w i = 0 . It is easy to obtain that the above equation has a solution f ( z ) = e z − 1 ( 1 1 + e − 1 e + ( 1 + z ) e ( − e − 1 ) z ) .</p><p>Example 1.5. If c = π i , A = 1 , B = 1 in (1.8), then the exponential polynomial solutions of the following equation</p><p>f ′ ( z ) + f ( z + π i ) = e z + 1</p><p>must satisfy f ( z ) = e z + 1 ( a 0 + 1 1 − π i z + ∑ i = 1 m     b i e w i z ) , where a 0 ,   b i ∈ ℂ , e ( 1 + w i ) π i + 1 + w i = 0 . It is easy to obtain that the above equation has a solution f ( z ) = e z + 1 ( 1 + 1 1 − π i z ) .</p><p>Example 1.6. If c = − 1 e , A = − e , B = 1 in (1.8), then the exponential polynomial solutions of the following equation</p><p>f ′ ( z ) + f ( z − 1 e ) = e − e z + 1</p><p>must satisfy f ( z ) = e − e z + 1 ( a 0 + a 1 z + e z 2 + ∑ i = 1 m     b i e w i z ) , where a 0 ,   a 1 ,   b i ∈ ℂ , e ( − e + w i ) ( − 1 e ) − e + w i = 0 . It is easy to obtain that the above equation has a solution f ( z ) = e − e z + 1 ( 1 + z + e z 2 ) .</p><p>Theorem 1.3. The transcendental entire solutions of</p><p>f ′ ( z ) 2 + f ( z + c ) 2 = e A z + B (1.9)</p><p>must satisfy</p><p>f ( z ) = e h ( z − c ) − e − h ( z − c ) 2 i e A c 2 e A z + B 2 ,</p><p>where h ( z ) = a z + b , a 2 = A 2 4 − e A c and c = ln a − A 2 i + 2 k π i A 2 − a .</p><p>Remark 1. Since for a particular choice of A = B = 0 in Theorem 1.3, then e A z + B = 1 , a 2 = A 2 4 − e A c = − 1 , namely a = &#177; i . If a = i , then c = 2 k π , f ( z ) = sin ( z − B i ) , if a = − i , then c = ( 2 k + 1 ) π , f ( z ) = sin ( z + B i ) , k is an integer. The result obtained is the same as Theorem B, and Theorem 1.3 omit the condition of the finite order. Therefore, Theorem 1.3 improves and extends Theorem B.</p><p>Theorem 1.4. The following equation</p><p>f ′ ( z ) n + f ( z + c ) n = e A z + B (1.10)</p><p>has no nontrivial meromorphic solutions, where n ≥ 3 is positive integers and c ∈ ℂ \ { 0 } .</p><p>Theorem 1.5 Let m , n be positive integers satisfying 1 m + 1 n &lt; 2 3 , then Equation (1.7) has no nontrivial meromorphic solutions with ρ ( f ) ≠ 1 .</p></sec><sec id="s2"><title>2. Some Lemmas</title><p>Lemma 2.1. (see [<xref ref-type="bibr" rid="scirp.120219-ref2">2</xref>]) Let f j ( z ) ( j = 1 , 2 , ⋯ , n ) ( n ≥ 2 ) be meromorphic functions, g j ( z ) ( j = 1 , 2 , ⋯ , n ) be entire functions satisfying following conditions:</p><p>1) ∑ j = 1 n     f j ( z ) e g j ( z ) ≡ 0 ;</p><p>2) for 1 ≤   j &lt;   k ≤   n , g j − g k are not constants;</p><p>3) for 1 ≤   j ≤   n , 1 ≤   h &lt;   k ≤   n ,</p><p>T ( r , f j ) = o { T ( r , e g h − g k ) } , r →   ∞ , r ∉   E .</p><p>where E ⊂ ( 1, ∞ ) , E is a possible exceptional set of finite logarithmic measure, then f j ( z ) ≡ 0   ( j = 1 , 2 , ⋯ , n ) .</p><p>Lemma 2.2. (see [<xref ref-type="bibr" rid="scirp.120219-ref2">2</xref>]) Let f 1 ( z ) , f 2 ( z ) , f 3 ( z ) be meromorphic functions and satisfying ∑ i = 1 3     f i ( z ) ≡ 1 , f 1 be nonconstant and</p><p>∑ j = 1 3     N ( r , 1 f j ) + 2 ∑ j = 2 3     N &#175; ( r , f j ) &lt; ( λ + o ( 1 ) ) T ( r ) , r ∈ I</p><p>where 0 ≤ λ &lt; 1 , T ( r ) = max 1 &lt; j &lt; 3 { T ( r , f j ) } , and I has infinite linear measure, then f 2 ( z ) ≡ 1 or f 3 ( z ) ≡ 1 .</p><p>Lemma 2.3. (see [<xref ref-type="bibr" rid="scirp.120219-ref2">2</xref>]) Let f ( z ) be a nonconstant meromorphic function in the complex plane and R ( f ) = P ( f ) Q ( f ) , where P ( f ) = ∑ k = 0 p     a k f k and Q ( f ) = ∑ j = 0 q     b j f j are two mutually prime polynomials in f. If the coefficients { a k ( z ) } , { b j ( z ) } are small functions of f and a p ( z ) ≡ 0 , b q ( z ) ≡ 0 , then</p><p>T ( r , R ( f ) ) = max { p , q } ⋅ T ( r , f ) + S ( r , f ) .</p><p>Lemma 2.4. (see [<xref ref-type="bibr" rid="scirp.120219-ref2">2</xref>]) Let h ( z ) be a nonconstant entire function and f ( z ) = e h ( z ) , then T ( r , h ′ ) = o ( T ( r , f ) ) .</p><p>Lemma 2.5. (see [<xref ref-type="bibr" rid="scirp.120219-ref9">9</xref>]) Let a ( z ) , b ( z ) , f ( z ) , g ( z ) be meromorphic functions and satisfying T ( r , a ( z ) ) = o ( T ( r , f ) ) , T ( r , b ( z ) ) = o ( T ( r , g ) ) . If max { m , n } &gt; 3 , min { m , n } ≥ 3 , then the following equation</p><p>a ( z ) f n ( z ) + b ( z ) g m ( z ) = 1</p><p>has no meromorphic solution.</p><p>Lemma 2.6. (see [<xref ref-type="bibr" rid="scirp.120219-ref11">11</xref>]) Let f ( z ) be a nonconstant meromorphic function with ρ ( f ) &lt; + ∞ , c ∈ ℂ , then for ε &gt; 0 we have</p><p>m ( r , f ( z + c ) f ( z ) ) = O ( r ρ − 1 + ε ) ,</p><p>for all r outside of a set of finite logarithmic measure.</p><p>Lemma 2.7. (see [<xref ref-type="bibr" rid="scirp.120219-ref12">12</xref>]) Let f ( z ) be a nonconstant meromorphic function with ρ ( f ) &lt; + ∞ , c ∈ ℂ , then for ε &gt; 0 , we have</p><p>T ( r , f ( z + c ) ) = T ( r , f ( z ) ) + O ( r ρ − 1 + ε ) + O ( log   r ) ,</p><p>for all r outside of a set of finite logarithmic measure.</p><p>Lemma 2.8. (see [<xref ref-type="bibr" rid="scirp.120219-ref20">20</xref>]) Let f ( z ) be a nonconstant meromorphic function, then ρ ( f ) = ρ ( f ′ ) and μ ( f ) = μ ( f ′ ) .</p><p>Lemma 2.9 (see [<xref ref-type="bibr" rid="scirp.120219-ref21">21</xref>]) Let f ( z ) be a nonconstant meromorphic function and f 1 ( z ) = f ( a z + b ) , a ≠ 0 , then ρ ( f ) = ρ ( f 1 ) .</p></sec><sec id="s3"><title>3. Proofs of Theorems</title><p>Proof of Theorem 1.1</p><p>Assume that f ( z ) is the exponential polynomial solutions of (1.6), substituting (1.5) into (1.6) yields</p><p>f ′ ( z ) + f ( z + c ) = H ′ 0 ( z ) + H 0 ( z + c ) + [ H ′ 1 ( z ) + ω 1 q z q − 1 H 1 ( z ) + H 1 ( z + c ) e ω 1 ( z + c ) q − ω 1 z q ] e ω 1 z q         + ⋯ + [ H ′ m ( z ) + ω m q z q − 1 H m ( z ) + H m ( z + c ) e ω m ( z + c ) q − ω m z q ] e ω m z q = 1. (3.1)</p><p>Let</p><p>f i = ( H ′ 0 ( z ) + H 0 ( z + c ) ,     i = 0 , H ′ i ( z ) + ω i q z q − 1 H i ( z ) + H i ( z + c ) e ω i ( z + c ) q − ω i z q ,     1 ≤ i ≤ m . (3.2)</p><p>g i = ( 0 ,     i = 0 , ω i z q ,     1 ≤ i ≤ m .</p><p>Further, we get</p><p>g j − g k = ( ω k z q ,     j = 0 ,   1 ≤ k ≤ m , ω j z q − ω k z q ,   1 ≤ j &lt; k ≤ m . (3.3)</p><p>From (3.2) and (3.3), for 0 ≤   i ≤   m , 0 ≤   j &lt;   k ≤   m , we have</p><p>T ( r , f i ) = o { T ( r , e g j − g k ) } , r →   ∞ .</p><p>Combining (3.1) with Lemma 2.1, we know that</p><p>{ H ′ 0 ( z ) + H 0 ( z + c ) − 1 ≡ 0 , H ′ 1 ( z ) + ω 1 q z q − 1 H 1 ( z ) + H 1 ( z + c ) e ω 1 ( z + c ) q − ω 1 z q ≡ 0 ,                                                   ⋮ H ′ i ( z ) + ω i q z q − 1 H i ( z ) + H i ( z + c ) e ω i ( z + c ) q − ω i z q ≡ 0 ,                                                   ⋮ H ′ m ( z ) + ω m q z q − 1 H m ( z ) + H m ( z + c ) e ω m ( z + c ) q − ω m z q ≡ 0. (3.4)</p><p>We deduce from (3.4) that q = 1 . If not, suppose that q ≥ 2 , we have</p><p>H ′ i ( z ) + ω i q z q − 1 H i ( z ) + H i ( z + c ) e ω i ( z + c ) q − ω i z q ≡ 0 ,   ( i = 1 , 2 , ⋯ , m ) .</p><p>Namely</p><p>e ω i ( z + c ) q − ω i z q ≡ − ( H ′ i ( z ) H i ( z + c ) + ω i q z q − 1 H i ( z ) H i ( z + c ) ) ,   ( i = 1 , 2 , ⋯ , m ) . (3.5)</p><p>Using logarithmic derivative Lemma and Lemma 2.6 in (3.5), then for ε &gt; 0 , we have</p><p>m ( r , e ω i ( z + c ) q − ω i z q ) = m ( r , H ′ i ( z ) H i ( z + c ) + ω i q z q − 1 H i ( z ) H i ( z + c ) ) = m ( r , H ′ i ( z ) H i ( z ) H i ( z ) H i ( z + c ) + ω i q z q − 1 H i ( z ) H i ( z + c ) ) ≤ m ( r , H ′ i ( z ) H i ( z ) ) + 2   m ( r , H i ( z ) H i ( z + c ) ) + m ( r , ω i q z q − 1 ) + log 2 ≤ S ( r , H i ( z ) ) + O ( r q − 2 + ε ) + O ( log r ) ≤ o ( r q − 1 ) ,</p><p>which implies that q = 1 . Thus, we have</p><p>f ( z ) = H 0 ( z ) + H 1 ( z ) e ω 1 z + ⋯ + H m ( z ) e ω m z ,</p><p>where H 0 ( z ) , H 1 ( z ) , ⋯ , H m ( z ) are polynomials.</p><p>Assume that</p><p>H 0 ( z ) = a k z k + a k − 1 z k − 1 + ⋯ + a 1 z + a 0 .</p><p>Further, we have</p><p>H ′ 0 ( z ) = k a k z k − 1 + ( k − 1 ) a k − 1 z k − 2 + ⋯ + a 1 , H 0 ( z + c ) = a k ( z + c ) k + a k − 1 ( z + c ) k − 1 + ⋯ + a 1 ( z + c ) + a 0 . (3.6)</p><p>Substituting (3.6) into H ′ 0 ( z ) + H 0 ( z + c ) − 1 ≡ 0 yields</p><p>( a k = 0 , C k 1 ( 1 + c ) a k + a k − 1 = 0 , C k 2 c 2 a k + C k − 1 1 ( 1 + c ) a k − 1 + a k − 2 = 0 ,                             ⋮ C k i c i a k + C k − 1 i − 1 c i − 1 a k − 1 + ⋯ + C k − i + 1 1 ( 1 + c ) a k − i + 1 + a k − i = 0 ,                             ⋮ C k k − 1 c k − 1 a k + C k − 1 k − 2 c k − 2 a k − 1 + ⋯ + C 2 1 ( 1 + c ) a 2 + a 1 = 0 , c k a k + c k − 1 a k − 1 + ⋯ + ( 1 + c ) a 1 + a 0 = 1 , (3.7)</p><p>where C k i = k ! i ! ( k − i ) ! .</p><p>Assume that</p><p>H i ( z ) = a t i z t i + a t i − 1 z t i − 1 + ⋯ + a 1 i z + b i ,     ( i = 1 , 2 , ⋯ , m ) .</p><p>Further, we get</p><p>H ′ i ( z ) = t i a t i z t i − 1 + ( t i − 1 ) a t i − 1 z t i − 2 + ⋯ + 2 a 2 i z + a 1 i , H i ( z + c ) = a t i ( z + c ) t i + a t i − 1 ( z + c ) t i − 1 + ⋯ + a 1 i ( z + c ) + b i       ( i = 1 , 2 , ⋯ , m ) . (3.8)</p><p>Substituting (3.8) into H ′ i ( z ) + ω i H i ( z ) + H i ( z + c ) e ω i c ≡ 0 yields</p><p>( ( e w i c + w i ) a t i = 0 , ( c e w i c + 1 ) t i a t i + ( e w i c + w i ) a t i − 1 = 0 , C t i 2 c 2 e w i c a t i + ( c e w i c + 1 ) ( t i − 1 ) a t i − 1 + ( e w i c + w i ) a t i − 2 = 0 ,                         ⋮ C t i j c j e w i c a t i + ⋯ + C t i − j + 2 2 c 2 e w i c a t i − j + 2 + ( c e w i c + 1 ) ( t i − j + 1 ) a t i − j + 1 + ( e w i c + w i ) a t i − j = 0 ,                         ⋮ C t i t i − 1 c t i − 1 e w i c a t i + ⋯ + C 3 2 c 2 e w i c a 3 i + ( c e w i c + 1 ) 2 a 2 i + ( e w i c + w i ) a 1 i = 0 , c t i e w i c a t i + ⋯ + ⋯ + c 2 e w i c a 2 i + ( c e w i c + 1 ) a 1 i + ( e w i c + w i ) b i = 0. (3.9)</p><p>From (3.7), we can deduce that a k = a k − 1 = a k − 2 = ⋯ = a 1 = 0 and a 0 = 1 , which implies that H 0 ( z ) = 1 .</p><p>From (3.9), we can conclude the following</p><p>1) If e w i c + w i ≠ 0 , we obtain a t i = a t i − 1 = ⋯ = a 1 i = b i = 0 , then H i ( z ) = 0 , which contradicts that f ( z ) is nonconstant.</p><p>2) If e w i c + w i = 0 and w i c ≠ 1 , we obtain a t i = a t i − 1 = ⋯ = a 1 i = 0 , then H i ( z ) = b i , where b i ∈ ℂ .</p><p>3) If e w i c + w i = 0 and w i c = 1 , we obtain a t i = a t i − 1 = ⋯ = a 2 i = 0 , then H i ( z ) = a 1 i z + b i , where a 1 i , b i ∈ ℂ .</p><p>From the above discussion, we can get that the case of the exponential polynomial solutions of Equation (1.6) is as follows.</p><p>Case 1. If c = − 1 e , then the exponential polynomial solutions of Equation (1.6) must satisfy f ( z ) = 1 + ( a z + b ) e − e z + ∑ i = 1 m     b i e w i z , where a , b , b i ∈ ℂ , w i satisfy e − 1 e w i + w i = 0   ( w i ≠ − e ) .</p><p>Case 2. If c ≠ − 1 e , then the exponential polynomial solutions of Equation (1.6) must satisfy f ( z ) = 1 + ∑ i = 1 m     b i e w i z , where b i ∈ ℂ , w i satisfy e w i c + w i = 0 .</p><p>This completes the proof of Theorem 1.1.</p><p>Proof of Theorem 1.2</p><p>We rewrite (1.8) as follows</p><p>e − ( A z + B ) f ′ ( z ) + e − ( A z + B ) f ( z + c ) = 1. (3.10)</p><p>Assume that f ( z ) is the exponential polynomial solutions of (3.10) and let</p><p>f ( z ) = e A z + B ( H 0 ( z ) + H 1 ( z ) e ω 1 z q + ⋯ + H m ( z ) e ω m z q ) .</p><p>Thus, we have</p><p>f ′ ( z ) = A e A z + B ( H 0 ( z ) + H 1 ( z ) e ω 1 z q + ⋯ + H m ( z ) e ω m z q )                         + e A z + B ( H ′ 0 ( z ) + H ′ 1 ( z ) e ω 1 z q + H 1 ( z ) ω 1 q z q − 1 e ω 1 z q + ⋯                         + H ′ m ( z ) e ω m z q + H m ( z ) ω m q z q − 1 e ω m z q ) , f ( z + c ) = e A c e A z + B ( H 0 ( z + c ) + H 1 ( z + c ) e ω 1 ( z + c ) q + ⋯                                   + H m ( z + c ) e ω m ( z + c ) q ) . (3.11)</p><p>Substituting (3.11) into (3.10) yields</p><p>e − ( A z + B ) f ′ ( z ) + e − ( A z + B ) f ( z + c ) = A H 0 ( z ) + H ′ 0 ( z ) + e A c H 0 ( z + c )     + ( A H 1 ( z ) + H ′ 1 ( z ) + H 1 ( z ) ω 1 q z q − 1 + e A c H 1 ( z + c ) e ω 1 ( z + c ) q − ω 1 z q ) e ω 1 z q + ⋯     + ( A H m ( z ) + H ′ m ( z ) + H m ( z ) ω m q z q − 1 + e A c H m ( z + c ) e ω m ( z + c ) q − ω m z q ) e ω m z q = 1. (3.12)</p><p>Let</p><p>f i = ( A H 0 ( z ) + H ′ 0 ( z ) + e A c H 0 ( z + c ) − 1 ,     i = 0 , A H i ( z ) + H ′ i ( z ) + H i ( z ) ω i q z q − 1 + e A c H i ( z + c ) e ω i ( z + c ) q − ω i z q ,     1 ≤ i ≤ m . (3.13)</p><p>g i = ( 0 ,     i = 0 , ω i z q ,     1 ≤ i ≤ m .</p><p>Further, we have</p><p>g j − g k = ( ω k z q ,     j = 0 ,   1 ≤ k ≤ m , ω j z q − ω k z q ,   1 ≤ j &lt; k ≤ m . (3.14)</p><p>From (3.13) and (3.14), for 0 ≤   i ≤   m , 0 ≤   j &lt;   k ≤   m , we have</p><p>T ( r , f i ) = o { T ( r , e g j − g k ) } ,       r →   ∞ .</p><p>Combining Lemma 2.1 with (3.12), we know that</p><p>( A H 0 ( z ) + H ′ 0 ( z ) + e A c H 0 ( z + c ) − 1 ≡ 0 , A H 1 ( z ) + H ′ 1 ( z ) + H 1 ( z ) ω 1 q z q − 1 + e A c H 1 ( z + c ) e ω 1 ( z + c ) q − ω 1 z q ≡ 0 ,                                                 ⋮ A H i ( z ) + H ′ i ( z ) + H i ( z ) ω i q z q − 1 + e A c H i ( z + c ) e ω i ( z + c ) q − ω i z q ≡ 0 ,                                                 ⋮ A H m ( z ) + H ′ m ( z ) + H m ( z ) ω m q z q − 1 + e A c H m ( z + c ) e ω m ( z + c ) q − ω m z q ≡ 0. (3.15)</p><p>We deduce from (3.4) that q = 1 . If not, suppose that q ≥ 2 , we have</p><p>( A + ω i q z q − 1 ) H i ( z ) + H ′ i ( z ) + e A c H i ( z + c ) e ω i ( z + c ) q − ω i z q ≡ 0 ,     ( i = 1 , 2 , ⋯ , m ) .</p><p>Namely</p><p>e ω i ( z + c ) q − ω i z q ≡ − 1 e A c ( H ′ i ( z ) H i ( z + c ) + ( A + ω i q z q − 1 ) H i ( z ) H i ( z + c ) ) ,       ( i = 1 , 2 , ⋯ , m ) . (3.16)</p><p>Using logarithmic derivative Lemma and Lemma 2.6 in (3.16), then for ∀ ε &gt; 0 , we have</p><p>m ( r , e ω i ( z + c ) q − ω i z q ) = m ( r , H ′ i ( z ) H i ( z + c ) + ( A + ω i q z q − 1 ) H i ( z ) H i ( z + c ) ) + O ( 1 ) = m ( r , H ′ i ( z ) H i ( z ) H i ( z ) H i ( z + c ) + ( A + ω i q z q − 1 ) H i ( z ) H i ( z + c ) ) + O ( 1 ) ≤ m ( r , H ′ i ( z ) H i ( z ) ) + 2   m ( r , H i ( z ) H i ( z + c ) ) + m ( r , A + ω i q z q − 1 ) + O ( 1 ) ≤ S ( r , H i ( z ) ) + O ( r q − 2 + ε ) + O ( log r ) ≤ o ( r q − 1 ) ,</p><p>which implies that q = 1 . Thus, we have</p><p>f ( z ) = e A z + B ( H 0 ( z ) + H 1 ( z ) e ω 1 z + ⋯ + H m ( z ) e ω m z ) ,</p><p>where H 0 ( z ) , H 1 ( z ) , ⋯ , H m ( z ) are polynomials.</p><p>Let</p><p>H 0 ( z ) = a k z k + a k − 1 z k − 1 + ⋯ + a 1 z + a 0 . (3.17)</p><p>Further, we have</p><p>H ′ 0 ( z ) = k a k z k − 1 + ( k − 1 ) a k − 1 z k − 2 + ⋯ + a 1 , H 0 ( z + c ) = a k ( z + c ) k + a k − 1 ( z + c ) k − 1 + ⋯ + a 1 ( z + c ) + a 0 . (3.18)</p><p>Substituting (3.17), (3.18) into A H 0 ( z ) + H ′ 0 ( z ) + e A c H 0 ( z + c ) − 1 ≡ 0 yields</p><p>( ( A + e A c ) a k = 0 , C k 1 ( 1 + c e A c ) a k + ( A + e A c ) a k − 1 = 0 , C k 2 e A c c 2 a k + C k − 1 1 ( 1 + c e A c ) a k − 1 + ( A + e A c ) a k − 2 = 0 ,                                     ⋮ C k i e A c c i a k + C k − 1 i − 1 e A c c i − 1 a k − 1 + ⋯ + C k − i + 1 1 ( 1 + c e A c ) a k − i + 1 + ( A + e A c ) a k − i = 0 ,                                     ⋮ C k k − 1 e A c c k − 1 a k + C k − 1 k − 2 e A c c k − 2 a k − 1 + ⋯ + C 2 1 ( 1 + c e A c ) a 2 + ( A + e A c ) a 1 = 0 , e A c c k a k + e A c c k − 1 a k − 1 + ⋯ + e A c c 2 a 2 + ( 1 + c e A c ) a 1 + ( A + e A c ) a 0 = 1 , (3.19)</p><p>where C k i = k ! i ! ( k − i ) ! .</p><p>Let</p><p>H i ( z ) = a t i z t i + a t i − 1 z t i − 1 + ⋯ + a 1 i z + b i ,       ( i = 1 , 2 , ⋯ , m ) . (3.20)</p><p>Further, we have</p><p>H ′ i ( z ) = t i a t i z t i − 1 + ( t i − 1 ) a t i − 1 z t i − 2 + ⋯ + 2 a 2 i z + a 1 i , H i ( z + c ) = a t i ( z + c ) t i + a t i − 1 ( z + c ) t i − 1 + ⋯ + a 1 i ( z + c ) + b i     ( i = 1 , 2 , ⋯ , m ) . (3.21)</p><p>Substituting (3.20), (3.21) into ( A + ω i ) H i ( z ) + H ′ i ( z ) + e ( A + ω i ) c H i ( z + c ) ≡ 0 yields</p><p>( ( e ( A + w i ) c + A + w i ) a t i = 0 , ( c e ( A + w i ) c + 1 ) t i a t i + ( e ( A + w i ) c + A + w i ) a t i − 1 = 0 , C t i 2 c 2 e ( A + w i ) c a t i + ( c e ( A + w i ) c + 1 ) ( t i − 1 ) a t i − 1 + ( e ( A + w i ) c + A + w i ) a t i − 2 = 0 ,                                               ⋮ C t i j c j e ( A + w i ) c a t i + ⋯ + C t i − j + 2 2 c 2 e ( A + w i ) c a t i − j + 2 + ( c e ( A + w i ) c + 1 ) ( t i − j + 1 ) a t i − j + 1 + ( e ( A + w i ) c + A + w i ) a t i − j = 0 ,                                               ⋮ C t i t i − 1 c t i − 1 e ( A + w i ) c a t i + ⋯ + C 3 2 c 2 e ( A + w i ) c a 3 + C 2 1 ( c e ( A + w i ) c + 1 ) a 2 + ( e ( A + w i ) c + A + w i ) a 1 = 0 , c t i e ( A + w i ) c a t i + ⋯ + c 2 e ( A + w i ) c a 2 i + ( c e ( A + w i ) c + 1 ) a 1 i + ( e ( A + w i ) c + A + w i ) b i = 0. (3.22)</p><p>From (3.19), we can conclude the following</p><p>(i) If A + e A c ≠ 0 , we obtain a k = a k − 1 = ⋯ = a 2 = a 1 = 0 , a 0 = 1 A + e A c , then H 0 ( z ) = 1 A + e A c .</p><p>(ii) If A + e A c = 0 and A c ≠ 1 , we obtain a k = a k − 1 = ⋯ = a 2 = 0 , a 1 = 1 1 + c e A c , then H 0 ( z ) = 1 1 + c e A c z + a 0 , where a 0 ∈ ℂ .</p><p>(iii) If A + e A c = 0 and A c = 1 , we obtain a k = a k − 1 = ⋯ = a 3 = 0 , a 2 = 1 c 2 e A c , then H 0 ( z ) = 1 c 2 e A c z 2 + a 1 z + a 0 , where a 0 ,   a 1 ∈ ℂ .</p><p>From (3.22), we can conclude the following</p><p>(i) If e ( A + w i ) c + A + w i ≠ 0 , we obtain a t i = a t i − 1 = ⋯ = a 1 i = b i = 0 , then H i ( z ) = 0 , which contradicts that f ( z ) is nonconstant.</p><p>(ii) If e ( A + w i ) c + A + w i = 0 and ( A + w i ) c ≠ 1 , we obtain a t i = a t i − 1 = ⋯ = a 1 i = 0 , then H i ( z ) = b i , where b i ∈ ℂ .</p><p>(iii) If e ( A + w i ) c + A + w i = 0 and ( A + w i ) c = 1 , we obtain a t i = a t i − 1 = ⋯ = a 2 i = 0 , then H i ( z ) = a 1 i z + b i , where a 1 i , b i ∈ ℂ .</p><p>From the above discussion, we can get that the case of the exponential polynomial solutions of Equation (1.8) is as follows.</p><p>Case 1. If A + e A c ≠ 0 and c = − 1 e , then f ( z ) = e A z + B ( 1 A + e A c + ( a z + b ) e ( − e − A ) z + ∑ i = 1 m     b i e w i z ) , where a , b , b i ∈ ℂ , w i satisfy e − 1 e ( A + w i ) + A + w i = 0 . If A + e A c ≠ 0 and c ≠ − 1 e , then f ( z ) = e A z + B ( 1 A + e A c + ∑ i = 1 m     b i e w i z ) , where b i ∈ ℂ , w i satisfy e ( A + w i ) c + A + w i = 0 .</p><p>Case 2. If A + e A c = 0 , c = − 1 e and A c ≠ 1 (namely A ≠ − e ), then f ( z ) = e A z + B ( 1 1 + c e A c z + a 0 + ( a z + b ) e ( − e − A ) z + ∑ i = 1 m     b i e w i z ) , where a 0 , a , b , b i ∈ ℂ , w i satisfy e − 1 e ( A + w i ) + A + w i = 0 . If A + e A c = 0 , c ≠ − 1 e and A c ≠ 1 , then f ( z ) = e A z + B ( 1 1 + c e A c z + a 0 + ∑ i = 1 m     b i e w i z ) , where a 0 , b i ∈ ℂ , w i satisfy e ( A + w i ) c + A + w i = 0 .</p><p>Case 3. If A + e A c = 0 , c = − 1 e and A = − e (namely A c = 1 ), then f ( z ) = e A z + B ( 1 c 2 e A c z 2 + a 0 + a 1 z + ∑ i = 1 m     b i e w i z ) , where a 0 , a 1 , b i ∈ ℂ , w i satisfy e − 1 e ( − e + w i ) − e + w i = 0 .</p><p>Thus, we complete the proof of Theorem 1.2.</p><p>Proof of Theorem 1.3</p><p>Assume that f ( z ) is a transcendental entire solution of (1.9), we rewrite (1.9) as follows</p><p>( e − A z + B 2 f ′ ( z ) ) 2 + ( e − A z + B 2 f ( z + c ) ) 2 = 1 , (3.23)</p><p>then</p><p>( e − A z + B 2 f ′ ( z ) + i e − A z + B 2 f ( z + c ) ) ( e − A z + B 2 f ′ ( z ) − i e − A z + B 2 f ( z + c ) ) = 1.</p><p>It then follows that e − A z + B 2 f ′ ( z ) + i e − A z + B 2 f ( z + c ) , e − A z + B 2 f ′ ( z ) − i e − A z + B 2 f ( z + c ) have no zeros. With Welerstrass factorization theorem for entire functions, we have</p><p>( e − A z + B 2 f ′ ( z ) + i e − A z + B 2 f ( z + c ) = e h ( z ) , e − A z + B 2 f ′ ( z ) − i e − A z + B 2 f ( z + c ) = e − h ( z ) , (3.24)</p><p>where h ( z ) is a entire function. From (3.24), we get</p><p>( f ′ ( z ) = e h ( z ) + e − h ( z ) 2 e A z + B 2 , f ( z + c ) = e h ( z ) − e − h ( z ) 2 i e A z + B 2 . (3.25)</p><p>From (3.25), on the one hand, we obtain f ( z ) = e h ( z − c ) − e − h ( z − c ) 2 i e A c 2 e A z + B 2 , on the other hand, we have</p><p>i ( e h ( z + c ) + e − h ( z + c ) ) e A c 2 = ( h ′ ( z ) + A 2 ) e h ( z ) + ( h ′ ( z ) − A 2 ) e − h ( z ) . (3.26)</p><p>Next we divide our discussion into two cases.</p><p>Case 1. If h ( z ) is a constant, then</p><p>i ( e h ( z ) + e − h ( z ) ) e A c 2 = A 2 e h ( z ) − A 2 e − h ( z ) ,</p><p>from the above identity, we can deduce that h ( z ) = 1 2 ( ln A 2 + i e A c 2 A 2 − i e A c 2 + 2 k π i ) .</p><p>Case 2. If h ( z ) is a non-constant entire function, then from (3.26), we get</p><p>− e 2 h ( z + c ) + h ′ ( z ) + A 2 i e A c 2 e h ( z + c ) + h ( z ) + h ′ ( z ) − A 2 i e A c 2 e h ( z + c ) − h ( z ) = 1. (3.27)</p><p>Denote</p><p>f 1 = − e 2 h ( z + c ) ,   f 2 = h ′ ( z ) + A 2 i e A c 2 e h ( z + c ) + h ( z )   , f 3 = h ′ ( z ) − A 2 i e A c 2 e h ( z + c ) − h ( z ) .</p><p>Obviously, f 1 is a nonconstant and by Lemma 2.4 and 2.9, we can obtain that T ( r , h ′ ( z ) ) = o ( T ( r , e 2 h ( z + c ) ) ) . Thus, we obtain</p><p>∑ j = 1 3     N ( r , 1 f j ) + 2 ∑ j = 2 3     N &#175; ( r , f j ) = o ( T ( r , e 2 h ( z + c ) ) ) . (3.28)</p><p>Combining (3.28) and Lemma 2.2, we get f 2 ( z ) ≡ 1 or f 3 ( z ) ≡ 1 .</p><p>Now two subcases will be considered in the following.</p><p>Subcase 2.1. If f 2 ( z ) ≡ 1 , then from (3.28), we have</p><p>e h ( z + c ) + h ( z ) = i e A c 2 h ′ ( z ) + A 2 = h ′ ( z ) − A 2 i e A c 2 .</p><p>Further, we get</p><p>− e A c = ( h ′ ( z ) ) 2 − A 2 4 ,</p><p>which implies that h ( z ) must be a polynomial and deg ( h ) = 1 . Note that e h ( z + c ) + h ( z ) is a transcendental entire function and h ′ ( z ) − A 2 i e A c 2 is a constant, which is a contradiction.</p><p>Subcase 2.2. If f 3 ( z ) ≡ 1 , then from (3.28), we have</p><p>e h ( z + c ) − h ( z ) = i e A c 2 h ′ ( z ) − A 2 = h ′ ( z ) + A 2 i e A c 2 .</p><p>From the above identity, we can get that</p><p>− e A c = ( h ′ ( z ) ) 2 − A 2 4 , (3.29)</p><p>which implies that h ( z ) must be a polynomial and deg ( h ) = 1 . Assume that h ( z ) = a z + b , from (3.29), we have a 2 = A 2 4 − e A c and c = ln a − A 2 i + 2 k π i A 2 − a .</p><p>This completes the proof of Theorem 1.3.</p><p>Proof of Theorem 1.4</p><p>Now we divide our discussion into two cases.</p><p>Case 1. Assume that f ( z ) is a nonconstant entire solutions of (1.10), we rewrite (1.10) as follows</p><p>( e − A z + B n f ′ ( z ) ) n + ( e − A z + B n f ( z + c ) ) n = 1. (3.30)</p><p>Denote F = e − A z + B n f ′ ( z ) , G = e − A z + B n f ( z + c ) , from the references [ [<xref ref-type="bibr" rid="scirp.120219-ref5">5</xref>], Theorem3], we get the equation F 2 + G 2 = 1 has no nonconstant entire function solution when n &gt; 2 . Thus, Equation (3.30) has no nontrivial entire function solution when n &gt; 2 .</p><p>Case 2. Assume that f ( z ) is a meromorphic solutions with at least one pole of (1.10), we rewrite (1.10) as follows</p><p>f ′ ( z − c ) n = e A z + B − f ( z ) n . (3.31)</p><p>Suppose that z 0 is p multiplicity pole of f ( z ) . From (3.31), we get z 0 − c is p multiplicity pole of f ′ ( z ) , which implies that z 0 − c is p − 1 multiplicity pole of f ( z ) . Thus we get z 0 − 2 c is p − 1 multiplicity pole of f ′ ( z ) , which implies that z 0 − 2 c is p − 2 multiplicity pole of f ( z ) . Sequential recurrence, we can get that z 0 − p c is 1 multiplicity pole of f ′ ( z ) , this contradiction with f ( z ) is a meromorphic function with at least one pole.</p><p>This completes the proof of Theorem 1.4.</p><p>Proof of Theorem 1.5</p><p>Assume that f ( z ) is a meromorphic solutions of (1.7), we rewrite (1.7) as follows</p><p>e − A z − B f ′ ( z ) n + e − A z − B f ( z + c ) m = 1. (3.32)</p><p>Next we discuss the following two cases.</p><p>Case 1. If ρ ( f ( z ) ) &gt; 1 , then by lemma 2.8 and lemma 2.9, we can obtain that ρ ( f ( z ) ) = ρ ( f ′ ( z ) ) = ρ ( f ( z + c ) ) &gt; 1 . This means that T ( r , e − A z − B ) = o ( T ( r , f ′ ( z ) ) ) and T ( r , e − A z − B ) = o ( T ( r , f ( z + c ) ) ) . This, combining with lemma 2.5, we can get that the Equation (3.32) has no nontrivial meromorphic solutions when 1 m + 1 n &lt; 2 3 .</p><p>Case 2. If ρ ( f ( z ) ) &lt; 1 , then by lemma 2.8 and lemma 2.9, we get ρ ( f ( z ) ) = ρ ( f ′ ( z ) ) = ρ ( f ( z + c ) ) &lt; 1 . This means that T ( r , f ′ ( z ) ) = T ( r , f ( z + c ) ) = O ( T ( r , f ( z ) ) ) = o ( r ) . Now, comparing the characteristic functions of both side of (1.7), by lemma 2.3, we have T ( r , f ′ ( z ) n + f ( z + c ) m ) = o ( r ) , and we know that T ( r , e A z + B ) = O ( r ) , which is a contradiction. Thus Equation (1.7) has no nontrivial meromorphic solutions with ρ ( f ) &lt; 1 .</p><p>This completes the proof of Theorem 1.5.</p></sec><sec id="s4"><title>Funding</title><p>This work is supported by the National Natural Science Foundation of China (Grant No. 11801291) and the Natural Science Foundation of Fujian Province, China (Grant Nos. 2020R0039; 2019J05047; 2019J01672).</p></sec><sec id="s5"><title>Conflicts of Interest</title><p>The authors declare no conflicts of interest regarding the publication of this paper.</p></sec><sec id="s6"><title>Cite this paper</title><p>Liu, D.F. and Pan, B. (2022) On the Meromorphic Solutions of Fermat-Type Differential Equations. Journal of Applied Mathematics and Physics, 10, 2820-2836. https://doi.org/10.4236/jamp.2022.109188</p></sec><sec id="s7"><title>NOTES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.120219-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Hayman, W.K. (1964) Meromorphic Functions. Clarendon Press, Oxford.</mixed-citation></ref><ref id="scirp.120219-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Yi, H.X. and Yang, C.C. (2003) Uniqueness Theory of Meromorphic Functions. Kluwer Academic Publishers, Dordrecht.</mixed-citation></ref><ref id="scirp.120219-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">Chen, Z.X. (2014) Complex Differences and Difference Equations. Science Press, Beijing. https://doi.org/10.1155/2014/124843</mixed-citation></ref><ref id="scirp.120219-ref4"><label>4</label><mixed-citation publication-type="other" xlink:type="simple">Laine, I. (1993) Nevanlinna Theory and Complex Differential Equations. Walter de Gruyte, Berlin. https://doi.org/10.1515/9783110863147</mixed-citation></ref><ref id="scirp.120219-ref5"><label>5</label><mixed-citation publication-type="other" xlink:type="simple">Montel, P. (1927) Lecons sur les familles normales de fonctions analytiques et leurs applications. Gauthier Villars, Paris, 135-136.</mixed-citation></ref><ref id="scirp.120219-ref6"><label>6</label><mixed-citation publication-type="other" xlink:type="simple">Gross, F. (1966) On the Equation f&lt;sup&gt;n&lt;/sup&gt; + g&lt;sup&gt;n&lt;/sup&gt; = 1. I. Bulletin of the American Mathematical Society, 72, 86-88. https://doi.org/10.1090/S0002-9904-1966-11429-5</mixed-citation></ref><ref id="scirp.120219-ref7"><label>7</label><mixed-citation publication-type="other" xlink:type="simple">Gross, F. (1968) On the Equation f&lt;sup&gt;n&lt;/sup&gt; + g&lt;sup&gt;n&lt;/sup&gt; = 1. II. Bulletin of the American Mathematical Society, 74, 647-648. https://doi.org/10.1090/S0002-9904-1968-11975-5</mixed-citation></ref><ref id="scirp.120219-ref8"><label>8</label><mixed-citation publication-type="other" xlink:type="simple">Baker, I.N. (1966) On a Class of Meromorphic Functions. Proceedings of the American Mathematical Society, 17, 819-822. https://doi.org/10.1090/S0002-9939-1966-0197732-X</mixed-citation></ref><ref id="scirp.120219-ref9"><label>9</label><mixed-citation publication-type="other" xlink:type="simple">Yang, C.C. (1970) A Generalization of a Theorem of P. Montel on Entire Functions. Proceedings of the American Mathematical Society, 26, 332-334. https://doi.org/10.1090/S0002-9939-1970-0264080-X</mixed-citation></ref><ref id="scirp.120219-ref10"><label>10</label><mixed-citation publication-type="other" xlink:type="simple">Hu, P.C., Li, P. and Yang, C.C. (2003) Unicity of Meromorphic Mappings. Springer, Berlin. https://doi.org/10.1007/978-1-4757-3775-2</mixed-citation></ref><ref id="scirp.120219-ref11"><label>11</label><mixed-citation publication-type="other" xlink:type="simple">Halburd, R.G. and Korhonen, R.J. (2006) Difference Analogue of the Lemma on the Logarithmic Derivative with Applications to Difference Equations. Journal of Mathematical Analysis and Applications, 314, 477-487. https://doi.org/10.1016/j.jmaa.2005.04.010</mixed-citation></ref><ref id="scirp.120219-ref12"><label>12</label><mixed-citation publication-type="other" xlink:type="simple">Chiang, Y.M. and Feng, S.J. (2008) On the Nevanlinna Characteristic of f(z + &amp;#951;) and Difference Equations in the Complex Plane. The Ramanujan Journal, 16, 105-129. https://doi.org/10.1007/s11139-007-9101-1</mixed-citation></ref><ref id="scirp.120219-ref13"><label>13</label><mixed-citation publication-type="other" xlink:type="simple">Liu, K., Cao, T.B. and Cao, H.Z. (2012) Entire Solutions of Fermat Type Differential-Difference Equations. Archiv der Mathematik, 99, 147-155. https://doi.org/10.1007/s00013-012-0408-9</mixed-citation></ref><ref id="scirp.120219-ref14"><label>14</label><mixed-citation publication-type="other" xlink:type="simple">Liu, K., Yang, L.Z. and Liu, X.L. (2011) Existence of Entire Solutions of Nonlinear Difference Equations. Czechoslovak Mathematical Journal, 61, 565-576. https://doi.org/10.1007/s10587-011-0075-1</mixed-citation></ref><ref id="scirp.120219-ref15"><label>15</label><mixed-citation publication-type="other" xlink:type="simple">Liu, K., Yang, L.Z. and Liu, X.L. (2013) On Entire Solutions of Some Differential-Difference Equations. Computational Methods and Function Theory, 13, 433-447. https://doi.org/10.1007/s40315-013-0030-2</mixed-citation></ref><ref id="scirp.120219-ref16"><label>16</label><mixed-citation publication-type="other" xlink:type="simple">Lü, F. and Han, Q. (2017) On the Fermat-Type Equation f&lt;sup&gt;3&lt;/sup&gt;(z) + f&lt;sup&gt;3&lt;/sup&gt;(z + c) = 1. Aequationes Mathematicae, 91, 129-136. https://doi.org/10.1007/s00010-016-0443-x</mixed-citation></ref><ref id="scirp.120219-ref17"><label>17</label><mixed-citation publication-type="other" xlink:type="simple">Lü, F. and Han, Q. (2019) On the Equation f&lt;sup&gt;n&lt;/sup&gt;(z) + g&lt;sup&gt;n&lt;/sup&gt;(z) = e&lt;sup&gt;Az+B&lt;/sup&gt;. Journal of Contemporary Mathematical Analysis, 54, 98-102. https://doi.org/10.3103/S1068362319020067</mixed-citation></ref><ref id="scirp.120219-ref18"><label>18</label><mixed-citation publication-type="other" xlink:type="simple">Xu, H.Y., Liu, S. and Wang, H. (2021) Entire Solutions for Several Second-Order Partial Differential-Difference Equations of Fermat Type with Two Complex Variables. Advances in Difference Equations, 1, 1-24. https://doi.org/10.1186/s13662-020-03201-y</mixed-citation></ref><ref id="scirp.120219-ref19"><label>19</label><mixed-citation publication-type="other" xlink:type="simple">Steinmetz, N. (1978) Zur wertverteilung von exponentialpolynomen. Manuscripta Mathematica, 26, 155-167. https://doi.org/10.1007/BF01167971</mixed-citation></ref><ref id="scirp.120219-ref20"><label>20</label><mixed-citation publication-type="other" xlink:type="simple">Yang, L. (1993) Value Distribution Theory. Springer-Verlag, Berlin.</mixed-citation></ref><ref id="scirp.120219-ref21"><label>21</label><mixed-citation publication-type="other" xlink:type="simple">Goldberg, A.A. and Ostrovskii, I.V. (2008) Value Distribution of Meromorphic Functions. American Mathematical Society, Providence.</mixed-citation></ref></ref-list></back></article>