Most results in this section are stated without proof.
|
|
- Trevor Scott
- 5 years ago
- Views:
Transcription
1 Leture 8 Level 4 v2 he Expliit formula. Most results in this setion are stated without proof. Reall that we have shown that ζ (s has only one pole, a simple one at s =. It has trivial zeros at the negative even integers. Any other zeros ρ lie in the ritial strip 0 Re ρ. his means that ζ (s /ζ (s has simple poles at s =, residue, and at the negative even integers and the zeros in the ritial strip with residue. Lemma For > 0 we have { ( +i y s + O y 2πi i s ds = log y if y > 0 + O ( y log y if 0 < y <. I have written the result in this way to show that the integral is an approximation to the harateristi funtion, if y > and 0 if y <. Proof Apply Cauhy s heorem to y s /s integrated around the square i, + i, U + i and U i, with U > if y > and U < 0 if 0 < y <. Estimate the ontribution from the three edges other than [ i, + i ], and then let U + or U respetively. his is similar to a result in letures: if x > 0 and > 0 then { +i x s x 2πi i s (s + ds = if x > 0 if x <, and there is a variation where the integral is trunated at ±. he Lemma is applied in the proof of heorem Perron s formula.let f (s = n= a nn s, and suppose that n= a n n σ < for all σ >. Further assume that a n A (n, where A (x > 0 is a monotonially inreasing funtion of x, and n= ( a n n σ = O (σ α,
2 as σ +, for some α > 0. hen for >, and x = N + /2 for N N, n x a n = +i ( f (s xs 2πi i s ds + O n= x ( α + O ( xa (2x log x. ( Idea of Proof Without justifying the interhange of integration and summation we have +i f (s xs 2πi i s ds = ( +i ( x s ds a n = a n + R 2πi i n s n x by the Lemma, and where ( ( x R = O a n n log x. n= his sum is split into two parts. Problems might arise from n lose to x, for then x/n is lose to and log (x/n is small. Being on the denominator means its ontribution ould be large. Notie that in demanding x = N +/2 with N N means that x/n, whih otherwise would be a problem. Nevertheless the ontribution from n with /2 x/n 2 an be bounded by by the seond error in (. he remaining terms, for n satisfying either x/n < /2 or x/n > 2, an be bounded by the first error in (. We are going to apply this to f (s = ζ (s /ζ (s in whih ase a n = Λ (n. he pole of ζ (s at s = beomes a simple pole of the logarithmi derivative ζ (s /ζ (s, i.e. ζ (s ζ (s = g (s (s, for some funtion g, holomorphi at s =. hus the α will be. Reall that Λ (n = 0 unless n = p a, when Λ (n = log p log p a = log n. herefore A (x an be hosen as log x. As in most appliation hoose = + log x for then x = x +log x = xe log x/ log x = ex. n 2
3 hus ψ (x = n x Λ (n = +i 2πi i ζ (s x s ζ (s s ds + O ( x log 2 x. Now look upon the line [ i, + i ] as the right hand vertial line of a retangle, Γ say, with orners i, + i, /2 + i and /2 i. he idea is that +i = i Γ /2+i +i /2 i /2+i i /2 i We use Cauhy s residue theorem in this losed ontour Γ to get = x x ρ ρ ζ (0 ζ (0. Γ Im ρ. he first term omes from the pole of ζ (s /ζ (s at s =, the sum from the non-trivial zeros ρ of ζ (s, and the final term from the pole of /s whih appears in the integrand. We now have to estimate the integrals over the three sides [ + i, /2 + i ], [ /2, i, i ] and [ /2 + i, /2 i ]. here is a subtle point here onerning the horizontal lines of integration, [ + i, /2 + i ] and [ /2, i, i ]. hese ross the ritial strip, 0 < Re s <. his strip ontains the ritial zeros and it is important that the lines of integration do not go over any of these zeros, for otherwise the integrand will have a pole. Definition. Let N ( = {ρ : ζ (ρ = 0, 0 < Re ρ <, 0 < Im ρ < }. he first result gives an upper bound on the number of ritial zeros. Lemma For > 0 suffiiently large N ( + N ( log. (2 Proof not given. 3
4 Note this does atually say there are any non-trivial zeros satisfying 0 < Re ρ <, < Im ρ < +. It an be shown though that for suffiiently large we have N ( = ( 2π log 2π 2π + O ( log 2. his says quite aurately that there are many ritial zeros. But (2 is suffiient for us to say that given suffiiently large we an hoose [, + ] suh that the horizontal lines Im s = and Im s = are a distane log away from any non-trivial zero. his is suffiient to give bounds on ζ (s /ζ (s that lead to the error term in heorem Expliit formula Let 2 > < x. hen ψ (x = n x Λ (n = x Im ρ x ρ ρ + O ( x log 2 x Corollary Prime Number heorem with an error term. On the Riemann Hypothesis ψ (x = x + O ( x /2 log 2 x. Proof Reall that the Riemann Hypothesis means that Re ρ = /2 for all ritial zeros. hus x ρ ρ x Re ρ = x /2 ρ ρ Im ρ Im ρ Im ρ For this sum, split Im ρ into the union of n Im ρ < n+, for n <. he first ritial zero has imaginary part approximately so we only 4
5 need n 4 in this sum. hus Im ρ ρ = = n=4 n Im ρ <n+ n=4 ρ n=4 (N (n + N (n n n n Im ρ <n+ n=4 log n n using (2 log n=4 n log2. Combining ψ (x = x + O ( x /2 log 2 ( x log 2 x + O. Simply hoose as a large power of x, i.e. x 00, to get the stated result. Results on the position of the ritial zeros are most often given in terms of the regions not ontaining zeros, i.e. the zero-free regions. So the Riemann Hypothesis is that there are no zeros in /2 < Re s <. his has not been proved; it has not even been proved that there exists δ > 0 suh that there are no zeros in /2 + δ < Re s <. Most positive results are of the form that there exists a funtion η ( 0 as + for whih is zero-free for suffiiently large. {s : η ( < Re s <, Im s < } By the methods in letures it an be shown that we may hoose η ( = log 9, for some onstant > 0, due first to Landau. With a little more work we an take η ( = log, 5
6 due to Hadamard and de la Vallee Poussin, 896. he best possible result to date is η ( = (log 2/3 (log log, /3 due to Vinogradov and Korobov, 958. Whatever the zero-free region, the expliit formula gives ψ (x = x + O ( x η( log 2 ( x log 2 x + O. (3 Here is a parameter to be hosen and we do so by equalising the two error terms, i.e. setting log 2 x η( aking logarithms, = log2 x, i.e. log2 = x η( log 2 x. log + 2 log log = η ( log x + 2 log log x. he hoie of will be suh that log log and log log x are of approximately the same size, so we demand Example he zero free region log for all suffiiently large implies ψ (x = x + O log = η ( log x. (4 < Re s <, Im s < ( ( x exp log x, for some onstant > 0 and x suffiiently large. Solution Choose to satisfy log = ( log log x, i.e. = exp log x. Here I am using the standard notation that represents a onstant that may not be the same at eah ourrene. Note that log log = log log x + log. 2 6
7 Note also that for any ε > 0 we have (take logs. hus x log 2 x log 2 x < exp ( ε log x, ( ( = O x exp log x. here is no need to look at the other error term in (3 sine we have hosen to make these terms the same size. 7
8 Problems What error terms in the Prime number heorem arise from the following zero-free regions? a Re s > /2 + δ for any fixed δ > 0? b (Hard log 9 < Re s <, Im s <? < Re s <, Im s <? (log 2/3 /3 (log log 8
Zero-Free Region for ζ(s) and PNT
Contents Zero-Free Region for ζs an PN att Rosenzweig Chebyshev heory ellin ransforms an Perron s Formula Zero-Free Region of Zeta Funtion 6. Jensen s Inequality..........................................
More informationChapter 8 Hypothesis Testing
Leture 5 for BST 63: Statistial Theory II Kui Zhang, Spring Chapter 8 Hypothesis Testing Setion 8 Introdution Definition 8 A hypothesis is a statement about a population parameter Definition 8 The two
More informationCMSC 451: Lecture 9 Greedy Approximation: Set Cover Thursday, Sep 28, 2017
CMSC 451: Leture 9 Greedy Approximation: Set Cover Thursday, Sep 28, 2017 Reading: Chapt 11 of KT and Set 54 of DPV Set Cover: An important lass of optimization problems involves overing a ertain domain,
More informationRIEMANN S FIRST PROOF OF THE ANALYTIC CONTINUATION OF ζ(s) AND L(s, χ)
RIEMANN S FIRST PROOF OF THE ANALYTIC CONTINUATION OF ζ(s AND L(s, χ FELIX RUBIN SEMINAR ON MODULAR FORMS, WINTER TERM 6 Abstrat. In this hapter, we will see a proof of the analyti ontinuation of the Riemann
More informationMethods of evaluating tests
Methods of evaluating tests Let X,, 1 Xn be i.i.d. Bernoulli( p ). Then 5 j= 1 j ( 5, ) T = X Binomial p. We test 1 H : p vs. 1 1 H : p>. We saw that a LRT is 1 if t k* φ ( x ) =. otherwise (t is the observed
More informationHankel Optimal Model Order Reduction 1
Massahusetts Institute of Tehnology Department of Eletrial Engineering and Computer Siene 6.245: MULTIVARIABLE CONTROL SYSTEMS by A. Megretski Hankel Optimal Model Order Redution 1 This leture overs both
More informationRemark 4.1 Unlike Lyapunov theorems, LaSalle s theorem does not require the function V ( x ) to be positive definite.
Leture Remark 4.1 Unlike Lyapunov theorems, LaSalle s theorem does not require the funtion V ( x ) to be positive definite. ost often, our interest will be to show that x( t) as t. For that we will need
More informationFirst, let me recall the formula I want to prove. Again, ψ is the function. ψ(x) = n<x
8.785: Analytic Number heory, MI, spring 007 (K.S. Kedlaya) von Mangoldt s formula In this unit, we derive von Mangoldt s formula estimating ψ(x) x in terms of the critical zeroes of the Riemann zeta function.
More informationSPLINE ESTIMATION OF SINGLE-INDEX MODELS
SPLINE ESIMAION OF SINGLE-INDEX MODELS Li Wang and Lijian Yang University of Georgia and Mihigan State University Supplementary Material his note ontains proofs for the main results he following two propositions
More informationComputer Science 786S - Statistical Methods in Natural Language Processing and Data Analysis Page 1
Computer Siene 786S - Statistial Methods in Natural Language Proessing and Data Analysis Page 1 Hypothesis Testing A statistial hypothesis is a statement about the nature of the distribution of a random
More informationGeneration of EM waves
Generation of EM waves Susan Lea Spring 015 1 The Green s funtion In Lorentz gauge, we obtained the wave equation: A 4π J 1 The orresponding Green s funtion for the problem satisfies the simpler differential
More informationChapter 1. Introduction to prime number theory. 1.1 The Prime Number Theorem
Chapter 1 Introduction to prime number theory 1.1 The Prime Number Theorem In the first part of this course, we focus on the theory of prime numbers. We use the following notation: we write f g as if lim
More informationRelative Maxima and Minima sections 4.3
Relative Maxima and Minima setions 4.3 Definition. By a ritial point of a funtion f we mean a point x 0 in the domain at whih either the derivative is zero or it does not exists. So, geometrially, one
More information22.54 Neutron Interactions and Applications (Spring 2004) Chapter 6 (2/24/04) Energy Transfer Kernel F(E E')
22.54 Neutron Interations and Appliations (Spring 2004) Chapter 6 (2/24/04) Energy Transfer Kernel F(E E') Referenes -- J. R. Lamarsh, Introdution to Nulear Reator Theory (Addison-Wesley, Reading, 1966),
More informationLECTURE NOTES FOR , FALL 2004
LECTURE NOTES FOR 18.155, FALL 2004 83 12. Cone support and wavefront set In disussing the singular support of a tempered distibution above, notie that singsupp(u) = only implies that u C (R n ), not as
More informationREFINED UPPER BOUNDS FOR THE LINEAR DIOPHANTINE PROBLEM OF FROBENIUS. 1. Introduction
Version of 5/2/2003 To appear in Advanes in Applied Mathematis REFINED UPPER BOUNDS FOR THE LINEAR DIOPHANTINE PROBLEM OF FROBENIUS MATTHIAS BECK AND SHELEMYAHU ZACKS Abstrat We study the Frobenius problem:
More informationMOLECULAR ORBITAL THEORY- PART I
5.6 Physial Chemistry Leture #24-25 MOLECULAR ORBITAL THEORY- PART I At this point, we have nearly ompleted our rash-ourse introdution to quantum mehanis and we re finally ready to deal with moleules.
More informationTheorem 1.1 (Prime Number Theorem, Hadamard, de la Vallée Poussin, 1896). let π(x) denote the number of primes x. Then x as x. log x.
Chapter 1 Introduction 1.1 The Prime Number Theorem In this course, we focus on the theory of prime numbers. We use the following notation: we write f( g( as if lim f(/g( = 1, and denote by log the natural
More informationmax min z i i=1 x j k s.t. j=1 x j j:i T j
AM 221: Advaned Optimization Spring 2016 Prof. Yaron Singer Leture 22 April 18th 1 Overview In this leture, we will study the pipage rounding tehnique whih is a deterministi rounding proedure that an be
More informationLECTURE 2 Geometrical Properties of Rod Cross Sections (Part 2) 1 Moments of Inertia Transformation with Parallel Transfer of Axes.
V. DEMENKO MECHNCS OF MTERLS 05 LECTURE Geometrial Properties of Rod Cross Setions (Part ) Moments of nertia Transformation with Parallel Transfer of xes. Parallel-xes Theorems S Given: a b = S = 0. z
More informationUPPER-TRUNCATED POWER LAW DISTRIBUTIONS
Fratals, Vol. 9, No. (00) 09 World Sientifi Publishing Company UPPER-TRUNCATED POWER LAW DISTRIBUTIONS STEPHEN M. BURROUGHS and SARAH F. TEBBENS College of Marine Siene, University of South Florida, St.
More informationOn zeros of cubic L-functions
Journal of Number heory 124 2007 415 428 wwwelsevierom/loate/jnt On zeros of ubi L-funtions Honggang ia Department of Mathematis, Ohio State University, Columbus, OH 43210, USA Reeived 21 July 2005; revised
More informationJournal of Inequalities in Pure and Applied Mathematics
Journal of Inequalities in Pure and Applied Mathematis A NEW ARRANGEMENT INEQUALITY MOHAMMAD JAVAHERI University of Oregon Department of Mathematis Fenton Hall, Eugene, OR 97403. EMail: javaheri@uoregon.edu
More informationMTH 142 Solution Practice for Exam 2
MTH 4 Solution Pratie for Eam Updated /7/4, 8: a.m.. (a) = 4/, hene MID() = ( + + ) +/ +6/ +/ ( 4 ) =. ( LEFT = ( 4..). =.7 and RIGHT = (.. ). =.7. Hene TRAP =.7.. (a) MID = (.49 +.48 +.9 +.98). = 4.96.
More informationNOTES ON RIEMANN S ZETA FUNCTION. Γ(z) = t z 1 e t dt
NOTES ON RIEMANN S ZETA FUNCTION DRAGAN MILIČIĆ. Gamma function.. Definition of the Gamma function. The integral Γz = t z e t dt is well-defined and defines a holomorphic function in the right half-plane
More informationThe Prime Number Theorem
he Prime Number heorem Yuuf Chebao he main purpoe of thee note i to preent a fairly readable verion of a proof of the Prime Number heorem (PN, epanded from Setion 7-8 of Davenport tet [3]. We intend to
More informationLecture 3 - Lorentz Transformations
Leture - Lorentz Transformations A Puzzle... Example A ruler is positioned perpendiular to a wall. A stik of length L flies by at speed v. It travels in front of the ruler, so that it obsures part of the
More informationAdvanced Computational Fluid Dynamics AA215A Lecture 4
Advaned Computational Fluid Dynamis AA5A Leture 4 Antony Jameson Winter Quarter,, Stanford, CA Abstrat Leture 4 overs analysis of the equations of gas dynamis Contents Analysis of the equations of gas
More informationChapter 1. Introduction to prime number theory. 1.1 The Prime Number Theorem
Chapter 1 Introduction to prime number theory 1.1 The Prime Number Theorem In the first part of this course, we focus on the theory of prime numbers. We use the following notation: we write f( g( as if
More informationLECTURE 22: MAPPING DEGREE, POINCARE DUALITY
LECTURE 22: APPING DEGREE, POINCARE DUALITY 1. The mapping degree and its appliations Let, N be n-dimensional onneted oriented manifolds, and f : N a proper map. (If is ompat, then any smooth map f : N
More informationStrauss PDEs 2e: Section Exercise 3 Page 1 of 13. u tt c 2 u xx = cos x. ( 2 t c 2 2 x)u = cos x. v = ( t c x )u
Strauss PDEs e: Setion 3.4 - Exerise 3 Page 1 of 13 Exerise 3 Solve u tt = u xx + os x, u(x, ) = sin x, u t (x, ) = 1 + x. Solution Solution by Operator Fatorization Bring u xx to the other side. Write
More informationTests of fit for symmetric variance gamma distributions
Tests of fit for symmetri variane gamma distributions Fragiadakis Kostas UADPhilEon, National and Kapodistrian University of Athens, 4 Euripidou Street, 05 59 Athens, Greee. Keywords: Variane Gamma Distribution,
More informationOrdered fields and the ultrafilter theorem
F U N D A M E N T A MATHEMATICAE 59 (999) Ordered fields and the ultrafilter theorem by R. B e r r (Dortmund), F. D e l o n (Paris) and J. S h m i d (Dortmund) Abstrat. We prove that on the basis of ZF
More informationA Characterization of Wavelet Convergence in Sobolev Spaces
A Charaterization of Wavelet Convergene in Sobolev Spaes Mark A. Kon 1 oston University Louise Arakelian Raphael Howard University Dediated to Prof. Robert Carroll on the oasion of his 70th birthday. Abstrat
More information10.2 The Occurrence of Critical Flow; Controls
10. The Ourrene of Critial Flow; Controls In addition to the type of problem in whih both q and E are initially presribed; there is a problem whih is of pratial interest: Given a value of q, what fators
More informationLecture 7: z-transform Properties, Sampling and Nyquist Sampling Theorem
EE518 Digital Signal Proessing University of Washington Autumn 21 Dept. of Eletrial Engineering ure 7: z-ransform Properties, Sampling and Nyquist Sampling heorem Ot 22, 21 Prof: J. Bilmes
More informationWavetech, LLC. Ultrafast Pulses and GVD. John O Hara Created: Dec. 6, 2013
Ultrafast Pulses and GVD John O Hara Created: De. 6, 3 Introdution This doument overs the basi onepts of group veloity dispersion (GVD) and ultrafast pulse propagation in an optial fiber. Neessarily, it
More informationLecture 7: Sampling/Projections for Least-squares Approximation, Cont. 7 Sampling/Projections for Least-squares Approximation, Cont.
Stat60/CS94: Randomized Algorithms for Matries and Data Leture 7-09/5/013 Leture 7: Sampling/Projetions for Least-squares Approximation, Cont. Leturer: Mihael Mahoney Sribe: Mihael Mahoney Warning: these
More informationRiemann Zeta Function and Prime Number Distribution
Riemann Zeta Function and Prime Number Distribution Mingrui Xu June 2, 24 Contents Introduction 2 2 Definition of zeta function and Functional Equation 2 2. Definition and Euler Product....................
More informationAppendix A Market-Power Model of Business Groups. Robert C. Feenstra Deng-Shing Huang Gary G. Hamilton Revised, November 2001
Appendix A Market-Power Model of Business Groups Roert C. Feenstra Deng-Shing Huang Gary G. Hamilton Revised, Novemer 200 Journal of Eonomi Behavior and Organization, 5, 2003, 459-485. To solve for the
More informationProduct Policy in Markets with Word-of-Mouth Communication. Technical Appendix
rodut oliy in Markets with Word-of-Mouth Communiation Tehnial Appendix August 05 Miro-Model for Inreasing Awareness In the paper, we make the assumption that awareness is inreasing in ustomer type. I.e.,
More information2. The Energy Principle in Open Channel Flows
. The Energy Priniple in Open Channel Flows. Basi Energy Equation In the one-dimensional analysis of steady open-hannel flow, the energy equation in the form of Bernoulli equation is used. Aording to this
More informationLinear Quadratic Regulator (LQR) - State Feedback Design
Linear Quadrai Regulaor (LQR) - Sae Feedbak Design A sysem is expressed in sae variable form as x = Ax + Bu n m wih x( ) R, u( ) R and he iniial ondiion x() = x A he sabilizaion problem using sae variable
More informationAppendix lecture 9: Extra terms.
Appendi lecture 9: Etra terms The Hyperolic method has een used to prove that d n = log + 2γ + O /2 n This can e used within the Convolution Method to prove Theorem There eists a constant C such that n
More informationCHBE320 LECTURE X STABILITY OF CLOSED-LOOP CONTOL SYSTEMS. Professor Dae Ryook Yang
CHBE320 LECTURE X STABILITY OF CLOSED-LOOP CONTOL SYSTEMS Professor Dae Ryook Yang Spring 208 Dept. of Chemial and Biologial Engineering 0- Road Map of the Leture X Stability of losed-loop ontrol system
More informationRouth-Hurwitz Lecture Routh-Hurwitz Stability test
ECE 35 Routh-Hurwitz Leture Routh-Hurwitz Staility test AStolp /3/6, //9, /6/ Denominator of transfer funtion or signal: s n s n s n 3 s n 3 a s a Usually of the Closed-loop transfer funtion denominator
More informationWord of Mass: The Relationship between Mass Media and Word-of-Mouth
Word of Mass: The Relationship between Mass Media and Word-of-Mouth Roman Chuhay Preliminary version Marh 6, 015 Abstrat This paper studies the optimal priing and advertising strategies of a firm in the
More informationQuasi-Monte Carlo Algorithms for unbounded, weighted integration problems
Quasi-Monte Carlo Algorithms for unbounded, weighted integration problems Jürgen Hartinger Reinhold F. Kainhofer Robert F. Tihy Department of Mathematis, Graz University of Tehnology, Steyrergasse 30,
More informationBefore giving the detailed proof, we outline our strategy. Define the functions. for Re s > 1.
Chapter 7 The Prime number theorem for arithmetic progressions 7. The Prime number theorem We denote by π( the number of primes. We prove the Prime Number Theorem. Theorem 7.. We have π( as. log Before
More informationLOGISTIC REGRESSION IN DEPRESSION CLASSIFICATION
LOGISIC REGRESSIO I DEPRESSIO CLASSIFICAIO J. Kual,. V. ran, M. Bareš KSE, FJFI, CVU v Praze PCP, CS, 3LF UK v Praze Abstrat Well nown logisti regression and the other binary response models an be used
More informationMillennium Relativity Acceleration Composition. The Relativistic Relationship between Acceleration and Uniform Motion
Millennium Relativity Aeleration Composition he Relativisti Relationship between Aeleration and niform Motion Copyright 003 Joseph A. Rybzyk Abstrat he relativisti priniples developed throughout the six
More informationThe Hanging Chain. John McCuan. January 19, 2006
The Hanging Chain John MCuan January 19, 2006 1 Introdution We onsider a hain of length L attahed to two points (a, u a and (b, u b in the plane. It is assumed that the hain hangs in the plane under a
More informationOn the Licensing of Innovations under Strategic Delegation
On the Liensing of Innovations under Strategi Delegation Judy Hsu Institute of Finanial Management Nanhua University Taiwan and X. Henry Wang Department of Eonomis University of Missouri USA Abstrat This
More informationarxiv:gr-qc/ v2 6 Feb 2004
Hubble Red Shift and the Anomalous Aeleration of Pioneer 0 and arxiv:gr-q/0402024v2 6 Feb 2004 Kostadin Trenčevski Faulty of Natural Sienes and Mathematis, P.O.Box 62, 000 Skopje, Maedonia Abstrat It this
More informationSQUARE ROOTS AND AND DIRECTIONS
SQUARE ROOS AND AND DIRECIONS We onstrut a lattie-like point set in the Eulidean plane that eluidates the relationship between the loal statistis of the frational parts of n and diretions in a shifted
More informationMAC Calculus II Summer All you need to know on partial fractions and more
MC -75-Calulus II Summer 00 ll you need to know on partial frations and more What are partial frations? following forms:.... where, α are onstants. Partial frations are frations of one of the + α, ( +
More information( ) ( ) Volumetric Properties of Pure Fluids, part 4. The generic cubic equation of state:
CE304, Spring 2004 Leture 6 Volumetri roperties of ure Fluids, part 4 The generi ubi equation of state: There are many possible equations of state (and many have been proposed) that have the same general
More informationGeometry of Transformations of Random Variables
Geometry of Transformations of Random Variables Univariate distributions We are interested in the problem of finding the distribution of Y = h(x) when the transformation h is one-to-one so that there is
More informationWave equation II: Qualitative Properties of solutions
Chapter 5 Wave equation II: Qualitative Properties of solutions In this hapter, we disuss some of the important qualitative properties of solutions to wave equation. Solutions of wave equation in one spae
More informationUTC. Engineering 329. Proportional Controller Design. Speed System. John Beverly. Green Team. John Beverly Keith Skiles John Barker.
UTC Engineering 329 Proportional Controller Design for Speed System By John Beverly Green Team John Beverly Keith Skiles John Barker 24 Mar 2006 Introdution This experiment is intended test the variable
More informationSolutions Manual. Selected odd-numbered problems in. Chapter 2. for. Proof: Introduction to Higher Mathematics. Seventh Edition
Solutions Manual Seleted odd-numbered problems in Chapter for Proof: Introdution to Higher Mathematis Seventh Edition Warren W. Esty and Norah C. Esty 5 4 3 1 Setion.1. Sentenes with One Variable Chapter
More informationR13 SET - 1 PART-A. is analytic. c) Write the test statistic for the differences of means of two large samples. about z =1.
R3 SET - II B. Teh I Semester Regular Examinations, Jan - 5 COMPLEX VARIABLES AND STATISTICAL METHODS (Eletrial and Eletronis Engineering) Time: 3 hours Max. Marks: 7 Note:. Question Paper onsists of two
More informationMASSACHUSETTS INSTITUTE OF TECHNOLOGY Physics Department Physics 8.286: The Early Universe December 21, 2013 Prof. Alan Guth QUIZ 3 SOLUTIONS
MASSACHUSETTS INSTITUTE OF TECHNOLOGY Physis Department Physis 8.286: The Early Universe Deember 2, 203 Prof. Alan Guth QUIZ 3 SOLUTIONS Quiz Date: Deember 5, 203 PROBLEM : DID YOU DO THE READING? (35
More informationA population of 50 flies is expected to double every week, leading to a function of the x
4 Setion 4.3 Logarithmi Funtions population of 50 flies is epeted to doule every week, leading to a funtion of the form f ( ) 50(), where represents the numer of weeks that have passed. When will this
More informationFundamental Theorem of Calculus
Chater 6 Fundamental Theorem of Calulus 6. Definition (Nie funtions.) I will say that a real valued funtion f defined on an interval [a, b] is a nie funtion on [a, b], if f is ontinuous on [a, b] and integrable
More informationAssessing the Performance of a BCI: A Task-Oriented Approach
Assessing the Performane of a BCI: A Task-Oriented Approah B. Dal Seno, L. Mainardi 2, M. Matteui Department of Eletronis and Information, IIT-Unit, Politenio di Milano, Italy 2 Department of Bioengineering,
More informationThe shape of a hanging chain. a project in the calculus of variations
The shape of a hanging hain a projet in the alulus of variations April 15, 218 2 Contents 1 Introdution 5 2 Analysis 7 2.1 Model............................... 7 2.2 Extremal graphs.........................
More informationRiemann s Zeta Function and the Prime Number Theorem
Riemann s Zeta Function and the Prime Number Theorem Dan Nichols nichols@math.umass.edu University of Massachusetts Dec. 7, 2016 Let s begin with the Basel problem, first posed in 1644 by Mengoli. Find
More informationA Queueing Model for Call Blending in Call Centers
A Queueing Model for Call Blending in Call Centers Sandjai Bhulai and Ger Koole Vrije Universiteit Amsterdam Faulty of Sienes De Boelelaan 1081a 1081 HV Amsterdam The Netherlands E-mail: {sbhulai, koole}@s.vu.nl
More informationModal Horn Logics Have Interpolation
Modal Horn Logis Have Interpolation Marus Kraht Department of Linguistis, UCLA PO Box 951543 405 Hilgard Avenue Los Angeles, CA 90095-1543 USA kraht@humnet.ula.de Abstrat We shall show that the polymodal
More informationTo work algebraically with exponential functions, we need to use the laws of exponents. You should
Prealulus: Exponential and Logisti Funtions Conepts: Exponential Funtions, the base e, logisti funtions, properties. Laws of Exponents memorize these laws. To work algebraially with exponential funtions,
More informationCase I: 2 users In case of 2 users, the probability of error for user 1 was earlier derived to be 2 A1
MUTLIUSER DETECTION (Letures 9 and 0) 6:33:546 Wireless Communiations Tehnologies Instrutor: Dr. Narayan Mandayam Summary By Shweta Shrivastava (shwetash@winlab.rutgers.edu) bstrat This artile ontinues
More informationarxiv: v2 [math.pr] 9 Dec 2016
Omnithermal Perfet Simulation for Multi-server Queues Stephen B. Connor 3th Deember 206 arxiv:60.0602v2 [math.pr] 9 De 206 Abstrat A number of perfet simulation algorithms for multi-server First Come First
More informationPh1c Analytic Quiz 2 Solution
Ph1 Analyti Quiz 2 olution Chefung Chan, pring 2007 Problem 1 (6 points total) A small loop of width w and height h falls with veloity v, under the influene of gravity, into a uniform magneti field B between
More informationOn Certain Singular Integral Equations Arising in the Analysis of Wellbore Recharge in Anisotropic Formations
On Certain Singular Integral Equations Arising in the Analysis of Wellbore Reharge in Anisotropi Formations C. Atkinson a, E. Sarris b, E. Gravanis b, P. Papanastasiou a Department of Mathematis, Imperial
More informationSubject: Introduction to Component Matching and Off-Design Operation % % ( (1) R T % (
16.50 Leture 0 Subjet: Introdution to Component Mathing and Off-Design Operation At this point it is well to reflet on whih of the many parameters we have introdued (like M, τ, τ t, ϑ t, f, et.) are free
More informationAfter the completion of this section the student should recall
Chapter I MTH FUNDMENTLS I. Sets, Numbers, Coordinates, Funtions ugust 30, 08 3 I. SETS, NUMERS, COORDINTES, FUNCTIONS Objetives: fter the ompletion of this setion the student should reall - the definition
More information2. Properties of Functions
2. PROPERTIES OF FUNCTIONS 111 2. Properties of Funtions 2.1. Injetions, Surjetions, an Bijetions. Definition 2.1.1. Given f : A B 1. f is one-to-one (short han is 1 1) or injetive if preimages are unique.
More informationLecture 1: Small Prime Gaps: From the Riemann Zeta-Function and Pair Correlation to the Circle Method. Daniel Goldston
Lecture 1: Small Prime Gaps: From the Riemann Zeta-Function and Pair Correlation to the Circle Method Daniel Goldston π(x): The number of primes x. The prime number theorem: π(x) x log x, as x. The average
More information4. (12) Write out an equation for Poynting s theorem in differential form. Explain in words what each term means physically.
Eletrodynamis I Exam 3 - Part A - Closed Book KSU 205/2/8 Name Eletrodynami Sore = 24 / 24 points Instrutions: Use SI units. Where appropriate, define all variables or symbols you use, in words. Try to
More informationHarmonic sets and the harmonic prime number theorem
Harmonic sets and the harmonic prime number theorem Version: 9th September 2004 Kevin A. Broughan and Rory J. Casey University of Waikato, Hamilton, New Zealand E-mail: kab@waikato.ac.nz We restrict primes
More informationMath 213b (Spring 2005) Yum-Tong Siu 1. Explicit Formula for Logarithmic Derivative of Riemann Zeta Function
Math 3b Sprig 005 Yum-og Siu Expliit Formula for Logarithmi Derivative of Riema Zeta Futio he expliit formula for the logarithmi derivative of the Riema zeta futio i the appliatio to it of the Perro formula
More informationWhere as discussed previously we interpret solutions to this partial differential equation in the weak sense: b
Consider the pure initial value problem for a homogeneous system of onservation laws with no soure terms in one spae dimension: Where as disussed previously we interpret solutions to this partial differential
More informationSOME MEAN VALUE THEOREMS FOR THE RIEMANN ZETA-FUNCTION AND DIRICHLET L-FUNCTIONS D.A. KAPTAN, Y. KARABULUT, C.Y. YILDIRIM 1.
SOME MEAN VAUE HEOREMS FOR HE RIEMANN ZEA-FUNCION AND DIRICHE -FUNCIONS D.A. KAPAN Y. KARABUU C.Y. YIDIRIM Dedicated to Professor Akio Fujii on the occasion of his retirement 1. INRODUCION he theory of
More informationMath 32B Review Sheet
Review heet Tau Beta Pi - Boelter 6266 Contents ouble Integrals 2. Changing order of integration.................................... 4.2 Integrating over more general domains...............................
More informationLearning to model sequences generated by switching distributions
earning to model sequenes generated by swithing distributions Yoav Freund A Bell abs 00 Mountain Ave Murray Hill NJ USA Dana on omputer Siene nstitute Hebrew University Jerusalem srael Abstrat We study
More informationF = F x x + F y. y + F z
ECTION 6: etor Calulus MATH20411 You met vetors in the first year. etor alulus is essentially alulus on vetors. We will need to differentiate vetors and perform integrals involving vetors. In partiular,
More informationPlanning with Uncertainty in Position: an Optimal Planner
Planning with Unertainty in Position: an Optimal Planner Juan Pablo Gonzalez Anthony (Tony) Stentz CMU-RI -TR-04-63 The Robotis Institute Carnegie Mellon University Pittsburgh, Pennsylvania 15213 Otober
More informationAcoustic Waves in a Duct
Aousti Waves in a Dut 1 One-Dimensional Waves The one-dimensional wave approximation is valid when the wavelength λ is muh larger than the diameter of the dut D, λ D. The aousti pressure disturbane p is
More informationThe Prime Number Theorem
The Prime Number Theorem We study the distribution of primes via the function π(x) = the number of primes x 6 5 4 3 2 2 3 4 5 6 7 8 9 0 2 3 4 5 2 It s easier to draw this way: π(x) = the number of primes
More informationEECS 120 Signals & Systems University of California, Berkeley: Fall 2005 Gastpar November 16, Solutions to Exam 2
EECS 0 Signals & Systems University of California, Berkeley: Fall 005 Gastpar November 6, 005 Solutions to Exam Last name First name SID You have hour and 45 minutes to omplete this exam. he exam is losed-book
More informationBeams on Elastic Foundation
Professor Terje Haukaas University of British Columbia, Vanouver www.inrisk.ub.a Beams on Elasti Foundation Beams on elasti foundation, suh as that in Figure 1, appear in building foundations, floating
More informationSingular Event Detection
Singular Event Detetion Rafael S. Garía Eletrial Engineering University of Puerto Rio at Mayagüez Rafael.Garia@ee.uprm.edu Faulty Mentor: S. Shankar Sastry Researh Supervisor: Jonathan Sprinkle Graduate
More informationLong time stability of regularized PML wave equations
Long time stability of regularized PML wave equations Dojin Kim Email:kimdojin@knu.a.kr Yonghyeon Jeon Email:dydgus@knu.a.kr Philsu Kim Email:kimps@knu.a.kr Abstrat In this paper, we onsider two dimensional
More informationEXPERIMENTAL INVESTIGATION OF CRITICAL STRAIN FOR VISCOPLASTIC MATERIALS WITH DIFFERENT GEOMETRIES AND RHEOMETERS
EXPERIMENTAL INVESTIGATION OF CRITICAL STRAIN FOR VISCOPLASTIC MATERIALS WITH DIFFERENT GEOMETRIES AND RHEOMETERS Guilherme A. S. Balvedi, 2 Diogo E. V. Andrade, 3 Admilson T. Frano e 3 Cezar O. R. Negrão
More informationn n=1 (air) n 1 sin 2 r =
Physis 55 Fall 7 Homework Assignment #11 Solutions Textbook problems: Ch. 7: 7.3, 7.4, 7.6, 7.8 7.3 Two plane semi-infinite slabs of the same uniform, isotropi, nonpermeable, lossless dieletri with index
More informationTail-robust Scheduling via Limited Processor Sharing
Performane Evaluation Performane Evaluation 00 200) 22 Tail-robust Sheduling via Limited Proessor Sharing Jayakrishnan Nair a, Adam Wierman b, Bert Zwart a Department of Eletrial Engineering, California
More informationCoefficients of the Inverse of Strongly Starlike Functions
BULLETIN of the MALAYSIAN MATHEMATICAL SCIENCES SOCIETY Bull. Malaysian Math. S. So. (Seond Series) 6 (00) 6 7 Coeffiients of the Inverse of Strongly Starlie Funtions ROSIHAN M. ALI Shool of Mathematial
More informationarxiv:physics/ v1 14 May 2002
arxiv:physis/0205041 v1 14 May 2002 REPLY TO CRITICISM OF NECESSITY OF SIMULTANEOUS CO-EXISTENCE OF INSTANTANEOUS AND RETARDED INTERACTIONS IN CLASSICAL ELECTRODYNAMICS by J.D.Jakson ANDREW E. CHUBYKALO
More informationFinal Review. A Puzzle... Special Relativity. Direction of the Force. Moving at the Speed of Light
Final Review A Puzzle... Diretion of the Fore A point harge q is loated a fixed height h above an infinite horizontal onduting plane. Another point harge q is loated a height z (with z > h) above the plane.
More information