On Computational Applications of the Levi-Civita Field
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An Introduction to Nonstandard Analysis 11
AN INTRODUCTION TO NONSTANDARD ANALYSIS ISAAC DAVIS Abstract. In this paper we give an introduction to nonstandard analysis, starting with an ultrapower construction of the hyperreals. We then demon- strate how theorems in standard analysis \transfer over" to nonstandard anal- ysis, and how theorems in standard analysis can be proven using theorems in nonstandard analysis. 1. Introduction For many centuries, early mathematicians and physicists would solve problems by considering infinitesimally small pieces of a shape, or movement along a path by an infinitesimal amount. Archimedes derived the formula for the area of a circle by thinking of a circle as a polygon with infinitely many infinitesimal sides [1]. In particular, the construction of calculus was first motivated by this intuitive notion of infinitesimal change. G.W. Leibniz's derivation of calculus made extensive use of “infinitesimal” numbers, which were both nonzero but small enough to add to any real number without changing it noticeably. Although intuitively clear, infinitesi- mals were ultimately rejected as mathematically unsound, and were replaced with the common -δ method of computing limits and derivatives. However, in 1960 Abraham Robinson developed nonstandard analysis, in which the reals are rigor- ously extended to include infinitesimal numbers and infinite numbers; this new extended field is called the field of hyperreal numbers. The goal was to create a system of analysis that was more intuitively appealing than standard analysis but without losing any of the rigor of standard analysis. In this paper, we will explore the construction and various uses of nonstandard analysis. In section 2 we will introduce the notion of an ultrafilter, which will allow us to do a typical ultrapower construction of the hyperreal numbers. -
A Functional Equation Characterization of Archimedean Ordered Fields
A FUNCTIONAL EQUATION CHARACTERIZATION OF ARCHIMEDEAN ORDERED FIELDS RALPH HOWARD, VIRGINIA JOHNSON, AND GEORGE F. MCNULTY Abstract. We prove that an ordered field is Archimedean if and only if every continuous additive function from the field to itself is linear over the field. In 1821 Cauchy, [1], observed that any continuous function S on the real line that satisfies S(x + y) = S(x) + S(y) for all reals x and y is just multiplication by a constant. Another way to say this is that S is a linear operator on R, viewing R as a vector space over itself. The constant is evidently S(1). The displayed equation is Cauchy's functional equation and solutions to this equation are called additive. To see that Cauchy's result holds, note that only a small amount of work is needed to verify the following steps: first S(0) = 0, second S(−x) = −S(x), third S(nx) = S(x)n for all integers, and finally that S(r) = S(1)r for every rational number r. But then S and the function x 7! S(1)x are continuous functions that agree on a dense set (the rationals) and therefore are equal. So Cauchy's result follows, in part, from the fact that the rationals are dense in the reals. In 1875 Darboux, in [2], extended Cauchy's result by noting that if an additive function is continuous at just one point, then it is continuous everywhere. Therefore the conclusion of Cauchy's theorem holds under the weaker hypothesis that S is just continuous at a single point. -
Accessing Bernoulli-Numbers by Matrix-Operations Gottfried Helms 3'2006 Version 2.3
Accessing Bernoulli-Numbers by Matrix-Operations Gottfried Helms 3'2006 Version 2.3 Accessing Bernoulli-Numbers by Matrixoperations ........................................................................ 2 1. Introduction....................................................................................................................................................................... 2 2. A common equation of recursion (containing a significant error)..................................................................................... 3 3. Two versions B m and B p of bernoulli-numbers? ............................................................................................................... 4 4. Computation of bernoulli-numbers by matrixinversion of (P-I) ....................................................................................... 6 5. J contains the eigenvalues, and G m resp. G p contain the eigenvectors of P z resp. P s ......................................................... 7 6. The Binomial-Matrix and the Matrixexponential.............................................................................................................. 8 7. Bernoulli-vectors and the Matrixexponential.................................................................................................................... 8 8. The structure of the remaining coefficients in the matrices G m - and G p........................................................................... 9 9. The original problem of Jacob Bernoulli: "Powersums" - from G -
First-Order Continuous Induction, and a Logical Study of Real Closed Fields
c 2019 SAEED SALEHI & MOHAMMADSALEH ZARZA 1 First-Order Continuous Induction, and a Logical Study of Real Closed Fields⋆ Saeed Salehi Research Institute for Fundamental Sciences (RIFS), University of Tabriz, P.O.Box 51666–16471, Bahman 29th Boulevard, Tabriz, IRAN http://saeedsalehi.ir/ [email protected] Mohammadsaleh Zarza Department of Mathematics, University of Tabriz, P.O.Box 51666–16471, Bahman 29th Boulevard, Tabriz, IRAN [email protected] Abstract. Over the last century, the principle of “induction on the continuum” has been studied by differentauthors in differentformats. All of these differentreadings are equivalentto one of the arXiv:1811.00284v2 [math.LO] 11 Apr 2019 three versions that we isolate in this paper. We also formalize those three forms (of “continuous induction”) in first-order logic and prove that two of them are equivalent and sufficiently strong to completely axiomatize the first-order theory of the real closed (ordered) fields. We show that the third weaker form of continuous induction is equivalent with the Archimedean property. We study some equivalent axiomatizations for the theory of real closed fields and propose a first- order scheme of the fundamental theorem of algebra as an alternative axiomatization for this theory (over the theory of ordered fields). Keywords: First-Order Logic; Complete Theories; Axiomatizing the Field of Real Numbers; Continuous Induction; Real Closed Fields. 2010 AMS MSC: 03B25, 03C35, 03C10, 12L05. Address for correspondence: SAEED SALEHI, Research Institute for Fundamental Sciences (RIFS), University of Tabriz, P.O.Box 51666–16471, Bahman 29th Boulevard, Tabriz, IRAN. ⋆ This is a part of the Ph.D. thesis of the second author written under the supervision of the first author at the University of Tabriz, IRAN. -
Sums of Powers and the Bernoulli Numbers Laura Elizabeth S
Eastern Illinois University The Keep Masters Theses Student Theses & Publications 1996 Sums of Powers and the Bernoulli Numbers Laura Elizabeth S. Coen Eastern Illinois University This research is a product of the graduate program in Mathematics and Computer Science at Eastern Illinois University. Find out more about the program. Recommended Citation Coen, Laura Elizabeth S., "Sums of Powers and the Bernoulli Numbers" (1996). Masters Theses. 1896. https://thekeep.eiu.edu/theses/1896 This is brought to you for free and open access by the Student Theses & Publications at The Keep. It has been accepted for inclusion in Masters Theses by an authorized administrator of The Keep. For more information, please contact [email protected]. THESIS REPRODUCTION CERTIFICATE TO: Graduate Degree Candidates (who have written formal theses) SUBJECT: Permission to Reproduce Theses The University Library is rece1v1ng a number of requests from other institutions asking permission to reproduce dissertations for inclusion in their library holdings. Although no copyright laws are involved, we feel that professional courtesy demands that permission be obtained from the author before we allow theses to be copied. PLEASE SIGN ONE OF THE FOLLOWING STATEMENTS: Booth Library of Eastern Illinois University has my permission to lend my thesis to a reputable college or university for the purpose of copying it for inclusion in that institution's library or research holdings. u Author uate I respectfully request Booth Library of Eastern Illinois University not allow my thesis -
The Structure of Bernoulli Numbers
The structure of Bernoulli numbers Bernd C. Kellner Abstract We conjecture that the structure of Bernoulli numbers can be explicitly given in the closed form n 2 −1 −1 n−l −1 −1 Bn = (−1) |n|p |p (χ(p,l) − p−1 )|p p p,l ∈ irr p−1∤n ( ) Ψ1 p−1|n Y n≡l (modY p−1) Y irr where the χ(p,l) are zeros of certain p-adic zeta functions and Ψ1 is the set of irregular pairs. The more complicated but improbable case where the conjecture does not hold is also handled; we obtain an unconditional structural formula for Bernoulli numbers. Finally, applications are given which are related to classical results. Keywords: Bernoulli number, Kummer congruences, irregular prime, irregular pair of higher order, Riemann zeta function, p-adic zeta function Mathematics Subject Classification 2000: 11B68 1 Introduction The classical Bernoulli numbers Bn are defined by the power series ∞ z zn = B , |z| < 2π , ez − 1 n n! n=0 X where all numbers Bn are zero with odd index n > 1. The even-indexed rational 1 1 numbers Bn alternate in sign. First values are given by B0 = 1, B1 = − 2 , B2 = 6 , 1 arXiv:math/0411498v1 [math.NT] 22 Nov 2004 B4 = − 30 . Although the first numbers are small with |Bn| < 1 for n = 2, 4,..., 12, these numbers grow very rapidly with |Bn|→∞ for even n →∞. For now, let n be an even positive integer. An elementary property of Bernoulli numbers is the following discovered independently by T. Clausen [Cla40] and K. -
Tight Bounds on the Mutual Coherence of Sensing Matrices for Wigner D-Functions on Regular Grids
Tight bounds on the mutual coherence of sensing matrices for Wigner D-functions on regular grids Arya Bangun, Arash Behboodi, and Rudolf Mathar,∗ October 7, 2020 Abstract Many practical sampling patterns for function approximation on the rotation group utilizes regu- lar samples on the parameter axes. In this paper, we relate the mutual coherence analysis for sensing matrices that correspond to a class of regular patterns to angular momentum analysis in quantum mechanics and provide simple lower bounds for it. The products of Wigner d-functions, which ap- pear in coherence analysis, arise in angular momentum analysis in quantum mechanics. We first represent the product as a linear combination of a single Wigner d-function and angular momentum coefficients, otherwise known as the Wigner 3j symbols. Using combinatorial identities, we show that under certain conditions on the bandwidth and number of samples, the inner product of the columns of the sensing matrix at zero orders, which is equal to the inner product of two Legendre polynomials, dominates the mutual coherence term and fixes a lower bound for it. In other words, for a class of regular sampling patterns, we provide a lower bound for the inner product of the columns of the sensing matrix that can be analytically computed. We verify numerically our theoretical results and show that the lower bound for the mutual coherence is larger than Welch bound. Besides, we provide algorithms that can achieve the lower bound for spherical harmonics. 1 Introduction In many applications, the goal is to recover a function defined on a group, say on the sphere S2 and the rotation group SO(3), from only a few samples [1{5]. -
Higher Order Bernoulli and Euler Numbers
David Vella, Skidmore College [email protected] Generating Functions and Exponential Generating Functions • Given a sequence {푎푛} we can associate to it two functions determined by power series: • Its (ordinary) generating function is ∞ 풏 푓 풙 = 풂풏풙 풏=ퟏ • Its exponential generating function is ∞ 풂 품 풙 = 풏 풙풏 풏! 풏=ퟏ Examples • The o.g.f and the e.g.f of {1,1,1,1,...} are: 1 • f(x) = 1 + 푥 + 푥2 + 푥3 + ⋯ = , and 1−푥 푥 푥2 푥3 • g(x) = 1 + + + + ⋯ = 푒푥, respectively. 1! 2! 3! The second one explains the name... Operations on the functions correspond to manipulations on the sequence. For example, adding two sequences corresponds to adding the ogf’s, while to shift the index of a sequence, we multiply the ogf by x, or differentiate the egf. Thus, the functions provide a convenient way of studying the sequences. Here are a few more famous examples: Bernoulli & Euler Numbers • The Bernoulli Numbers Bn are defined by the following egf: x Bn n x x e 1 n1 n! • The Euler Numbers En are defined by the following egf: x 2e En n Sech(x) 2x x e 1 n0 n! Catalan and Bell Numbers • The Catalan Numbers Cn are known to have the ogf: ∞ 푛 1 − 1 − 4푥 2 퐶 푥 = 퐶푛푥 = = 2푥 1 + 1 − 4푥 푛=1 • Let Sn denote the number of different ways of partitioning a set with n elements into nonempty subsets. It is called a Bell number. It is known to have the egf: ∞ 푆 푥 푛 푥푛 = 푒 푒 −1 푛! 푛=1 Higher Order Bernoulli and Euler Numbers th w • The n Bernoulli Number of order w, B n is defined for positive integer w by: w x B w n xn x e 1 n1 n! th w • The n Euler Number of -
Approximation Properties of G-Bernoulli Polynomials
Approximation properties of q-Bernoulli polynomials M. Momenzadeh and I. Y. Kakangi Near East University Lefkosa, TRNC, Mersiin 10, Turkey Email: [email protected] [email protected] July 10, 2018 Abstract We study the q−analogue of Euler-Maclaurin formula and by introducing a new q-operator we drive to this form. Moreover, approximation properties of q-Bernoulli polynomials is discussed. We estimate the suitable functions as a combination of truncated series of q-Bernoulli polynomials and the error is calculated. This paper can be helpful in two different branches, first solving differential equations by estimating functions and second we may apply these techniques for operator theory. 1 Introduction The present study has sough to investigate the approximation of suitable function f(x) as a linear com- bination of q−Bernoulli polynomials. This study by using q−operators through a parallel way has achived to the kind of Euler expansion for f(x), and expanded the function in terms of q−Bernoulli polynomials. This expansion offers a proper tool to solve q-difference equations or normal differential equation as well. There are many approaches to approximate the capable functions. According to properties of q-functions many q-function have been used in order to approximate a suitable function.For example, at [28], some identities and formulae for the q-Bernstein basis function, including the partition of unity property, formulae for representing the monomials were studied. In addition, a kind of approximation of a function in terms of Bernoulli polynomials are used in several approaches for solving differential equations, such as [7, 20, 21]. -
สมบัติหลักมูลของฟีลด์อันดับ Fundamental Properties Of
DOI: 10.14456/mj-math.2018.5 วารสารคณิตศาสตร์ MJ-MATh 63(694) Jan–Apr, 2018 โดย สมาคมคณิตศาสตร์แห่งประเทศไทย ในพระบรมราชูปถัมภ์ http://MathThai.Org [email protected] สมบตั ิหลกั มูลของฟี ลดอ์ นั ดบั Fundamental Properties of Ordered Fields ภัทราวุธ จันทร์เสงี่ยม Pattrawut Chansangiam Department of Mathematics, Faculty of Science, King Mongkut’s Institute of Technology Ladkrabang, Ladkrabang, Bangkok, 10520, Thailand Email: [email protected] บทคดั ย่อ เราอภิปรายสมบัติเชิงพีชคณิต สมบัติเชิงอันดับและสมบัติเชิงทอพอโลยีที่สาคัญของ ฟีลด์อันดับ ในข้อเท็จจริงนั้น ค่าสัมบูรณ์ในฟีลด์อันดับใดๆ มีสมบัติคล้ายกับค่าสัมบูรณ์ของ จ านวนจริง เราให้บทพิสูจน์อย่างง่ายของการสมมูลกันระหว่าง สมบัติอาร์คิมีดิสกับความ หนาแน่น ของฟีลด์ย่อยตรรกยะ เรายังให้เงื่อนไขที่สมมูลกันสาหรับ ฟีลด์อันดับที่จะมีสมบัติ อาร์คิมีดิส ซึ่งเกี่ยวกับการลู่เข้าของลาดับและการทดสอบอนุกรมเรขาคณิต คำส ำคัญ: ฟิลด์อันดับ สมบัติของอาร์คิมีดิส ฟีลด์ย่อยตรรกยะ อนุกรมเรขาคณิต ABSTRACT We discuss fundamental algebraic-order-topological properties of ordered fields. In fact, the absolute value in any ordered field has properties similar to those of real numbers. We give a simple proof of the equivalence between the Archimedean property and the density of the rational subfield. We also provide equivalent conditions for an ordered field to be Archimedean, involving convergence of certain sequences and the geometric series test. Keywords: Ordered Field, Archimedean Property, Rational Subfield, Geometric Series วารสารคณิตศาสตร์ MJ-MATh 63(694) Jan-Apr, 2018 37 1. Introduction to those of -
Euler-Maclaurin Summation Formula
4 Euler-Maclaurin Summation Formula 4.1 Bernoulli Number & Bernoulli Polynomial 4.1.1 Definition of Bernoulli Number Bernoulli numbers Bk ()k =1,2,3, are defined as coefficients of the following equation. x Bk k x =Σ x e -1 k=0 k! 4.1.2 Expreesion of Bernoulli Numbers B B x 0 1 B2 2 B3 3 B4 4 = + x + x + x + x + (1,1) ex-1 0! 1! 2! 3! 4! ex-1 1 x x2 x3 x4 = + + + + + (1.2) x 1! 2! 3! 4! 5! Making the Cauchy product of (1.1) and (1.1) , B1 B0 B2 B1 B0 1 = B + + x + + + x2 + 0 1!1! 0!2! 2!1! 1!2! 0!3! In order to holds this for arbitrary x , B1 B0 B2 B1 B0 B =1 , + =0 , + + =0 , 0 1!1! 0!2! 2!1! 1!2! 0!3! n The coefficient of x is as follows. Bn Bn-1 Bn-2 B1 B0 + + + + + = 0 n!1! ()n -1 !2! ()n-2 !3! 1!n ! 0!()n +1 ! Multiplying both sides by ()n +1 ! , Bn()n +1 ! Bn-1()n+1 ! Bn-2()n +1 ! B1()n +1 ! B0 + + + + + = 0 n !1! ()n-1 !2! ()n -2 !3! 1!n ! 0! Using binomial coefficiets, n +1Cn Bn + n +1Cn-1 Bn-1 + n +1Cn-2 Bn-2 + + n +1C 1 B1 + n +1C 0 B0 = 0 Replacing n +1 with n , (1.3) nnC -1 Bn-1 + nnC -2 Bn-2 + nnC -3 Bn-3 + + nC1 B1 + nC0 B0 = 0 Substituting n =2, 3, 4, for this one by one, 1 21C B + 20C B = 0 B = - 1 0 2 2 1 32C B + 31C B + 30C B = 0 B = 2 1 0 2 6 Thus, we obtain Bernoulli numbers. -
Mathstudio Manual
MathStudio Manual Abs(z) Returns the complex modulus (or magnitude) of a complex number. abs(-3) abs(-x) abs(\im) AiryAi(z) Returns the Airy function Ai(z). AiryAi(2) AiryAi(3-\im) AiryAi(\pi/2) AiryAi(-9) Plot(AiryAi(x),x=[-10,1],numbers=0) Page 1/187 MathStudio Manual AiryBi(z) Returns the Airy function Bi(z). AiryBi(0) AiryBi(10) AiryBi(1+\im) Plot(AiryBi(x),x=[-10,1],numbers=0) AlternatingSeries(n, [terms]) Page 2/187 MathStudio Manual This function approximates the given real number in an alternating series. The result is returned in a matrix with the top row = numerator and the bottom row = denominator of the different terms. Note the alternating sign in the numerator! AlternatingSeries(\pi,7) AlternatingSeries(ln(2),10) AlternatingSeries(sqrt(2),10) AlternatingSeries(-3.23) AlternatingSeries(123456789/987654321) AlternatingSeries(.666) AlternatingSeries(.12121212) Page 3/187 MathStudio Manual AlternatingSeries(.36363) Angle(A, B) Returns the angle between the two vectors A and B. Angle([a@1,b@1,c@1],[a@2,b@2,c@2]) Angle([1,2,3],[4,5,6]) Animate(variable, start, end, [step]) This function creates an animated entry. The variable is initialized to the start value and at each frame is incremented by step and the entry is reevaluated creating animation. When the variable is greater than the value end it is set back to start. Animate(n,1,100) ImagePlot(Random(0,1,n,n)) Page 4/187 MathStudio Manual Apart(f(x), x) Performs partial fraction decomposition on the polynomial function. Apart performs the opposite operation of Together.