Startseite Singular direction of meromorphic functions with finite logarithmic order
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Singular direction of meromorphic functions with finite logarithmic order

  • Keqi Hu und Qingcai Zhang EMAIL logo
Veröffentlicht/Copyright: 29. Mai 2025

Abstract

In this article, we construct filling disks for meromorphic functions of order zero and that way we prove the existence of Borel directions of these functions. In the latter part of this article, we demonstrate the existence of filling disks using the Borel direction of meromorphic functions.

MSC 2010: 30D30; 30D35

1 Introduction

We assume the reader is familiar with the basic notion of Nevanlinna’s value distribution theory such as T ( r , f ) , m ( r , f ) , N ( r , f ) , n ( r , f ) , and so on, which can be found, for instance, in [14]. The theory of finite positive-order meromorphic functions is well known to be more affluent than the theory of zero-order meromorphic functions. Techniques that work well for functions of finite positive-order often do not work for functions of zero order.

There are many results on the Borel direction of meromorphic functions [4]. At the end of the nineteenth century, Picard and Borel obtained Picard’s theorem and Borel’s theorem, respectively. In studying the behavior of an entire or meromorphic function near a ray, Milloux [5] introduced the concept of filling disks.

In 1928, Valiron [6] obtained the Borel direction for meromorphic functions of finite positive order based on Nevanlinna’s theory.

Rauch [7] proved in 1933 that a sequence of filling disks can be obtained from the Borel direction of meromorphic functions. Shortly after this, Hiong [8] obtained the result about the Borel direction for meromorphic functions of infinite order.

In 1982, Yang [4] improved the proof of these theorems. The natural question is whether a sequence of filling disks exists for meromorphic functions of finite logarithmic order and whether a sequence of filling disks can be obtained from the Borel direction of the function. Results on the Borel direction of meromorphic function have also been studied by many scholars in recent decades [916].

Valiron [17] was the first to investigate the Borel direction for meromorphic functions of zero order. In 1995, Rossi [18] studied filling disks for meromorphic functions satisfying the growth condition (1.1). In order to facilitate the study of meromorphic functions of zero order, Chern [19,20] obtained some results on meromorphic functions of zero order using the concept of logarithmic order

ρ = lim r ¯ log T ( r , f ) log log r .

In 2004, he used the Ahlfors theory to obtain the existence of the Borel direction for meromorphic functions of zero order.

Theorem A

[21] Let f ( z ) be a meromorphic function in the complex plane C with finite logarithmic order ρ , if f ( z ) satisfies the growth condition

(1.1) lim r ¯ T ( r , f ) ( log r ) 2 = ,

then there exists a direction arg z = θ 0 ( 0 θ 0 < 2 π ) , such that for every small positive number ε and every a C ˆ , the equation

lim r ¯ log n ( r , θ 0 , ε , f = a ) log log r = ρ 1

holds with at most two possible exceptional values of a, where n ( r , θ 0 , ε , f = a ) denotes the number of zeros of f ( z ) a in the angular region { z : arg z θ 0 ε , z < r } .

The ray arg z = θ 0 in Theorem A is called a Borel direction of finite logarithmic order ρ 1 for f ( z ) . It is natural to wonder if we can determine the existence of Borel directions for meromorphic functions of zero order by constructing the filling disks.

In 2004, Wang [22] obtained the following results by way of constructing the filling disks.

Theorem B

[22] Let f ( z ) be a meromorphic function in the complex plane C with finite logarithmic order ρ , then there exists a direction arg z = θ 0 ( 0 θ 0 < 2 π ) , such that for every small positive number ε and every a C ˆ , the equation

lim r ¯ log n ( r , θ 0 , ε , f = a ) log log r ρ 2

holds with at most two possible exceptional values of a.

However, we found that his result is inaccurate compared to Chern’s. Next, we construct a sequence of filling disks using the method of Yang [4] to obtain the following two theorems.

Theorem 1.1

Let f ( z ) be a meromorphic function in the complex plane C with finite logarithmic order, that for every sufficiently large R and k > 1 , satisfies the following inequality in the annulus r < z < R :

(1.2) T ( R , f ) max 240 , 240 log R r log k , 12 T ( r , f ) , 12 T ( k r , f ) log k log R r .

Then, there must exist a point z j in the annulus r < z < R such that f ( z ) takes every complex number at least n = C T ( R , f ) q 2 log q log R r log log R r times in z z j < 4 π log q 1 z j , where C is a constant and q is sufficiently large positive integer, except possibly for those numbers contained in two spherical disks each with radius e n .

Theorem 1.2

Let f ( z ) be a meromorphic function in the complex plane C with finite logarithmic order ρ . If f ( z ) satisfies the growth condition (1.1), then there exists a sequence of disks

Γ j : z z j < ε j z j , lim j ε j = 0 , lim j z j = ( j = 1 , 2 , ) ,

such that f ( z ) takes every complex number at least ( log z j ) ρ 1 δ j times in Γ j , where lim j δ j = 0 , except possibly for those numbers contained in two spherical disks each with radius e ( log z j ) ρ 1 δ j .

Theorem A can be obtained by using the method of Yang in Theorem 3.8 of [4] from the aforementioned two theorems. This means that we obtain another proof for Theorem A. Conversely, given the Borel direction of the function, can we derive a sequence of filling disks? The answer is given in Theorem 1.5.

Theorem 1.3

Let f ( z ) be a meromorphic function in the angular domain arg z θ 0 < η , and there are three distinct values a ν ( ν = 1, 2, 3) and a positive number σ , such that

(1.3) j ( log r j ( θ 0 , η , f = a ν ) ) σ

converges, where ν = 1, 2, 3, and r j ( θ 0 , η , f = a ν ) ( j = 1 , 2 , ) denote the moduli of the zeros of f ( z ) a ν in the domain { z : arg z θ 0 < η , z > 1 } , arranged by nondecreasing order and counted with their multiplicities. Then, j ( log r j ( θ 0 , η ε , f = a ) ) σ is convergent, for any positive number ε < η and all a C ˆ , possibly except at most for a set whose line measure is zero.

Theorem 1.4

Let f ( z ) be a meromorphic function in the complex plane C with finite logarithmic order λ + 1 , if f ( z ) has no Borel direction of finite logarithmic order λ in the angular domain θ 1 < arg z < θ 2 , then for any small positive number α , there exist three distinct values a ν ( ν = 1, 2, 3) and a positive number τ ( < λ ) , such that

ν = 1 3 n ( r , θ 1 + α , θ 2 α , f = a ν ) < ( log r ) τ ,

where n ( r , θ 1 + α , θ 2 α , f = a ν ) denotes the number of zeros of f ( z ) a in the domain { z : θ 1 + α arg z θ 2 α , 1 < z < r } .

Theorem 1.5

Let f ( z ) be a meromorphic function in the complex plane C with finite logarithmic order λ + 1 > 2 , if

B : arg z = θ 0 , 0 θ 0 < 2 π

is a Borel direction of finite logarithmic order λ for f ( z ) , then there exists a sequence of disks

Γ j : z z j < ε j z j , lim j ε j = 0 , lim j z j = ( j = 1 , 2 , )

such that f ( z ) takes every complex number at least ( log z j ) λ δ j times in Γ j , where lim j δ j = 0 , except possibly for those numbers contained in two spherical disks each with radius j 3 .

2 Some lemmas

The following lemmas will be needed in the sequel.

Lemma 2.1

[4] Assume that f ( z ) is a meromorphic function in the complex plane C , and D is a bounded region. Divide D into p subregions D j ( j = 1 , 2 , , p ) . For each D j , make a disk K j D j , and then make a concentric disk K j of K j , such that the radius is twice as large as K j . If the set of complex number a such that n ( D , f = a ) N cannot be covered by a collection of spherical disks with radius total equal to 1 2 on the Riemann sphere, then there must exist a circle K j with a constant C such that f ( z ) takes every complex number at least C N p times in K j , except possibly for those numbers contained in two spherical disks each with radius e C N p .

Lemma 2.2

[4] Assume that f ( z ) is a meromorphic function in the disk z < R , and let

N = n ( R , f = a 1 ) + n ( R , f = a 2 ) + n ( R , f = a 3 ) ,

where a 1 , a 2 , and a 3 are three distinct complex numbers, with their spherical distances larger than a positive number d. Then, there exists a point z 0 , with z 0 < R , such that for every r ( 0 , R ) , and any complex number a,

n ( r , f = a ) < C R 2 ( R r ) 2 × ( N + 1 ) log 2 R R r + log + 1 d + log 1 f ( z 0 ) , a ,

where C is a positive constant, and f ( z 0 ) , a denotes the spherical distance between f ( z 0 ) and a.

Lemma 2.3

[4] Let a μ ( μ = 1 , 2 , , n ) be n complex numbers and h a positive number. Then, the points that satisfy the inequality

μ = 1 n z , a μ h e n

can be covered by a collection of spherical disks whose number does not exceed n and the sum of whose radii does not exceed 2 h .

Lemma 2.4

Assume that f ( z ) is a meromorphic function in the complex plane C , and let r j ( j = 1 , 2 , ) be the moduli of the poles of f ( z ) in the domain { z : z > 1 } , with r j ( a ) r j + 1 ( a ) . For any r 0 > 1 , if σ > 0 , then the series ( log r j ) σ and r 0 n ( t , f ) ( log t ) σ + 1 t d t are either simultaneously convergent or simultaneously divergent.

Proof

For any R > r 0 with r 0 > 1 , let z j 0 , , z J be the poles of f within the annulus { z : r 0 < z < R } , and denote r j 0 = z j 0 , , r J = z J , arranged by nondecreasing order and counted with their multiplicities. It follows from the equation

(2.1) j = j 0 J 1 ( log r j ) σ = r 0 R 1 ( log t ) σ d n ( t , f ) = n ( t , f ) ( log t ) σ r 0 R + r 0 R σ n ( t , f ) ( log t ) σ + 1 t d t ,

if ( log r j ) σ converges, then r 0 n ( t , f ) ( log t ) σ + 1 t d t also converges.

Conversely, if the series r 0 n ( t , f ) ( log t ) σ + 1 t d t converges, combine

lim R n ( R , f ) σ ( log R ) σ = lim R n ( R , f ) R 1 ( log t ) σ + 1 t d t lim R R n ( t , f ) ( log t ) σ + 1 t d t = 0 .

with (2.1), ( log r j ) σ also converging.

So ( log r j ) σ and r 0 n ( t , f ) ( log t ) σ + 1 t d t are either simultaneously convergent or simultaneously divergent.□

Similarly, the following lemma can be obtained in the angular domain.

Lemma 2.5

Assume that f ( z ) is a meromorphic function in the complex plane C , 0 θ 0 < 2 π , η > 0 , a C . Let r j ( θ 0 , η , f = a ) be the moduli of the a-points of f ( z ) in the domain { z : arg z θ 0 < η , z > 1 } , with r j ( a ) r j + 1 ( a ) . For any r 0 > 1 , if σ > 0 , then the series ( log r j ( θ 0 , η , f = a ) ) σ and r 0 n ( t , θ 0 , η , f = a ) ( log t ) σ + 1 t d t are either simultaneously convergent or simultaneously divergent.

3 Proofs of Theorems 1.1 and 1.2

In this section, the proof method is based on the content of [4] (Section 3 in Chapter 3), but there are some differences in the details of constructing the filling disks. This construction method provides a different perspective for proving Theorem A.

Proof of Theorem 1.1

Assume that f ( z ) is a meromorphic function in the complex plane C , by the definitions of n ( r , f = a ) and N ( r , f = a ) , we have

(3.1) n ( R , f = a ) = n ( R , f = a ) log R r r R d t t N ( R , f = a ) N ( r , f = a ) log R r

and

(3.2) n ( r , f = a ) = n ( r , f = a ) log k r k r d t t 1 log k N ( k r , f = a ) .

From the second fundamental theorem of Nevanlinna, for suitably large R and every complex number a , we have

(3.3) N ( R , f = a ) > T ( R , f ) 4 , f ( 0 ) , a > 1 3 ,

except possibly for those numbers contained in a sequence of disks with total spherical radius 1 2 . Combining (1.2) with (3.3), we have

n ( R , f = a ) n ( r , f = a ) N ( R , f = a ) log R r N ( r , f = a ) log R r N ( k r , f = a ) log k 1 4 T ( R , f ) log R r T ( r , f = a ) log R r T ( k r , f = a ) log k 1 4 T ( R , f ) log R r T ( r , f ) + log 1 f ( 0 ) , a + log 2 log R r T ( k r , f ) + log 1 f ( 0 ) , a + log 2 log k T ( R , f ) 4 log R r 1 4 T ( r , f ) T ( R , f ) 4 log 6 T ( R , f ) 4 T ( k r , f ) T ( R , f ) log R r log k 4 log 6 T ( R , f ) log R r log k T ( R , f ) 15 log R r .

Taking a sufficiently large positive integer q , the annulus r < z < R is divided as follows:

Make q rays from the origin, the angle between two consecutive rays is 2 π q , and then make 1 + s [ log q ] circles

z = r , r + r ( e ( 1 + 2 π q ) 1 ) [ log q ] , r + 2 r ( e ( 1 + 2 π q ) 1 ) [ log q ] , , r e ( 1 + 2 π q ) , r e ( 1 + 2 π q ) + r ( e ( 1 + 2 π q ) 2 e ( 1 + 2 π q ) ) [ log q ] , , r e ( 1 + 2 π q ) 2 , r e ( 1 + 2 π q ) s 1 + r ( e ( 1 + 2 π q ) s e ( 1 + 2 π q ) s 1 ) [ log q ] , , , r e ( 1 + 2 π q ) s ,

where s = log log R r log ( 1 + 2 π q ) + 1 .

Thus, the annulus r < z < R is divided into p curved quadrilaterals D j , where

p q log log R r log 1 + 2 π q + 1 [ log q ] < q 2 log q log log R r 2 .

Let z j ( j = 1 , , p ) be the center of D j , then D j K j = { z : z z j < 2 π log q 1 z j } . The division of the annulus is shown in Figure 1.

By Lemma 2.1, then there must exist a concentric circle K j = { z : z z j < 4 π log q 1 z j } with a constant C , such that f ( z ) takes every complex number at least n = C T ( R , f ) q 2 log q log R r log log R r times in K j , except possibly for those numbers contained in two spherical disks each with radius e n .□

Figure 1 
               The division of the annulus.
Figure 1

The division of the annulus.

Proof of Theorem 1.2

Since f ( z ) is a meromorphic function with finite logarithmic order ρ and (1.1) holds, there exists a sequence { r k } that tends to infinity such that

lim k T ( r k , f ) ( log r k ) 2 = , lim k log T ( r k , f ) log log r k = ρ .

Taking a suitably large r k 1 , such that

T ( r k 1 , f ) max 240 , 240 log ( r k 1 ) log 2 , 12 T ( 1 , f ) , 12 T ( 2 , f ) log 2 log r k 1 ,

and

q 1 = log log r k 1 .

By Theorem 1.1, there exists a point z 1 in the annulus 1 < z < r k 1 such that f ( z ) takes every complex number at least n 1 = C T ( r k 1 , f ) log r k 1 ( log log r k 1 ) 3 log log log r k 1 times in Γ 1 : z z 1 < 4 π log log log r k 1 1 z 1 , except possibly for those numbers contained in two spherical disks each with radius e n 1 , where C is a constant.

Take r k 1 such that r k 1 > 2 r k 1 . Then, take r k 2 such that

T ( r k 2 , f ) max 240 , 240 log r k 2 log 2 , 12 T ( r k 1 , f ) , 12 T ( 2 r k 1 , f ) log 2 log r k 2 ,

and

q 2 = log log r k 2 .

By Theorem 1.1, there exists a point z 2 in the annulus r k 1 < z < r k 2 such that f ( z ) takes every complex number at least n 2 = C T ( r , f ) log r k 2 ( log log r k 2 ) 3 log log log r k 2 times in Γ 2 : z z 2 < 4 π log log log r k 2 1 z 2 , except possibly for those numbers contained in two spherical disks each with radius e n 2 , where C is a constant.

By induction, we can obtain a sequence of disks

Γ j : z z j < ε j z j , lim j ε j = 0 , lim j z j = ( j = 1 , 2 , )

such that f ( z ) takes every complex number at least

n j = C T ( r , f ) log r k j ( log log r k j ) 3 log log log r k j > ( log r k j ) ρ 1 δ j = ( log z k j ) ρ 1 δ j

times in Γ j , except possibly for those numbers contained in two spherical disks each with radius e ( log z j ) ρ 1 δ j , where C is a constant and lim j δ j = 0 .□

4 Proof of Theorems 1.3 and 1.5

In [4] (Section 4 in Chapter 3), the relevant results about finite-order meromorphic functions are given. Here, we use the identical method but the quadrangles we split are different.

Proof of Theorem 1.3

Split the angular domain arg z θ 0 < η ε with rays from the origin so that the angle of each small angular domain does not exceed ε 4 , the total number of these small angular domains is J 4 ( η ε ) ε 4 + 1 . Then, take a suitably large positive number r 0 > 1 , take the origin as the center, and make circles z = r 0 , r 0 exp { 1 + ε 4 } , r 0 exp { ( 1 + ε 4 ) 2 } , . such that ( z > r 0 ) ( arg z θ 0 < η ε ) is divided into some small curved quadrilateral Ω j l ( j = 1 , 2 , , J ; l = 1 , 2 , , L ). For each Ω j l , there exists a small disk Γ j l and a disk Γ j l of radius two times its radius, such that Ω j l Γ j l Γ j l ( arg z θ 0 < η ) . It is easy to see that for each Γ j 0 l 0 , there is a fixed upper bound for the number of other Γ j l intersecting it. At the same time, combining (1.3) with Lemma 2.5, we obtain

(4.1) r 0 n ( t , θ 0 , η , f = a ν ) ( log t ) σ + 1 t d t < ( ν = 1 , 2 , 3 ) .

By Lemmas 2.2 and 2.3, for any a C ˆ , the equation

(4.2) n ( Ω j l , f = a ) < C ν = 1 3 n ( Γ j l , f = a ν ) + log 1 exp σ 2 log r 0 + ( 1 + ε 4 ) l

holds in each Γ j l , except possibly for those numbers contained in the disk D j l with spherical radius exp σ 2 log r 0 + ( 1 + ε 4 ) l .

Let D l = j = 1 J D j l , D = k = 1 ( l = k D l ) , and we see that mes D = lim k mes ( l = k D l ) = 0 .

For any complex a D , there exists l 0 , such that a l = l 0 D l . So when l l 0 , (4.2) holds for j = 1 , 2 , , J .

Thus,

l = l 0 L j = 1 J n ( Ω j l , f = a ) < C l = l 0 L j = 1 J ν = 1 3 n ( Γ j l , f = a ν ) + J l = l 0 L σ 2 log r 0 + 1 + ε 4 l ,

which implies

n ( r , θ 0 , η ε , f = a ) < C ν = 1 3 n ( 2 r , θ 0 , η ε , f = a ν ) + log r .

By (4.1), for any complex a D , we have

r 0 n ( r , θ 0 , η ε , f = a ) ( log r ) σ + 1 r d r < .

Furthermore, by Lemma 2.5, the theorem is proved.□

Proof of Theorem 1.4

According to the conditions of the theorem, for any φ [ θ 1 + α , θ 2 α ] , arg z = φ is not a Borel direction of finite logarithmic order for f ( z ) . Nevertheless, there must exist three distinct values β j ( j = 1, 2, 3) and positive numbers ε ( φ ) , τ ( φ ) ( < λ ) , such that

n ( r , φ , ε ( φ ) , f = β j ) < ( log r ) τ ( φ ) ( j = 1 , 2 , 3 ) .

It follows that, for τ 1 ( φ ) ( τ ( φ ) < τ 1 ( φ ) < λ ) and r 0 > 1 , we have

r 0 n ( t , φ , ε ( φ ) , f = β j ) ( log t ) τ 1 ( φ ) + 1 t d t < ( j = 1 , 2 , 3 ) .

By Lemma 2.5, the series ( log r ( φ , ε ( φ ) , f = β j ) ) τ 1 ( φ ) is convergent. As a result of applying Theorem 1.3, for any complex number a , the series ( log r ( φ , ε ( φ ) 2 , f = a ) ) τ 1 ( φ ) is convergent possibly except for at most a set D ( φ ) whose line measure is zero.

We note that { ( φ ε ( φ ) 2 , φ + ε ( φ ) 2 ) : θ 1 + α φ θ 2 α } forms an open covering of the closed interval [ θ 1 + α , θ 2 α ] . Therefore, there exists a finite set of intervals ( φ l ε l 2 , φ l + ε l 2 ) ( l = 1 , 2 , , L ) that are an open covering of [ θ 1 + α , θ 2 α ] .

Corresponding to each φ l , its exceptional zero measure set is D l = D ( φ l ) . Let D = l = 1 L D l , then it is still the zero measure set. If τ 1 = max 1 l L { τ 1 ( φ l ) } , then 0 < τ 1 < λ .

Hence, for every complex number a ( D ) , we obtain

log r j φ l , ε l 2 , f = a τ 1 < .

So

log r j θ 1 + θ 2 2 , θ 2 θ 1 2 α , f = a τ 1 < .

By Lemma 2.5, we obtain

r 0 n ( t , θ 1 + α , θ 2 α , f = a ) ( log t ) τ 1 + 1 t d t < .

In particular, this holds for any three distinct complex numbers a ν ( ν = 1, 2, 3) that do not belong to D , and positive numbers τ ( τ 1 < τ < λ ) . Hence, we obtain

ν = 1 3 n ( r , θ 1 + α , θ 2 α , f = a ν ) < ( log r ) τ .

Proof of Theorem 1.5

Choose a small angular region with B as its bisector, which is defined by

Ω z : arg z θ 0 < η 2 .

Using the arcs of circumferences z = 2 j ( j = 1 , 2 , ) , divide Ω into a sequence of small quadrangles

Ω j z : ( 2 j z 2 j + 1 ) arg z θ 0 < η 2 .

Subsequently, each Ω j is further divided by s 1 arcs of z = 2 j ( 1 + η ) l , ( l = 1 , 2 , , s 1 ) , where s is a positive integer determined by 2 j ( 1 + η ) s 1 < 2 j + 1 2 j ( 1 + η ) s . This results in s smaller quadrangles, denoted as Ω j l ( l = 1 , 2 , , s ) . Choose concentric disks Γ j l and Γ j l with radius C 2 j + 1 η and 2 C 2 j + 1 η , respectively, such that

Ω j l Γ j l Γ j l .

Define n j l as follows:

n j l min v = 1 3 n ( Γ j l , f = a v ) ,

where the minimum is taken over all the triples of complex numbers, provided that the mutual spherical distances among these three complex numbers are at least j 3 . By Lemma 2.2, f ( z ) takes every complex number a at most C { n j l + [ log j ] + 1 } times in Ω j l , except for those complex numbers contained in a disk with spherical radius j 3 .

For each fixed value of j , there exist s exceptional spherical disks. As j varies, the aggregate radius of these exceptional spherical disks is given by the series:

j = 1 s j 3 .

By selecting a sufficiently large value for j 0 , we can ensure that

j = j 0 s j 3 < 1 2 .

Since B is a Borel direction of logarithmic order λ of f ( z ) , by Lemma 2.5, the series

log r n θ 0 , η 2 , f = a τ

diverges for any positive number τ < λ and every complex value a , except for at most two values. If a is not an exceptional value and does not belong to all the exceptional spherical disks, then we have

(4.3) log r n θ 0 , η 2 , f = a τ = .

On the other hand, by setting n j = max 1 l s n j l , we have

(4.4) log r n θ 0 , η 2 , f = a τ < C j s ( n j + [ log j ] + 1 ) ( log 2 j ) τ < C j n j η ( log 2 j ) τ + j [ log j ] + 1 η ( log 2 j ) τ ,

where τ < λ .

Choose a decreasing sequence { η l } of positive numbers tending to zero and an increasing sequence of positive numbers { τ l } tending to λ . Let τ 1 > 1 , then j [ log j ] + 1 η 1 ( log 2 j ) τ 1 < . Combining (4.3) with (4.4), we have j n j η 1 ( log 2 j ) τ 1 = . Thus, there is a positive integer j 1 such that

n j 1 > η 1 ( log 2 j 1 + 1 ) τ 1 j 1 ( log j 1 ) 2 > ( log 2 j 1 + 1 ) 2 τ 1 λ .

Similarly, from j = j 1 + 1 [ log j ] + 1 η 2 ( log 2 j ) τ 2 < , we have j = j 1 + 1 n j η 2 ( log 2 j ) τ 2 = . Hence, n j 2 > ( log 2 j 2 + 1 ) 2 τ 2 λ for a certain positive integer j 2 .

Thus, we obtain a sequence of disks Γ l : z z l < C η l z l , where arg z l = θ 0 , such that f ( z ) takes every complex value at least ( log z l ) λ 2 ( λ τ l ) times, except possibly for those values contained in two spherical disks each with radius j l 3 .□

Acknowledgment

The authors are very thankful to referees for their valuable comments that improved the presentation of this manuscript.

  1. Funding information: Authors state no funding involved.

  2. Author contributions: All authors have accepted responsibility for the entire content of this manuscript and consented to its submission to the journal, reviewed all the results, and approved the final version of the manuscript. KQH completed the main part of this article. QCZ corrected the main theorems. All authors gave the final approval for publication.

  3. Conflict of interest: The authors state no conflict of interests.

  4. Data availability statement: No data were used to support this study.

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Received: 2024-04-17
Revised: 2024-12-23
Accepted: 2025-04-03
Published Online: 2025-05-29

© 2025 the author(s), published by De Gruyter

This work is licensed under the Creative Commons Attribution 4.0 International License.

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