Introduction to the Gamma Function
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Class 1/28 1 Zeros of an Analytic Function
Math 752 Spring 2011 Class 1/28 1 Zeros of an analytic function Towards the fundamental theorem of algebra and its statement for analytic functions. Definition 1. Let f : G → C be analytic and f(a) = 0. a is said to have multiplicity m ≥ 1 if there exists an analytic function g : G → C with g(a) 6= 0 so that f(z) = (z − a)mg(z). Definition 2. If f is analytic in C it is called entire. An entire function has a power series expansion with infinite radius of convergence. Theorem 1 (Liouville’s Theorem). If f is a bounded entire function then f is constant. 0 Proof. Assume |f(z)| ≤ M for all z ∈ C. Use Cauchy’s estimate for f to obtain that |f 0(z)| ≤ M/R for every R > 0 and hence equal to 0. Theorem 2 (Fundamental theorem of algebra). For every non-constant polynomial there exists a ∈ C with p(a) = 0. Proof. Two facts: If p has degree ≥ 1 then lim p(z) = ∞ z→∞ where the limit is taken along any path to ∞ in C∞. (Sometimes also written as |z| → ∞.) If p has no zero, its reciprocal is therefore entire and bounded. Invoke Liouville’s theorem. Corollary 1. If p is a polynomial with zeros aj (multiplicity kj) then p(z) = k k km c(z − a1) 1 (z − a2) 2 ...(z − am) . Proof. Induction, and the fact that p(z)/(z − a) is a polynomial of degree n − 1 if p(a) = 0. 1 The zero function is the only analytic function that has a zero of infinite order. -
Introduction to Analytic Number Theory the Riemann Zeta Function and Its Functional Equation (And a Review of the Gamma Function and Poisson Summation)
Math 229: Introduction to Analytic Number Theory The Riemann zeta function and its functional equation (and a review of the Gamma function and Poisson summation) Recall Euler’s identity: ∞ ∞ X Y X Y 1 [ζ(s) :=] n−s = p−cps = . (1) 1 − p−s n=1 p prime cp=0 p prime We showed that this holds as an identity between absolutely convergent sums and products for real s > 1. Riemann’s insight was to consider (1) as an identity between functions of a complex variable s. We follow the curious but nearly universal convention of writing the real and imaginary parts of s as σ and t, so s = σ + it. We already observed that for all real n > 0 we have |n−s| = n−σ, because n−s = exp(−s log n) = n−σe−it log n and e−it log n has absolute value 1; and that both sides of (1) converge absolutely in the half-plane σ > 1, and are equal there either by analytic continuation from the real ray t = 0 or by the same proof we used for the real case. Riemann showed that the function ζ(s) extends from that half-plane to a meromorphic function on all of C (the “Riemann zeta function”), analytic except for a simple pole at s = 1. The continuation to σ > 0 is readily obtained from our formula ∞ ∞ 1 X Z n+1 X Z n+1 ζ(s) − = n−s − x−s dx = (n−s − x−s) dx, s − 1 n=1 n n=1 n since for x ∈ [n, n + 1] (n ≥ 1) and σ > 0 we have Z x −s −s −1−s −1−σ |n − x | = s y dy ≤ |s|n n so the formula for ζ(s) − (1/(s − 1)) is a sum of analytic functions converging absolutely in compact subsets of {σ + it : σ > 0} and thus gives an analytic function there. -
The Digamma Function and Explicit Permutations of the Alternating Harmonic Series
The digamma function and explicit permutations of the alternating harmonic series. Maxim Gilula February 20, 2015 Abstract The main goal is to present a countable family of permutations of the natural numbers that provide explicit rearrangements of the alternating harmonic series and that we can easily define by some closed expression. The digamma function presents its ubiquity in mathematics once more by being the key tool in computing explicitly the simple rearrangements presented in this paper. The permutations are simple in the sense that composing one with itself will give the identity. We show that the count- able set of rearrangements presented are dense in the reals. Then, slight generalizations are presented. Finally, we reprove a result given originally by J.H. Smith in 1975 that for any conditionally convergent real series guarantees permutations of infinite cycle type give all rearrangements of the series [4]. This result provides a refinement of the well known theorem by Riemann (see e.g. Rudin [3] Theorem 3.54). 1 Introduction A permutation of order n of a conditionally convergent series is a bijection φ of the positive integers N with the property that φn = φ ◦ · · · ◦ φ is the identity on N and n is the least such. Given a conditionally convergent series, a nat- ural question to ask is whether for any real number L there is a permutation of order 2 (or n > 1) such that the rearrangement induced by the permutation equals L. This turns out to be an easy corollary of [4], and is reproved below with elementary methods. Other \simple"rearrangements have been considered elsewhere, such as in Stout [5] and the comprehensive references therein. -
On the Stability of a Cauchy Type Functional Equation
Demonstr. Math. 2018; 51:323–331 Research Article Open Access Abbas Najati, Jung Rye Lee*, Choonkil Park, and Themistocles M. Rassias On the stability of a Cauchy type functional equation https://doi.org/10.1515/dema-2018-0026 Received May 31, 2018; accepted November 11, 2018 Abstract: In this work, the Hyers-Ulam type stability and the hyperstability of the functional equation (︁ x + y )︁ (︁ x − y )︁ f + xy + f − xy = f(x) 2 2 are proved. Keywords: Hyers-Ulam stability, additive mapping, hyperstability, topological vector space MSC: 39B82, 34K20, 26D10 1 Introduction The functional equation (ξ) is called stable if any function g satisfying the equation (ξ) approximately, is near to a true solution of (ξ). Ulam, in 1940 [1], introduced the stability of homomorphisms between two groups. More precisely, he proposed the following problem: given a group (G1,.), a metric group (G2, *, d) and a positive number ϵ, does there exist a δ > 0 such that if a function f : G1 ! G2 satisfies the inequal- ity d(f (x.y), f (x) * f(y)) < δ for all x, y 2 G1, then there exists a homomorphism T : G1 ! G2 such that d(f(x), T(x)) < ϵ for all x 2 G1? If this problem has a solution, we say that the homomorphisms from G1 to G2 are stable. In 1941, Hyers [2] gave a partial solution of Ulam’s problem for the case of approximate addi- tive mappings under the assumption that G1 and G2 are Banach spaces. Aoki [3] and Rassias [4] provided a generalization of the Hyers’ theorem for additive and linear mappings, respectively, by allowing the Cauchy difference to be unbounded. -
Topic 7 Notes 7 Taylor and Laurent Series
Topic 7 Notes Jeremy Orloff 7 Taylor and Laurent series 7.1 Introduction We originally defined an analytic function as one where the derivative, defined as a limit of ratios, existed. We went on to prove Cauchy's theorem and Cauchy's integral formula. These revealed some deep properties of analytic functions, e.g. the existence of derivatives of all orders. Our goal in this topic is to express analytic functions as infinite power series. This will lead us to Taylor series. When a complex function has an isolated singularity at a point we will replace Taylor series by Laurent series. Not surprisingly we will derive these series from Cauchy's integral formula. Although we come to power series representations after exploring other properties of analytic functions, they will be one of our main tools in understanding and computing with analytic functions. 7.2 Geometric series Having a detailed understanding of geometric series will enable us to use Cauchy's integral formula to understand power series representations of analytic functions. We start with the definition: Definition. A finite geometric series has one of the following (all equivalent) forms. 2 3 n Sn = a(1 + r + r + r + ::: + r ) = a + ar + ar2 + ar3 + ::: + arn n X = arj j=0 n X = a rj j=0 The number r is called the ratio of the geometric series because it is the ratio of consecutive terms of the series. Theorem. The sum of a finite geometric series is given by a(1 − rn+1) S = a(1 + r + r2 + r3 + ::: + rn) = : (1) n 1 − r Proof. -
Algebraic Generality Vs Arithmetic Generality in the Controversy Between C
Algebraic generality vs arithmetic generality in the controversy between C. Jordan and L. Kronecker (1874). Frédéric Brechenmacher (1). Introduction. Throughout the whole year of 1874, Camille Jordan and Leopold Kronecker were quarrelling over two theorems. On the one hand, Jordan had stated in his 1870 Traité des substitutions et des équations algébriques a canonical form theorem for substitutions of linear groups; on the other hand, Karl Weierstrass had introduced in 1868 the elementary divisors of non singular pairs of bilinear forms (P,Q) in stating a complete set of polynomial invariants computed from the determinant |P+sQ| as a key theorem of the theory of bilinear and quadratic forms. Although they would be considered equivalent as regard to modern mathematics (2), not only had these two theorems been stated independently and for different purposes, they had also been lying within the distinct frameworks of two theories until some connections came to light in 1872-1873, breeding the 1874 quarrel and hence revealing an opposition over two practices relating to distinctive cultural features. As we will be focusing in this paper on how the 1874 controversy about Jordan’s algebraic practice of canonical reduction and Kronecker’s arithmetic practice of invariant computation sheds some light on two conflicting perspectives on polynomial generality we shall appeal to former publications which have already been dealing with some of the cultural issues highlighted by this controversy such as tacit knowledge, local ways of thinking, internal philosophies and disciplinary ideals peculiar to individuals or communities [Brechenmacher 200?a] as well as the different perceptions expressed by the two opponents of a long term history involving authors such as Joseph-Louis Lagrange, Augustin Cauchy and Charles Hermite [Brechenmacher 200?b]. -
Infinite Product of a Number
International Journal of Pure and Applied Mathematical Sciences. ISSN 0972-9828 Volume 10, Number 2 (2017), pp. 107-110 © Research India Publications http://www.ripublication.com Infinite Product of a Number Rushal Sohal Student The Lexicon International School, Wagholi, Pune, India. Abstract It seems that multiplying a positive number infinite times would give something extremely huge (infinity), but is it so? In this paper, we will show that any positive integer (>1) raised to the power infinity (i.e. infinite product of n ∞ ∞ =∏푖=1 푛=푛×푛×푛...= 푛 , 푛 > 1) is not infinity; we will use simple mathematical equations and also use some known sums to prove that the infinite product of a positive integer (>1) is not equal to infinity, ∞i.e. 푛∞ ≠ . Keywords: positive integer(퐼+); infinity*(∞); Riemann zeta function 휁(푠). 1. INTRODUCTION So, what is the infinite product of a positive integer (>1), i.e. what is 푛∞? Is it ∞ or something else? Till now, not much research has been done on this topic, and by convention we assume 푛∞ to be equal to ∞. In this paper, we will make simple equations and also use some known sums and prove that 푛∞ = 0 and that, it is not equal to ∞. We are going to approach the problem by observing patterns, assigning and re- assigning variables, and finally solving the equations. But first, we need to prove that 푛∞ ≠ ∞. 2. METHODS The methods for solving the problem are simple but a bit counter-intuitive. In this paper, we will make simple mathematical equations and firstly prove that 푛∞ ≠ ∞. -
Regularized Integral Representations of the Reciprocal Function
Preprints (www.preprints.org) | NOT PEER-REVIEWED | Posted: 25 December 2018 doi:10.20944/preprints201812.0310.v1 Peer-reviewed version available at Fractal Fract 2019, 3, 1; doi:10.3390/fractalfract3010001 Article Regularized Integral Representations of the Reciprocal G Function Dimiter Prodanov Correspondence: Environment, Health and Safety, IMEC vzw, Kapeldreef 75, 3001 Leuven, Belgium; [email protected]; [email protected] Version December 25, 2018 submitted to Preprints 1 Abstract: This paper establishes a real integral representation of the reciprocal G function in terms 2 of a regularized hypersingular integral. The equivalence with the usual complex representation is 3 demonstrated. A regularized complex representation along the usual Hankel path is derived. 4 Keywords: gamma function; reciprocal gamma function; integral equation 5 MSC: 33B15; 65D20, 30D10 6 1. Introduction 7 Applications of the Gamma function are ubiquitous in fractional calculus and the special function 8 theory. It has numerous interesting properties summarized in [1]. It is indispensable in the theory of 9 Laplace transforms. The history of the Gamma function is surveyed in [2]. In a previous note I have 10 investigated an approach to regularize derivatives at points, where the ordinary limit diverges [5]. 11 This paper exploits the same approach for the purposes of numerical computation of singular integrals, 12 such as the Euler G integrals for negative arguments. The paper also builds on an observations in [4]. 13 The present paper proves a real singular integral representation of the reciprocal G function. The 14 algorithm is implemented in the Computer Algebra System Maxima for reference and demonstration 15 purposes. -
The Riemann and Hurwitz Zeta Functions, Apery's Constant and New
The Riemann and Hurwitz zeta functions, Apery’s constant and new rational series representations involving ζ(2k) Cezar Lupu1 1Department of Mathematics University of Pittsburgh Pittsburgh, PA, USA Algebra, Combinatorics and Geometry Graduate Student Research Seminar, February 2, 2017, Pittsburgh, PA A quick overview of the Riemann zeta function. The Riemann zeta function is defined by 1 X 1 ζ(s) = ; Re s > 1: ns n=1 Originally, Riemann zeta function was defined for real arguments. Also, Euler found another formula which relates the Riemann zeta function with prime numbrs, namely Y 1 ζ(s) = ; 1 p 1 − ps where p runs through all primes p = 2; 3; 5;:::. A quick overview of the Riemann zeta function. Moreover, Riemann proved that the following ζ(s) satisfies the following integral representation formula: 1 Z 1 us−1 ζ(s) = u du; Re s > 1; Γ(s) 0 e − 1 Z 1 where Γ(s) = ts−1e−t dt, Re s > 0 is the Euler gamma 0 function. Also, another important fact is that one can extend ζ(s) from Re s > 1 to Re s > 0. By an easy computation one has 1 X 1 (1 − 21−s )ζ(s) = (−1)n−1 ; ns n=1 and therefore we have A quick overview of the Riemann function. 1 1 X 1 ζ(s) = (−1)n−1 ; Re s > 0; s 6= 1: 1 − 21−s ns n=1 It is well-known that ζ is analytic and it has an analytic continuation at s = 1. At s = 1 it has a simple pole with residue 1. -
INTEGRALS of POWERS of LOGGAMMA 1. Introduction The
PROCEEDINGS OF THE AMERICAN MATHEMATICAL SOCIETY Volume 139, Number 2, February 2011, Pages 535–545 S 0002-9939(2010)10589-0 Article electronically published on August 18, 2010 INTEGRALS OF POWERS OF LOGGAMMA TEWODROS AMDEBERHAN, MARK W. COFFEY, OLIVIER ESPINOSA, CHRISTOPH KOUTSCHAN, DANTE V. MANNA, AND VICTOR H. MOLL (Communicated by Ken Ono) Abstract. Properties of the integral of powers of log Γ(x) from 0 to 1 are con- sidered. Analytic evaluations for the first two powers are presented. Empirical evidence for the cubic case is discussed. 1. Introduction The evaluation of definite integrals is a subject full of interconnections of many parts of mathematics. Since the beginning of Integral Calculus, scientists have developed a large variety of techniques to produce magnificent formulae. A partic- ularly beautiful formula due to J. L. Raabe [12] is 1 Γ(x + t) (1.1) log √ dx = t log t − t, for t ≥ 0, 0 2π which includes the special case 1 √ (1.2) L1 := log Γ(x) dx =log 2π. 0 Here Γ(x)isthegamma function defined by the integral representation ∞ (1.3) Γ(x)= ux−1e−udu, 0 for Re x>0. Raabe’s formula can be obtained from the Hurwitz zeta function ∞ 1 (1.4) ζ(s, q)= (n + q)s n=0 via the integral formula 1 t1−s (1.5) ζ(s, q + t) dq = − 0 s 1 coupled with Lerch’s formula ∂ Γ(q) (1.6) ζ(s, q) =log √ . ∂s s=0 2π An interesting extension of these formulas to the p-adic gamma function has recently appeared in [3]. -
The History of the Abel Prize and the Honorary Abel Prize the History of the Abel Prize
The History of the Abel Prize and the Honorary Abel Prize The History of the Abel Prize Arild Stubhaug On the bicentennial of Niels Henrik Abel’s birth in 2002, the Norwegian Govern- ment decided to establish a memorial fund of NOK 200 million. The chief purpose of the fund was to lay the financial groundwork for an annual international prize of NOK 6 million to one or more mathematicians for outstanding scientific work. The prize was awarded for the first time in 2003. That is the history in brief of the Abel Prize as we know it today. Behind this government decision to commemorate and honor the country’s great mathematician, however, lies a more than hundred year old wish and a short and intense period of activity. Volumes of Abel’s collected works were published in 1839 and 1881. The first was edited by Bernt Michael Holmboe (Abel’s teacher), the second by Sophus Lie and Ludvig Sylow. Both editions were paid for with public funds and published to honor the famous scientist. The first time that there was a discussion in a broader context about honoring Niels Henrik Abel’s memory, was at the meeting of Scan- dinavian natural scientists in Norway’s capital in 1886. These meetings of natural scientists, which were held alternately in each of the Scandinavian capitals (with the exception of the very first meeting in 1839, which took place in Gothenburg, Swe- den), were the most important fora for Scandinavian natural scientists. The meeting in 1886 in Oslo (called Christiania at the time) was the 13th in the series. -
Applied Mathematics Letters Exponential Functional Equation On
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Elsevier - Publisher Connector Applied Mathematics Letters 23 (2010) 156–160 Contents lists available at ScienceDirect Applied Mathematics Letters journal homepage: www.elsevier.com/locate/aml Exponential functional equation on spheres Justyna Sikorska Institute of Mathematics, Silesian University, Bankowa 14, PL-40-007 Katowice, Poland article info a b s t r a c t Article history: We study the exponential functional equation f .x C y/ D f .x/f .y/ on spheres in real Received 28 February 2009 normed linear spaces. Regardless of the solutions of this equation, which are already Received in revised form 4 September 2009 known, we investigate its stability and consider the pexiderized version of it. Accepted 4 September 2009 ' 2009 Elsevier Ltd. All rights reserved. Keywords: Conditional exponential functional equation Stability Approximation 1. Introduction Alsina and Garcia-Roig [1] considered the conditional functional equation f .x C y/ D f .x/ C f .y/ whenever kxk D kyk (1) with a continuous function f : X ! Y mapping a real inner product space .X; h·; ·i/ with dim X ≥ 2 into a real topological vector space Y . In [2], Szabó solved (1) in case where .X; k · k/ is a real normed linear space with dim X ≥ 3 and .Y ; C/ is an Abelian group. In [3], Ger and the author proceeded with the study of (1) with the norm replaced by an abstract function fulfilling suitable conditions. We dealt also with more general structures than those considered in [1,2].