ANALYTIC COMBINATORICS — COMPLEX ASYMPTOTICS (Chapters IV, V, VI, VII)
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The Saddle Point Method in Combinatorics Asymptotic Analysis: Successes and Failures (A Personal View)
Pn The number of inversions in permutations Median versus A (A large) for a Luria-Delbruck-like distribution, with parameter A Sum of positions of records in random permutations Merten's theorem for toral automorphisms Representations of numbers as k=−n "k k The q-Catalan numbers A simple case of the Mahonian statistic Asymptotics of the Stirling numbers of the first kind revisited The Saddle point method in combinatorics asymptotic analysis: successes and failures (A personal view) Guy Louchard May 31, 2011 Guy Louchard The Saddle point method in combinatorics asymptotic analysis: successes and failures (A personal view) Pn The number of inversions in permutations Median versus A (A large) for a Luria-Delbruck-like distribution, with parameter A Sum of positions of records in random permutations Merten's theorem for toral automorphisms Representations of numbers as k=−n "k k The q-Catalan numbers A simple case of the Mahonian statistic Asymptotics of the Stirling numbers of the first kind revisited Outline 1 The number of inversions in permutations 2 Median versus A (A large) for a Luria-Delbruck-like distribution, with parameter A 3 Sum of positions of records in random permutations 4 Merten's theorem for toral automorphisms Pn 5 Representations of numbers as k=−n "k k 6 The q-Catalan numbers 7 A simple case of the Mahonian statistic 8 Asymptotics of the Stirling numbers of the first kind revisited Guy Louchard The Saddle point method in combinatorics asymptotic analysis: successes and failures (A personal view) Pn The number of inversions in permutations Median versus A (A large) for a Luria-Delbruck-like distribution, with parameter A Sum of positions of records in random permutations Merten's theorem for toral automorphisms Representations of numbers as k=−n "k k The q-Catalan numbers A simple case of the Mahonian statistic Asymptotics of the Stirling numbers of the first kind revisited The number of inversions in permutations Let a1 ::: an be a permutation of the set f1;:::; ng. -
The Unilateral Z–Transform and Generating Functions
The Unilateral z{Transform and Generating Functions Recall from \Discrete{Time Linear, Time Invariant Systems and z-Transforms" that the behaviour of a discrete{time LTI system is determined by its impulse response function h[n] and that the z{transform of h[n] is 1 k H(z) = z− h[k] k=X −∞ If the LTI system is causal, then h[n] = 0 for all n < 0 and 1 k H(z) = z− h[k] Xk=0 Definition 1 (Unilateral z{Transform) The unilateral z{transform of the discrete{time signal x[n] (whether or not x[n] = 0 for negative n's) is defined to be 1 n (z) = z− x[n] X nX=0 When there is any danger of confusing the regular z{transform with the unilateral z{transform, 1 n X(z) = z− x[n] nX= 1 − is called the bilateral z{transform. Example 2 The signal x[n] = anu[n] is zero for all n < 0. So the unilateral z{transform of x[n] is the same as the ordinary z{transform. So, as we saw in Example 7 of \Discrete{Time Linear, Time Invariant Systems and z-Transforms", 1 n n 1 (z) = X(z) = z− a = 1 X 1 z− a nX=0 − 1 provided that z− a < 1, or equivalently z > a . Since the unilateral z{transform of any x[n] is always j j j j j j equal to the bilateral z{transform of the right{sided signal x[n]u[n], the region of convergence of a unilateral z{transform is always the exterior of a circle. -
Poles and Zeros of Generalized Carathéodory Class Functions
W&M ScholarWorks Undergraduate Honors Theses Theses, Dissertations, & Master Projects 5-2011 Poles and Zeros of Generalized Carathéodory Class Functions Yael Gilboa College of William and Mary Follow this and additional works at: https://scholarworks.wm.edu/honorstheses Part of the Mathematics Commons Recommended Citation Gilboa, Yael, "Poles and Zeros of Generalized Carathéodory Class Functions" (2011). Undergraduate Honors Theses. Paper 375. https://scholarworks.wm.edu/honorstheses/375 This Honors Thesis is brought to you for free and open access by the Theses, Dissertations, & Master Projects at W&M ScholarWorks. It has been accepted for inclusion in Undergraduate Honors Theses by an authorized administrator of W&M ScholarWorks. For more information, please contact [email protected]. Poles and Zeros of Generalized Carathéodory Class Functions A thesis submitted in partial fulfillment of the requirement for the degree of Bachelor of Science with Honors in Mathematics from The College of William and Mary by Yael Gilboa Accepted for (Honors) Vladimir Bolotnikov, Committee Chair Ilya Spiktovsky Leiba Rodman Julie Agnew Williamsburg, VA May 2, 2011 POLES AND ZEROS OF GENERALIZED CARATHEODORY´ CLASS FUNCTIONS YAEL GILBOA Date: May 2, 2011. 1 2 YAEL GILBOA Contents 1. Introduction 3 2. Schur Class Functions 5 3. Generalized Schur Class Functions 13 4. Classical and Generalized Carath´eodory Class Functions 15 5. PolesandZerosofGeneralizedCarath´eodoryFunctions 18 6. Future Research and Acknowledgments 28 References 29 POLES AND ZEROS OF GENERALIZED CARATHEODORY´ CLASS FUNCTIONS 3 1. Introduction The goal of this thesis is to establish certain representations for generalized Carath´eodory functions in terms of related classical Carath´eodory functions. Let denote the Carath´eodory class of functions f that are analytic and that have a nonnegativeC real part in the open unit disk D = z : z < 1 . -
Ordinary Generating Functions
CHAPTER 10 Ordinary Generating Functions Introduction We’ll begin this chapter by introducing the notion of ordinary generating functions and discussing the basic techniques for manipulating them. These techniques are merely restatements and simple applications of things you learned in algebra and calculus. You must master these basic ideas before reading further. In Section 2, we apply generating functions to the solution of simple recursions. This requires no new concepts, but provides practice manipulating generating functions. In Section 3, we return to the manipulation of generating functions, introducing slightly more advanced methods than those in Section 1. If you found the material in Section 1 easy, you can skim Sections 2 and 3. If you had some difficulty with Section 1, those sections will give you additional practice developing your ability to manipulate generating functions. Section 4 is the heart of this chapter. In it we study the Rules of Sum and Product for ordinary generating functions. Suppose that we are given a combinatorial description of the construction of some structures we wish to count. These two rules often allow us to write down an equation for the generating function directly from this combinatorial description. Without such tools, we may get bogged down in lengthy algebraic manipulations. 10.1 What are Generating Functions? In this section, we introduce the idea of ordinary generating functions and look at some ways to manipulate them. This material is essential for understanding later material on generating functions. Be sure to work the exercises in this section before reading later sections! Definition 10.1 Ordinary generating function (OGF) Suppose we are given a sequence a0,a1,.. -
Asymptotic Analysis for Periodic Structures
ASYMPTOTIC ANALYSIS FOR PERIODIC STRUCTURES A. BENSOUSSAN J.-L. LIONS G. PAPANICOLAOU AMS CHELSEA PUBLISHING American Mathematical Society • Providence, Rhode Island ASYMPTOTIC ANALYSIS FOR PERIODIC STRUCTURES ASYMPTOTIC ANALYSIS FOR PERIODIC STRUCTURES A. BENSOUSSAN J.-L. LIONS G. PAPANICOLAOU AMS CHELSEA PUBLISHING American Mathematical Society • Providence, Rhode Island M THE ATI A CA M L ΤΡΗΤΟΣ ΜΗ N ΕΙΣΙΤΩ S A O C C I I R E E T ΑΓΕΩΜΕ Y M A F O 8 U 88 NDED 1 2010 Mathematics Subject Classification. Primary 80M40, 35B27, 74Q05, 74Q10, 60H10, 60F05. For additional information and updates on this book, visit www.ams.org/bookpages/chel-374 Library of Congress Cataloging-in-Publication Data Bensoussan, Alain. Asymptotic analysis for periodic structures / A. Bensoussan, J.-L. Lions, G. Papanicolaou. p. cm. Originally published: Amsterdam ; New York : North-Holland Pub. Co., 1978. Includes bibliographical references. ISBN 978-0-8218-5324-5 (alk. paper) 1. Boundary value problems—Numerical solutions. 2. Differential equations, Partial— Asymptotic theory. 3. Probabilities. I. Lions, J.-L. (Jacques-Louis), 1928–2001. II. Papani- colaou, George. III. Title. QA379.B45 2011 515.353—dc23 2011029403 Copying and reprinting. Individual readers of this publication, and nonprofit libraries acting for them, are permitted to make fair use of the material, such as to copy a chapter for use in teaching or research. Permission is granted to quote brief passages from this publication in reviews, provided the customary acknowledgment of the source is given. Republication, systematic copying, or multiple reproduction of any material in this publication is permitted only under license from the American Mathematical Society. -
Definite Integrals in an Asymptotic Setting
A Lost Theorem: Definite Integrals in An Asymptotic Setting Ray Cavalcante and Todor D. Todorov 1 INTRODUCTION We present a simple yet rigorous theory of integration that is based on two axioms rather than on a construction involving Riemann sums. With several examples we demonstrate how to set up integrals in applications of calculus without using Riemann sums. In our axiomatic approach even the proof of the existence of the definite integral (which does use Riemann sums) becomes slightly more elegant than the conventional one. We also discuss an interesting connection between our approach and the history of calculus. The article is written for readers who teach calculus and its applications. It might be accessible to students under a teacher’s supervision and suitable for senior projects on calculus, real analysis, or history of mathematics. Here is a summary of our approach. Let ρ :[a, b] → R be a continuous function and let I :[a, b] × [a, b] → R be the corresponding integral function, defined by y I(x, y)= ρ(t)dt. x Recall that I(x, y) has the following two properties: (A) Additivity: I(x, y)+I (y, z)=I (x, z) for all x, y, z ∈ [a, b]. (B) Asymptotic Property: I(x, x + h)=ρ (x)h + o(h)ash → 0 for all x ∈ [a, b], in the sense that I(x, x + h) − ρ(x)h lim =0. h→0 h In this article we show that properties (A) and (B) are characteristic of the definite integral. More precisely, we show that for a given continuous ρ :[a, b] → R, there is no more than one function I :[a, b]×[a, b] → R with properties (A) and (B). -
Control Systems
ECE 380: Control Systems Course Notes: Winter 2014 Prof. Shreyas Sundaram Department of Electrical and Computer Engineering University of Waterloo ii c Shreyas Sundaram Acknowledgments Parts of these course notes are loosely based on lecture notes by Professors Daniel Liberzon, Sean Meyn, and Mark Spong (University of Illinois), on notes by Professors Daniel Davison and Daniel Miller (University of Waterloo), and on parts of the textbook Feedback Control of Dynamic Systems (5th edition) by Franklin, Powell and Emami-Naeini. I claim credit for all typos and mistakes in the notes. The LATEX template for The Not So Short Introduction to LATEX 2" by T. Oetiker et al. was used to typeset portions of these notes. Shreyas Sundaram University of Waterloo c Shreyas Sundaram iv c Shreyas Sundaram Contents 1 Introduction 1 1.1 Dynamical Systems . .1 1.2 What is Control Theory? . .2 1.3 Outline of the Course . .4 2 Review of Complex Numbers 5 3 Review of Laplace Transforms 9 3.1 The Laplace Transform . .9 3.2 The Inverse Laplace Transform . 13 3.2.1 Partial Fraction Expansion . 13 3.3 The Final Value Theorem . 15 4 Linear Time-Invariant Systems 17 4.1 Linearity, Time-Invariance and Causality . 17 4.2 Transfer Functions . 18 4.2.1 Obtaining the transfer function of a differential equation model . 20 4.3 Frequency Response . 21 5 Bode Plots 25 5.1 Rules for Drawing Bode Plots . 26 5.1.1 Bode Plot for Ko ....................... 27 5.1.2 Bode Plot for sq ....................... 28 s −1 s 5.1.3 Bode Plot for ( p + 1) and ( z + 1) . -
The Bloch-Wigner-Ramakrishnan Polylogarithm Function
Math. Ann. 286, 613424 (1990) Springer-Verlag 1990 The Bloch-Wigner-Ramakrishnan polylogarithm function Don Zagier Max-Planck-Insfitut fiir Mathematik, Gottfried-Claren-Strasse 26, D-5300 Bonn 3, Federal Republic of Germany To Hans Grauert The polylogarithm function co ~n appears in many parts of mathematics and has an extensive literature [2]. It can be analytically extended to the cut plane ~\[1, ~) by defining Lira(x) inductively as x [ Li m_ l(z)z-tdz but then has a discontinuity as x crosses the cut. However, for 0 m = 2 the modified function O(x) = ~(Liz(x)) + arg(1 -- x) loglxl extends (real-) analytically to the entire complex plane except for the points x=0 and x= 1 where it is continuous but not analytic. This modified dilogarithm function, introduced by Wigner and Bloch [1], has many beautiful properties. In particular, its values at algebraic argument suffice to express in closed form the volumes of arbitrary hyperbolic 3-manifolds and the values at s= 2 of the Dedekind zeta functions of arbitrary number fields (cf. [6] and the expository article [7]). It is therefore natural to ask for similar real-analytic and single-valued modification of the higher polylogarithm functions Li,. Such a function Dm was constructed, and shown to satisfy a functional equation relating D=(x-t) and D~(x), by Ramakrishnan E3]. His construction, which involved monodromy arguments for certain nilpotent subgroups of GLm(C), is completely explicit, but he does not actually give a formula for Dm in terms of the polylogarithm. In this note we write down such a formula and give a direct proof of the one-valuedness and functional equation. -
Real Rational Filters, Zeros and Poles
Real Rational Filters, Zeros and Poles Jack Xin (Lecture) and J. Ernie Esser (Lab) ∗ Abstract Classnotes on real rational filters, causality, stability, frequency response, impulse response, zero/pole analysis, minimum phase and all pass filters. 1 Real Rational Filter and Frequency Response A real rational filter takes the form of difference equations in the time domain: a(1)y(n) = b(1)x(n)+ b(2)x(n 1) + + b(nb + 1)x(n nb) − ··· − a(2)y(n 1) a(na + 1)y(n na), (1) − − −···− − where na and nb are nonnegative integers (number of delays), x is input signal, y is filtered output signal. In the z-domain, the z-transforms X and Y are related by: Y (z)= H(z) X(z), (2) where X and Y are z-transforms of x and y respectively, and H is called the transfer function: b(1) + b(2)z−1 + + b(nb + 1)z−nb H(z)= ··· . (3) a(1) + a(2)z−1 + + a(na + 1)z−na ··· The filter is called real rational because H is a rational function of z with real coefficients in numerator and denominator. The frequency response of the filter is H(ejθ), where j = √ 1, θ [0, π]. The θ [π, 2π] − ∈ ∈ portion does not contain more information due to complex conjugacy. In Matlab, the frequency response is obtained by: [h, θ] = freqz(b, a, N), where b = [b(1), b(2), , b(nb + 1)], a = [a(1), a(2), , a(na + 1)], N refers to number of ··· ··· sampled points for θ on the upper unit semi-circle; h is a complex vector with components H(ejθ) at sampled points of θ. -
Residue Theorem
Topic 8 Notes Jeremy Orloff 8 Residue Theorem 8.1 Poles and zeros f z z We remind you of the following terminology: Suppose . / is analytic at 0 and f z a z z n a z z n+1 ; . / = n. * 0/ + n+1. * 0/ + § a ≠ f n z n z with n 0. Then we say has a zero of order at 0. If = 1 we say 0 is a simple zero. f z Suppose has an isolated singularity at 0 and Laurent series b b b n n*1 1 f .z/ = + + § + + a + a .z * z / + § z z n z z n*1 z z 0 1 0 . * 0/ . * 0/ * 0 < z z < R b ≠ f n z which converges on 0 * 0 and with n 0. Then we say has a pole of order at 0. n z If = 1 we say 0 is a simple pole. There are several examples in the Topic 7 notes. Here is one more Example 8.1. z + 1 f .z/ = z3.z2 + 1/ has isolated singularities at z = 0; ,i and a zero at z = *1. We will show that z = 0 is a pole of order 3, z = ,i are poles of order 1 and z = *1 is a zero of order 1. The style of argument is the same in each case. At z = 0: 1 z + 1 f .z/ = ⋅ : z3 z2 + 1 Call the second factor g.z/. Since g.z/ is analytic at z = 0 and g.0/ = 1, it has a Taylor series z + 1 g.z/ = = 1 + a z + a z2 + § z2 + 1 1 2 Therefore 1 a a f .z/ = + 1 +2 + § : z3 z2 z This shows z = 0 is a pole of order 3. -
Introducing Taylor Series and Local Approximations Using a Historical and Semiotic Approach Kouki Rahim, Barry Griffiths
Introducing Taylor Series and Local Approximations using a Historical and Semiotic Approach Kouki Rahim, Barry Griffiths To cite this version: Kouki Rahim, Barry Griffiths. Introducing Taylor Series and Local Approximations using a Historical and Semiotic Approach. IEJME, Modestom LTD, UK, 2019, 15 (2), 10.29333/iejme/6293. hal- 02470240 HAL Id: hal-02470240 https://hal.archives-ouvertes.fr/hal-02470240 Submitted on 7 Feb 2020 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. INTERNATIONAL ELECTRONIC JOURNAL OF MATHEMATICS EDUCATION e-ISSN: 1306-3030. 2020, Vol. 15, No. 2, em0573 OPEN ACCESS https://doi.org/10.29333/iejme/6293 Introducing Taylor Series and Local Approximations using a Historical and Semiotic Approach Rahim Kouki 1, Barry J. Griffiths 2* 1 Département de Mathématique et Informatique, Université de Tunis El Manar, Tunis 2092, TUNISIA 2 Department of Mathematics, University of Central Florida, Orlando, FL 32816-1364, USA * CORRESPONDENCE: [email protected] ABSTRACT In this article we present the results of a qualitative investigation into the teaching and learning of Taylor series and local approximations. In order to perform a comparative analysis, two investigations are conducted: the first is historical and epistemological, concerned with the pedagogical evolution of semantics, syntax and semiotics; the second is a contemporary institutional investigation, devoted to the results of a review of curricula, textbooks and course handouts in Tunisia and the United States. -
An Introduction to Asymptotic Analysis Simon JA Malham
An introduction to asymptotic analysis Simon J.A. Malham Department of Mathematics, Heriot-Watt University Contents Chapter 1. Order notation 5 Chapter 2. Perturbation methods 9 2.1. Regular perturbation problems 9 2.2. Singular perturbation problems 15 Chapter 3. Asymptotic series 21 3.1. Asymptotic vs convergent series 21 3.2. Asymptotic expansions 25 3.3. Properties of asymptotic expansions 26 3.4. Asymptotic expansions of integrals 29 Chapter 4. Laplace integrals 31 4.1. Laplace's method 32 4.2. Watson's lemma 36 Chapter 5. Method of stationary phase 39 Chapter 6. Method of steepest descents 43 Bibliography 49 Appendix A. Notes 51 A.1. Remainder theorem 51 A.2. Taylor series for functions of more than one variable 51 A.3. How to determine the expansion sequence 52 A.4. How to find a suitable rescaling 52 Appendix B. Exam formula sheet 55 3 CHAPTER 1 Order notation The symbols , o and , were first used by E. Landau and P. Du Bois- Reymond and areOdefined as∼ follows. Suppose f(z) and g(z) are functions of the continuous complex variable z defined on some domain C and possess D ⊂ limits as z z0 in . Then we define the following shorthand notation for the relative!propertiesD of these functions in the limit z z . ! 0 Asymptotically bounded: f(z) = (g(z)) as z z ; O ! 0 means that: there exists constants K 0 and δ > 0 such that, for 0 < z z < δ, ≥ j − 0j f(z) K g(z) : j j ≤ j j We say that f(z) is asymptotically bounded by g(z) in magnitude as z z0, or more colloquially, and we say that f(z) is of `order big O' of g(z).