Meromorphic Dirichlet Series
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Riemann Sums Fundamental Theorem of Calculus Indefinite
Riemann Sums Partition P = {x0, x1, . , xn} of an interval [a, b]. ck ∈ [xk−1, xk] Pn R(f, P, a, b) = k=1 f(ck)∆xk As the widths ∆xk of the subintervals approach 0, the Riemann Sums hopefully approach a limit, the integral of f from a to b, written R b a f(x) dx. Fundamental Theorem of Calculus Theorem 1 (FTC-Part I). If f is continuous on [a, b], then F (x) = R x 0 a f(t) dt is defined on [a, b] and F (x) = f(x). Theorem 2 (FTC-Part II). If f is continuous on [a, b] and F (x) = R R b b f(x) dx on [a, b], then a f(x) dx = F (x) a = F (b) − F (a). Indefinite Integrals Indefinite Integral: R f(x) dx = F (x) if and only if F 0(x) = f(x). In other words, the terms indefinite integral and antiderivative are synonymous. Every differentiation formula yields an integration formula. Substitution Rule For Indefinite Integrals: If u = g(x), then R f(g(x))g0(x) dx = R f(u) du. For Definite Integrals: R b 0 R g(b) If u = g(x), then a f(g(x))g (x) dx = g(a) f( u) du. Steps in Mechanically Applying the Substitution Rule Note: The variables do not have to be called x and u. (1) Choose a substitution u = g(x). du (2) Calculate = g0(x). dx du (3) Treat as if it were a fraction, a quotient of differentials, and dx du solve for dx, obtaining dx = . -
The Radius of Convergence of the Lam\'{E} Function
The radius of convergence of the Lame´ function Yoon-Seok Choun Department of Physics, Hanyang University, Seoul, 133-791, South Korea Abstract We consider the radius of convergence of a Lame´ function, and we show why Poincare-Perron´ theorem is not applicable to the Lame´ equation. Keywords: Lame´ equation; 3-term recursive relation; Poincare-Perron´ theorem 2000 MSC: 33E05, 33E10, 34A25, 34A30 1. Introduction A sphere is a geometric perfect shape, a collection of points that are all at the same distance from the center in the three-dimensional space. In contrast, the ellipsoid is an imperfect shape, and all of the plane sections are elliptical or circular surfaces. The set of points is no longer the same distance from the center of the ellipsoid. As we all know, the nature is nonlinear and geometrically imperfect. For simplicity, we usually linearize such systems to take a step toward the future with good numerical approximation. Indeed, many geometric spherical objects are not perfectly spherical in nature. The shape of those objects are better interpreted by the ellipsoid because they rotates themselves. For instance, ellipsoidal harmonics are shown in the calculation of gravitational potential [11]. But generally spherical harmonics are preferable to mathematically complex ellipsoid harmonics. Lame´ functions (ellipsoidal harmonic fuctions) [7] are applicable to diverse areas such as boundary value problems in ellipsoidal geometry, Schrodinger¨ equations for various periodic and anharmonic potentials, the theory of Bose-Einstein condensates, group theory to quantum mechanical bound states and band structures of the Lame´ Hamiltonian, etc. As we apply a power series into the Lame´ equation in the algebraic form or Weierstrass’s form, the 3-term recurrence relation starts to arise and currently, there are no general analytic solutions in closed forms for the 3-term recursive relation of a series solution because of their mathematical complexity [1, 5, 13]. -
Generalized Riemann Hypothesis Léo Agélas
Generalized Riemann Hypothesis Léo Agélas To cite this version: Léo Agélas. Generalized Riemann Hypothesis. 2019. hal-00747680v3 HAL Id: hal-00747680 https://hal.archives-ouvertes.fr/hal-00747680v3 Preprint submitted on 29 May 2019 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. Generalized Riemann Hypothesis L´eoAg´elas Department of Mathematics, IFP Energies nouvelles, 1-4, avenue de Bois-Pr´eau,F-92852 Rueil-Malmaison, France Abstract (Generalized) Riemann Hypothesis (that all non-trivial zeros of the (Dirichlet L-function) zeta function have real part one-half) is arguably the most impor- tant unsolved problem in contemporary mathematics due to its deep relation to the fundamental building blocks of the integers, the primes. The proof of the Riemann hypothesis will immediately verify a slew of dependent theorems (Borwien et al.(2008), Sabbagh(2002)). In this paper, we give a proof of Gen- eralized Riemann Hypothesis which implies the proof of Riemann Hypothesis and Goldbach's weak conjecture (also known as the odd Goldbach conjecture) one of the oldest and best-known unsolved problems in number theory. 1. Introduction The Riemann hypothesis is one of the most important conjectures in math- ematics. -
Absolute and Conditional Convergence, and Talk a Little Bit About the Mathematical Constant E
MATH 8, SECTION 1, WEEK 3 - RECITATION NOTES TA: PADRAIC BARTLETT Abstract. These are the notes from Friday, Oct. 15th's lecture. In this talk, we study absolute and conditional convergence, and talk a little bit about the mathematical constant e. 1. Random Question Question 1.1. Suppose that fnkg is the sequence consisting of all natural numbers that don't have a 9 anywhere in their digits. Does the corresponding series 1 X 1 nk k=1 converge? 2. Absolute and Conditional Convergence: Definitions and Theorems For review's sake, we repeat the definitions of absolute and conditional conver- gence here: P1 P1 Definition 2.1. A series n=1 an converges absolutely iff the series n=1 janj P1 converges; it converges conditionally iff the series n=1 an converges but the P1 series of absolute values n=1 janj diverges. P1 (−1)n+1 Example 2.2. The alternating harmonic series n=1 n converges condition- ally. This follows from our work in earlier classes, where we proved that the series itself converged (by looking at partial sums;) conversely, the absolute values of this series is just the harmonic series, which we know to diverge. As we saw in class last time, most of our theorems aren't set up to deal with series whose terms alternate in sign, or even that have terms that occasionally switch sign. As a result, we developed the following pair of theorems to help us manipulate series with positive and negative terms: 1 Theorem 2.3. (Alternating Series Test / Leibniz's Theorem) If fangn=0 is a se- quence of positive numbers that monotonically decreases to 0, the series 1 X n (−1) an n=1 converges. -
Some Questions About Spaces of Dirichlet Series
Some questions about spaces of Dirichlet series. Jos´eBonet Instituto Universitario de Matem´aticaPura y Aplicada Universitat Polit`ecnicade Val`encia Eichstaett, June 2017 Jos´eBonet Some questions about spaces of Dirichlet series Dirichlet Series P1 an A Dirichlet Series is an expression of the form n=1 ns with s 2 C. Riemann's zeta function: If s 2 C, 1 1 1 X 1 ζ(s) := 1 + + + ::: = : 2s 3s ns n=1 Euler 1737 considered it for s real: He proved ζ(2) = π2=6, and he relation with the prime numbers: −1 Y 1 ζ(s) = 1 − ; ps p the product extended to all the prime numbers p. Jos´eBonet Some questions about spaces of Dirichlet series Riemann Riemann (1826-1866) and his Memoir \Uber¨ die Anzahl der Primzahlen unter einer gegebenen Gr¨osse", in which he formulated the \Riemann Hypothesis". Jos´eBonet Some questions about spaces of Dirichlet series Riemann The series ζ(s) converges if the real part of s is greater than 1, and ζ(s) has an analytic extension to all the complex plane except s = 1, where it has a simple pole. Obtained the functional equation. s s−1 ζ(s) = 2 π sen(πs=2)Γ(1 − s)ζ(1 − s); s 2 C: Proved that there are no zeros of ζ(s) outside 0 ≤ <(s) ≤ 1, except the trivial zeros s = −2; −4; −6; :::. Jos´eBonet Some questions about spaces of Dirichlet series Riemann's Hypothesis Riemann conjectured that all the non-trivial zeros of ζ(s) are in the line <(s) = 1=2. -
Arxiv:Math/0201082V1
2000]11A25, 13J05 THE RING OF ARITHMETICAL FUNCTIONS WITH UNITARY CONVOLUTION: DIVISORIAL AND TOPOLOGICAL PROPERTIES. JAN SNELLMAN Abstract. We study (A, +, ⊕), the ring of arithmetical functions with unitary convolution, giving an isomorphism between (A, +, ⊕) and a generalized power series ring on infinitely many variables, similar to the isomorphism of Cashwell- Everett[4] between the ring (A, +, ·) of arithmetical functions with Dirichlet convolution and the power series ring C[[x1,x2,x3,... ]] on countably many variables. We topologize it with respect to a natural norm, and shove that all ideals are quasi-finite. Some elementary results on factorization into atoms are obtained. We prove the existence of an abundance of non-associate regular non-units. 1. Introduction The ring of arithmetical functions with Dirichlet convolution, which we’ll denote by (A, +, ·), is the set of all functions N+ → C, where N+ denotes the positive integers. It is given the structure of a commutative C-algebra by component-wise addition and multiplication by scalars, and by the Dirichlet convolution f · g(k)= f(r)g(k/r). (1) Xr|k Then, the multiplicative unit is the function e1 with e1(1) = 1 and e1(k) = 0 for k> 1, and the additive unit is the zero function 0. Cashwell-Everett [4] showed that (A, +, ·) is a UFD using the isomorphism (A, +, ·) ≃ C[[x1, x2, x3,... ]], (2) where each xi corresponds to the function which is 1 on the i’th prime number, and 0 otherwise. Schwab and Silberberg [9] topologised (A, +, ·) by means of the norm 1 arXiv:math/0201082v1 [math.AC] 10 Jan 2002 |f| = (3) min { k f(k) 6=0 } They noted that this norm is an ultra-metric, and that ((A, +, ·), |·|) is a valued ring, i.e. -
Dirichlet’S Test
4. CONDITIONALLY CONVERGENT SERIES 23 4. Conditionally convergent series Here basic tests capable of detecting conditional convergence are studied. 4.1. Dirichlet’s test. Theorem 4.1. (Dirichlet’s test) n Let a complex sequence {An}, An = k=1 ak, be bounded, and the real sequence {bn} is decreasing monotonically, b1 ≥ b2 ≥ b3 ≥··· , so that P limn→∞ bn = 0. Then the series anbn converges. A proof is based on the identity:P m m m m−1 anbn = (An − An−1)bn = Anbn − Anbn+1 n=k n=k n=k n=k−1 X X X X m−1 = An(bn − bn+1)+ Akbk − Am−1bm n=k X Since {An} is bounded, there is a number M such that |An|≤ M for all n. Therefore it follows from the above identity and non-negativity and monotonicity of bn that m m−1 anbn ≤ An(bn − bn+1) + |Akbk| + |Am−1bm| n=k n=k X X m−1 ≤ M (bn − bn+1)+ bk + bm n=k ! X ≤ 2Mbk By the hypothesis, bk → 0 as k → ∞. Therefore the right side of the above inequality can be made arbitrary small for all sufficiently large k and m ≥ k. By the Cauchy criterion the series in question converges. This completes the proof. Example. By the root test, the series ∞ zn n n=1 X converges absolutely in the disk |z| < 1 in the complex plane. Let us investigate the convergence on the boundary of the disk. Put z = eiθ 24 1. THE THEORY OF CONVERGENCE ikθ so that ak = e and bn = 1/n → 0 monotonically as n →∞. -
Aspects of Quantum Field Theory and Number Theory, Quantum Field Theory and Riemann Zeros, © July 02, 2015
juan guillermo dueñas luna ASPECTSOFQUANTUMFIELDTHEORYAND NUMBERTHEORY ASPECTSOFQUANTUMFIELDTHEORYANDNUMBER THEORY juan guillermo dueñas luna Quantum Field Theory and Riemann Zeros Theoretical Physics Department. Brazilian Center For Physics Research. July 02, 2015. Juan Guillermo Dueñas Luna: Aspects of Quantum Field Theory and Number Theory, Quantum Field Theory and Riemann Zeros, © July 02, 2015. supervisors: Nami Fux Svaiter. location: Rio de Janeiro. time frame: July 02, 2015. ABSTRACT The Riemann hypothesis states that all nontrivial zeros of the zeta function lie in the critical line Re(s) = 1=2. Motivated by the Hilbert- Pólya conjecture which states that one possible way to prove the Riemann hypothesis is to interpret the nontrivial zeros in the light of spectral theory, a lot of activity has been devoted to establish a bridge between number theory and physics. Using the techniques of the spectral zeta function we show that prime numbers and the Rie- mann zeros have a different behaviour as the spectrum of a linear operator associated to a system with countable infinite number of degrees of freedom. To explore more connections between quantum field theory and number theory we studied three systems involving these two sequences of numbers. First, we discuss the renormalized zero-point energy for a massive scalar field such that the Riemann zeros appear in the spectrum of the vacuum modes. This scalar field is defined in a (d + 1)-dimensional flat space-time, assuming that one of the coordinates lies in an finite interval [0, a]. For even dimensional space-time we found a finite reg- ularized energy density, while for odd dimensional space-time we are forced to introduce mass counterterms to define a renormalized vacuum energy. -
Shintani's Zeta Function Is Not a Finite Sum of Euler Products
SHINTANI’S ZETA FUNCTION IS NOT A FINITE SUM OF EULER PRODUCTS FRANK THORNE Abstract. We prove that the Shintani zeta function associated to the space of binary cubic forms cannot be written as a finite sum of Euler products. Our proof also extends to several closely related Dirichlet series. This answers a question of Wright [22] in the negative. 1. Introduction In this paper, we will prove that Shintani’s zeta function is not a finite sum of Euler products. We will also prove the same for the Dirichlet series counting cubic fields. Our work is motivated by a beautiful paper of Wright [22]. To illustrate Wright’s work, we recall a classical example, namely the Dirichlet series associated to fundamental discrim- inants. We have s 1 s s ζ(s) s L(s, χ4) (1.1) D− = 1 2− +2 4− + 1 4− , 2 − · ζ(2s) − L(2s, χ4) D>0 X as well as a similar formula for negative discriminants. These formulas may look a bit messy. However, if one combines positive and negative discriminants, one has the beautiful formulas s s s ζ(s) 1 s (1.2) D − = 1 2− +2 4− = Disc(K ) , | | − · ζ(2s) 2 | v |p p [Kv:Qp] 2 X Y X≤ and L(s, χ4) arXiv:1112.1397v3 [math.NT] 9 Nov 2012 s s (1.3) sgn(D) D − = 1 4− . | | − L(2s, χ4) X These are special cases of much more general results. Wright obtains similar formulas for quadratic extensions of any global field k of characteristic not equal to 2, which are in turn n the case n = 2 of formulas for Dirichlet series parameterizing the elements of k×/(k×) . -
The Mobius Function and Mobius Inversion
Ursinus College Digital Commons @ Ursinus College Transforming Instruction in Undergraduate Number Theory Mathematics via Primary Historical Sources (TRIUMPHS) Winter 2020 The Mobius Function and Mobius Inversion Carl Lienert Follow this and additional works at: https://digitalcommons.ursinus.edu/triumphs_number Part of the Curriculum and Instruction Commons, Educational Methods Commons, Higher Education Commons, Number Theory Commons, and the Science and Mathematics Education Commons Click here to let us know how access to this document benefits ou.y Recommended Citation Lienert, Carl, "The Mobius Function and Mobius Inversion" (2020). Number Theory. 12. https://digitalcommons.ursinus.edu/triumphs_number/12 This Course Materials is brought to you for free and open access by the Transforming Instruction in Undergraduate Mathematics via Primary Historical Sources (TRIUMPHS) at Digital Commons @ Ursinus College. It has been accepted for inclusion in Number Theory by an authorized administrator of Digital Commons @ Ursinus College. For more information, please contact [email protected]. The Möbius Function and Möbius Inversion Carl Lienert∗ January 16, 2021 August Ferdinand Möbius (1790–1868) is perhaps most well known for the one-sided Möbius strip and, in geometry and complex analysis, for the Möbius transformation. In number theory, Möbius’ name can be seen in the important technique of Möbius inversion, which utilizes the important Möbius function. In this PSP we’ll study the problem that led Möbius to consider and analyze the Möbius function. Then, we’ll see how other mathematicians, Dedekind, Laguerre, Mertens, and Bell, used the Möbius function to solve a different inversion problem.1 Finally, we’ll use Möbius inversion to solve a problem concerning Euler’s totient function. -
Chapter 3: Infinite Series
Chapter 3: Infinite series Introduction Definition: Let (an : n ∈ N) be a sequence. For each n ∈ N, we define the nth partial sum of (an : n ∈ N) to be: sn := a1 + a2 + . an. By the series generated by (an : n ∈ N) we mean the sequence (sn : n ∈ N) of partial sums of (an : n ∈ N) (ie: a series is a sequence). We say that the series (sn : n ∈ N) generated by a sequence (an : n ∈ N) is convergent if the sequence (sn : n ∈ N) of partial sums converges. If the series (sn : n ∈ N) is convergent then we call its limit the sum of the series and we write: P∞ lim sn = an. In detail: n→∞ n=1 s1 = a1 s2 = a1 + a + 2 = s1 + a2 s3 = a + 1 + a + 2 + a3 = s2 + a3 ... = ... sn = a + 1 + ... + an = sn−1 + an. Definition: A series that is not convergent is called divergent, ie: each series is ei- P∞ ther convergent or divergent. It has become traditional to use the notation n=1 an to represent both the series (sn : n ∈ N) generated by the sequence (an : n ∈ N) and the sum limn→∞ sn. However, this ambiguity in the notation should not lead to any confu- sion, provided that it is always made clear that the convergence of the series must be established. Important: Although traditionally series have been (and still are) represented by expres- P∞ sions such as n=1 an they are, technically, sequences of partial sums. So if somebody comes up to you in a supermarket and asks you what a series is - you answer “it is a P∞ sequence of partial sums” not “it is an expression of the form: n=1 an.” n−1 Example: (1) For 0 < r < ∞, we may define the sequence (an : n ∈ N) by, an := r for each n ∈ N. -
Dirichlet Series
数理解析研究所講究録 1088 巻 1999 年 83-93 83 Overconvergence Phenomena For Generalized Dirichlet Series Daniele C. Struppa Department of Mathematical Sciences George Mason University Fairfax, VA 22030 $\mathrm{U}.\mathrm{S}$ . A 84 1 Introduction This paper contains the text of the talk I delivered at the symposium “Resurgent Functions and Convolution Equations”, and is an expanded version of a joint paper with T. Kawai, which will appear shortly and which will contain the full proofs of the results. The goal of our work has been to provide a new approach to the classical topic of overconvergence for Dirichlet series, by employing results in the theory of infinite order differential operators with constant coefficients. The possibility of linking infinite order differential operators with gap theorems and related subjects such as overconvergence phenomena was first suggested by Ehrenpreis in [6], but in a form which could not be brought to fruition. In this paper we show how a wide class of overconvergence phenomena can be described in terms of infinite order differential operators, and that we can provide a multi-dimensional analog for such phenomena. Let us begin by stating the problem, as it was first observed by Jentzsch, and subsequently made famous by Ostrowski (see [5]). Consider a power series $f(z)= \sum_{=n0}^{+\infty}anZ^{n}$ (1) whose circle of convergence is $\triangle(0, \rho)=\{z\in C : |z|<\rho\}$ , with $\rho$ given, therefore, by $\rho=\varliminf|a_{n}|^{-1/}n$ . Even though we know that the series given in (1) cannot converge outside of $\Delta=\Delta(0, \rho)$ , it is nevertheless possible that some subsequence of its sequence of partial sums may converge in a region overlapping with $\triangle$ .