1 Introduction and main result
We denote by
$T(r,f)$
the Nevanlinna characteristic of a meromorphic function f. The notation
$S(r,f)$
denotes any quantity satisfying
as
$r\to \infty $
outside a possible exceptional set of finite logarithmic measure. The hyper-order of f is defined by
For all other standard notation from Nevanlinna theory, we refer to [Reference Hayman4].
Following Laine and Latreuch [Reference Laine and Latreuch5], let
$\mathcal A$
denote the class of transcendental meromorphic functions h for which
Laine and Latreuch proved in [Reference Laine and Latreuch5, Theorem 2.2] that a meromorphic solution f satisfying
$\rho _2(f)<1$
of the equation
satisfies one of the following two alternatives:
or
The authors observed that the construction of a concrete example realising alternative (II) remained open [Reference Laine and Latreuch5, Remark 2.3(c)]. Our main result shows that no such example exists.
Theorem 1.1 (Complete classification).
Let
$c\in \mathbb C\setminus \{0\}$
, let
$h\in \mathcal A$
and let f be a meromorphic solution of equation (1.1) satisfying
$\rho _2(f)<1$
. Then, there exist
$a,b\in \mathbb C$
such that
Conversely, the functions given by (1.2) satisfy (1.1); moreover,
$h\in \mathcal A$
and
$\rho _2(f)<1$
.
Corollary 1.2 (Answer to the question of Laine and Latreuch).
Under the hypotheses of [Reference Laine and Latreuch5, Theorem 2.2], alternative (II) cannot occur for any meromorphic solution. Consequently, the question posed in [Reference Laine and Latreuch5, Remark 2.3(c)] has a negative answer.
The hyper-order restriction in Theorem 1.1 is sharp. Remark 2.2 below provides a solution of hyper-order
$1$
, which is not of the form (1.2).
2 Proof of the main result
We shall need the following elementary quadratic case of the Tumura–Clunie argument; for the general form of this argument, see [Reference Hayman4, Section 3.5, page 69].
Lemma 2.1 (Quadratic reduction).
Let x be a transcendental meromorphic function such that
$ N(r,x)=S(r,x), $
and let A and B be meromorphic functions that are small with respect to x, that is,
$ T(r,A)+T(r,B)=S(r,x). $
Set
$ H=x^2+Ax+B. $
If
$ N(r,{1}/{H})=S(r,x), $
then
Proof. Set
$ g=x+{A}/{2}, \, a=B-{A^2}/{4}. $
Then,
$ H=g^2+a. $
Since A and B are small functions with respect to x,
Moreover,
Suppose that
$a\not \equiv 0$
and consider the meromorphic function
$ F={g^2}/{a}. $
It follows from the standard properties of the Nevanlinna characteristic that
However,
Hence,
$ T(r,F)=2T(r,g)+S(r,g) $
and, in particular, F is nonconstant.
The poles and zeros of F satisfy the estimates
and
Since
$ F+1={(g^2+a)}/{a}={H}/{a}, $
the hypothesis of the lemma gives
Applying Nevanlinna’s second main theorem to F and the three values
$0$
,
$-1$
and
$\infty $
, we obtain
Together with the identity
$ T(r,F)=2T(r,g)+S(r,g), $
this yields
which is impossible since g is a transcendental meromorphic function.
Hence,
$a\equiv 0$
, that is,
$ B={A^2}/{4}. $
Therefore,
Proof of Theorem 1.1.
We divide the proof into four steps. First, we obtain an affine representation of the shift
$f(z+c)$
with small coefficients and then reduce h to a perfect square. Next, we prove that the corresponding small function s is identically equal to
$1$
, after which we rule out alternative (II) and complete the classification.
Step 1. An affine relation for the shift. By [Reference Laine and Latreuch5, Theorem 2.2], it suffices to rule out alternative (II). Suppose that this alternative holds.
Set
Since
$h\in \mathcal A$
, [Reference Laine and Latreuch5, Lemma 2.1] implies that f is a transcendental meromorphic function and
Since
$h\in \mathcal A$
, the classical lemma on the logarithmic derivative [Reference Hayman4, Lemma 2.3] gives
Moreover, the difference analogue of Clunie’s lemma used in [Reference Laine and Latreuch5, Proof of Theorem 2.2] gives
$ T(r,\phi )=S(r,f). $
For any meromorphic function u, we write
$ u_c(z):=u(z+c). $
The estimate for the characteristic of a shifted function [Reference Chiang and Feng1, (1.2)], together with [Reference Halburd, Korhonen and Tohge3, Lemma 8.3], shows that, for
$\rho _2(F)<1$
,
and that
$T(r,v)=S(r,F)$
implies
$ T(r,v_c)=S(r,F). $
In particular,
We next show that
$\phi \not \equiv 0$
. If
$\phi \equiv 0$
, then
$ ({f^2}/{h})'=0, $
and hence,
$f^2=A_0h$
for some constant
$A_0\ne 0$
. Differentiating (1.1) and using
$2f'=\alpha f$
, we obtain
$f_c'=\alpha f_c$
, whence
$f_c=B_0h$
for some constant
$B_0\ne 0$
. Therefore,
which is impossible. Thus,
$\phi \not \equiv 0$
.
Differentiating (1.1) and using
$h'=\alpha h$
, we obtain from the definition of
$\phi $
that
Since
$ \phi _c=2f_c'-\alpha _c f_c, $
eliminating
$f_c'$
from this identity and (2.1) gives
Set
$ d:=\alpha _c-2\alpha. $
If
$d\equiv 0$
, then (2.2) would imply
$ f=-{\phi _c}/{2\phi }, $
and hence,
which is impossible. Therefore,
$d\not \equiv 0$
and
Since
we obtain
Step 2. Quadratic reduction. Substituting (2.3) into (1.1), we obtain
We have already established that f is a transcendental meromorphic function and that
$ N(r,f)=S(r,f), $
while the smallness of L and M follows from (2.4). Moreover,
$h\in \mathcal A$
and
$T(r,h)\asymp T(r,f)$
imply that
Therefore, Lemma 2.1 can be applied to (2.5) with
It yields
$M=L^2/4$
and
Moreover,
Step 3. Rigidity of the auxiliary function. It follows from (2.7) and [Reference Gundersen2, Lemma 5] that, for every
$\lambda>1$
,
for all sufficiently large r. Therefore, if s is nonconstant, then
Set
$ U:=f+s. $
From (1.1) and (2.6), we have
$ f_c=2sf+s^2. $
Hence,
Since
$T(r,s)=S(r,f)$
,
Therefore, U is a transcendental meromorphic function,
$\rho _2(U)<1$
and
$S(r,f)=S(r,U)$
. Moreover,
$h=U^2$
and
$h\in \mathcal A$
imply that
Applying the shift estimate established in Step 1 with
$F=U$
and
$v=s$
, we obtain
$T(r,s_c)=S(r,U)$
. Hence,
Choose
$\eta \in (0,1-\rho _2(U))$
. The difference analogue of the lemma on the logarithmic derivative [Reference Halburd, Korhonen and Tohge3, (5.3)] gives
However, by (2.8), (2.9) and (2.10),
Consequently,
Dividing (2.8) by U, and using (2.10) and (2.11), we obtain
If
$t\not \equiv 0$
, then
$ 1/U=(t/U)(1/t) $
would imply that
which is impossible. Hence,
$t\equiv 0$
and
We now show that s is constant. Suppose the contrary. Choose
$\varepsilon \in (0,1)$
and set
$ q:={2}/{(1+\varepsilon )}>1. $
By the first equation in (2.12) and the estimate for the characteristic of a shifted function [Reference Chiang and Feng1, (1.2)], we have, for all sufficiently large r,
Consequently,
for all sufficiently large r. Choose
$r_0$
sufficiently large so that the preceding inequality holds for all
$r\geq r_0$
and
$T(r_0,s)>0$
. Iterating this inequality gives
Hence,
which contradicts the previously established inequality
$\rho _2(s)<1$
. Thus, s is constant.
The first equation in (2.12) now gives
$s=s^2$
and, hence,
$s\in \{0,1\}$
. The case
$s=0$
is impossible: the second equation would then imply
$U_c\equiv 0$
and, consequently,
$U\equiv 0$
and
$h=U^2\equiv 0$
, contrary to
$h\in \mathcal A$
. Therefore,
$s=1$
and
Step 4. Exclusion of the second alternative. We now have
$U=f+1$
. Set
$ W:={U'}/{U}. $
Since U is a transcendental meromorphic function,
$W\not \equiv 0$
. By the classical lemma on the logarithmic derivative [Reference Hayman4, Lemma 2.3],
$ m(r,W)=S(r,U). $
Every pole of W is a zero or a pole of U and, hence, by (2.9),
Therefore,
Since
$f'=U'=UW$
,
This contradicts (II), since it would imply that
Thus, alternative (II) is impossible.
By [Reference Laine and Latreuch5, Theorem 2.2(1)], alternative (I) must hold; that is,
$ f(z)=e^{az+b}-1, \, e^{ac}=2 $
for some
$a,b\in \mathbb C$
. Then,
and hence,
$ h(z)=e^{2az+2b}. $
Conversely, for any
$a,b\in \mathbb C$
satisfying
$e^{ac}=2$
, the preceding calculation shows that the functions
$ f(z)=e^{az+b}-1, \, h(z)=e^{2az+2b}, $
satisfy (1.1). In this case,
$a\ne 0$
, so h is a zero-free transcendental entire function and
Therefore,
$h\in \mathcal A$
. Moreover, f has finite order and, hence,
$ \rho _2(f)=0<1. $
Remark 2.2 (Sharpness of the hyper-order restriction).
Choose
$a\in \mathbb C$
such that
${e^{ac} =2}$
, and set
Since
we have
Therefore,
The function h is a zero-free transcendental entire function. Hence,
and, therefore,
$h\in \mathcal A$
.
The function g is a transcendental entire function of order one. By [Reference Yang and Yi6, Theorem 1.45], every nonconstant entire function g satisfies
Since
$U=e^g$
, it follows that
Since
$f=U-1$
, we have
$ T(r,f)=T(r,U)+O(1), $
and hence,
$ \rho _2(f)=1. $
Moreover,
is nonconstant. Therefore, f cannot be of the form
$e^{\alpha z+\beta }-1$
. Thus, the condition
$\rho _2(f)<1$
in Theorem 1.1 cannot be replaced by
$\rho _2(f)\leq 1$
.






