Demonstration of Riemann Hypothesis
|
|
- Lorin Manning
- 5 years ago
- Views:
Transcription
1 Demontration of Riemann Hypothei Diego arin June 2, 204 Abtract We define an infinite ummation which i proportional to the revere of Riemann Zeta function ζ(). Then we demontrate that uch function can have ingularitie only for Re = /n with n N \ 0. Finally, uing the functional equation, we reduce thee poibilitie to the only Re = /2. dmarin.math@gmail.com
2 Content Target 3 2 Strategy 4 3 Application of the Euler-acLaurin formula 5 4 Calculating the limiting function 3 2
3 Target Riemann hypothei, propoed by Bernhard Riemann in the 859, i a conjecture that regard an apparently imple function of complex variable. Such function, called Riemann Zeta Function, i defined for Re > via the following ummation ζ() = n For every integer n, an unique decompoition a product of (power of) prime number exit. In thi way ζ() = + p=2 j=0 n= p j = + p=2 p where we have ued the ummation rule for the geometric erie j= w j = w for w <. Riemann Zeta function can t have zero in the convergence area, becaue no term in the product can be equal to zero. Neverthele an holomorphic extenion of ζ() can be defined over the entire complex plane C, with the exception of =. Such extenion ha infinite zero correponding to all negative even integer; that i, ζ() = 0 when i one of 2, 4, 6,.... Thee are the o-called trivial zero. Again for the holomorphic extenion, for we can prove the functional equation ζ() = 2 π in ( π ) Γ( )ζ( ) 2 The firt proof wa given by Bernhard Riemann in the 0-page paper Ueber die Anzahl der Primzahlen unter einer gegebenen Gre (uual Englih tranlation: On the Number of Prime Le Than a Given agnitude) publihed in the November 859 edition by onatberichte der Kniglich Preuichen Akademie der Wienchaften zu Berlin. 3
4 Leaving out the zero of in ( ) π 2 which aren t pole of Γ( ), i.e. for = 2n, n N, any other zero 0 mut have a mate zero 0 = 0. Becaue there are no zero for Re >, functional equation implie that there are no zero alo for Re < 0 (except for = 2n). Other work have excluded alo the preence of zero for Re = 0 and Re =. A conequence, all the non trivial zero of ζ() tay in the critical trip 0 < Re <. Riemann hypothei conjecture that all the non-trivial zero have real part equal to. Thi i what we aim to demontrate in the following. 2 2 Strategy We tart from the definition of ζ() a an infinite product of term, one term for every prime number p, running from 2 to + : ζ() = + p=2 p () The product converge for Re >. From here we fix = x + iy with C and x, y R. So the convergence condition i x >. Out of convergence area, ζ() i defined via holomorphic extenion. The derivative of a ingle term in the product () give d d p = ( p ) (log p 2 p ) = p log p p Hence the derivative ζ () of ζ() reult ζ () = d d ζ() = + p=2 p log p p p =2 and then ζ + () ζ() = log p p 4 p=2 (2)
5 For briefne we et C() = ζ (). The um (2) converge for x >. Otherwie we ζ() define C() a the holomorphic extenion of (2), recognizing it by the label H.e. : C() = H.e. n= log p n p n The uniquene of the holomorphic extenion enure that C() = ζ () ζ() x. At thi point we rely upon the following evidence: alo for Any ingularity of C() correpond to a zero of ζ() and/or to a ingularity of ζ (). We can exclude that a zero of ζ () hide a zero of ζ(): in fact, for any holomorphic function f(), if a point 0 exit which i a zero both for f() and f (), we have urely f( 0 ) f ( 0 ) = lim 0 k= f k( 0 ) k k= kf = lim k( 0 ) k 0 fˆk( 0 )ˆk ˆkfˆk( 0 )ˆk = lim 0 0 ˆk = 0 where ˆk i the minor k for which a Taylor coefficient f k i 0. Hence the zero of ζ() are ingularitie for C() alo when they are zero of both ζ() and ζ (). For thi reaon we ll proceed with finding an enemble of point which include all the ingularitie of C() and o, among them, all the zero of ζ(). 3 Application of the Euler-acLaurin formula We move from prime to integer number: C() = n= log p n p n (3) 5
6 where p n i the n-th prime number. For 0, no partial um C () = n= log p n p n with < + ha ingularitie. Hence, any function C () = n= log p n p n ha the ame ingularitie of C() for 0. Thi permit u to work with C () in place of C(), in uch a way to exploit the freedom in chooing. Conider now the Euler-acLaurin theorem at leading order: N f(l, ) l= N F N () = f(w, )dw F N () R + N dw d f(w, ) dw for ome f(w, a) analytic in w R and holomorphic in C except at mot for iolated point, provided that in uch point we have w / N. Conider now lim N F N ()! = F (). If F () exit (i finite) in a open et x > A (with A ome real number) except at mot for iolated point, then the Dominated Convergence Theorem enure (for x > A) that N lim f(l, ) N l= N f(w, )dw F () (4) Now it i poible that the um and the integral in the left ide converge only for x > B with B > A. For A < x B we can eparate the holomorphic extenion of 6
7 the ummation (H.e.) from it divergent piece (D.p.): f(l, ) = H.e. l= We can do the ame for the integral: f(w, )dw = H.e. Inerting them in (4) we obtain: f(l, ) + D.p. l= H.e. f(l, ) + D.p. f(l, ) H.e. l= l= f(l, ) l= f(w, )dw + D.p. f(w, )dw D.p. f(w, )dw Being F () finite (except for iolated point), it ha to be true and o for A < x B. D.p. f(l, ) = D.p. l= H.e. f(l, ) H.e. l= f(w, )dw f(w, )dw F () f(w, )dw F () Hence we can apply the Euler-aclaurin formula not only for a comparion between um and integral, but alo between their holomorphic extenion, at leat until F () i finite. Our cae i n= log p n p n log p(t) dt p(t) F () Here p(t) i any analytic function which poe analytic invere t(p) and atifie 7
8 p(n) = p n. oreover dt d log p(t) dt p(t) [ dt dp(t) dt p(t)(p(t) ) p(t) log p(t) (p(t) ) 2 ] (5) The right ide converge for x > 0 with the exception of iolated point. The function t(p n ) return the cardinality n of the prime number p n. Thi i equivalent to return how many prime number exit that are le than or equal to p n, i.e. t(p) = π(p), where π(p) i the prime-counting function. A holomorphic definition wa given by Rieel, Edward and Derbyhire 2 : For p + we have π(p) = π (p) = lim T + lim T + 2+iT 2πi 2 it p log ζ()d 2+iT p log ζ()d 2πi 2 it π(p) π (p) = dπ(p) dp p log p ( ) log p log p log p Before going any further, we prove that (the holomorphic extenion of) the integral in, H.e. p dp dt(p) dp log p p = H.e. p dp π (p) log p p, (6) 2 Rieel, H. The Riemann Prime Number Formula Prime Number and Computer ethod for Factorization, 2nd ed. Boton, A: Birkhuer, pp , 994; Edward, H.. Riemann Zeta Function. New York: Dover, 200; Derbyhire, J. Prime Obeion: Bernhard Riemann and the Greatet Unolved Problem in athematic. New York: Penguin,
9 9
10 ha no ingularitie. We introduce firt a redefinition of the ame integral which permit to calculate it alo for x. Thi i dp π 2i in(π) Cε log p ( p) (p), (7) p which i equivalent to (6) for x >, o giving the relative holomorphic extenion. The Cauchy principle enure that integral maintain the ame value for every choice of ε (until the path doen t touch any pole of the integrated function); for demontration we find ueful to work in the limit ε 0 +. The contribute at i null for x >. Thi i unique zone of interet to check the equivalence between (6) and (7); o, at thi aim, we can forget about it. log p ( p) lim p + π (p) = 0 for x > p Having aid thi, we proceed by calculating eparately the contribute to the integral along Γ, Γ 3 and Γ 2 : Γ [ ] = lim ε 0 + p = e iπ dp π (p) p = e iπ p dt π (t + iε) log(t + iε) e log(t+iε)+iπ e log(t+iε) log p p p dp π (p) log p p Γ 3 [ ] = lim ε 0 + p + = e iπ dp π (p) p = e iπ p dt π log(t iε) iπ log(t iε) e (t iε) e log(t iε) log p p p dp π (p) log p p 0
11 For the integral in Γ 2, we poe p = εe iθ + p, dp = iεe iθ dθ, Γ 2 [ ] = lim 3π 4 ε 0 = lim ε 0 iε 3π 4 3π 4 dθ π (εe iθ + p ) log(εe iθ + p )(εe iθ + p ) e iπ iεe iθ (εe iθ + p ) 3π 4 dθ π (p ) log(p )(p ) e iπ e iθ (p ) = lim iε π (p ) log(p )e iπ ε 0 p = lim ε π (p ) log(p )e iπ [ ε 0 p = lim ε 0 iε 3π 4 3π 4 dθ e iθ e i 3π 4 e i 3π 4 2 π (p ) log(p )e iπ p = 0 ] In the end: dp π 2i in(π) Cε log p ( p) (p) = p = = = [ [ ] + 2i in(π) Γ 2i in(π) ] [ ] + [ ] Γ 2 Γ 3 ( e iπ e iπ) dp π (p) log p p 2i in(π) 2i in(π) p dp π (p) log p p p + p dp π (p) log p p CVD. At thi tage we can doubtle affirm that (7) i the holomorphic extenion of (6). Uing the Cauchy integral theorem, the integral in (7) can be tranformed into a um over the minimal circuitation around all the pole. Thee it at p = exp ( ) 2πik, k Z. A ingle term i the following: (k) iε in(π) [ ] = lim ε 0 + 2i 2π 0 e iθ dθ π (e 2πik + εe iθ ) 2πik log(e + εe iθ ) (e 2πik + εe iθ ) eiπ = ε = lim ε π 0 e iθ dθ π (e 2πik + εe iθ ) 2πik log( + εeiθ ) + 2πk e 2πik 2πik iθ ( + εe ) eiπ =
12 ε = lim ε π 0 e iθ dθ π (e 2πik ε = lim ε π By umming over all the pole: in(π) H.e. p 0 + εe iθ ) e iθ dθ π (e 2πik = lim ε π 2πik log( + εeiθ ) + 2πk 2πik iθ ( + εe ) 2πik + εe iθ εeiθ ) e iθ dθ π (e 2πik + 2πk 2πik iθ εe 2πk ) 2πik iθ 0 e = πk 2π 2 π (e 2πik )e 2πik +iπ = 2π2 k 2 dp π (p) log p p = eiπ = π 2 eiπ log ζ(2 + iw)dw = π 2 eiπ log ζ(2 + iw)dw Ue now the ummation rule k= k= = e iπ + k= k= k= ke ka = d e ka = d [ ] da da e a k= π (e 2πik 2π 2 k 2 2π 2 k 2 0 )e 2πik +iπ e iπ = e iπ = e iπ = dθ = π (e 2πik )e 2πki π (e 2πik )e 2πik 2 ke 2πik(+iw) 2 e 2πik 2 [ k = e 2πik(2+iw) 2 ] e 2πik(2+iw) 2 e a ( e a ) = 2 (e a/2 e a/2 ) 2 The lat term in the right i the correct value of ummation only for Re a < 0. Neverthele, when we climb over the line Re a = 0, it give the correponding holomorphic extenion. Hence we can ue the rule without care of convergence 2
13 criterium: = π 2 eiπ log ζ(2 + iw)dw (e πi(2+iw) 2 e πi(2+iw) 2 ) 2 For w + the integrand goe like π 2 eiπ log ζ(2 + iw) e 2πw 2 and o the integral converge at + (remember that Re = x > 0). Similarly, for w the integrand goe like π 2 eiπ log ζ(2 + iw) e 2πw 2 and o the integral converge at. Being know that ζ(2 + iw) ha neither zero nor pole for w R, we can ay that (the Holomorphic Extenion of) the integral in ha no ingularitie for C \ R. The inecapable concluion i that all ingularitie of C() in the critical trip emerge from the difference between it and the correponding integral, i.e. they are among the iolated point where F () = +. 4 Calculating the limiting function Let recover the reult (5): dt dp(t) dt dt dp(t) dt [ p(t)(p(t) ) p(t) log p(t) (p(t) ) 2 I t [ ] dt dp(t) dt ] ] [ I t ] [ where I t = if dp(t) dt 0 and I t = 0 otherwie. Ue now dt dp(t) dt = dp to achieve an 3
14 advantageou change of variable: p + p p p [ ] dp I t(p) dp [ I t(p) ] [ ] p [ ] dp I t(p) + dp [ I t(p) ] [ ] p [ ] dp p(p ) p log p (p ) 2 dp p p log p p(p ) 2 Now conider the following inequality: p 2 = (p )(p ) = p + p p + = p 2x 2p x co(y log p) + p 2x 2p x + = (p x ) 2 For x > 0 we have alo p p log p 2 = (p p log p)(p p log p) = p 2x 2p x co(y log p) + 2xp 2x log p + 2xp x log p co(y log p) 2yp x log p in(y log p) + 2 p 2x 2 log 2 p p 2x + 2p x + + 2xp 2x log p + 2xp x log p + +2 y p x log p + (x 2 + y 2 )p 2x 2 log 2 p 4
15 p 2x + 2p x + + 2xp 2x log p + 2xp x log p + +2 y p x log p + (x 2 + y 2 )p 2x 2 log 2 p + +2x y p 2x 2 log 2 p + 2 y p 2x log p = = (p x + + (x + y )p x log p) 2 Hence p dp px + + (x + y )p x log p p(p x ) 2 2 x( p x ) log( p x ) x (x+ y ) log p((px )Φ ( px,, ) +x) x x 2 p(p x ) p Φ(w, a, b) i the Lerch Trancendent 3 which goe at + in the firt variable a w ; in our cae a p x. A conequence, the contribute at + i null. Finally 2 log( p x + x(p x ) x ) + (x+ y ) log p((px )Φ( p x,, ) x +x) x 2 p (p x ) The Lerch Trancendent Φ(w, a, b) ha ingularitie (if a N\0) only for b N\0. In our cae, a = and o we have ingularitie for x = n with n N \ 0 Thi mean that the zero of ζ() in the trip 0 < x < have to atify x = n for ome n N \ 0. oreover the functional equation ζ() = 2 π in ( π ) Γ( )ζ( ) 2 reveal that if 0 i a non-trivial zero, then 0 i a zero too. Hence we earch 3 Φ(w, a, b) i uually defined a the holomorphic extenion of Φ(w, a, b) = + t a e bt Γ(w) 0 we dt t which work for {Re b > 0 Re a > 0 w < } {Re b > 0 Re a > w = }. 5
16 for two integer m, n uch that m = n, but the unique olution of thi equation i m = n = 2. non-trivial zero of zeta mut have real part equal to /2. CVD Conequently, all the 6
Riemann s Functional Equation is Not Valid and its Implication on the Riemann Hypothesis. Armando M. Evangelista Jr.
Riemann Functional Equation i Not Valid and it Implication on the Riemann Hypothei By Armando M. Evangelita Jr. On November 4, 28 ABSTRACT Riemann functional equation wa formulated by Riemann that uppoedly
More informationRiemann s Functional Equation is Not a Valid Function and Its Implication on the Riemann Hypothesis. Armando M. Evangelista Jr.
Riemann Functional Equation i Not a Valid Function and It Implication on the Riemann Hypothei By Armando M. Evangelita Jr. armando78973@gmail.com On Augut 28, 28 ABSTRACT Riemann functional equation wa
More informationLecture 3. January 9, 2018
Lecture 3 January 9, 208 Some complex analyi Although you might have never taken a complex analyi coure, you perhap till know what a complex number i. It i a number of the form z = x + iy, where x and
More informationLecture 17: Analytic Functions and Integrals (See Chapter 14 in Boas)
Lecture 7: Analytic Function and Integral (See Chapter 4 in Boa) Thi i a good point to take a brief detour and expand on our previou dicuion of complex variable and complex function of complex variable.
More informationProof of Bernhard Riemann s Functional Equation using Gamma Function
Journal of Mathematic and Statitic 4 (3): 8-85, 8 ISS 549-3644 8 Science Publication Proof of Bernhard Riemann Functional Equation uing Gamma Function Mbaïtiga Zacharie Department of Media Information
More informationChapter 4. The Laplace Transform Method
Chapter 4. The Laplace Tranform Method The Laplace Tranform i a tranformation, meaning that it change a function into a new function. Actually, it i a linear tranformation, becaue it convert a linear combination
More information6 Global definition of Riemann Zeta, and generalization of related coefficients. p + p >1 (1.1)
6 Global definition of Riemann Zeta, and generalization of related coefficient 6. Patchy definition of Riemann Zeta Let' review the definition of Riemann Zeta. 6.. The definition by Euler The very beginning
More information7.2 INVERSE TRANSFORMS AND TRANSFORMS OF DERIVATIVES 281
72 INVERSE TRANSFORMS AND TRANSFORMS OF DERIVATIVES 28 and i 2 Show how Euler formula (page 33) can then be ued to deduce the reult a ( a) 2 b 2 {e at co bt} {e at in bt} b ( a) 2 b 2 5 Under what condition
More informationLecture 8: Period Finding: Simon s Problem over Z N
Quantum Computation (CMU 8-859BB, Fall 205) Lecture 8: Period Finding: Simon Problem over Z October 5, 205 Lecturer: John Wright Scribe: icola Rech Problem A mentioned previouly, period finding i a rephraing
More informationLaplace Transformation
Univerity of Technology Electromechanical Department Energy Branch Advance Mathematic Laplace Tranformation nd Cla Lecture 6 Page of 7 Laplace Tranformation Definition Suppoe that f(t) i a piecewie continuou
More informationThe machines in the exercise work as follows:
Tik-79.148 Spring 2001 Introduction to Theoretical Computer Science Tutorial 9 Solution to Demontration Exercie 4. Contructing a complex Turing machine can be very laboriou. With the help of machine chema
More informationThe Riemann Transform
The Riemann Tranform By Armando M. Evangelita Jr. armando78973@gmail.com Augut 28, 28 ABSTRACT In hi 859 paper, Bernhard Riemann ued the integral equation f (x ) x dx to develop an explicit formula for
More informationAn introduction to the Riemann hypothesis
An introduction to the Riemann hypothei Author: Alexander Bielik abielik@kth.e Supervior: Pär Kurlberg SA4X Degree Project in Engineering Phyic Royal Intitute of Technology KTH Department of Mathematic
More informationarxiv: v2 [math.nt] 30 Apr 2015
A THEOREM FOR DISTINCT ZEROS OF L-FUNCTIONS École Normale Supérieure arxiv:54.6556v [math.nt] 3 Apr 5 943 Cachan November 9, 7 Abtract In thi paper, we etablih a imple criterion for two L-function L and
More informationSingular perturbation theory
Singular perturbation theory Marc R. Rouel June 21, 2004 1 Introduction When we apply the teady-tate approximation (SSA) in chemical kinetic, we typically argue that ome of the intermediate are highly
More informationCoordinate independence of quantum-mechanical q, qq. path integrals. H. Kleinert ), A. Chervyakov Introduction
vvv Phyic Letter A 10045 000 xxx www.elevier.nlrlocaterpla Coordinate independence of quantum-mechanical q, qq path integral. Kleinert ), A. Chervyakov 1 Freie UniÕeritat Berlin, Intitut fur Theoretiche
More information1. Preliminaries. In [8] the following odd looking integral evaluation is obtained.
June, 5. Revied Augut 8th, 5. VA DER POL EXPASIOS OF L-SERIES David Borwein* and Jonathan Borwein Abtract. We provide concie erie repreentation for variou L-erie integral. Different technique are needed
More informationLecture 21. The Lovasz splitting-off lemma Topics in Combinatorial Optimization April 29th, 2004
18.997 Topic in Combinatorial Optimization April 29th, 2004 Lecture 21 Lecturer: Michel X. Goeman Scribe: Mohammad Mahdian 1 The Lovaz plitting-off lemma Lovaz plitting-off lemma tate the following. Theorem
More informationHELICAL TUBES TOUCHING ONE ANOTHER OR THEMSELVES
15 TH INTERNATIONAL CONFERENCE ON GEOMETRY AND GRAPHICS 0 ISGG 1-5 AUGUST, 0, MONTREAL, CANADA HELICAL TUBES TOUCHING ONE ANOTHER OR THEMSELVES Peter MAYRHOFER and Dominic WALTER The Univerity of Innbruck,
More informationDIFFERENTIAL EQUATIONS
DIFFERENTIAL EQUATIONS Laplace Tranform Paul Dawkin Table of Content Preface... Laplace Tranform... Introduction... The Definition... 5 Laplace Tranform... 9 Invere Laplace Tranform... Step Function...4
More informationON ASYMPTOTIC FORMULA OF THE PARTITION FUNCTION p A (n)
#A2 INTEGERS 15 (2015) ON ASYMPTOTIC FORMULA OF THE PARTITION FUNCTION p A (n) A David Chritopher Department of Mathematic, The American College, Tamilnadu, India davchrame@yahoocoin M Davamani Chritober
More informationTRIPLE SOLUTIONS FOR THE ONE-DIMENSIONAL
GLASNIK MATEMATIČKI Vol. 38583, 73 84 TRIPLE SOLUTIONS FOR THE ONE-DIMENSIONAL p-laplacian Haihen Lü, Donal O Regan and Ravi P. Agarwal Academy of Mathematic and Sytem Science, Beijing, China, National
More informationMoment of Inertia of an Equilateral Triangle with Pivot at one Vertex
oment of nertia of an Equilateral Triangle with Pivot at one Vertex There are two wa (at leat) to derive the expreion f an equilateral triangle that i rotated about one vertex, and ll how ou both here.
More informationSOME RESULTS ON INFINITE POWER TOWERS
NNTDM 16 2010) 3, 18-24 SOME RESULTS ON INFINITE POWER TOWERS Mladen Vailev - Miana 5, V. Hugo Str., Sofia 1124, Bulgaria E-mail:miana@abv.bg Abtract To my friend Kratyu Gumnerov In the paper the infinite
More informationPythagorean Triple Updated 08--5 Drlnoordzij@leennoordzijnl wwwleennoordzijme Content A Roadmap for generating Pythagorean Triple Pythagorean Triple 3 Dicuion Concluion 5 A Roadmap for generating Pythagorean
More informationLecture 15 - Current. A Puzzle... Advanced Section: Image Charge for Spheres. Image Charge for a Grounded Spherical Shell
Lecture 15 - Current Puzzle... Suppoe an infinite grounded conducting plane lie at z = 0. charge q i located at a height h above the conducting plane. Show in three different way that the potential below
More informationLaplace Adomian Decomposition Method for Solving the Nonlinear Volterra Integral Equation with Weakly Kernels
Studie in Nonlinear Science (4): 9-4, ISSN -9 IDOSI Publication, Laplace Adomian Decompoition Method for Solving the Nonlinear Volterra Integral Equation with Weakly Kernel F.A. Hendi Department of Mathematic
More informationRiemann Paper (1859) Is False
Riemann Paper (859) I Fale Chun-Xuan Jiang P O Box94, Beijing 00854, China Jiangchunxuan@vipohucom Abtract In 859 Riemann defined the zeta function ζ () From Gamma function he derived the zeta function
More informationWeber Schafheitlin-type integrals with exponent 1
Integral Tranform and Special Function Vol., No., February 9, 47 53 Weber Schafheitlin-type integral with exponent Johanne Kellendonk* and Serge Richard Univerité de Lyon, Univerité Lyon, Intitut Camille
More informationBogoliubov Transformation in Classical Mechanics
Bogoliubov Tranformation in Claical Mechanic Canonical Tranformation Suppoe we have a et of complex canonical variable, {a j }, and would like to conider another et of variable, {b }, b b ({a j }). How
More informationCodes Correcting Two Deletions
1 Code Correcting Two Deletion Ryan Gabry and Frederic Sala Spawar Sytem Center Univerity of California, Lo Angele ryan.gabry@navy.mil fredala@ucla.edu Abtract In thi work, we invetigate the problem of
More informationChapter 2 Sampling and Quantization. In order to investigate sampling and quantization, the difference between analog
Chapter Sampling and Quantization.1 Analog and Digital Signal In order to invetigate ampling and quantization, the difference between analog and digital ignal mut be undertood. Analog ignal conit of continuou
More informationWeek 3 Statistics for bioinformatics and escience
Week 3 Statitic for bioinformatic and escience Line Skotte 28. november 2008 2.9.3-4) In thi eercie we conider microrna data from Human and Moue. The data et repreent 685 independent realiation of the
More informationProblem Set 8 Solutions
Deign and Analyi of Algorithm April 29, 2015 Maachuett Intitute of Technology 6.046J/18.410J Prof. Erik Demaine, Srini Devada, and Nancy Lynch Problem Set 8 Solution Problem Set 8 Solution Thi problem
More informationMath 201 Lecture 17: Discontinuous and Periodic Functions
Math 2 Lecture 7: Dicontinuou and Periodic Function Feb. 5, 22 Many example here are taken from the textbook. he firt number in () refer to the problem number in the UA Cutom edition, the econd number
More informationLecture 9: Shor s Algorithm
Quantum Computation (CMU 8-859BB, Fall 05) Lecture 9: Shor Algorithm October 7, 05 Lecturer: Ryan O Donnell Scribe: Sidhanth Mohanty Overview Let u recall the period finding problem that wa et up a a function
More informationSampling and the Discrete Fourier Transform
Sampling and the Dicrete Fourier Tranform Sampling Method Sampling i mot commonly done with two device, the ample-and-hold (S/H) and the analog-to-digital-converter (ADC) The S/H acquire a CT ignal at
More informationThe statistical properties of the primordial fluctuations
The tatitical propertie of the primordial fluctuation Lecturer: Prof. Paolo Creminelli Trancriber: Alexander Chen July 5, 0 Content Lecture Lecture 4 3 Lecture 3 6 Primordial Fluctuation Lecture Lecture
More informationReading assignment: In this chapter we will cover Sections Definition and the Laplace transform of simple functions
Chapter 4 Laplace Tranform 4 Introduction Reading aignment: In thi chapter we will cover Section 4 45 4 Definition and the Laplace tranform of imple function Given f, a function of time, with value f(t
More informationLecture 7: Testing Distributions
CSE 5: Sublinear (and Streaming) Algorithm Spring 014 Lecture 7: Teting Ditribution April 1, 014 Lecturer: Paul Beame Scribe: Paul Beame 1 Teting Uniformity of Ditribution We return today to property teting
More informationApproximate Analytical Solution for Quadratic Riccati Differential Equation
Iranian J. of Numerical Analyi and Optimization Vol 3, No. 2, 2013), pp 21-31 Approximate Analytical Solution for Quadratic Riccati Differential Equation H. Aminikhah Abtract In thi paper, we introduce
More informationAn Inequality for Nonnegative Matrices and the Inverse Eigenvalue Problem
An Inequality for Nonnegative Matrice and the Invere Eigenvalue Problem Robert Ream Program in Mathematical Science The Univerity of Texa at Dalla Box 83688, Richardon, Texa 7583-688 Abtract We preent
More informationLong-term returns in stochastic interest rate models
Long-term return in tochatic interet rate model G. Deeltra F. Delbaen Vrije Univeriteit Bruel Departement Wikunde Abtract In thi paper, we oberve the convergence of the long-term return, uing an extenion
More information1. The F-test for Equality of Two Variances
. The F-tet for Equality of Two Variance Previouly we've learned how to tet whether two population mean are equal, uing data from two independent ample. We can alo tet whether two population variance are
More informationON THE APPROXIMATION ERROR IN HIGH DIMENSIONAL MODEL REPRESENTATION. Xiaoqun Wang
Proceeding of the 2008 Winter Simulation Conference S. J. Maon, R. R. Hill, L. Mönch, O. Roe, T. Jefferon, J. W. Fowler ed. ON THE APPROXIMATION ERROR IN HIGH DIMENSIONAL MODEL REPRESENTATION Xiaoqun Wang
More informationarxiv: v1 [math.nt] 18 Jan 2016
A functional relation for L-function of graph equivalent to the Riemann Hypothei for Dirichlet L-function arxiv:60.04573v [math.nt] 8 Jan 206 Fabien Friedli September 9, 208 Abtract In thi note we define
More informationDIFFERENTIAL EQUATIONS Laplace Transforms. Paul Dawkins
DIFFERENTIAL EQUATIONS Laplace Tranform Paul Dawkin Table of Content Preface... Laplace Tranform... Introduction... The Definition... 5 Laplace Tranform... 9 Invere Laplace Tranform... Step Function...
More informationClustering Methods without Given Number of Clusters
Clutering Method without Given Number of Cluter Peng Xu, Fei Liu Introduction A we now, mean method i a very effective algorithm of clutering. It mot powerful feature i the calability and implicity. However,
More informationManprit Kaur and Arun Kumar
CUBIC X-SPLINE INTERPOLATORY FUNCTIONS Manprit Kaur and Arun Kumar manpreet2410@gmail.com, arun04@rediffmail.com Department of Mathematic and Computer Science, R. D. Univerity, Jabalpur, INDIA. Abtract:
More informationSocial Studies 201 Notes for November 14, 2003
1 Social Studie 201 Note for November 14, 2003 Etimation of a mean, mall ample ize Section 8.4, p. 501. When a reearcher ha only a mall ample ize available, the central limit theorem doe not apply to the
More informationEXAM 4 -B2 MATH 261: Elementary Differential Equations MATH 261 FALL 2012 EXAMINATION COVER PAGE Professor Moseley
EXAM 4 -B MATH 6: Elementary Differential Equation MATH 6 FALL 0 EXAMINATION COVER PAGE Profeor Moeley PRINT NAME ( ) Lat Name, Firt Name MI (What you wih to be called) ID # EXAM DATE Friday, Nov. 9, 0
More informationThe Hassenpflug Matrix Tensor Notation
The Haenpflug Matrix Tenor Notation D.N.J. El Dept of Mech Mechatron Eng Univ of Stellenboch, South Africa e-mail: dnjel@un.ac.za 2009/09/01 Abtract Thi i a ample document to illutrate the typeetting of
More informationProblem 1. Construct a filtered probability space on which a Brownian motion W and an adapted process X are defined and such that
Stochatic Calculu Example heet 4 - Lent 5 Michael Tehranchi Problem. Contruct a filtered probability pace on which a Brownian motion W and an adapted proce X are defined and uch that dx t = X t t dt +
More informationL 2 -transforms for boundary value problems
Computational Method for Differential Equation http://cmde.tabrizu.ac.ir Vol. 6, No., 8, pp. 76-85 L -tranform for boundary value problem Arman Aghili Department of applied mathematic, faculty of mathematical
More informationFUNDAMENTALS OF POWER SYSTEMS
1 FUNDAMENTALS OF POWER SYSTEMS 1 Chapter FUNDAMENTALS OF POWER SYSTEMS INTRODUCTION The three baic element of electrical engineering are reitor, inductor and capacitor. The reitor conume ohmic or diipative
More informationLINEAR ALGEBRA METHOD IN COMBINATORICS. Theorem 1.1 (Oddtown theorem). In a town of n citizens, no more than n clubs can be formed under the rules
LINEAR ALGEBRA METHOD IN COMBINATORICS 1 Warming-up example Theorem 11 (Oddtown theorem) In a town of n citizen, no more tha club can be formed under the rule each club have an odd number of member each
More informationEXAM 4 -A2 MATH 261: Elementary Differential Equations MATH 261 FALL 2010 EXAMINATION COVER PAGE Professor Moseley
EXAM 4 -A MATH 6: Elementary Differential Equation MATH 6 FALL 00 EXAMINATION COVER PAGE Profeor Moeley PRINT NAME ( ) Lat Name, Firt Name MI (What you wih to be called) ID # EXAM DATE Friday, Nov. 9,
More informationSocial Studies 201 Notes for March 18, 2005
1 Social Studie 201 Note for March 18, 2005 Etimation of a mean, mall ample ize Section 8.4, p. 501. When a reearcher ha only a mall ample ize available, the central limit theorem doe not apply to the
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 informationLie series An old concept going back to Sophus Lie, but already used by Newton and made rigorous by Cauchy. Widely exploited, e.g.
ÄÁ Ë ÊÁ Ë Æ ÄÁ ÌÊ ÆË ÇÊÅË Lie erie An old concept going back to Sophu Lie, but already ued by Newton and made rigorou by Cauchy Widely exploited, eg, in differential geometry Ued a a method for numerical
More informationTHE DIVERGENCE-FREE JACOBIAN CONJECTURE IN DIMENSION TWO
THE DIVERGENCE-FREE JACOBIAN CONJECTURE IN DIMENSION TWO J. W. NEUBERGER Abtract. A pecial cae, called the divergence-free cae, of the Jacobian Conjecture in dimenion two i proved. Thi note outline an
More informationDesign By Emulation (Indirect Method)
Deign By Emulation (Indirect Method he baic trategy here i, that Given a continuou tranfer function, it i required to find the bet dicrete equivalent uch that the ignal produced by paing an input ignal
More informationSECTION x2 x > 0, t > 0, (8.19a)
SECTION 8.5 433 8.5 Application of aplace Tranform to Partial Differential Equation In Section 8.2 and 8.3 we illutrated the effective ue of aplace tranform in olving ordinary differential equation. The
More informationSIMON FRASER UNIVERSITY School of Engineering Science ENSC 320 Electric Circuits II. Solutions to Assignment 3 February 2005.
SIMON FRASER UNIVERSITY School of Engineering Science ENSC 320 Electric Circuit II Solution to Aignment 3 February 2005. Initial Condition Source 0 V battery witch flip at t 0 find i 3 (t) Component value:
More informationCHBE320 LECTURE V LAPLACE TRANSFORM AND TRANSFER FUNCTION. Professor Dae Ryook Yang
CHBE3 ECTURE V APACE TRANSFORM AND TRANSFER FUNCTION Profeor Dae Ryook Yang Spring 8 Dept. of Chemical and Biological Engineering 5- Road Map of the ecture V aplace Tranform and Tranfer function Definition
More informationarxiv: v1 [hep-th] 10 Oct 2008
The boundary tate from open tring field arxiv:0810.1737 MIT-CTP-3990 UT-Komaba/08-14 IPMU 08-0074 arxiv:0810.1737v1 [hep-th] 10 Oct 2008 Michael Kiermaier 1,2, Yuji Okawa 3 and Barton Zwiebach 1 1 Center
More informationPractice Problems - Week #7 Laplace - Step Functions, DE Solutions Solutions
For Quetion -6, rewrite the piecewie function uing tep function, ketch their graph, and find F () = Lf(t). 0 0 < t < 2. f(t) = (t 2 4) 2 < t In tep-function form, f(t) = u 2 (t 2 4) The graph i the olid
More informationChapter 5 Consistency, Zero Stability, and the Dahlquist Equivalence Theorem
Chapter 5 Conitency, Zero Stability, and the Dahlquit Equivalence Theorem In Chapter 2 we dicued convergence of numerical method and gave an experimental method for finding the rate of convergence (aka,
More informationReading assignment: In this chapter we will cover Sections Definition and the Laplace transform of simple functions
Chapter 4 Laplace Tranform 4 Introduction Reading aignment: In thi chapter we will cover Section 4 45 4 Definition and the Laplace tranform of imple function Given f, a function of time, with value f(t
More informationHylleraas wavefunction for He. dv 2. ,! r 2. )dv 1. in the trial function. A simple trial function that does include r 12. is ) f (r 12.
Hylleraa wavefunction for He The reaon why the Hartree method cannot reproduce the exact olution i due to the inability of the Hartree wave-function to account for electron correlation. We know that the
More informationSynopsis of Complex Analysis. Ryan D. Reece
Synopsis of Complex Analysis Ryan D. Reece December 7, 2006 Chapter Complex Numbers. The Parts of a Complex Number A complex number, z, is an ordered pair of real numbers similar to the points in the real
More informationComputers and Mathematics with Applications. Sharp algebraic periodicity conditions for linear higher order
Computer and Mathematic with Application 64 (2012) 2262 2274 Content lit available at SciVere ScienceDirect Computer and Mathematic with Application journal homepage: wwweleviercom/locate/camwa Sharp algebraic
More informationHyperbolic Partial Differential Equations
Hyperbolic Partial Differential Equation Evolution equation aociated with irreverible phyical procee like diffuion heat conduction lead to parabolic partial differential equation. When the equation i a
More informationControl of Delayed Integrating Processes Using Two Feedback Controllers R MS Approach
Proceeding of the 7th WSEAS International Conference on SYSTEM SCIENCE and SIMULATION in ENGINEERING (ICOSSSE '8) Control of Delayed Integrating Procee Uing Two Feedback Controller R MS Approach LIBOR
More informationSymmetric Determinantal Representation of Formulas and Weakly Skew Circuits
Contemporary Mathematic Symmetric Determinantal Repreentation of Formula and Weakly Skew Circuit Bruno Grenet, Erich L. Kaltofen, Pacal Koiran, and Natacha Portier Abtract. We deploy algebraic complexity
More informationTMA4125 Matematikk 4N Spring 2016
Norwegian Univerity of Science and Technology Department of Mathematical Science TMA45 Matematikk 4N Spring 6 Solution to problem et 6 In general, unle ele i noted, if f i a function, then F = L(f denote
More informationFermi Distribution Function. n(e) T = 0 T > 0 E F
LECTURE 3 Maxwell{Boltzmann, Fermi, and Boe Statitic Suppoe we have a ga of N identical point particle in a box ofvolume V. When we ay \ga", we mean that the particle are not interacting with one another.
More informationDesign of Digital Filters
Deign of Digital Filter Paley-Wiener Theorem [ ] ( ) If h n i a caual energy ignal, then ln H e dω< B where B i a finite upper bound. One implication of the Paley-Wiener theorem i that a tranfer function
More informationGiven the following circuit with unknown initial capacitor voltage v(0): X(s) Immediately, we know that the transfer function H(s) is
EE 4G Note: Chapter 6 Intructor: Cheung More about ZSR and ZIR. Finding unknown initial condition: Given the following circuit with unknown initial capacitor voltage v0: F v0/ / Input xt 0Ω Output yt -
More informationA SIMPLE NASH-MOSER IMPLICIT FUNCTION THEOREM IN WEIGHTED BANACH SPACES. Sanghyun Cho
A SIMPLE NASH-MOSER IMPLICIT FUNCTION THEOREM IN WEIGHTED BANACH SPACES Sanghyun Cho Abtract. We prove a implified verion of the Nah-Moer implicit function theorem in weighted Banach pace. We relax the
More informationLecture 10 Filtering: Applied Concepts
Lecture Filtering: Applied Concept In the previou two lecture, you have learned about finite-impule-repone (FIR) and infinite-impule-repone (IIR) filter. In thee lecture, we introduced the concept of filtering
More informationON THE DETERMINATION OF NUMBERS BY THEIR SUMS OF A FIXED ORDER J. L. SELFRIDGE AND E. G. STRAUS
ON THE DETERMINATION OF NUMBERS BY THEIR SUMS OF A FIXED ORDER J. L. SELFRIDGE AND E. G. STRAUS 1. Introduction. We wih to treat the following problem (uggeted by a problem of L. Moer [2]): Let {x} = {x
More informationThe Laplace Transform , Haynes Miller and Jeremy Orloff
The Laplace Tranform 8.3, Hayne Miller and Jeremy Orloff Laplace tranform baic: introduction An operator take a function a input and output another function. A tranform doe the ame thing with the added
More informationTHE SPLITTING SUBSPACE CONJECTURE
THE SPLITTING SUBSPAE ONJETURE ERI HEN AND DENNIS TSENG Abtract We anwer a uetion by Niederreiter concerning the enumeration of a cla of ubpace of finite dimenional vector pace over finite field by proving
More informationThe Laplace Transform
The Laplace Tranform Prof. Siripong Potiuk Pierre Simon De Laplace 749-827 French Atronomer and Mathematician Laplace Tranform An extenion of the CT Fourier tranform to allow analyi of broader cla of CT
More informationCDMA Signature Sequences with Low Peak-to-Average-Power Ratio via Alternating Projection
CDMA Signature Sequence with Low Peak-to-Average-Power Ratio via Alternating Projection Joel A Tropp Int for Comp Engr and Sci (ICES) The Univerity of Texa at Autin 1 Univerity Station C0200 Autin, TX
More informationBy Xiaoquan Wen and Matthew Stephens University of Michigan and University of Chicago
Submitted to the Annal of Applied Statitic SUPPLEMENTARY APPENDIX TO BAYESIAN METHODS FOR GENETIC ASSOCIATION ANALYSIS WITH HETEROGENEOUS SUBGROUPS: FROM META-ANALYSES TO GENE-ENVIRONMENT INTERACTIONS
More informationSOLUTIONS TO ALGEBRAIC GEOMETRY AND ARITHMETIC CURVES BY QING LIU. I will collect my solutions to some of the exercises in this book in this document.
SOLUTIONS TO ALGEBRAIC GEOMETRY AND ARITHMETIC CURVES BY QING LIU CİHAN BAHRAN I will collect my olution to ome of the exercie in thi book in thi document. Section 2.1 1. Let A = k[[t ]] be the ring of
More informationAvoiding Forbidden Submatrices by Row Deletions
Avoiding Forbidden Submatrice by Row Deletion Sebatian Wernicke, Jochen Alber, Jen Gramm, Jiong Guo, and Rolf Niedermeier Wilhelm-Schickard-Intitut für Informatik, niverität Tübingen, Sand 13, D-72076
More informationIEOR 3106: Fall 2013, Professor Whitt Topics for Discussion: Tuesday, November 19 Alternating Renewal Processes and The Renewal Equation
IEOR 316: Fall 213, Profeor Whitt Topic for Dicuion: Tueday, November 19 Alternating Renewal Procee and The Renewal Equation 1 Alternating Renewal Procee An alternating renewal proce alternate between
More informationConvergence criteria and optimization techniques for beam moments
Pure Appl. Opt. 7 (1998) 1221 1230. Printed in the UK PII: S0963-9659(98)90684-5 Convergence criteria and optimization technique for beam moment G Gbur and P S Carney Department of Phyic and Atronomy and
More informationMODERN CONTROL SYSTEMS
MODERN CONTROL SYSTEMS Lecture 1 Root Locu Emam Fathy Department of Electrical and Control Engineering email: emfmz@aat.edu http://www.aat.edu/cv.php?dip_unit=346&er=68525 1 Introduction What i root locu?
More informationCHE302 LECTURE V LAPLACE TRANSFORM AND TRANSFER FUNCTION. Professor Dae Ryook Yang
CHE3 ECTURE V APACE TRANSFORM AND TRANSFER FUNCTION Profeor Dae Ryook Yang Fall Dept. of Chemical and Biological Engineering Korea Univerity CHE3 Proce Dynamic and Control Korea Univerity 5- SOUTION OF
More informationAdvanced methods for ODEs and DAEs
Lecture : Implicit Runge Kutta method Bojana Roić, 9. April 7 What you need to know before thi lecture numerical integration: Lecture from ODE iterative olver: Lecture 5-8 from ODE 9. April 7 Bojana Roić
More informationOnline Appendix for Managerial Attention and Worker Performance by Marina Halac and Andrea Prat
Online Appendix for Managerial Attention and Worker Performance by Marina Halac and Andrea Prat Thi Online Appendix contain the proof of our reult for the undicounted limit dicued in Section 2 of the paper,
More informationPacific Journal of Mathematics
Pacific Journal of Mathematic OSCILLAION AND NONOSCILLAION OF FORCED SECOND ORDER DYNAMIC EQUAIONS MARIN BOHNER AND CHRISOPHER C. ISDELL Volume 230 No. March 2007 PACIFIC JOURNAL OF MAHEMAICS Vol. 230,
More informationUSPAS Course on Recirculated and Energy Recovered Linear Accelerators
USPAS Coure on Recirculated and Energy Recovered Linear Accelerator G. A. Krafft and L. Merminga Jefferon Lab I. Bazarov Cornell Lecture 6 7 March 005 Lecture Outline. Invariant Ellipe Generated by a Unimodular
More informationApplication of Laplace Adomian Decomposition Method on Linear and Nonlinear System of PDEs
Applied Mathematical Science, Vol. 5, 2011, no. 27, 1307-1315 Application of Laplace Adomian Decompoition Method on Linear and Nonlinear Sytem of PDE Jaem Fadaei Mathematic Department, Shahid Bahonar Univerity
More informationFeedback Control Systems (FCS)
Feedback Control Sytem (FCS) Lecture19-20 Routh-Herwitz Stability Criterion Dr. Imtiaz Huain email: imtiaz.huain@faculty.muet.edu.pk URL :http://imtiazhuainkalwar.weebly.com/ Stability of Higher Order
More informationTHE THERMOELASTIC SQUARE
HE HERMOELASIC SQUARE A mnemonic for remembering thermodynamic identitie he tate of a material i the collection of variable uch a tre, train, temperature, entropy. A variable i a tate variable if it integral
More information