An Introduction to the Bernoulli Function
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An Identity for Generalized Bernoulli Polynomials
1 2 Journal of Integer Sequences, Vol. 23 (2020), 3 Article 20.11.2 47 6 23 11 An Identity for Generalized Bernoulli Polynomials Redha Chellal1 and Farid Bencherif LA3C, Faculty of Mathematics USTHB Algiers Algeria [email protected] [email protected] [email protected] Mohamed Mehbali Centre for Research Informed Teaching London South Bank University London United Kingdom [email protected] Abstract Recognizing the great importance of Bernoulli numbers and Bernoulli polynomials in various branches of mathematics, the present paper develops two results dealing with these objects. The first one proposes an identity for the generalized Bernoulli poly- nomials, which leads to further generalizations for several relations involving classical Bernoulli numbers and Bernoulli polynomials. In particular, it generalizes a recent identity suggested by Gessel. The second result allows the deduction of similar identi- ties for Fibonacci, Lucas, and Chebyshev polynomials, as well as for generalized Euler polynomials, Genocchi polynomials, and generalized numbers of Stirling. 1Corresponding author. 1 1 Introduction Let N and C denote, respectively, the set of positive integers and the set of complex numbers. (α) In his book, Roman [41, p. 93] defined generalized Bernoulli polynomials Bn (x) as follows: for all n ∈ N and α ∈ C, we have ∞ tn t α B(α)(x) = etx. (1) n n! et − 1 Xn=0 The Bernoulli numbers Bn, classical Bernoulli polynomials Bn(x), and generalized Bernoulli (α) numbers Bn are, respectively, defined by (1) (α) (α) Bn = Bn(0), Bn(x)= Bn (x), and Bn = Bn (0). (2) The Bernoulli numbers and the Bernoulli polynomials play a fundamental role in various branches of mathematics, such as combinatorics, number theory, mathematical analysis, and topology. -
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 -
A Note on Some Constants Related to the Zeta–Function and Their Relationship with the Gregory Coefficients
A note on some constants related to the zeta–function and their relationship with the Gregory coefficients Iaroslav V. Blagouchine∗ Steklov Institute of Mathematics at St.-Petersburg, Russia. Marc–Antoine Coppo Université Côte d’Azur, CNRS, LJAD (UMR 7351), France. Abstract In this article, new series for the first and second Stieltjes constants (also known as generalized Eu- ler’s constant), as well as for some closely related constants are obtained. These series contain rational terms only and involve the so–called Gregory coefficients, which are also known as (reciprocal) log- arithmic numbers, Cauchy numbers of the first kind and Bernoulli numbers of the second kind. In addition, two interesting series with rational terms for Euler’s constant g and the constant ln 2p are given, and yet another generalization of Euler’s constant is proposed and various formulas for the cal- culation of these constants are obtained. Finally, we mention in the paper that almost all the constants considered in this work admit simple representations via the Ramanujan summation. Keywords: Stieltjes constants, Generalized Euler’s constants, Series expansions, Ramanujan summation, Harmonic product of sequences, Gregory’s coefficients, Logarithmic numbers, Cauchy numbers, Bernoulli numbers of the second kind, Stirling numbers of the first kind, Harmonic numbers. I. Introduction and definitions The zeta-function ¥ z(s) := ∑ n−s , Re s > 1, n=1 is of fundamental and long-standing importance in analytic number theory, modern analysis, theory of L–functions, prime number theory and in a variety of other fields. The z–function is a meromorphic function on the entire complex plane, except at the point s = 1 at which it has one simple pole with residue 1. -
A New Family of Zeta Type Functions Involving the Hurwitz Zeta Function and the Alternating Hurwitz Zeta Function
mathematics Article A New Family of Zeta Type Functions Involving the Hurwitz Zeta Function and the Alternating Hurwitz Zeta Function Daeyeoul Kim 1,* and Yilmaz Simsek 2 1 Department of Mathematics and Institute of Pure and Applied Mathematics, Jeonbuk National University, Jeonju 54896, Korea 2 Department of Mathematics, Faculty of Science, University of Akdeniz, Antalya TR-07058, Turkey; [email protected] * Correspondence: [email protected] Abstract: In this paper, we further study the generating function involving a variety of special numbers and ploynomials constructed by the second author. Applying the Mellin transformation to this generating function, we define a new class of zeta type functions, which is related to the interpolation functions of the Apostol–Bernoulli polynomials, the Bernoulli polynomials, and the Euler polynomials. This new class of zeta type functions is related to the Hurwitz zeta function, the alternating Hurwitz zeta function, and the Lerch zeta function. Furthermore, by using these functions, we derive some identities and combinatorial sums involving the Bernoulli numbers and polynomials and the Euler numbers and polynomials. Keywords: Bernoulli numbers and polynomials; Euler numbers and polynomials; Apostol–Bernoulli and Apostol–Euler numbers and polynomials; Hurwitz–Lerch zeta function; Hurwitz zeta function; alternating Hurwitz zeta function; generating function; Mellin transformation MSC: 05A15; 11B68; 26C0; 11M35 Citation: Kim, D.; Simsek, Y. A New Family of Zeta Type Function 1. Introduction Involving the Hurwitz Zeta Function The families of zeta functions and special numbers and polynomials have been studied and the Alternating Hurwitz Zeta widely in many areas. They have also been used to model real-world problems. -
The Euler-Maclaurin Summation Formula and Bernoulli Polynomials R 1 Consider Two Different Ways of Applying Integration by Parts to 0 F(X)Dx
The Euler-Maclaurin Summation Formula and Bernoulli Polynomials R 1 Consider two different ways of applying integration by parts to 0 f(x)dx. Z 1 Z 1 Z 1 1 0 0 f(x)dx = [xf(x)]0 − xf (x)dx = f(1) − xf (x)dx (1) 0 0 0 Z 1 Z 1 Z 1 1 0 f(1) + f(0) 0 f(x)dx = [(x − 1/2)f(x)]0 − (x − 1/2)f (x)dx = − (x − 1/2)f (x)dx (2) 0 0 2 0 The constant of integration was chosen to be 0 in (1), but −1/2 in (2). Which way is better? In general R 1 (2) is better. Since 0 (x − 1/2)dx = 0, that is x − 1/2 has zero average in (0, 1), it has better chance of reducing the last integral term, which is regarded as the error in estimating the given integral. We can again apply integration by parts to (2). Then the last integral will have f 00(x) multiplied by an integral of x − 1/2. We can select the constant of integration in such a way that the new polynomial multiplying f 00(x) will have zero average in the interval. If we continue this way we will get a formula which will have a higher derivative of f in the last integral multiplying a higher degree polynomial in x. If at each step the constant of integration is chosen in such a way that the new polynomial has zero average over (0, 1), we will get the Euler-Maclaurin summation formula. -
Two Series Expansions for the Logarithm of the Gamma Function Involving Stirling Numbers and Containing Only Rational −1 Coefficients for Certain Arguments Related to Π
J. Math. Anal. Appl. 442 (2016) 404–434 Contents lists available at ScienceDirect Journal of Mathematical Analysis and Applications www.elsevier.com/locate/jmaa Two series expansions for the logarithm of the gamma function involving Stirling numbers and containing only rational −1 coefficients for certain arguments related to π Iaroslav V. Blagouchine ∗ University of Toulon, France a r t i c l e i n f o a b s t r a c t Article history: In this paper, two new series for the logarithm of the Γ-function are presented and Received 10 September 2015 studied. Their polygamma analogs are also obtained and discussed. These series Available online 21 April 2016 involve the Stirling numbers of the first kind and have the property to contain only Submitted by S. Tikhonov − rational coefficients for certain arguments related to π 1. In particular, for any value of the form ln Γ( 1 n ± απ−1)andΨ ( 1 n ± απ−1), where Ψ stands for the Keywords: 2 k 2 k 1 Gamma function kth polygamma function, α is positive rational greater than 6 π, n is integer and k Polygamma functions is non-negative integer, these series have rational terms only. In the specified zones m −2 Stirling numbers of convergence, derived series converge uniformly at the same rate as (n ln n) , Factorial coefficients where m =1, 2, 3, ..., depending on the order of the polygamma function. Explicit Gregory’s coefficients expansions into the series with rational coefficients are given for the most attracting Cauchy numbers −1 −1 1 −1 −1 1 −1 values, such as ln Γ(π ), ln Γ(2π ), ln Γ( 2 + π ), Ψ(π ), Ψ( 2 + π )and −1 Ψk(π ). -
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. -
Expansions of Generalized Euler's Constants Into the Series Of
Journal of Number Theory 158 (2016) 365–396 Contents lists available at ScienceDirect Journal of Number Theory www.elsevier.com/locate/jnt Expansions of generalized Euler’s constants into −2 the series of polynomials in π and into the formal enveloping series with rational coefficients only Iaroslav V. Blagouchine 1 University of Toulon, France a r t i c l e i n f o a b s t r a c t Article history: In this work, two new series expansions for generalized Received 1 January 2015 Euler’s constants (Stieltjes constants) γm are obtained. The Received in revised form 26 June first expansion involves Stirling numbers of the first kind, 2015 − contains polynomials in π 2 with rational coefficients and Accepted 29 June 2015 converges slightly better than Euler’s series n−2. The Available online 18 August 2015 Communicated by David Goss second expansion is a semi-convergent series with rational coefficients only. This expansion is particularly simple and Keywords: involves Bernoulli numbers with a non-linear combination of Generalized Euler’s constants generalized harmonic numbers. It also permits to derive an Stieltjes constants interesting estimation for generalized Euler’s constants, which Stirling numbers is more accurate than several well-known estimations. Finally, Factorial coefficients in Appendix A, the reader will also find two simple integral Series expansion definitions for the Stirling numbers of the first kind, as well Divergent series Semi-convergent series an upper bound for them. Formal series © 2015 Elsevier Inc. All rights reserved. Enveloping series Asymptotic expansions Approximations Bernoulli numbers Harmonic numbers Rational coefficients Inverse pi E-mail address: [email protected]. -
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].