Research Article Exceptional Values of Meromorphic ...2. Basic Notions in the Nevanlinna Theory on...
Transcript of Research Article Exceptional Values of Meromorphic ...2. Basic Notions in the Nevanlinna Theory on...
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Hindawi Publishing CorporationThe Scientific World JournalVolume 2013, Article ID 937584, 7 pageshttp://dx.doi.org/10.1155/2013/937584
Research ArticleExceptional Values of Meromorphic Function on Annulus
Hong-Yan Xu
Department of Informatics and Engineering, Jingdezhen Ceramic Institute, Jingdezhen, Jiangxi 333403, China
Correspondence should be addressed to Hong-Yan Xu; [email protected]
Received 5 June 2013; Accepted 9 July 2013
Academic Editors: A. Agouzal, A. Barbagallo, and A. Fiorenza
Copyright Β© 2013 Hong-Yan Xu.This is an open access article distributed under the Creative Commons Attribution License, whichpermits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.
The main purpose of this paper is to study the exceptional values of meromorphic function and its derivative on annulus. We alsogive some theorems and corollaries about exceptional values of meromorphic function on the annulus, which are the improvementof the previous results given by Chen and Wu.
1. Introduction
It is a very interesting problem on the exceptional values ofmeromorphic functions in the value distribution theory andargument distributed theory such as the Picard exceptionalvalue and the Borel exceptional value. It is well known thatevery class of exceptional value is always responding toa singular direction, such as, the Picard exceptional valuerelating with Juliaβs direction and the Borel exceptional valuerelating with Borelβs direction. In the 1970s, Gopalakrishnaand Bhoosnurmath [1, 2] and Singh and Gopalakrishna[3] investigated Borel exceptional values of meromorphicfunction and its derivative on the whole complex plane. In2011, Peng and Sun [4] gave some examples on T exceptionalvalue which is an exceptional value relating with T direction.
In fact, Peng, Sun, Singh, Gopalakrishna, and so forthonly studied exceptional values of meromorphic functionsin the whole complex planeβsingle-connected region. Formeromorphic function on the double-connected domain andseveral-connected region, there were few papers about itsexceptional values. In 2005, Khrystiyanyn and Kondratyuk[5, 6] proposed the Nevanlinna theory for meromorphicfunctions on annuli (see also [7]). In 2010, FernaΜndez [8]further investigated the value distribution of meromorphicfunctions on annuli. In 2012, Xu and Xuan [9] studied theuniqueness of meromorphic functions sharing some valueson annuli. At the same year, Chen andWu [10] firstly studiedthe Borel exceptional values of meromorphic function andits derivative on annulus. In this paper, we will further
investigate the exceptional value of meromorphic functionand its derivative on annulus and obtain a series of resultswhich are improvement of previous theorems given by Chenand Wu [10].
The structure of this paper is as follows. In Section 2,we introduce the basic notations and fundamental theoremsof meromorphic functions on annulus. Sections 3 and 4 aredevoted to study the Borel exceptional values of meromor-phic function on annulus and give some consequences of ourtheorems. Section 5 are devoted to study the Borel excep-tional values of meromorphic function and its derivative onannulus.
2. Basic Notions in the NevanlinnaTheory on Annuli
Let π be a meromorphic function on the annulus A = {π§ :1/π 0< |π§| < π
0}, where 1 < π < π
0β€ +β. The notations
of the Nevanlinna theory on annuli will be introduced asfollows. Let
π1(π , π)=β«
1
1/π
π1(π‘, π)
π‘ππ‘, π
2(π , π)=β«
π
1
π2(π‘, π)
π‘ππ‘,
π0(π , π) = π (π , π) + π(
1
π , π) ,
π0(π , π) = π
1(π , π) + π
2(π , π) ,
(1)
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where π1(π‘, π) and π
2(π‘, π) are the counting functions of poles
of the function π in {π§ : π‘ < |π§| β€ 1} and {π§ : 1 < |π§| β€π‘}, respectively. The Nevanlinna characteristic of π on theannulus A is defined by
π0(π , π) = π
0(π , π) β 2π (1, π) + π
0(π , π) . (2)
Similarly, for π β C, we have
π0(π,
1
π β π) = π
1(π ,
1
π β π) + π
2(π ,
1
π β π)
= β«1
1/π
π1(π‘, 1/ (π β π))
π‘ππ‘
+ β«π
1
π2(π‘, 1/ (π β π))
π‘ππ‘
(3)
in which each zero of the functionπβπ is counted only once.In addition, we use ππ)
1(π‘, 1/(π β π)) (or π(π
1(π‘, 1/(π β π))) to
denote the counting function of poles of the function 1/(πβπ)with multiplicities β€ π (or > π) in {π§ : π‘ < |π§| β€ 1}, each pointcounted only once. Similarly, we have the notationsππ)
1(π‘, π),
π(π
1(π‘, π),ππ)
2(π‘, π),π(π
2(π‘, π), andππ)
0(π‘, π),π(π
0(π‘, π).
For a nonconstant meromorphic function π on theannulus A = {π§ : 1/π
0< |π§| < π
0}, where 1 < π < π
0β€ +β,
the following properties will be used in this paper (see [5]):
(i) π0(π , π) = π
0(π , 1/π),
(ii) max{π0(π , π1β π2), π0(π , π1/π2), π0(π , π1+ π2)} β€
π0(π , π1) + π0(π , π2) + π(1),
(iii) π0(π , 1/(πβπ)) = π
0(π , π)+π(1), for every fixed π β
C.
Khrystiyanyn and Kondratyuk [6] also obtained thelemma on the logarithmic derivative on the annulus A.
Theorem 1 (see [6] lemma on the logarithmic derivative). Letπ be a nonconstant meromorphic function on the annulusA ={π§ : 1/π
0< |π§| < π
0}, where π
0β€ +β, and let π > 0. Then
(i) in the case π 0= +β,
π0(π ,
π
π) = π (log (π π
0(π , π))) (4)
for π β (1, +β) except for the set Ξπ such that β«
Ξπ
π πβ1ππ <+β,
(ii) if π 0< +β, then
π0(π ,
π
π) = π(log(
π0(π , π)
π 0β π
)) (5)
for π β (1, π 0) except for the set Ξ
π such that β«
Ξ
π
(ππ /(π 0β
π )πβ1) < +β.
In 2005,The second fundamental theoremon the annulusA was first obtained by Khrystiyanyn and Kondratyuk [6].Cao et al. [11] introduce other forms of the second fundamen-tal theorem on annuli as follows.
Theorem 2 ([11, Theorem 2.3] The second fundamentaltheorem). Let π be a nonconstant meromorphic function onthe annulusA = {π§ : (1/π
0) < |π§| < π
0}, where 1 < π
0β€ +β.
Let π1, π2, . . . , π
πbe π distinct complex numbers in the extended
complex plane C. Let π1, π2, . . . , π
πbe π positive integers, and
let π β₯ 0. Then
(π β 2) π0(π , π) <
π
βπ=1
π0(π ,
1
π β ππ
) + π (π , π) , (6)
where (i) in the case π 0= +β,
π (π , π) = π (log (π π0(π , π))) (7)
for π β (1, +β) except for the set Ξπ such that β«
Ξπ
π πβ1ππ <+β,
(ii) if π 0< +β, then
π (π , π) = π(log(π0(π , π)
π 0β π
)) (8)
for π β (1, π 0) except for the set Ξ
π such that β«
Ξ
π
(ππ /(π 0β
π )πβ1) < +β.
Definition 3. Let π(π§) be a nonconstant meromorphic func-tion on the annulus A = {π§ : 1/π
0< |π§| < π
0}, where
1 < π 0β€ +β. The function π is called a transcendental or
admissible meromorphic function on the annulus A whichprovided that
lim supπ ββ
π0(π , π)
logπ = β, 1 < π < π
0= +β (9)
or
lim supπ βπ 0
π0(π , π)
β log (π 0β π )
= β, 1 < π < π 0< +β, (10)
respectively.
Thus for a transcendental or admissible meromorphicfunction on the annulus A, π(π , π) = π(π
0(π , π)) holds for
all 1 < π < π 0except for the set Ξ
π or the set Ξ
π mentioned
inTheorem 1, respectively.
Definition 4 (see [10], Definition 2.1). Let π(π§) be a noncon-stant meromorphic function on the annulus A = {π§ : 1/π
0<
|π§| < π 0}, where π
0= +β. Then the order of π(π§) is defined
by
π (π) = lim supπ β+β
π0(π , π)
logπ . (11)
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Definition 5 (see [10], Definition 3.1). Let π(π§) be a noncon-stant meromorphic function of order π (0 < π < β) on theannulus A = {π§ : 1/π
0< |π§| < π
0}, where 1 < π
0β€ +β, and
let π β CΜ. Then we say that π is
(i) an evB (exceptional value in the sense of Borel) for πon A for distinct zeros of order β€ π if π
π(π, π) < π;
(ii) an evB (exceptional value in the sense of Borel) for πon A for distinct zeros if π(π, π) < π;
(iii) an evB (the Borel exceptional value) for π on A ifπ(π, π) < π, where
ππ(π, π) = lim sup
π β+β
ππ)
0(π , 1/ (π β π))
logπ ,
π (π, π) = lim supπ β+β
π0(π , 1/ (π β π))
logπ ,
π (π, π) = lim supπ β+β
π0(π , 1/ (π β π))
logπ .
(12)
In particular, we say that π is an evB for π on A for simplezeros if π = 1 and π is an evB forπ onA for simple and doublezeros if π = 2.
3. The Main Results
Now, the main theorems of this paper are listed as follows.
Theorem 6. Let π be transcendental meromorphic functionof order π (0 < π < β) on the annulus A :={π§ : 1/π
0< |π§| < π
0}, where π
0= +β. If there
exist π11, . . . , π1
π1, π21, . . . , π2
π2, . . . , π]
1, . . . , π]
π]β CΜ such that
ππ1, ππ2, . . . , ππ
ππare evBs forπ onA for distinct zeros of orderβ€ π
π,
π = 1, 2, . . . , ], where π1, . . . , π], ] β N+, and π1, π2, . . . , π] are
positive integers or infinity. Then
Ξ :=]
βπ=1
ππππ
1 + ππ
+]
βπ=1
1
1 + ππ
ππ
βπ=1
πΏππ
0(πππ, π) β€ 2. (13)
Remark 7. Under the assumptions of Theorem 6, if ] = 3,π1= π, π
2= π‘, π
3= π and π
1= π, π
2= π, π
3= π, since
πΏππ
0(πππ, π) β₯ 0, then we can get
ππ
π + 1+
π‘π
π + 1+
π π
π + 1β€
]
βπ=1
ππππ
1 + ππ
+]
βπ=1
1
1 + ππ
ππ
βπ=1
πΏππ
0(πππ, π) β€ 2.
(14)
This shows thatTheorem 6 is an improvement of results givenby Chen and Wu [10].
Definition 8. For positive integers π,π, we define that
πΏπ0(π, π) = 1 β lim sup
π β+β
ππ0(π , 1/ (π β π))
π0(π , π)
,
Ξ0(π, π) = 1 β lim sup
π β+β
π0(π , 1/ (π β π))
π0(π , π)
,
(15)
whereππ0(π , 1/(πβπ)) is the counting function of π-points of
π onAwhere an π-point of multiplicityπ is countedπ timesifπ β€ π and 1+π times ifπ > π. In particular, if π = β, then
πΏβ0(π, π) = πΏ
0(π, π) = lim inf
π β+β
π0(π , 1/ (π β π))
π0(π , π)
= 1 β lim supπ β+β
π0(π , 1/ (π β π))
π0(π , π)
.
(16)
Theorem 9. Let π be transcendental meromorphic function oforder π (0 < π < β) on the annulus A := {π§ : 1/π
0< |π§| <
π 0}, where π
0= +β. If there exist π β CΜ and two positive
integers π and π such that
(1 + π)Ξ0(π, π) + β
π ΜΈ= π
πΏ0(π, π) > 2 β π (π β 1) , (17)
then there exist at most π elements CΜ \ {π} which are evBs forπ on A for distinct zeros of order not exceeding π.
3.1. Proof of Theorem 6
Proof. For any positive integer π orβ and π β CΜ, we have
π0(π ,
1
π β π) β€
π
1 + πππ)
0(π ,
1
π β π)
+1
1 + πππ0(π ,
1
π β π) ,
(18)
where π/(π + 1) = 1 and 1/(π + 1) = 0 if π = β. Then, from(18) andTheorem 2, we have
(]
βπ=1
ππβ 2)π
0(π , π)
β€]
βπ=1
ππ
1 + ππ
ππ
βπ=1
πππ)
0(π ,
1
π β πππ
)
+]
βπ=1
1
1 + ππ
ππ
βπ=1
πππ
0(π ,
1
π β πππ
) + π (π , π) .
(19)
From Definition 5 and the assumptions of Theorem 6, thereexists a constant π (0 < π < π) such that for sufficiently largeπ ,
πππ)
0(π ,
1
π β πππ
) < π π, π = 1, 2, . . . , ππ, π = 1, 2, . . . , ].
(20)
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Hence, from (19) and (20) and for sufficiently largeπ , we have
(]
βπ=1
ππβ 2)π
0(π , π) β€
]
βπ=1
1
1 + ππ
ππ
βπ=1
πππ
0(π ,
1
π β πππ
)
+ π (π π) + π (π , π) .
(21)
Thus, for sufficiently large π and taking arbitrary π(> 0), wecan get from (21) and the definition of πΏ
π(π, π) that
(]
βπ=1
ππβ 2)π
0(π , π)
β€]
βπ=1
1
1 + ππ
ππ
βπ=1
(1 β πΏπππ(πππ, π) + π) π
0(π , π)
+ π (π π) + π (π , π) .
(22)
Since π = +β, it follows that
(Ξ β 2 β π) π0(π , π) β€ π (π π) + π (logπ π
0(π , π)) , (23)
for π β (1, +β) except for the set Ξπ such that β«
Ξπ
π πβ1ππ <
+β. If πΌ = [π , π ) β Ξπ , we have
π π β π π = πβ«π
π
π₯πβ1ππ₯ β€ πβ«Ξπ
π πβ1ππ < π, (24)
whereπ is a constant. Thus,
(Ξ β 2 β π) π0(π , π) β€ π (π π) + π (logπ π
0(π , π)) (25)
holds for all π . If Ξ > 2, we can choose an arbitrary π (0 <π < Ξ β 2) satisfying π + π < π. Thus, from (25) and forsufficiently large π , we can get a contradiction to (13) easily.
Therefore, we can get the conclusion of Theorem 6.
3.2. The Proof of Theorem 9
Lemma 10. Let π be transcendental meromorphic function oforder π (0 < π < β) on the annulus A := {π§ : 1/π
0< |π§| <
π 0}, where 1 < π
0β€ +β. Then
lim supπ β+β
π0(π , 1/π)
π0(π , π)
β€ 2 β Ξ0(β, π) β β
πβC
πΏ0(π, π) .
(26)
Proof. Suppose that π1, π2, . . . , π
π‘β C are π‘ distinct complex
constants. From the definitions ofπ0(π , π), π
0(π , π), we have
π‘
βπ=1
π0(π,
1
π β ππ
) β€ π0(π,
1
π) + π (π , π) β€ π
0(π , π)
β π0(π ,
1
π) + π (π , π) .
(27)
And since π0(π , π) β€ π
0(π , π) +π
0(π , π) + π(π , π), then we
have
π‘
βπ=1
π0(π ,
1
π β ππ
) + π0(π ,
1
π) β€ π
0(π , π)
+ π0(π , π) + π (π , π) .
(28)
It follows from the definitions of πΏ0(π, π), Ξ
0(π, π) that
π‘
βπ=1
πΏ0(ππ, π) + lim sup
π β+β
π0(π , 1/π)
π0(π , π)
β€ 2 β Ξ0(β, π) .
(29)
From (29) and π‘ is arbitrary, the proof of Lemma 10 iscompleted easily.
Proof of Theorem 9. Without loss of generality, we assumethat π = β. Next, we will employ reductio ad absurdum toprove the conclusion of Theorem 9. Suppose that there existπ+ 1 elements π
1, π2, . . . , π
π+1β C which are evBs for π onA
for distinct zeros of multiplicity β€ π. We know that if π§0is a
zero of π β π onA of multiplicity π (> 1) for π β C, then π§0is
a zero of π on A of multiplicity π β 1. It follows that
π+1
βπ=1
π0(π ,
1
π β ππ
) β€
π+1
βπ=1
ππ)
0(π ,
1
π β ππ
) +1
ππ0(π ,
1
π) .
(30)
Therefore, by Theorem 2 we have
ππ0(π , π) β€
π+1
βπ=1
π0(π ,
1
π β ππ
) + π0(π , π) + π (π , π)
β€
π+1
βπ=1
ππ)
0(π ,
1
π β ππ
) +1
ππ0(π ,
1
π)
+ π0(π , π) + π (π , π) .
(31)
From the definitions of order and evB of π on A, there existsa constant π (0 < π < π) such that for sufficiently large π , wehave
ππ)
0(π ,
1
π β ππ
) < π π, π = 1, 2, . . . , π + 1. (32)
From (31), (32), and Lemma 10, for sufficiently large π , itfollows that
(π β 1 β1
π(2 β Ξ
0(β, π) β β
π ΜΈ=β
πΏ0(π, π)) + Ξ
0(β, π))
Γ π0(π , π) β€ π π + π (π , π) ,
(33)
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for π β (1, +β) except for the set Ξπ such that β«
Ξπ
π πβ1ππ <
+β. Since π 0
= +β, similar to the argument as inTheorem 6, from (33) we find that
(π β 1 β2 β (π + 1)Ξ
0(β, π) β β
π ΜΈ=βπΏ0(π, π)
π)π0(π , π)
β€ π π + π (log (π π0(π , π)))
(34)
holds for allπ . Since π < π, from (34) and for sufficiently largeπ , we can get
(1 + π)Ξ0(β, π) + β
π ΜΈ=β
πΏ0(π, π) > 2 β π (π β 1) , (35)
which is contradiction with the assumption of Theorem 9.Thus, this completes the proof of Theorem 9.
4. Some Consequences of Theorems 6 and 9
In this section, wewill give some consequences ofTheorems 6and 9. Before we give these results, some definitions will beintroduced below.
Definition 11. Letπ bemeromorphic function on the annulusA := {π§ : 1/π
0< |π§| < π
0}, where π
0= +β. For π β CΜ, then
we say that
(i) π is called an exceptional value in the sense ofNevanlinna (evN for short) forπ onA, if πΏ
0(π, π) > 0;
(ii) π is called a normal value in the sense of Nevanlinna(nvN for short) for π on A, if πΏ
0(π, π) = 0.
In addition, similar to the Picard exceptional value in thewhole complex plane, we define that π is called an exceptionalvalue in the sense of Picard (evP for short) forπ onA, ifπ hasat most a finite number of π-points on A.
Consequence 1. Under the assumptions of Theorem 6, if π1=
1, fromTheorem 6, we get
π1+ 2
]
βπ=2
ππππ
1 + ππ
+
π1
βπ=1
πΏ10(π1π, π) +
]
βπ=2
2
1 + ππ
ππ
βπ=1
πΏ10(πππ, π) β€ 4.
(36)
Since ππβ₯ 0 and πΏ1
0(πππ, π) β₯ 0 for π = 1, . . . , ], it follows that
(i) if π has an evB for simple zeros which is also an evNfor π on A, then π has at most three evBs for simplezeros on A;
(ii) if π1and π
2are two evPs for π on A then no other
element is an evB for π for simple zeros on A;(iii) there exist at most four elements which are evBs for π
simple zeros on A since πΏ1(π1π, π) β₯ 0. Moreover, all
these four values are nvNs for π on A.
Consequence 2. Under the assumptions of Theorem 6, letπ1= 1, π
1= 1, then
(a) if π2= 2, we have
2π2
3+
]
βπ=3
ππππ
1 + ππ
+1
2πΏ10(π11, π) +
1
3
π2
βπ=1
πΏ20(π2π, π)
+]
βπ=3
1
1 + ππ
ππ
βπ=1
πΏππ
0(πππ, π) β€
3
2.
(37)
Since ππβ₯ 0 and πΏππ
0(πππ, π) β₯ 0, it follows from (37) that π
2<
3. Thus, if π11is an evB for π on A for simple zeros, that is,
πΏ10(π11, π) > 0, then there exist at most two other elements
which are evBs forπ onA for distinct simple zeros and doublezeros. Furthermore,
(i) if πΏ10(π11, π) = 1/3, then two other elements evBs are
also evNs for π on A;
(ii) if any of the two other elements π21and π2
2, say π2
1,
satisfies πΏ10(π21, π) = 1/2, then π1
1, π22are also evNs for
π on A;(b) if π
2= 3, we have
3π2
4+
]
βπ=3
ππππ
1 + ππ
+1
2πΏ10(π1, π) +
1
4
π2
βπ=1
πΏ30(π2π, π)
+]
βπ=3
1
1 + ππ
ππ
βπ=1
πΏππ
0(πππ, π) β€
3
2.
(38)
From the above inequality and πΏ0(π, π) β₯ 0 for π β CΜ, we get
that π1= 1, π
2β€ 2 and π
1= 1, π
2= 2, π
π= 0 (π = 3, . . . , ]).
Thus, ifπ has an evB for simple zeros onA, then there exist atmost two other elementswhich are evBs forπdistinct zeros ofmultiplicity β€ 3 on A. Moreover, all these exceptional valuesare nvNs for π on A.
Consequence 3. Under the assumptions ofTheorem 6, if π1=
2, then we have
2π1
3+
]
βπ=2
ππππ
1 + ππ
+1
3
π1
βπ=1
πΏ20(π1π, π)
+]
βπ=2
1
1 + ππ
ππ
βπ=1
πΏππ
0(πππ, π) β€ 2.
(39)
Sinceβ]π=2(ππππ/(1+π
π))+β
]π=2(1/(1+π
π)) βππ
π=1πΏππ
0(πππ, π) β₯ 0,
then from (39) we have
2π1
3+1
3
π1
βπ=1
πΏ20(π1π, π) β€ 2. (40)
Thus, it follows that π1β€ 3 and π
1= 3, π
π= 0, π = 2, . . . , ].
Hence, we have that π has at most three evBs for distinctsimple and double zeros on A. Moreover, all three evBs fordistinct simple and double zeros are nvNs for π on A.
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6 The Scientific World Journal
Consequence 4. Under the assumptions of Theorem 6, letπ1= 2, π
1= 1.
(a) If π2= 1, then we have
π2+ 2
]
βπ=3
ππππ
1 + ππ
+2
3πΏ20(π11, π) +
π2
βπ=1
πΏ10(π2π, π)
+]
βπ=3
2
1 + ππ
ππ
βπ=1
πΏππ
0(πππ, π) β€
8
3.
(41)
Thus, it follows that π2β€ 2. So, if there exists an evB for π
on A for distinct and double zeros, say π11, then there exist at
most two other evBs for π on A for simple zeros, say π21, π22.
Furthermore, if π1= 1, π
2= 2, it follows that
2πΏ20(π11, π) + 3πΏ1
0(π21, π) + πΏ1
0(π22, π) β€ 2. (42)
Thus, we can see that any one of π21, π22may not be an evP for
π on A. Furthermore, if π11is an evP for π on A. Then π2
1, π22
are nvNs for π on A;
(b) if π2= 1, π
2= 3, π3= 1, then we have
π3+
]
βπ=4
2ππππ
1 + ππ
+2
3πΏ20(π11, π) +
1
2πΏ30(π21, π)
+
π3
βπ=1
πΏ10(π3π, π) +
]
βπ=4
2
1 + ππ
ππ
βπ=1
πΏππ
0(πππ, π) β€
7
6.
(43)
Thus, we can get that π3β€ 1. That is, if π have two evBs onA,
say π11and π21and π11is for distinct simple and double zeros,
π21for distinct zeros of order β€ 3, then π has at most one evB
for simple zeros on A. Furthermore, if π3= 1, then
2
3πΏ20(π11, π) +
1
2πΏ30(π21, π) + πΏ1
0(π31, π) β€
1
6. (44)
It follows that πΏ20(π11, π) β€ 1/4, πΏ3
0(π21, π) β€ 1/3 and
πΏ10(π31, π) β€ 1/6. Thus, if any equality of these three inequali-
ties holds, then the other two are nvNs for π on A.Now, we will give some consequences of Theorem 9 as
follows.
Consequence 5. Under the assumptions of Theorem 9, if π =1 and
2Ξ0(π, π) + β
π ΜΈ= π
πΏ0(π, π) > 3 β π, (45)
we have the following:
(i) if π = 1 and 2Ξ0(π, π)+β
π ΜΈ= ππΏ0(π, π) > 2, then there
exists at most one element π ΜΈ= π which is an evB for πonA for simple zeros; in particular, this holds if thereexists an π β CΜ satisfying Ξ
0(π, π) = 1;
(ii) if π = 2 and 2Ξ0(π, π)+β
π ΜΈ= ππΏ0(π, π) > 1, then there
exists at most two elements π1, π2ΜΈ= π which are evBs
for π onA for simple zeros; in particular, this holds ifthere exists an π β CΜ satisfying Ξ
0(π, π) > 1/2;
(iii) if π = 3 and 2Ξ0(π, π)+β
π ΜΈ= ππΏ0(π, π) > 0, then there
exists at most three elements π1, π2, π3ΜΈ= π which are
evBs for π on A for simple zeros; in particular, thisholds if there exists an π β CΜ satisfying Ξ
0(π, π) > 0.
Remark 12. Under the assumptions of Theorem 9, fromConsequence 5, we have that if there exist four distinctelements π
1, π2, π3, π4β CΜwhich are evBs forπ onA for simple
zeros, then Ξ0(ππ, π) β€ 1/2 and Ξ
0(π, π) = 0 for π ΜΈ= π
πand
π = 1, 2, 3, 4.
Consequence 6. Under the assumptions of Theorem 9, if π =2 and
3Ξ0(π, π) + β
π ΜΈ= π
πΏ0(π, π) > 4 β 2π, (46)
we have the following:
(i) if π = 1 and 3Ξ0(π, π) + β
π ΜΈ= ππΏ0(π, π) > 2, then
there exists at most one element π ΜΈ= π which is an evBfor π on A for distinct simple and double zeros; inparticular, this holds if there exists an π β CΜ satisfyingΞ0(π, π) > 2/3;
(ii) if π = 2 and 3Ξ0(π, π)+β
π ΜΈ= ππΏ0(π, π) > 0, then there
exists at most two elements π1, π2ΜΈ= π which are evBs
for π on A for distinct simple and double zeros; inparticular, this holds if there exists an π β CΜ satisfyingΞ0(π, π) > 0.
Remark 13. Under the assumptions ofTheorem 9, fromCon-sequence 6, we have that if there exist four distinct elementsπ1, π2, π3β CΜ which are evBs for π on A for distinct simple
and double zeros, then Ξ0(ππ, π) β€ 2/3 and Ξ
0(π, π) = 0 for
π ΜΈ= ππand π = 1, 2, 3.
5. Exceptional Value of MeromorphicFunction and Its Derivative
In this section, we will study the exceptional value ofmeromorphic functionπ onA and its differential polynomialof the form
π[π] := π[π, π, . . . , π(π)] = ππ(π§)π0(π)
π1β β β (π(π))
ππ
,
(47)
where π0, π1, . . . , π
πβ N, π β N
+, and π( ΜΈ= 0) β C is a complex
constant.
Theorem 14. Let π be transcendental meromorphic functionof order π (0 < π < β) on the annulus A := {π§ : 1/π
0<
|π§| < π 0}, where π
0= +β. If 0 and β are evBs for π on
A for distinct zeros, thenπ[π] has no evB for simple zeros inCΜ \ {0,β}.
Proof. From (21), set π = π0+ π1+ β β β + π
π. Since π is a
transcendental meromorphic function on A, similar to themethod of [12, Theorem 1.21], we can get that π and π[π]
-
The Scientific World Journal 7
have the same order π onA. By applyingTheorem 1 forπ[π],for π( ΜΈ= 0) β C we have
π0(π ,π [π]) β€ π
0(π ,
1
π [π]) + π
0(π ,π [π])
+ π0(π ,
1
π [π] β π) + π (π ,π [π])
β€ π0(π ,
1
π [π]) + π
0(π , π)
+1
2π1)
0(π ,
1
π [π] β π)
+1
2π1
0(π ,
1
π [π] β π) + π (π , π)
β€ π0(π ,
1
π [π]) + π
0(π , π)
+1
2π1)
0(π ,
1
π [π] β π)
+1
2π0(π , π) + π (π , π) .
(48)
Since
π0(π ,
1
π [π]) β€ π
0(π ,
ππ
π[π]) + π
0(π ,
1
ππ)
β€ π0(π ,
π [π]
ππ) + π
0(π ,
1
π) + π (π , π)
β€ π0(π ,
π [π]
ππ) + π
0(π ,
1
π) + π (π , π)
β€ π(π0(π ,
1
π) + π
0(π , π)) + π (π , π) .
(49)
and 0 andβ are evBs forπ onA for distinct zeros, then thereexists a constant π (0 < π < π) such that for sufficiently largeπ , we have
π0(π ,
1
π) < π π, π
0(π , π) < π π. (50)
Suppose that π is an evB forπ[π] on A for simple zeros,since π[π] is of order π. Then for sufficiently large π , thereexists a constant π½ < π such that
π1)
0(π ,
1
π [π] β π) < π π½. (51)
Thus, from (48)β(50), it follows that
1
2π0(π ,π [π]) β€ π(ππ½
) + π (logπ π0(π , π)) , (52)
where π½ = max{π, π½} and for π β (1, +β) except for the setΞπ such that β«
Ξπ
π πβ1ππ < +β. Since π[π] is of order π,then there exists a sequence {π
π} tending toβ such that
π0(π π,π [π]) > π πΌ
π, (53)
where πΌ (π½ < πΌ < π) is a constant. Thus, we can get acontradiction by using the same argument as inTheorem 6.
Therefore,π[π] has no evB for simple zeros in CΜ\{0,β}.
Acknowledgments
The author was supported by the NNSF of China (no.61202313) and the Natural Science Foundation of Jiang-XiProvince in China (2010GQS0119 and 20132BAB211001).
References
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