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http://dx.doi.org/10.4236/apm.2013.39098

Value Distribution of L-Functions with Rational Moving

Targets

Matthew Cardwell1, Zhuan Ye2* 1Intelligent Medical Objects, Inc., Northbrook, USA

2Department of Mathematical Sciences, Northern Illinois University, DeKalb, USA Email: mcardwell@e-imo.com, *ye@math.niu.edu

Received August 26, 2013; revised September 26, 2013; accepted October 1,2013

Copyright © 2013 Matthew Cardwell, Zhuan Ye. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited. In accordance of the Creative Commons Attribution License all Copyrights © 2013 are reserved for SCIRP and the owner of the intellectual property Matthew Cardwell, Zhuan Ye. All Copyright © 2013 are guarded by law and by SCIRP as a guardian.

ABSTRACT

We prove some value-distribution results for a class of L-functions with rational moving targets. The class contains Selberg class, as well as the Riemann-zeta function.

Keywords: Value Distribution; Moving Target; L-Function; Selberg Class

1. Introduction

We define the class  to be the collection of functions

 

1

 

s,

n

L s

a n n satisfying Ramanujan hypothesis,

Analytic continuation and Functional equation. We also denote the degree of a function L by dL which is a non-negative real number. We refer the reader to Chapter six of [1] for a complete definitions. Obviously,

the class contains the Selberg class. Also every

function in the class is an -function and the

Riemann-zeta function is in the class. In this paper, we prove a value-distribution theorem for the class with rational moving targets. The theorem generalizes the value-distribution results in Chapter seven of [1] from fixed targets to moving targets.

L

Theorem. Assume that L

 

1

and is a rational

function with . Let the roots of the

equation be denoted by

R

limsR s

 

0

R s

 

 

L sR RiR.

Then

(I) For any > max 1,1 1 2 L

b

d

 

 

 ,

 

2

, as .

R R

R b T T

b O T T

 

   

   

(II) For sufficiently large negative b,

  

< 2

4

2π log log ,

as .

R

R L

T T

T

b b d T O T

e T

  

   

 

Proof of (I). It is known that if L, then

 

 

 

0

1

1 , as

s n

a n

L s O k

n

 

;

   

where 0 is the index of the first non-zero term of the

sequence of k

 

a n

n 2 

 , s  it with ,t. Since

 

R s

 

0

limL s   , there exists 0> 0 such that

 

 

L sR s 0 for Re >s 0 . It follows that

0

<

R

  for all real part of zeros of the function

 

 

L sR s . We set R z

 

P

   

q

z

,

Q z where the

degrees of P Q, are p , respectively; and define

   

ssR s

 

.



Thus, there is 1 such that is analytic in the

region

> 1

r 

1

>

s r since is a meromorphic function in

with the only pole at . We apply Littlewood’s

argument principle [3] to in the rectangle

L

s1



c

: c T, 2

1,

it b

 

    t T

> max c

 where are

parameters satisfying . Thus,

, c T 0 b T

, >r1

 

log d 2π , d

b

s s i   

  



 

where the given logarithm is defined as in Littlewood’s argument principle [3]. To prove our result, however, we first decompose our auxiliary function by

(2)

 

   

 

 

   

   

 

   

1

2

1 : for

1 : for >

L s

P s P s s p q

P s Q s

s

L s

R s R s s p q

R s

  

 

 

  

 

 

 

  

 

 

1

(1)

Without loss of generality, we may assume that

whenever since we can always write

,

p qpq

 

 

N

 

N

R sP s s Q s s for due to our

choice of the parameters which define the rectangle . However, the modification will guarantee in the case of

0 s

1

k that exhibit polynomial growth, which is

necessary for our proof. In the case of ,

already exhibits polynomial growth, and no such adjustment is necessary. We now integrate the logarithm of to get

,

P Q

>

p q R



 

 

 

 

 

 

 

1

2

log log d for log d

log log d for >

s P s s O T p q

s s

s R s s O T p q

 

   

  

 



 

 

where the terms are the integrals of the maxi-

mum contribution from writing

 

O T

 

s

 as a sum of loga-

rithms. By our choice of T , both and

are analytic in Hence, Cauchy’s Theorem gives

logP logR

.

 

 

 

 

 

1

2

log for log

log f

d d

or d

s s O T p q

s s

s s O T p q

 

  

  

 



 

 

(2)

To connect this integral with Littlewood’s argument principle [3], we note that the definition of guaran- c

tees that

2

2

d d

2π , 2π

2π .

R R

R R

R

c

b b

b T T

R b T T

i i

i b

 

 

  

  

  

  

  

(3)

In light of (2) and because the quantity given in (3) is imaginary-valued, we get for k1, 2

 

2

2

2

2 2

Im log arg log arg

log 2 arg 2 log arg

log log arg a

d d

d d

d d d rg

R R

R b T T

c T

k k k k

b T

c T

k k k k

b T

T T c c

k k k

T T b b

i b

i iT i iT i c it i c it t

iT i iT i b it i b it t O T

i b it t c it t iT

 

  

  

 

  

       

        

        

   

   

  

 

4

, 1

2

:

d

,

k

j k j

iT O T

I O T

 



1

(4)

for instance.

We now estimate I1,k. For T large enough, we have for tT k,  (since p q, 1),

1

1 1

log log log

log 1 log 1 log log 2.

L b it L b it

b it

P b it Q b it P b it Q b it

L b itL b itL b it

 

 

      

   

        

Then for large enough, , we find in a

similar fashion that

T tT k, 2

2

log log 1

log log 2.

L b it b it

R b it

b it

 

  

  

Since we have the same estimate for , we find

that

1, 2

k

 

 

 

2

1, 1,

2 2

2 2

, log

log 2

1 log 2

d

d

d

T

k k T

T T

T T

I T b I b it t O T

b it T

t O T

T

T

L b it t O T

T

   

 

 

 

(3)

It is known [2] that for > max 1,1 1 2 L

b

d

 

 

 ,

 

 

2

2 2

2 1

d

1 1 .

lim TT

T n

a n

L b it t O

T n



 

Hence, I1,k

T b,

O T

uniformly in

1 1 ,1 2 dL

 

 

 

> max

b .

We next move to estimate 2,k. For sufficiently large

positive real number , we have I c

1 and

1,

L c it L c it

P c it R c it

 

 

  (5)

so

1

log c it log 1 L c it

P c it

  

 

since q1. Furthermore,

2

log c it 1 L c it .

R c it

  

 

Since we may take large enough so that c

1

k cit

 , we may write using a

Taylor series expansion in the rectangle log k

. For c it

k1, we have after taking real parts that

 

 

 

1

1

1 1

1

1 1 1 1

1

log Re

1

Re .

k

k k c it

k n

k

k c

k n n

k

a n c it

n k P c it

a n a n

n n

k P c it

 

 

  

  

it

 

 

  

 

 

 

 

 

 

 

 

 

We now observe that for sufficiently large T and some constant M we have

2 1

1

1,

T k

k it k

T

k

t T

MT

P c it n n P c iT

 

 

 

 

for kN and

1 1

1 1 1

1 lim sup

k k

c c

k k n nn n

 

 

  

 

 

for sufficiently large . In light of these bounds and the definition of , we have (6)

c

where the last equality holds because c could be

sufficiently large. Replacing by in the above

computations, we see analogously that

P R

 

2,2 1

IO .

Finally, we estimate I3,k and I4,k. We show the com-

putation for I3,k explicitly and note that the bound for

follows analogously. We first suppose that

4,k

Ik

iT

N zeros for

has exactly b  c. T are at

most N 1

hen, there

 subinterv ounting for multiplicities, in

which

als, c

Re k  iT is of consta signt n. Thus,

arg k  iTN1 π. (7) It remains to estimate N. To this end, we define

 

1

.

2

k k k

g z   ziT  ziT

Then

 

1

Re

,

2

k k k k

g    iT  iT   iT

for  

 

b c,

0

k  iT

so that if , then

 

0

g   .

Now let R2 c b and R> max

r1, 2

that T > 2R

R , and

choose T large enough so  . Then

1

> >

ziT RR for zc <R, showing that no zeros or poles of k

ziT

are located in zc <R. Thus, both k

ziT

and gk

 

z are analytic in

<

zc R. Letting nˆc k,

 

r denote the number of zeros of gk

 

z in z c r, we have

 

 

 

 

2 , 2 ,

0

2

, ,

ˆ ˆ

ˆ ˆ log 2

d d

. d

R c k R c k R R

c k R c k

n r n r

r r

r r

r

n R n R

r

 

  

 

 

By Jensen’s formula

 

 

2 ,

0 0

ˆ 1

log 2 e d lo 2π

d g

R c k i

k k

n r

r g c R g

r

  

c ,

and so

 

 

, 0

log 1

ˆ log 2 e .

2πlog 2 d log2

k i

c k k

g c

n R 

g cR  

(8)

 

 

 

 

 

 

1

1

2 1

2,1

1 1 1 1 1

1

1 1 1 1 1 1

1 Re

1 1 1 1 ,

d

k k

T k

c T k it

k n n k

k k

k

c c

k n n k n

k

a n a n t

I

k n n P c it n n

a n a n

O

k n n k n

  

  

    

    

 

 

 

 

 

 

 

  

  

 

 

 

 

(4)

By (5), log gk

 

c

operty of L

is bounded. Further, it is clear

from a pr functions that we have

 

B,as ,as ;

L sA t t  t 

for some positive absolute numbers A B,

estimate

in any vertical

strip of bounded width. The same must hold for

 

k

g z as well. Thus, the integral in (8) is O

logT

,

implying th O

logT

. Since the interval

 

at n

ˆc k,

 

R

2

, , ,

b cD c RD c R , it follows that

 

ˆ 

c k,  log

.

N n R O T

With this bound, we integrate (7) to deduce that

3, arg d 1 πd log .

c c

k

b b

1, , 4

j 

k

I

 it  

N  O T

As previously noted, we may bound I4,k in the same

way. Thus, we attain the desired bounds for and k1, 2. Consequently, the first part of t

is proved by using (4).

Proof of (II). As in the pro

theorem, we conclude that there exists a real number he theorem

of of the first part of the

0 

for which the real parts R of all R-values satisfy

0

<

R

  ; and also, there exist B T, > 0 for each rational function R such that no zeros of

 

 

s 0

L sR  lie in the quarter-plane  <B t, >T. As before, we define the rectangle

sit b:  c T, t 2T

       where b c T, ,

are parameters satisfying

0

r

< 1, > max 1, , > max , 1

b  B c   b T 1 T .

ding as in the proof of the first part of the theorem, we see that

Procee

 

2

1 ,

2

2π log

arg d arg 2 d

:

T

R T T k

c c

k k

b

j k j

i b i b it

iT O T

I I T

   

 

   

    

 



 

for where is defined as in (1). In the

equatio e, we n te that we have chosen to compute

4

O

b 

2

dt

Tlog c it dt

2

R

T T

iT

1, 2

k

n abov k

o

1

I separately. Indeed, this is the only estimate that we the integrals

will need. For Ij k,

pr

, and

, the bounds given as in the oo t part

eorem still hold. First, integral

unchanged. On the other hand, the integrals

have changed by our choice of but, as we ha

as before, we still have the desired bound

requirement is that we consid in a verti

of fixed width, which we have case.

We now bound

2,3, 4

j f of the firs

2,k is

1, 2

k h

of the t I

3,k, 4,k

I I

ve done since the only cal strip b

er in this

,

L

1

I . Since , we have by the

functional equation in the defi function,

<bB nition of L

 

 

  

  

  

 

  

 

1

L

L s R s s L s R s 1 1

1

1 1

L .

L

L

R s

s L s

s L s

  

 

R

s L s

L

    s

s

Taking logarithms, we get

    

 

 

 

 

 

log

log L log 1 log 1 .

L s R s

R s

s L s

L s

      (9)

niformly in

Since, for t> 1, we have, u ,

 

2

12

log

π 1

exp 1 ,

4

L

L

it L

d

L

s

i d

Q t itd O

t

 

  

   

  

 

 

  

where  , are two constants. It follows, for s  it as t , that

 

 

1

2 2 2

2 2

π 1 1

log log exp 1 log

4 2

1 1 1

log log 1 log log .

2

L L

L

it L

d d

L

it d

L

i d

s Q t it O Q t

t

Q t O d t Q O

t t

 

 

  

        

   

   

  

     

          

     

(5)

We now consider the last term in (9). Since,

log 1

, limsup

log 2 L

t

L b it

b d t



 

and noting b< 0, we have for any  > 0 and tT

12 b dL

L b it t

   

 

for sufficiently large T. Then we see the quotient

1

2

t 

1

L

b d

R b it R b it

O

L b it    t

  

  

  

when b is large enough so that

1

deg 1.

2 L

R b d  

 

 

 

Therefore, we find that

 

 

1

log 1 R s O .

L s t

 

  

 

Integrating in light of these estimates, we see

 

log

2

2 2

log

log log

2

log 1 .

d

d

d

T T

T T T

L b it R b it t

t Q t

L b it t O T

  

 

   

first i

2

1 T

L

b d

 

The ntegral is log4 log

 

2

L

T

d T T Q

e   , and the

second integral is O

 

1

ethod

for sufficiently large and

negative b by the m used to derive (6). Hence,

 

2

1

1 4

log log log .

2 L

T

I b d T T Q O T

e

  



  

With the estimates for the Ij k, ’s, we have proved the

se .

[1] J. Steuding,“Value Distribution of L-Functions,” Number

1877 in Lecture Notes in Mathematics, Springer, 2007.

[2] H. S. A. Potter, “The Mean Values of Certain Dirichlet

on

8.

plms/s2-46.1.467

cond part of the theorem

REFERENCES

Series I,” Proceedings Lond Mathematical Society, Vol.

46, No. 2, 1940, pp. 467-46 http://dx.doi.org/10.1112/

[3] E. C. Titchma nctions,” 2nd Edi-

References

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