Simple Algebraic Proofs of Fermat s Last Theorem. Samuel Bonaya Buya*

Size: px
Start display at page:

Download "Simple Algebraic Proofs of Fermat s Last Theorem. Samuel Bonaya Buya*"

Transcription

1 Avaiabe onine at eagia Research Library Advances in Appied Science Research, 017, 8(3:60-6 ISSN : CODEN (USA: AASRFC Simpe Agebraic roofs of Fermat s Last Theorem Samue Bonaya Buya* Ngao Girs Secondary Schoo, Kenya ABSTRACT In this research simpe proofs of Fermat s ast theorem of ast theorem are proposed. The proofs presented do not require any Gaois representation or concepts of eiptic curves. In the first proof a most genera agebraic coordinate representation of ythagorean integer tripes is proposed. The tripes wi be powered to some genera degree n to enabe derivation of the proof. In the second proof method a genera agebraic formua containing a the ythagorean tripes is proposed. The formua is then used to prove Fermat s ast theorem. The mathematics in this proposed agebraic form is trivia and within the scope of seventeenth century mathematics. Fermat caimed that he got a tremendous proof of his theorem. The objective of this paper is to show that there are simpe mathematica proofs of Fermat s ast theorem within the reach of the seventeenth century mathematics. Keywords: roof of Fermat's ast theorem, ythagorean tripes HISTORY AND OVERVIEW The integer soution of x + y = z is we known. Exampes of we-known tripets that satisfy the identity above are (3,, 5; (5, 1, 13. The Babyonians were aware of many different kinds of ythagorean integer tripets. In 1637 ierre de Fermat caimed that the Diophantine equation x + y = z has no soution for any N greater than. Fermat excaimed caimed that he got a marveous proof of his proposition. The proof of this statement has euded mathematicians for centuries. The first compete proof of Fermat s ast theorem for case N=3 was given Kar Friedrich Gauss. eter Dirichet and Andrien Legendre roved Fermat s ast theorem for the case N=5 in 185. Gabrie Laḿe proved Fermat s ast theorem for the case N=7 around Between 187 and 1853 Ernest Kummer pubished some masterfu piece of work in which he attempted the extent to which the function: { ao a1 a ai Z} Z{ ζ] = + ζ ζ : ζ = e πi (ι rime is a unique factorization domain (UFD The basic idea in the proof of Fermat s ast theory is to show is to factor and to show there is no soution of with Λ xyz [1]. x + y = z as ( 1 ( ζ...( ζ x+ y x+ y x+ y = z In 183 Sophie Germaine estabished a proof of conditions under which Fermat ast theorem has no soution. Arthur Wieferich aso proved conditions under which Fermat s ast theorem has no soution. eagia Research Library 60

2 Buya AdvApp Sci Res., 017, 8(3:60-6 There are many who contributed towards the modern proof of Fermat s ast theorem incuding Srinivasa Ramanujan, Andre Wei and John Tate among others. Study of Gaois representation s foowed from the work Andre Wei and John Tate invoving the study of eiptic curves of the form y = g( x On th October 199, Wies produced a manuscript which was vetted and pubished in May 1995 in which the moduarity theorem was estabished as the ast step in proving Fermat s ast theorem. In this paper attempts wi be made to present two simpe proofs of Fermat s ast theorem. In the first proof method an attempt wi be made to present a most genera form of the ythagorean tripets by an attempt wi be made to generaize them to the form a + b = c stricty for the cases N> In the second method I wi seek to present an nth degree poynomia equation by which I wi attempt to generaize ythagorean tripes for the case N> [-7]. METHOD 1 Many formuae for generating ythagorean tripes have been deveoped. Eucid s formua is known to be very successfu in generating many primitive tripes. Eucid s formua fais to produce a tripes. A ythagorean tripe representation wi be presented that takes care of a tripes. A very imited representation of the ythagorean tripes can be represented in the three ordered pair of co-ordinates beow. (N + 1 (M + 1 (N (M ( k(m 1(N 1, k, k Where k, N are integers With k=1 and N=5 000 for exampe we can construct the tripet: (10 001, , that satisfies the above identity. A more genera construction of ythagorean integer tripets can take the form: (N + 1 (M + 1 (N (M + 1 ( k(m + 1(N + 1, k, k 0. Where k, M and N are integers The tripet (8, 55, 73 can be constructed using k=1 M=5 and N=. The most genera construction of ythagorean integer tripets takes the form: ( + ( + ( + 1 ( + 1 ( ( + 1 M N M N ( k M 1 N 1, k, k 0.3 For positive integers in the tripet ( M + 1 > ( N + 1, M, N,, and k are integers. If we seect k=1, M=3, N= and ==5 we obtain the tripet the ythagorean tripet ( , , Notice the sum of the tripes 0.3 is given by ( 1 p ( 1 ( 1 s k N M N = For positive integers, k, M, N we can identify the foowing properties (from 0. of ythagorean tripes: 1. ositive Integers of any given ythagorean tripe add up to an even number.. Odd positive integers in any ythagorean tripe appear in a pair. 3. For any ythagorean positive integer tripe with an odd coordinate, N + 1, there exists at east some corresponding odd coordinate N + N + 1 and even coordinate N + N + 1 to make up the compete tripe.. The sum the coordinates of a ythagorean tripe with odd coordinates, (N+1, N + N + 1is (N+1 (N+ eagia Research Library 61

3 Buya AdvApp Sci Res., 017, 8(3: The coordinates N + N, N + N and n n n a + b = c of a ythagorean tripe are co-prime. The generaization of the concept of ythagorean tripes is the search of positive integers a, b and c such that n n n a + b = c for some n stricty greater than. The tripets 0.3 are the most appropriate for such a generaization since it contains a integer ythagorean tripes and is in power form. If we take (M+1 = a 0.5 (N+1 = b 0.5 The generaization of ythagorean tripes 0.3 woud take the ythagorean form: a b a + b a b + = 0.6 The expansion rearrangement and simpification of the generaization 0.3 above woud ead to the resut beow: a + b = a + b 0.7 If we take = Then the equation 0.7 takes the identity form: a + b = a + b 0.8 The basic idea in the proof of Fermat s ast theory is to show is to factor x + y = z for > We fai to achieve such a generaization with the most genera ythagorean tripes reationship. We end up with a staemate condition. In equation 0. if we take: x = k M + 1 N ( M 1 ( N 1 y k + + = ( M 1 ( N 1 z k = k,, M, N,, are integers. Then the tripets 0.3 take the ythagorean form x + y = z 1. = x k M N ( M + 1 ( N y k k M N (( 1 ( 1 = = + + ( M ( N z k k M N (( 1 ( 1 = = eagia Research Library 6

4 Buya AdvApp Sci Res., 017, 8(3:60-6 x, y and z are aways integers when = this is because ( 1 k M + ( N + 1 and are even numbers and ( + + are even numbers and 1 1 = k M 1 N 1 Therefore, x k ( M ( N = , 1 y k ( M 1 ( N 1 1 ( = are whoe numbers. z k M N Consider equations ; ( If we take k = ((M (N + 1 Then = + + and x= M N + 1 M + 1 N (( M+1 - ( N y= (( M+1 + ( N+1 (( M+1 -( N+1 = x M+1 N ( 1 ( 1 1 z = M + + N Again equations wi aways resut in integer vaues of x, y and z when =. Dividing 1.8 to 1.7 we get the foowing resuts: (( ( 1 M+1 - N+1 1 M+1 N+1 y x = = M+1 N N+1 M+1 > the quotient 1.9 is a surd (exceptiona case where M=N=0 in which case the quotient is zero. This is in which y=0. This means for greater than either x or y or both a radica number. This means that when >, x, y and z cannot simutaneousy yied integer vaues, except in the specia case in which either x or y is zero. Thus Fermat s ast theorem is proved. There is need for another confirmatory proof. METHOD Consider the agebraic equation: n n n n n (n n n n ( x+ m + x + 1 Cx ( x+ m + Cx ( x+ m n1 Cx ( x+ m = z 0.1 Its factorized form is given by: ( n x m x z n + + = 0. (Note here that the equation 0. further simpifies to ( x+ m + x = z a case true for n=1 Consider the imit case of 0.1 n n n x+ m + x = z 0.3a If we take = n 0.3a takes the form beow eagia Research Library 63

5 Buya AdvApp Sci Res., 017, 8(3:60-6 x+ m + x = z 0.3b In such a case Cx ( x + m + Cx ( x + m Cx ( x + m = 0 0. n n n 1 n 1 Equation 0.1 becomes equa to zero ony when x+m=0 When x+m, then the Diophantine equation 0.3 takes the form ( 0 + x = z 0.5 Thus for the genera case >, x+m=0 and equation 0.3 takes the form 0.5 This therefore authenticates Fermat s ast theorem. SUMMARY, CONCLUSION AND RECOMMENDATIONS Simpe methods for proving Fermat ast theorem do exist. It is very possibe for Fermat to come up with one of such proofs given that mathematics had deveoped enough in his time to come with such a proof. The genera forms of deriving the ythagorean tripes can be used to computer generate infinite number of ythagorean tripets. The coprime ythagorean tripes of the formuae can be used to generate and test a whoe host of infinite possibe prime numbers. REFERENCES [1] Boston N. The proof of Fermat s ast theorem. University of Wisconsin-Madison, 003. [] Darmon H, Diamond F, Tayor R. Fermat s ast theorem. Curr Dev Math, 1995, 1: 157. [3] Darmon H, Diamond F, Tayor R. Fermat s ast theorem. Eiptic curves, moduar forms and Fermat s ast theorem. Int ress, Cambridge, MA, USA, [] Singh S. Fermat's ast theorem: The story of a ridde that confounded the word's greatest minds for 358 years. Fourth Estate, [5] Edwards, Harod M. Fermat's ast theorem: A genetic introduction to agebraic number theory. Springer Science & Business Media, [6] Weisstein EW. Fermat's Last Theorem. Wofram Mathword, 00. [7] Wies A. Moduar eiptic curves and Fermat's ast theorem. Ann Math, 199, 11: eagia Research Library 6

(f) is called a nearly holomorphic modular form of weight k + 2r as in [5].

(f) is called a nearly holomorphic modular form of weight k + 2r as in [5]. PRODUCTS OF NEARLY HOLOMORPHIC EIGENFORMS JEFFREY BEYERL, KEVIN JAMES, CATHERINE TRENTACOSTE, AND HUI XUE Abstract. We prove that the product of two neary hoomorphic Hece eigenforms is again a Hece eigenform

More information

ON CERTAIN SUMS INVOLVING THE LEGENDRE SYMBOL. Borislav Karaivanov Sigma Space Inc., Lanham, Maryland

ON CERTAIN SUMS INVOLVING THE LEGENDRE SYMBOL. Borislav Karaivanov Sigma Space Inc., Lanham, Maryland #A14 INTEGERS 16 (2016) ON CERTAIN SUMS INVOLVING THE LEGENDRE SYMBOL Borisav Karaivanov Sigma Sace Inc., Lanham, Maryand borisav.karaivanov@sigmasace.com Tzvetain S. Vassiev Deartment of Comuter Science

More information

PRIME TWISTS OF ELLIPTIC CURVES

PRIME TWISTS OF ELLIPTIC CURVES PRIME TWISTS OF ELLIPTIC CURVES DANIEL KRIZ AND CHAO LI Abstract. For certain eiptic curves E/Q with E(Q)[2] = Z/2Z, we prove a criterion for prime twists of E to have anaytic rank 0 or 1, based on a mod

More information

4 1-D Boundary Value Problems Heat Equation

4 1-D Boundary Value Problems Heat Equation 4 -D Boundary Vaue Probems Heat Equation The main purpose of this chapter is to study boundary vaue probems for the heat equation on a finite rod a x b. u t (x, t = ku xx (x, t, a < x < b, t > u(x, = ϕ(x

More information

Pricing Multiple Products with the Multinomial Logit and Nested Logit Models: Concavity and Implications

Pricing Multiple Products with the Multinomial Logit and Nested Logit Models: Concavity and Implications Pricing Mutipe Products with the Mutinomia Logit and Nested Logit Modes: Concavity and Impications Hongmin Li Woonghee Tim Huh WP Carey Schoo of Business Arizona State University Tempe Arizona 85287 USA

More information

CONGRUENCES. 1. History

CONGRUENCES. 1. History CONGRUENCES HAO BILLY LEE Abstract. These are notes I created for a seminar tak, foowing the papers of On the -adic Representations and Congruences for Coefficients of Moduar Forms by Swinnerton-Dyer and

More information

THE PARTITION FUNCTION AND HECKE OPERATORS

THE PARTITION FUNCTION AND HECKE OPERATORS THE PARTITION FUNCTION AND HECKE OPERATORS KEN ONO Abstract. The theory of congruences for the partition function p(n depends heaviy on the properties of haf-integra weight Hecke operators. The subject

More information

Selmer groups and Euler systems

Selmer groups and Euler systems Semer groups and Euer systems S. M.-C. 21 February 2018 1 Introduction Semer groups are a construction in Gaois cohomoogy that are cosey reated to many objects of arithmetic importance, such as cass groups

More information

4 Separation of Variables

4 Separation of Variables 4 Separation of Variabes In this chapter we describe a cassica technique for constructing forma soutions to inear boundary vaue probems. The soution of three cassica (paraboic, hyperboic and eiptic) PDE

More information

The Partition Function and Ramanujan Congruences

The Partition Function and Ramanujan Congruences The Partition Function and Ramanujan Congruences Eric Bucher Apri 7, 010 Chapter 1 Introduction The partition function, p(n), for a positive integer n is the number of non-increasing sequences of positive

More information

PARTITION CONGRUENCES AND THE ANDREWS-GARVAN-DYSON CRANK

PARTITION CONGRUENCES AND THE ANDREWS-GARVAN-DYSON CRANK PARTITION CONGRUENCES AND THE ANDREWS-GARVAN-DYSON CRANK KARL MAHLBURG Abstract. In 1944, Freeman Dyson conjectured the existence of a crank function for partitions that woud provide a combinatoria proof

More information

Partial permutation decoding for MacDonald codes

Partial permutation decoding for MacDonald codes Partia permutation decoding for MacDonad codes J.D. Key Department of Mathematics and Appied Mathematics University of the Western Cape 7535 Bevie, South Africa P. Seneviratne Department of Mathematics

More information

ALGORITHMIC SUMMATION OF RECIPROCALS OF PRODUCTS OF FIBONACCI NUMBERS. F. = I j. ^ = 1 ^ -, and K w = ^. 0) n=l r n «=1 -*/!

ALGORITHMIC SUMMATION OF RECIPROCALS OF PRODUCTS OF FIBONACCI NUMBERS. F. = I j. ^ = 1 ^ -, and K w = ^. 0) n=l r n «=1 -*/! ALGORITHMIC SUMMATIO OF RECIPROCALS OF PRODUCTS OF FIBOACCI UMBERS Staney Rabinowitz MathPro Press, 2 Vine Brook Road, Westford, MA 0886 staney@tiac.net (Submitted May 997). ITRODUCTIO There is no known

More information

PhysicsAndMathsTutor.com

PhysicsAndMathsTutor.com . Two points A and B ie on a smooth horizonta tabe with AB = a. One end of a ight eastic spring, of natura ength a and moduus of easticity mg, is attached to A. The other end of the spring is attached

More information

Problem set 6 The Perron Frobenius theorem.

Problem set 6 The Perron Frobenius theorem. Probem set 6 The Perron Frobenius theorem. Math 22a4 Oct 2 204, Due Oct.28 In a future probem set I want to discuss some criteria which aow us to concude that that the ground state of a sef-adjoint operator

More information

QUADRATIC FORMS AND FOUR PARTITION FUNCTIONS MODULO 3

QUADRATIC FORMS AND FOUR PARTITION FUNCTIONS MODULO 3 QUADRATIC FORMS AND FOUR PARTITION FUNCTIONS MODULO 3 JEREMY LOVEJOY AND ROBERT OSBURN Abstract. Recenty, Andrews, Hirschhorn Seers have proven congruences moduo 3 for four types of partitions using eementary

More information

14 Separation of Variables Method

14 Separation of Variables Method 14 Separation of Variabes Method Consider, for exampe, the Dirichet probem u t = Du xx < x u(x, ) = f(x) < x < u(, t) = = u(, t) t > Let u(x, t) = T (t)φ(x); now substitute into the equation: dt

More information

Gauss Law. 2. Gauss s Law: connects charge and field 3. Applications of Gauss s Law

Gauss Law. 2. Gauss s Law: connects charge and field 3. Applications of Gauss s Law Gauss Law 1. Review on 1) Couomb s Law (charge and force) 2) Eectric Fied (fied and force) 2. Gauss s Law: connects charge and fied 3. Appications of Gauss s Law Couomb s Law and Eectric Fied Couomb s

More information

MATH 172: MOTIVATION FOR FOURIER SERIES: SEPARATION OF VARIABLES

MATH 172: MOTIVATION FOR FOURIER SERIES: SEPARATION OF VARIABLES MATH 172: MOTIVATION FOR FOURIER SERIES: SEPARATION OF VARIABLES Separation of variabes is a method to sove certain PDEs which have a warped product structure. First, on R n, a inear PDE of order m is

More information

FOURIER SERIES ON ANY INTERVAL

FOURIER SERIES ON ANY INTERVAL FOURIER SERIES ON ANY INTERVAL Overview We have spent considerabe time earning how to compute Fourier series for functions that have a period of 2p on the interva (-p,p). We have aso seen how Fourier series

More information

Lecture Notes for Math 251: ODE and PDE. Lecture 32: 10.2 Fourier Series

Lecture Notes for Math 251: ODE and PDE. Lecture 32: 10.2 Fourier Series Lecture Notes for Math 251: ODE and PDE. Lecture 32: 1.2 Fourier Series Shawn D. Ryan Spring 212 Last Time: We studied the heat equation and the method of Separation of Variabes. We then used Separation

More information

Efficient Algorithms for Pairing-Based Cryptosystems

Efficient Algorithms for Pairing-Based Cryptosystems CS548 Advanced Information Security Efficient Agorithms for Pairing-Based Cryptosystems Pauo S. L. M. Barreto, HaeY. Kim, Ben Lynn, and Michae Scott Proceedings of Crypto, 2002 2010. 04. 22. Kanghoon Lee,

More information

Course 2BA1, Section 11: Periodic Functions and Fourier Series

Course 2BA1, Section 11: Periodic Functions and Fourier Series Course BA, 8 9 Section : Periodic Functions and Fourier Series David R. Wikins Copyright c David R. Wikins 9 Contents Periodic Functions and Fourier Series 74. Fourier Series of Even and Odd Functions...........

More information

CS229 Lecture notes. Andrew Ng

CS229 Lecture notes. Andrew Ng CS229 Lecture notes Andrew Ng Part IX The EM agorithm In the previous set of notes, we taked about the EM agorithm as appied to fitting a mixture of Gaussians. In this set of notes, we give a broader view

More information

Week 6 Lectures, Math 6451, Tanveer

Week 6 Lectures, Math 6451, Tanveer Fourier Series Week 6 Lectures, Math 645, Tanveer In the context of separation of variabe to find soutions of PDEs, we encountered or and in other cases f(x = f(x = a 0 + f(x = a 0 + b n sin nπx { a n

More information

A Two-Parameter Trigonometric Series

A Two-Parameter Trigonometric Series A Two-Parameter Trigonometric Series Xiang-Qian Chang Xiang.Chang@bos.mcphs.edu Massachusetts Coege of Pharmacy and Heath Sciences Boston MA 25 Let us consider the foowing dua questions. A. Givenafunction

More information

LECTURE NOTES 8 THE TRACELESS SYMMETRIC TENSOR EXPANSION AND STANDARD SPHERICAL HARMONICS

LECTURE NOTES 8 THE TRACELESS SYMMETRIC TENSOR EXPANSION AND STANDARD SPHERICAL HARMONICS MASSACHUSETTS INSTITUTE OF TECHNOLOGY Physics Department Physics 8.07: Eectromagnetism II October, 202 Prof. Aan Guth LECTURE NOTES 8 THE TRACELESS SYMMETRIC TENSOR EXPANSION AND STANDARD SPHERICAL HARMONICS

More information

V.B The Cluster Expansion

V.B The Cluster Expansion V.B The Custer Expansion For short range interactions, speciay with a hard core, it is much better to repace the expansion parameter V( q ) by f( q ) = exp ( βv( q )), which is obtained by summing over

More information

1D Heat Propagation Problems

1D Heat Propagation Problems Chapter 1 1D Heat Propagation Probems If the ambient space of the heat conduction has ony one dimension, the Fourier equation reduces to the foowing for an homogeneous body cρ T t = T λ 2 + Q, 1.1) x2

More information

Separation of Variables and a Spherical Shell with Surface Charge

Separation of Variables and a Spherical Shell with Surface Charge Separation of Variabes and a Spherica She with Surface Charge In cass we worked out the eectrostatic potentia due to a spherica she of radius R with a surface charge density σθ = σ cos θ. This cacuation

More information

School of Electrical Engineering, University of Bath, Claverton Down, Bath BA2 7AY

School of Electrical Engineering, University of Bath, Claverton Down, Bath BA2 7AY The ogic of Booean matrices C. R. Edwards Schoo of Eectrica Engineering, Universit of Bath, Caverton Down, Bath BA2 7AY A Booean matrix agebra is described which enabes man ogica functions to be manipuated

More information

David Eigen. MA112 Final Paper. May 10, 2002

David Eigen. MA112 Final Paper. May 10, 2002 David Eigen MA112 Fina Paper May 1, 22 The Schrodinger equation describes the position of an eectron as a wave. The wave function Ψ(t, x is interpreted as a probabiity density for the position of the eectron.

More information

School of Electrical Engineering, University of Bath, Claverton Down, Bath BA2 7AY

School of Electrical Engineering, University of Bath, Claverton Down, Bath BA2 7AY The ogic of Booean matrices C. R. Edwards Schoo of Eectrica Engineering, Universit of Bath, Caverton Down, Bath BA2 7AY A Booean matrix agebra is described which enabes man ogica functions to be manipuated

More information

15. Bruns Theorem Definition Primes p and p < q are called twin primes if q = p + 2.

15. Bruns Theorem Definition Primes p and p < q are called twin primes if q = p + 2. 15 Bruns Theorem Definition 151 Primes and < q are caed twin rimes if q = π ) is the number of airs of twin rimes u to Conjecture 15 There are infinitey many twin rimes Theorem 153 π ) P ) = og og ) og

More information

Lecture Notes for Math 251: ODE and PDE. Lecture 34: 10.7 Wave Equation and Vibrations of an Elastic String

Lecture Notes for Math 251: ODE and PDE. Lecture 34: 10.7 Wave Equation and Vibrations of an Elastic String ecture Notes for Math 251: ODE and PDE. ecture 3: 1.7 Wave Equation and Vibrations of an Eastic String Shawn D. Ryan Spring 212 ast Time: We studied other Heat Equation probems with various other boundary

More information

2M2. Fourier Series Prof Bill Lionheart

2M2. Fourier Series Prof Bill Lionheart M. Fourier Series Prof Bi Lionheart 1. The Fourier series of the periodic function f(x) with period has the form f(x) = a 0 + ( a n cos πnx + b n sin πnx ). Here the rea numbers a n, b n are caed the Fourier

More information

arxiv: v1 [math.ca] 6 Mar 2017

arxiv: v1 [math.ca] 6 Mar 2017 Indefinite Integras of Spherica Besse Functions MIT-CTP/487 arxiv:703.0648v [math.ca] 6 Mar 07 Joyon K. Boomfied,, Stephen H. P. Face,, and Zander Moss, Center for Theoretica Physics, Laboratory for Nucear

More information

Lecture 9. Stability of Elastic Structures. Lecture 10. Advanced Topic in Column Buckling

Lecture 9. Stability of Elastic Structures. Lecture 10. Advanced Topic in Column Buckling Lecture 9 Stabiity of Eastic Structures Lecture 1 Advanced Topic in Coumn Bucking robem 9-1: A camped-free coumn is oaded at its tip by a oad. The issue here is to find the itica bucking oad. a) Suggest

More information

Theory of Generalized k-difference Operator and Its Application in Number Theory

Theory of Generalized k-difference Operator and Its Application in Number Theory Internationa Journa of Mathematica Anaysis Vo. 9, 2015, no. 19, 955-964 HIKARI Ltd, www.m-hiari.com http://dx.doi.org/10.12988/ijma.2015.5389 Theory of Generaized -Difference Operator and Its Appication

More information

A NOTE ON QUASI-STATIONARY DISTRIBUTIONS OF BIRTH-DEATH PROCESSES AND THE SIS LOGISTIC EPIDEMIC

A NOTE ON QUASI-STATIONARY DISTRIBUTIONS OF BIRTH-DEATH PROCESSES AND THE SIS LOGISTIC EPIDEMIC (January 8, 2003) A NOTE ON QUASI-STATIONARY DISTRIBUTIONS OF BIRTH-DEATH PROCESSES AND THE SIS LOGISTIC EPIDEMIC DAMIAN CLANCY, University of Liverpoo PHILIP K. POLLETT, University of Queensand Abstract

More information

Wave Equation Dirichlet Boundary Conditions

Wave Equation Dirichlet Boundary Conditions Wave Equation Dirichet Boundary Conditions u tt x, t = c u xx x, t, < x 1 u, t =, u, t = ux, = fx u t x, = gx Look for simpe soutions in the form ux, t = XxT t Substituting into 13 and dividing

More information

Math 124B January 17, 2012

Math 124B January 17, 2012 Math 124B January 17, 212 Viktor Grigoryan 3 Fu Fourier series We saw in previous ectures how the Dirichet and Neumann boundary conditions ead to respectivey sine and cosine Fourier series of the initia

More information

V.B The Cluster Expansion

V.B The Cluster Expansion V.B The Custer Expansion For short range interactions, speciay with a hard core, it is much better to repace the expansion parameter V( q ) by f(q ) = exp ( βv( q )) 1, which is obtained by summing over

More information

Theory and implementation behind: Universal surface creation - smallest unitcell

Theory and implementation behind: Universal surface creation - smallest unitcell Teory and impementation beind: Universa surface creation - smaest unitce Bjare Brin Buus, Jaob Howat & Tomas Bigaard September 15, 218 1 Construction of surface sabs Te aim for tis part of te project is

More information

Technical Data for Profiles. Groove position, external dimensions and modular dimensions

Technical Data for Profiles. Groove position, external dimensions and modular dimensions Technica Data for Profies Extruded Profie Symbo A Mg Si 0.5 F 25 Materia number.206.72 Status: artificiay aged Mechanica vaues (appy ony in pressing direction) Tensie strength Rm min. 245 N/mm 2 Yied point

More information

NOISE-INDUCED STABILIZATION OF STOCHASTIC DIFFERENTIAL EQUATIONS

NOISE-INDUCED STABILIZATION OF STOCHASTIC DIFFERENTIAL EQUATIONS NOISE-INDUCED STABILIZATION OF STOCHASTIC DIFFERENTIAL EQUATIONS TONY ALLEN, EMILY GEBHARDT, AND ADAM KLUBALL 3 ADVISOR: DR. TIFFANY KOLBA 4 Abstract. The phenomenon of noise-induced stabiization occurs

More information

Research Article On the Lower Bound for the Number of Real Roots of a Random Algebraic Equation

Research Article On the Lower Bound for the Number of Real Roots of a Random Algebraic Equation Appied Mathematics and Stochastic Anaysis Voume 007, Artice ID 74191, 8 pages doi:10.1155/007/74191 Research Artice On the Lower Bound for the Number of Rea Roots of a Random Agebraic Equation Takashi

More information

Generalized Bell polynomials and the combinatorics of Poisson central moments

Generalized Bell polynomials and the combinatorics of Poisson central moments Generaized Be poynomias and the combinatorics of Poisson centra moments Nicoas Privaut Division of Mathematica Sciences Schoo of Physica and Mathematica Sciences Nanyang Technoogica University SPMS-MAS-05-43,

More information

Chapter 4. Moving Observer Method. 4.1 Overview. 4.2 Theory

Chapter 4. Moving Observer Method. 4.1 Overview. 4.2 Theory Chapter 4 Moving Observer Method 4.1 Overview For a compete description of traffic stream modeing, one woud reuire fow, speed, and density. Obtaining these parameters simutaneousy is a difficut task if

More information

AFormula for N-Row Macdonald Polynomials

AFormula for N-Row Macdonald Polynomials Journa of Agebraic Combinatorics, 21, 111 13, 25 c 25 Springer Science + Business Media, Inc. Manufactured in The Netherands. AFormua for N-Row Macdonad Poynomias ELLISON-ANNE WILLIAMS North Caroina State

More information

HYDROGEN ATOM SELECTION RULES TRANSITION RATES

HYDROGEN ATOM SELECTION RULES TRANSITION RATES DOING PHYSICS WITH MATLAB QUANTUM PHYSICS Ian Cooper Schoo of Physics, University of Sydney ian.cooper@sydney.edu.au HYDROGEN ATOM SELECTION RULES TRANSITION RATES DOWNLOAD DIRECTORY FOR MATLAB SCRIPTS

More information

A Review on Dirac Jordan Transformation Theory

A Review on Dirac Jordan Transformation Theory Avaiabe onine at www.peagiaresearchibrary.com Avances in Appie Science Research, 01, 3 (4):474-480 A Review on Dirac Joran Transformation Theory F. Ashrafi, S.A. Babaneja, A. Moanoo Juybari, M. Jafari

More information

VTU-NPTEL-NMEICT Project

VTU-NPTEL-NMEICT Project MODUE-X -CONTINUOUS SYSTEM : APPROXIMATE METHOD VIBRATION ENGINEERING 14 VTU-NPTE-NMEICT Project Progress Report The Project on Deveopment of Remaining Three Quadrants to NPTE Phase-I under grant in aid

More information

Factorization of Cyclotomic Polynomials with Quadratic Radicals in the Coefficients

Factorization of Cyclotomic Polynomials with Quadratic Radicals in the Coefficients Advances in Pure Mathematics, 07, 7, 47-506 http://www.scirp.org/journa/apm ISSN Onine: 60-0384 ISSN Print: 60-0368 Factoriation of Cycotomic Poynomias with Quadratic Radicas in the Coefficients Afred

More information

$, (2.1) n="# #. (2.2)

$, (2.1) n=# #. (2.2) Chapter. Eectrostatic II Notes: Most of the materia presented in this chapter is taken from Jackson, Chap.,, and 4, and Di Bartoo, Chap... Mathematica Considerations.. The Fourier series and the Fourier

More information

Math 124B January 31, 2012

Math 124B January 31, 2012 Math 124B January 31, 212 Viktor Grigoryan 7 Inhomogeneous boundary vaue probems Having studied the theory of Fourier series, with which we successfuy soved boundary vaue probems for the homogeneous heat

More information

Kummer type congruences and Stickelberger subideals

Kummer type congruences and Stickelberger subideals ACTA ARITHMETICA LXXV.3 (1996) Kummer type congruences and Stickeberger subideas by Takashi Agoh (Chiba) and Ladisav Skua (Brno) 1. Introduction. Let be an odd prime, B m the Bernoui number defined by

More information

First-Order Corrections to Gutzwiller s Trace Formula for Systems with Discrete Symmetries

First-Order Corrections to Gutzwiller s Trace Formula for Systems with Discrete Symmetries c 26 Noninear Phenomena in Compex Systems First-Order Corrections to Gutzwier s Trace Formua for Systems with Discrete Symmetries Hoger Cartarius, Jörg Main, and Günter Wunner Institut für Theoretische

More information

SEMINAR 2. PENDULUMS. V = mgl cos θ. (2) L = T V = 1 2 ml2 θ2 + mgl cos θ, (3) d dt ml2 θ2 + mgl sin θ = 0, (4) θ + g l

SEMINAR 2. PENDULUMS. V = mgl cos θ. (2) L = T V = 1 2 ml2 θ2 + mgl cos θ, (3) d dt ml2 θ2 + mgl sin θ = 0, (4) θ + g l Probem 7. Simpe Penduum SEMINAR. PENDULUMS A simpe penduum means a mass m suspended by a string weightess rigid rod of ength so that it can swing in a pane. The y-axis is directed down, x-axis is directed

More information

How the backpropagation algorithm works Srikumar Ramalingam School of Computing University of Utah

How the backpropagation algorithm works Srikumar Ramalingam School of Computing University of Utah How the backpropagation agorithm works Srikumar Ramaingam Schoo of Computing University of Utah Reference Most of the sides are taken from the second chapter of the onine book by Michae Nieson: neuranetworksanddeepearning.com

More information

Section 6: Magnetostatics

Section 6: Magnetostatics agnetic fieds in matter Section 6: agnetostatics In the previous sections we assumed that the current density J is a known function of coordinates. In the presence of matter this is not aways true. The

More information

CE601-Structura Anaysis I UNIT-IV SOPE-DEFECTION METHOD 1. What are the assumptions made in sope-defection method? (i) Between each pair of the supports the beam section is constant. (ii) The joint in

More information

(1 α (1) l s )(1 α (2) a n n m b n n m p <ε

(1 α (1) l s )(1 α (2) a n n m b n n m p <ε L-INVARIANT OF p-adic L-FUNCTIONS HARUZO HIDA Let Q C be the fied of a agebraic numbers We fix a prime p>2and a p-adic absoute vaue p on Q Then C p is the competion of Q under p We write W = { x K x p

More information

arxiv: v1 [math.nt] 12 Feb 2019

arxiv: v1 [math.nt] 12 Feb 2019 Degenerate centra factoria numbers of the second ind Taeyun Kim, Dae San Kim arxiv:90.04360v [math.nt] Feb 09 In this paper, we introduce the degenerate centra factoria poynomias and numbers of the second

More information

STABILISATION OF THE LHS SPECTRAL SEQUENCE FOR ALGEBRAIC GROUPS. 1. Introduction

STABILISATION OF THE LHS SPECTRAL SEQUENCE FOR ALGEBRAIC GROUPS. 1. Introduction STABILISATION OF THE LHS SPECTRAL SEQUENCE FOR ALGEBRAIC GROUPS ALISON E. PARKER AND DAVID I. STEWART arxiv:140.465v1 [math.rt] 19 Feb 014 Abstract. In this note, we consider the Lyndon Hochschid Serre

More information

Reliability: Theory & Applications No.3, September 2006

Reliability: Theory & Applications No.3, September 2006 REDUNDANCY AND RENEWAL OF SERVERS IN OPENED QUEUING NETWORKS G. Sh. Tsitsiashvii M.A. Osipova Vadivosto, Russia 1 An opened queuing networ with a redundancy and a renewa of servers is considered. To cacuate

More information

6 Wave Equation on an Interval: Separation of Variables

6 Wave Equation on an Interval: Separation of Variables 6 Wave Equation on an Interva: Separation of Variabes 6.1 Dirichet Boundary Conditions Ref: Strauss, Chapter 4 We now use the separation of variabes technique to study the wave equation on a finite interva.

More information

ORTHOGONAL MULTI-WAVELETS FROM MATRIX FACTORIZATION

ORTHOGONAL MULTI-WAVELETS FROM MATRIX FACTORIZATION J. Korean Math. Soc. 46 2009, No. 2, pp. 281 294 ORHOGONAL MLI-WAVELES FROM MARIX FACORIZAION Hongying Xiao Abstract. Accuracy of the scaing function is very crucia in waveet theory, or correspondingy,

More information

#A48 INTEGERS 12 (2012) ON A COMBINATORIAL CONJECTURE OF TU AND DENG

#A48 INTEGERS 12 (2012) ON A COMBINATORIAL CONJECTURE OF TU AND DENG #A48 INTEGERS 12 (2012) ON A COMBINATORIAL CONJECTURE OF TU AND DENG Guixin Deng Schoo of Mathematica Sciences, Guangxi Teachers Education University, Nanning, P.R.China dengguixin@ive.com Pingzhi Yuan

More information

221B Lecture Notes Notes on Spherical Bessel Functions

221B Lecture Notes Notes on Spherical Bessel Functions Definitions B Lecture Notes Notes on Spherica Besse Functions We woud ike to sove the free Schrödinger equation [ h d r R(r) = h k R(r). () m r dr r m R(r) is the radia wave function ψ( x) = R(r)Y m (θ,

More information

1. Basic properties of Bernoulli and Euler polynomials. n 1. B k (n = 1, 2, 3, ). (1.1) k. k=0. E k (n = 1, 2, 3, ). (1.2) k=0

1. Basic properties of Bernoulli and Euler polynomials. n 1. B k (n = 1, 2, 3, ). (1.1) k. k=0. E k (n = 1, 2, 3, ). (1.2) k=0 A ecture given in Taiwan on June 6, 00. INTRODUCTION TO BERNOULLI AND EULER POLYNOMIALS Zhi-Wei Sun Departent of Matheatics Nanjing University Nanjing 10093 The Peope s Repubic of China E-ai: zwsun@nju.edu.cn

More information

Summation of p-adic Functional Series in Integer Points

Summation of p-adic Functional Series in Integer Points Fiomat 31:5 (2017), 1339 1347 DOI 10.2298/FIL1705339D Pubished by Facuty of Sciences and Mathematics, University of Niš, Serbia Avaiabe at: http://www.pmf.ni.ac.rs/fiomat Summation of p-adic Functiona

More information

The Group Structure on a Smooth Tropical Cubic

The Group Structure on a Smooth Tropical Cubic The Group Structure on a Smooth Tropica Cubic Ethan Lake Apri 20, 2015 Abstract Just as in in cassica agebraic geometry, it is possibe to define a group aw on a smooth tropica cubic curve. In this note,

More information

Volume 13, MAIN ARTICLES

Volume 13, MAIN ARTICLES Voume 13, 2009 1 MAIN ARTICLES THE BASIC BVPs OF THE THEORY OF ELASTIC BINARY MIXTURES FOR A HALF-PLANE WITH CURVILINEAR CUTS Bitsadze L. I. Vekua Institute of Appied Mathematics of Iv. Javakhishvii Tbiisi

More information

Chemical Kinetics Part 2

Chemical Kinetics Part 2 Integrated Rate Laws Chemica Kinetics Part 2 The rate aw we have discussed thus far is the differentia rate aw. Let us consider the very simpe reaction: a A à products The differentia rate reates the rate

More information

MA 201: Partial Differential Equations Lecture - 10

MA 201: Partial Differential Equations Lecture - 10 MA 201: Partia Differentia Equations Lecture - 10 Separation of Variabes, One dimensiona Wave Equation Initia Boundary Vaue Probem (IBVP) Reca: A physica probem governed by a PDE may contain both boundary

More information

Chemical Kinetics Part 2. Chapter 16

Chemical Kinetics Part 2. Chapter 16 Chemica Kinetics Part 2 Chapter 16 Integrated Rate Laws The rate aw we have discussed thus far is the differentia rate aw. Let us consider the very simpe reaction: a A à products The differentia rate reates

More information

Uniprocessor Feasibility of Sporadic Tasks with Constrained Deadlines is Strongly conp-complete

Uniprocessor Feasibility of Sporadic Tasks with Constrained Deadlines is Strongly conp-complete Uniprocessor Feasibiity of Sporadic Tasks with Constrained Deadines is Strongy conp-compete Pontus Ekberg and Wang Yi Uppsaa University, Sweden Emai: {pontus.ekberg yi}@it.uu.se Abstract Deciding the feasibiity

More information

Discrete Bernoulli s Formula and its Applications Arising from Generalized Difference Operator

Discrete Bernoulli s Formula and its Applications Arising from Generalized Difference Operator Int. Journa of Math. Anaysis, Vo. 7, 2013, no. 5, 229-240 Discrete Bernoui s Formua and its Appications Arising from Generaized Difference Operator G. Britto Antony Xavier 1 Department of Mathematics,

More information

17 Lecture 17: Recombination and Dark Matter Production

17 Lecture 17: Recombination and Dark Matter Production PYS 652: Astrophysics 88 17 Lecture 17: Recombination and Dark Matter Production New ideas pass through three periods: It can t be done. It probaby can be done, but it s not worth doing. I knew it was

More information

Discrete Applied Mathematics

Discrete Applied Mathematics Discrete Appied Mathematics 159 (2011) 812 825 Contents ists avaiabe at ScienceDirect Discrete Appied Mathematics journa homepage: www.esevier.com/ocate/dam A direct barter mode for course add/drop process

More information

A REFINEMENT OF KOBLITZ S CONJECTURE

A REFINEMENT OF KOBLITZ S CONJECTURE A REFINEMENT OF KOBLITZ S CONJECTURE DAVID ZYWINA Abstract. Let E be an eiptic curve over the rationas. In 1988, Kobitz conjectured an asymptotic for the number of primes p for which the cardinaity of

More information

Smoothness equivalence properties of univariate subdivision schemes and their projection analogues

Smoothness equivalence properties of univariate subdivision schemes and their projection analogues Numerische Mathematik manuscript No. (wi be inserted by the editor) Smoothness equivaence properties of univariate subdivision schemes and their projection anaogues Phiipp Grohs TU Graz Institute of Geometry

More information

Physics 116C Helmholtz s and Laplace s Equations in Spherical Polar Coordinates: Spherical Harmonics and Spherical Bessel Functions

Physics 116C Helmholtz s and Laplace s Equations in Spherical Polar Coordinates: Spherical Harmonics and Spherical Bessel Functions Physics 116C Hemhotz s an Lapace s Equations in Spherica Poar Coorinates: Spherica Harmonics an Spherica Besse Functions Peter Young Date: October 28, 2013) I. HELMHOLTZ S EQUATION As iscusse in cass,

More information

Lecture Note 3: Stationary Iterative Methods

Lecture Note 3: Stationary Iterative Methods MATH 5330: Computationa Methods of Linear Agebra Lecture Note 3: Stationary Iterative Methods Xianyi Zeng Department of Mathematica Sciences, UTEP Stationary Iterative Methods The Gaussian eimination (or

More information

1 Heat Equation Dirichlet Boundary Conditions

1 Heat Equation Dirichlet Boundary Conditions Chapter 3 Heat Exampes in Rectanges Heat Equation Dirichet Boundary Conditions u t (x, t) = ku xx (x, t), < x (.) u(, t) =, u(, t) = u(x, ) = f(x). Separate Variabes Look for simpe soutions in the

More information

Componentwise Determination of the Interval Hull Solution for Linear Interval Parameter Systems

Componentwise Determination of the Interval Hull Solution for Linear Interval Parameter Systems Componentwise Determination of the Interva Hu Soution for Linear Interva Parameter Systems L. V. Koev Dept. of Theoretica Eectrotechnics, Facuty of Automatics, Technica University of Sofia, 1000 Sofia,

More information

The EM Algorithm applied to determining new limit points of Mahler measures

The EM Algorithm applied to determining new limit points of Mahler measures Contro and Cybernetics vo. 39 (2010) No. 4 The EM Agorithm appied to determining new imit points of Maher measures by Souad E Otmani, Georges Rhin and Jean-Marc Sac-Épée Université Pau Veraine-Metz, LMAM,

More information

Laplace - Fibonacci transform by the solution of second order generalized difference equation

Laplace - Fibonacci transform by the solution of second order generalized difference equation Nonauton. Dyn. Syst. 017; 4: 30 Research Artice Open Access Sandra Pineas*, G.B.A Xavier, S.U. Vasantha Kumar, and M. Meganathan Lapace - Fibonacci transform by the soution of second order generaized difference

More information

Introduction to Simulation - Lecture 13. Convergence of Multistep Methods. Jacob White. Thanks to Deepak Ramaswamy, Michal Rewienski, and Karen Veroy

Introduction to Simulation - Lecture 13. Convergence of Multistep Methods. Jacob White. Thanks to Deepak Ramaswamy, Michal Rewienski, and Karen Veroy Introduction to Simuation - Lecture 13 Convergence of Mutistep Methods Jacob White Thans to Deepa Ramaswamy, Micha Rewiensi, and Karen Veroy Outine Sma Timestep issues for Mutistep Methods Loca truncation

More information

On nil-mccoy rings relative to a monoid

On nil-mccoy rings relative to a monoid PURE MATHEMATICS RESEARCH ARTICLE On ni-mccoy rings reative to a monoid Vahid Aghapouramin 1 * and Mohammad Javad Nikmehr 2 Received: 24 October 2017 Accepted: 29 December 2017 First Pubished: 25 January

More information

Biometrics Unit, 337 Warren Hall Cornell University, Ithaca, NY and. B. L. Raktoe

Biometrics Unit, 337 Warren Hall Cornell University, Ithaca, NY and. B. L. Raktoe NONISCMORPHIC CCMPLETE SETS OF ORTHOGONAL F-SQ.UARES, HADAMARD MATRICES, AND DECCMPOSITIONS OF A 2 4 DESIGN S. J. Schwager and w. T. Federer Biometrics Unit, 337 Warren Ha Corne University, Ithaca, NY

More information

PHYS 110B - HW #1 Fall 2005, Solutions by David Pace Equations referenced as Eq. # are from Griffiths Problem statements are paraphrased

PHYS 110B - HW #1 Fall 2005, Solutions by David Pace Equations referenced as Eq. # are from Griffiths Problem statements are paraphrased PHYS 110B - HW #1 Fa 2005, Soutions by David Pace Equations referenced as Eq. # are from Griffiths Probem statements are paraphrased [1.] Probem 6.8 from Griffiths A ong cyinder has radius R and a magnetization

More information

Strauss PDEs 2e: Section Exercise 1 Page 1 of 7

Strauss PDEs 2e: Section Exercise 1 Page 1 of 7 Strauss PDEs 2e: Section 4.3 - Exercise 1 Page 1 of 7 Exercise 1 Find the eigenvaues graphicay for the boundary conditions X(0) = 0, X () + ax() = 0. Assume that a 0. Soution The aim here is to determine

More information

Honors Thesis Bounded Query Functions With Limited Output Bits II

Honors Thesis Bounded Query Functions With Limited Output Bits II Honors Thesis Bounded Query Functions With Limited Output Bits II Daibor Zeený University of Maryand, Batimore County May 29, 2007 Abstract We sove some open questions in the area of bounded query function

More information

Quantum Mechanical Models of Vibration and Rotation of Molecules Chapter 18

Quantum Mechanical Models of Vibration and Rotation of Molecules Chapter 18 Quantum Mechanica Modes of Vibration and Rotation of Moecues Chapter 18 Moecuar Energy Transationa Vibrationa Rotationa Eectronic Moecuar Motions Vibrations of Moecues: Mode approximates moecues to atoms

More information

An explicit Jordan Decomposition of Companion matrices

An explicit Jordan Decomposition of Companion matrices An expicit Jordan Decomposition of Companion matrices Fermín S V Bazán Departamento de Matemática CFM UFSC 88040-900 Forianópois SC E-mai: fermin@mtmufscbr S Gratton CERFACS 42 Av Gaspard Coriois 31057

More information

Some Measures for Asymmetry of Distributions

Some Measures for Asymmetry of Distributions Some Measures for Asymmetry of Distributions Georgi N. Boshnakov First version: 31 January 2006 Research Report No. 5, 2006, Probabiity and Statistics Group Schoo of Mathematics, The University of Manchester

More information

Assignment 7 Due Tuessday, March 29, 2016

Assignment 7 Due Tuessday, March 29, 2016 Math 45 / AMCS 55 Dr. DeTurck Assignment 7 Due Tuessday, March 9, 6 Topics for this week Convergence of Fourier series; Lapace s equation and harmonic functions: basic properties, compuations on rectanges

More information