An arithmetic interpretation of generalized Li s criterion

Similar documents
Fractional Fourier Series with Applications

SLOW INCREASING FUNCTIONS AND THEIR APPLICATIONS TO SOME PROBLEMS IN NUMBER THEORY

LAPLACE TRANSFORMS. 1. Basic transforms

Extension of Hardy Inequality on Weighted Sequence Spaces

DERIVING THE DEMAND CURVE ASSUMING THAT THE MARGINAL UTILITY FUNCTIONS ARE LINEAR

Elzaki transform and the decomposition method for nonlinear fractional partial differential equations

ME 321 Kinematics and Dynamics of Machines S. Lambert Winter 2002

Meromorphic Functions Sharing Three Values *

Fourier series representations of the logarithms of the Euler gamma function and the Barnes multiple gamma functions. Donal F.

Existence Of Solutions For Nonlinear Fractional Differential Equation With Integral Boundary Conditions

Reinforcement Learning

CHAPTER 2 Quadratic diophantine equations with two unknowns

Laplace Transform. Definition of Laplace Transform: f(t) that satisfies The Laplace transform of f(t) is defined as.

An Extension of Hermite Polynomials

ERROR ESTIMATES FOR APPROXIMATING THE FOURIER TRANSFORM OF FUNCTIONS OF BOUNDED VARIATION

LOCUS 1. Definite Integration CONCEPT NOTES. 01. Basic Properties. 02. More Properties. 03. Integration as Limit of a Sum

x, x, e are not periodic. Properties of periodic function: 1. For any integer n,

ON PRODUCT SUMMABILITY OF FOURIER SERIES USING MATRIX EULER METHOD

On Absolute Indexed Riesz Summability of Orthogonal Series

A new approach to Kudryashov s method for solving some nonlinear physical models

Math 153: Lecture Notes For Chapter 1

In this section we will study periodic signals in terms of their frequency f t is said to be periodic if (4.1)

EE757 Numerical Techniques in Electromagnetics Lecture 9

ON BILATERAL GENERATING FUNCTIONS INVOLVING MODIFIED JACOBI POLYNOMIALS

G x, x E x E x E x E x. a a a a. is some matrix element. For a general single photon state. ), applying the operators.

The sphere of radius a has the geographical form. r (,)=(acoscos,acossin,asin) T =(p(u)cos v, p(u)sin v,q(u) ) T.

( ) ( ) ( ) ( ) ( ) ( ) ( ) (2)

NEIGHBOURHOODS OF A CERTAIN SUBCLASS OF STARLIKE FUNCTIONS. P. Thirupathi Reddy. E. mail:

Suggested Solution for Pure Mathematics 2011 By Y.K. Ng (last update: 8/4/2011) Paper I. (b) (c)

MODERN CONTROL SYSTEMS

NATURAL TRANSFORM AND SOLUTION OF INTEGRAL EQUATIONS FOR DISTRIBUTION SPACES

ELEC 372 LECTURE NOTES, WEEK 6 Dr. Amir G. Aghdam Concordia University

BINOMIAL THEOREM OBJECTIVE PROBLEMS in the expansion of ( 3 +kx ) are equal. Then k =

Inferences of Type II Extreme Value. Distribution Based on Record Values

Types Ideals on IS-Algebras

PRIMARY DECOMPOSITION, ASSOCIATED PRIME IDEALS AND GABRIEL TOPOLOGY

Note 7 Root-Locus Techniques

On New Prajapati-Shukla Functions And Polynomials

Fourier Series and Applications

Chapter #5 EEE Control Systems

ONE RANDOM VARIABLE F ( ) [ ] x P X x x x 3

Review for the Midterm Exam.

10.2 Series. , we get. which is called an infinite series ( or just a series) and is denoted, for short, by the symbol. i i n

CONTROL SYSTEMS. Chapter 3 : Time Response Analysis

IX.1.1 The Laplace Transform Definition 700. IX.1.2 Properties 701. IX.1.3 Examples 702. IX.1.4 Solution of IVP for ODEs 704

Coefficient Inequalities for Certain Subclasses. of Analytic Functions

arxiv:math/ v1 [math.fa] 1 Feb 1994

Week 8 Lecture 3: Problems 49, 50 Fourier analysis Courseware pp (don t look at French very confusing look in the Courseware instead)

Special Functions. Leon M. Hall. Professor of Mathematics University of Missouri-Rolla. Copyright c 1995 by Leon M. Hall. All rights reserved.

IX.1.1 The Laplace Transform Definition 700. IX.1.2 Properties 701. IX.1.3 Examples 702. IX.1.4 Solution of IVP for ODEs 704

On a Grouping Method for Constructing Mixed Orthogonal Arrays

CONTROL SYSTEMS. Chapter 3 : Time Response Analysis. [GATE EE 1991 IIT-Madras : 2 Mark]

[ 20 ] 1. Inequality exists only between two real numbers (not complex numbers). 2. If a be any real number then one and only one of there hold.

RESEARCH PAPERS FACULTY OF MATERIALS SCIENCE AND TECHNOLOGY IN TRNAVA SLOVAK UNIVERSITY OF TECHNOLOGY IN BRATISLAVA

The solution is often represented as a vector: 2xI + 4X2 + 2X3 + 4X4 + 2X5 = 4 2xI + 4X2 + 3X3 + 3X4 + 3X5 = 4. 3xI + 6X2 + 6X3 + 3X4 + 6X5 = 6.

Solution of Laplace s Differential Equation and Fractional Differential Equation of That Type

Laplace Examples, Inverse, Rational Form

Journal of Quality Measurement and Analysis JQMA 12(1-2) 2016, Jurnal Pengukuran Kualiti dan Analisis

Approximations of Definite Integrals

can be viewed as a generalized product, and one for which the product of f and g. That is, does

Extended Fermi-Dirac and Bose-Einstein functions with applications to the family of zeta functions

u t u 0 ( 7) Intuitively, the maximum principles can be explained by the following observation. Recall

Physics 232 Exam II Mar. 28, 2005

Name: Period: Date: 2.1 Rules of Exponents

Numerical Methods using the Successive Approximations for the Solution of a Fredholm Integral Equation

NOTES ON BERNOULLI NUMBERS AND EULER S SUMMATION FORMULA. B r = [m = 0] r

graph of unit step function t

A L A BA M A L A W R E V IE W

SUMMATION OF INFINITE SERIES REVISITED

, so the state may be taken to be l S ÅÅÅÅ

Area, Volume, Rotations, Newton s Method

S.E. Sem. III [EXTC] Applied Mathematics - III

OH BOY! Story. N a r r a t iv e a n d o bj e c t s th ea t e r Fo r a l l a g e s, fr o m th e a ge of 9

Supplement: Gauss-Jordan Reduction

The Inverse of Power Series and the Partial Bell Polynomials

Graphing Review Part 3: Polynomials

Introduction to Congestion Games

Contraction Mapping Principle Approach to Differential Equations

Review - Week 10. There are two types of errors one can make when performing significance tests:

Physics 232 Exam I Feb. 13, 2006

F.Y. Diploma : Sem. II [CE/CR/CS] Applied Mathematics

THE GENERALIZED WARING PROCESS

MATRIX ALGEBRA, Systems Linear Equations

Schrödinger Equation Via Laplace-Beltrami Operator

P-Convexity Property in Musielak-Orlicz Function Space of Bohner Type

Introduction to Modern Control Theory

Forced Oscillation of Nonlinear Impulsive Hyperbolic Partial Differential Equation with Several Delays

In an algebraic expression of the form (1), like terms are terms with the same power of the variables (in this case

Convergence rates of approximate sums of Riemann integrals

Physics 240: Worksheet 16 Name

[Nachlass] of the Theory of the Arithmetic-Geometric Mean and the Modulus Function.

We will look for series solutions to (1) around (at most) regular singular points, which without

Hadamard matrices from the Multiplication Table of the Finite Fields

Chapter4 Time Domain Analysis of Control System

Fractional Order EOQ Model with Linear Trend of Time-Dependent Demand

Fig. 1. I a. V ag I c. I n. V cg. Z n Z Y. I b. V bg

Section P.1 Notes Page 1 Section P.1 Precalculus and Trigonometry Review

Heat Equation: Maximum Principles

MA123, Chapter 9: Computing some integrals (pp )

A Level Mathematics Transition Work. Summer 2018

Transcription:

A riheic ierpreio o geerlized Li crierio Sergey K. Sekkii Lboroire de Phyique de l Mière Vive IPSB Ecole Polyechique Fédérle de Lue BSP H 5 Lue Swizerld E-il : Serguei.Sekki@epl.ch Recely we hve eblihed he geerlized Li crierio equivle o he Rie hypohei viz. deored h he u over ll o-rivil Rie ucio zeroe k Σ or y rel o equl o ½ re o-egive i d oly i he Rie hypohei hold rue; rxiv:34.7895 3 Ukrii Mh. J. 66 37-383 4. A riheic ierpreio o hi geerlized Li crierio i give here.

. Iroducio I rece pper [ ] we hve eblihed he geerlized Li crierio equivle o he Rie hypohei d ir dicovered i [3] ee e.g. [4] or geerl dicuio o properie o he Rie zeucio well he cloely reled geerlized Bobieri Lgri heore cocerig he locio o zeroe o ceri cople uber ulie [5]. Nely we hve deored h he u k Σ ke over he o-rivil Rie ze-ucio zeroe kig io ccou heir ulipliciie or y rel o equl o ½ well he derivive d! dz z l ξ z z 3... or y </ re o-egive i d oly i he Rie hypohei hold rue correpodigly he e derivive whe >/ hould be o-poiive or hi; cople couge zeroe re o be pired whe uig or. We lo eblihed he relio bewee hee u d ceri derivive o he Rie i-ucio: d! dz z l ξ z z The i o hi echicl Noe i o eblih riheic ierpreio o hi e geerlized Li crierio iilr o hi h bee doe or Li crierio by Bobieri d Lgri [5]... A riheic ierpreio Our coiderio cloely ollow h o Bobieri d Lgri [5]. For uible ucio Melli ror i deied ˆ d

3 while ivere Melli ror orul i c d i Re ˆ π wih pproprie vlue o c. The ollowig i ore or le repeiio o Le ro [5] which i priculr ce correpodig o. Le. For 3 d rbirry cople uber he ivere Melli ror o he ucio k i P g i < < g i g i > where P! l ;!!! i bioil coeicie. Proo. We hve or Re>: d d d d! l! I i rbirry cople uber wih Re > or he ucio g we c pply he o clled Eplici Forul o Weil ee [5-7] which i give i [5]: Λ ~ l ~ ~ ˆ d d d γ π Here Λ i v Mgold ucio le u reid h or Re> Λ ' ς ς [4] d : ~ hu i our ce he ucio

~ P l! hould be ued wheever pproprie. erily P L l d ~ P d d L l where L L! L c. [7].! d re geerlized Lguerre polyoil [6] Thi i ey o check h he ucio g do poe he ecery properie i ee o coiuiy d ypoic i priculr or oe δ poiive δ g O or eq. o be rue [5 8 9]. Such pplicio give {! lπ γ l { d l! d l Λ l d } Now i he ecod d hird iegrl i he r.h.. o 3 we ke vrible ror o / er wh hee iegrl ke he or I l d I d 3! { } 3. l d }. The ir wo iegrl re hdled by virue o eple 4.7.6 o GR l ; Re > µ ν book []: / d Γ µ ν µ ce we ge l d! µ d Re ν >. Adopig or our l! d. 4

5 The ecod pr o he hird iegrl I 3 i by virue o eple 3.44.3 o GR book [] equl o / 3 d I γ ψ ; here....57 γ i Euler Mcheroi co d ψ i dig ucio. I he ir pr o hi iegrl we ke he vrible chge ep-: 3! l d I d e e!. Applyig Tylor epio... 6 4 e e e e we ge urher I 3 /!! ς where : ς i Hurwiz ze-ucio. Uig he relio d collecig everyhig ogeher we hve prove he ollowig heore. Theore. For 3 d rbirry cople wih Re > we hve Λ / l / l! ς π ψ 4. Thi reul w publihed i Ukrii Mheicl Jourl [].

Our ecod reul i he ollowig ior Theore. For 3 d rbirry cople i i rel we hve i i i li! i i N N i ψ / i / lπ Λ l i i N l i d i ς / i / 5. Proo. lerly or he ce i which ke plce here he δ ucio g do o hve ypoic g O ecery o pply he Weil eplici orul eq. direcly o ollowig gi Bobieri Lgri pper [5] we eed o iroduce ruced ucio g < < : g g i < g g i g i <. Their pplicio give er pproprie vrible ror i he {} brcke i eq. 3 epreio Λ l { li l d} ied o / Λ l { }. A ew vrible ror ro o / uder he iegrl ig give he epreio preeed i 5 hu o iih he proo i re o how h he relio ˆ li g g ˆ hold or he ce hd. Thi i doe by 6

verbi repeiio o he eril give i pp. 84-85 o [5]; ee lo Secio 3 o he pree pper. Equliie 4 d 5 re he riheic ierpreio we hve erched or. Now ew rerk re plce. Rerk. Reid h hould be rel or he poiiviy o u queio i equivle o he Rie hypohei. Rerk. The ce o he Theore give well kow equliy Λ ee e.g. [4] ψ / lπ. Rerk 3. For he ce we o coure recover riheic ierpreio o Li crierio give by Bobieri d Lgri Theore l. We eed u o chge d l N relio ς / ς. N d ue he quie kow Rerk 4. Ariheicl ierpreio o geerlized Li crieri or uerou oher ze-ucio ee dicuio i [ ] c be eblihed log iilr lie; c. he riheic ierpreio o Li crierio or Selberg cl i []. 3. ocludig rerk I ee iereig o lyze he poibiliy o he ue o he e pproch ivolvig he ruced ucio g o hdle he ce wih ller vlue o Re viz. / < Re <. O coure hi require oe hypohei cocerig zeroe locio. For eple we c eblih he ollowig 7

Theore 3. Aue h he Rie ucio ς i o-vihig or > where rel < < /. The or 3 d rbirry Re / cople wih > Re / δ where δ i rbirry ll ied poiive uber we hve:! ψ / lπ li N N Λ l N l ς / d 6 Proo. Le u ke uch h Re δ. Repeiio o he clculio preeed bove urihe eq. 6 o i re o how h g ˆ li g ˆ. We hve gˆ ˆ g Tl d < l d where T d i pproprie co. Furher!! l d l l.... I codiio o he heore we lwy hve Re δ > hu he cor δ ed o zero le h i er h y egive power o l. Thi ogeher wih he circuce h i he codiio o he heore he u i iie or ll [4] iihe he proo. Tkig io ccou he well-kow relio ς ' lπ ψ ς [4] bove heore how h i we ue he codiio o Theore 3 he or rbirry pproprie 8

ς ' Λ N li N ς N. Diereiio o hi equliy wih repec o redily give uber o equliie ivolvig higher order derivive d d ς ' ς d u N Λ l. Thi queio ogeher wih deiled uericl clculio will be ully coidered i epre publicio. REFERENES. Sekkii S. K. Geerlized Bobieri Lgri heore d geerlized Li crierio rxiv:34.7895 3.. Sekkii S. K. Geerlized Bobieri Lgri heore d geerlized Li crierio wih i riheic ierpreio Ukrii Mh. J. 66 4 45 43. 3. Li X.-E. The poiiviy o equece o uber d he Rie hypohei J. Nub. Theor. 65 997 35-333. 4. Tichrh E.. d Heh-Brow E. R. The heory o he Rie Ze-ucio lredo Pre Oord 988. 5. Bobieri E. Lgri J.. oplee o Li crierio or he Rie hypohei J. Nub. Theor. 77 999 74-87. 6. G. Szegö Orhogol polyoil AMS Providece R.I. 939. 7. M. W. oey Towrd veriicio o he Rie Hypohei: pplicio o he Li crierio Mh. Phy. Al. Geo. 8 5-55. 8. Weil A. Sur le orule eplicie de l héorie de obre preier i Meddelde Fr Lud Uiv. Mh. Se. dedié M. Riez 95 pp. 5-65. 9. Bobieri E. Rerk o Weil qudric uciol i he heory o prie uber I Red. M. Acc. Licei 9 83-33. 9

. Grdhei I. S. Ryzhik I. M. Tble o iegrl erie d produc. N.- Y.: Acdeic 99.. Slovic L. O Li crierio or he Rie hypohei or he Selberg cl J. Nub. Theor. 3 88-85.