Coefficients of Algebraic Functions: Formulae and Asymptotics
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Field Theory Pete L. Clark
Field Theory Pete L. Clark Thanks to Asvin Gothandaraman and David Krumm for pointing out errors in these notes. Contents About These Notes 7 Some Conventions 9 Chapter 1. Introduction to Fields 11 Chapter 2. Some Examples of Fields 13 1. Examples From Undergraduate Mathematics 13 2. Fields of Fractions 14 3. Fields of Functions 17 4. Completion 18 Chapter 3. Field Extensions 23 1. Introduction 23 2. Some Impossible Constructions 26 3. Subfields of Algebraic Numbers 27 4. Distinguished Classes 29 Chapter 4. Normal Extensions 31 1. Algebraically closed fields 31 2. Existence of algebraic closures 32 3. The Magic Mapping Theorem 35 4. Conjugates 36 5. Splitting Fields 37 6. Normal Extensions 37 7. The Extension Theorem 40 8. Isaacs' Theorem 40 Chapter 5. Separable Algebraic Extensions 41 1. Separable Polynomials 41 2. Separable Algebraic Field Extensions 44 3. Purely Inseparable Extensions 46 4. Structural Results on Algebraic Extensions 47 Chapter 6. Norms, Traces and Discriminants 51 1. Dedekind's Lemma on Linear Independence of Characters 51 2. The Characteristic Polynomial, the Trace and the Norm 51 3. The Trace Form and the Discriminant 54 Chapter 7. The Primitive Element Theorem 57 1. The Alon-Tarsi Lemma 57 2. The Primitive Element Theorem and its Corollary 57 3 4 CONTENTS Chapter 8. Galois Extensions 61 1. Introduction 61 2. Finite Galois Extensions 63 3. An Abstract Galois Correspondence 65 4. The Finite Galois Correspondence 68 5. The Normal Basis Theorem 70 6. Hilbert's Theorem 90 72 7. Infinite Algebraic Galois Theory 74 8. A Characterization of Normal Extensions 75 Chapter 9. -
Good Reduction of Puiseux Series and Applications Adrien Poteaux, Marc Rybowicz
Good reduction of Puiseux series and applications Adrien Poteaux, Marc Rybowicz To cite this version: Adrien Poteaux, Marc Rybowicz. Good reduction of Puiseux series and applications. Journal of Symbolic Computation, Elsevier, 2012, 47 (1), pp.32 - 63. 10.1016/j.jsc.2011.08.008. hal-00825850 HAL Id: hal-00825850 https://hal.archives-ouvertes.fr/hal-00825850 Submitted on 24 May 2013 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. Good Reduction of Puiseux Series and Applications Adrien Poteaux, Marc Rybowicz XLIM - UMR 6172 Universit´ede Limoges/CNRS Department of Mathematics and Informatics 123 Avenue Albert Thomas 87060 Limoges Cedex - France Abstract We have designed a new symbolic-numeric strategy to compute efficiently and accurately floating point Puiseux series defined by a bivariate polynomial over an algebraic number field. In essence, computations modulo a well chosen prime number p are used to obtain the exact information needed to guide floating point computations. In this paper, we detail the symbolic part of our algorithm: First of all, we study modular reduction of Puiseux series and give a good reduction criterion to ensure that the information required by the numerical part is preserved. -
Section 1.2 – Mathematical Models: a Catalog of Essential Functions
Section 1-2 © Sandra Nite Math 131 Lecture Notes Section 1.2 – Mathematical Models: A Catalog of Essential Functions A mathematical model is a mathematical description of a real-world situation. Often the model is a function rule or equation of some type. Modeling Process Real-world Formulate Test/Check problem Real-world Mathematical predictions model Interpret Mathematical Solve conclusions Linear Models Characteristics: • The graph is a line. • In the form y = f(x) = mx + b, m is the slope of the line, and b is the y-intercept. • The rate of change (slope) is constant. • When the independent variable ( x) in a table of values is sequential (same differences), the dependent variable has successive differences that are the same. • The linear parent function is f(x) = x, with D = ℜ = (-∞, ∞) and R = ℜ = (-∞, ∞). • The direct variation function is a linear function with b = 0 (goes through the origin). • In a direct variation function, it can be said that f(x) varies directly with x, or f(x) is directly proportional to x. Example: See pp. 26-28 of the text. 1 Section 1-2 © Sandra Nite Polynomial Functions = n + n−1 +⋅⋅⋅+ 2 + + A function P is called a polynomial if P(x) an x an−1 x a2 x a1 x a0 where n is a nonnegative integer and a0 , a1 , a2 ,..., an are constants called the coefficients of the polynomial. If the leading coefficient an ≠ 0, then the degree of the polynomial is n. Characteristics: • The domain is the set of all real numbers D = (-∞, ∞). • If the degree is odd, the range R = (-∞, ∞). -
9<HTMERB=Eheihg>
Mathematics springer.com/NEWSonline Advances in Mathematical K. Alladi, University of Florida, Gainesville, FL, I. Amidror, Ecole Polytechnique Fédérale de USA; M. Bhargava, Princeton University, NJ, USA; Lausanne, Switzerland Economics D. Savitt, P. H. Tiep, University of Arizona, Tucson, AZ, USA (Eds) Mastering the Discrete Fourier Series editors: S. Kusuoka, R. Anderson, C. Castaing, Transform in One, Two or F. H. Clarke, E. Dierker, D. Duffie, L. C. Evans, Quadratic and Higher Degree T. Fujimoto, N. Hirano, T. Ichiishi, A. Ioffe, Forms Several Dimensions S. Iwamoto, K. Kamiya, K. Kawamata, H. Matano, Pitfalls and Artifacts M. K. Richter, Y. Takahashi, J.‑M. Grandmont, In the last decade, the areas of quadratic and T. Maruyama, M. Yano, A. Yamazaki, K. Nishimura higher degree forms have witnessed dramatic The discrete Fourier transform (DFT) is an ex- Volume 17 advances. This volume is an outgrowth of three tremely useful tool that finds application in many seminal conferences on these topics held in 2009, different disciplines. However, its use requires S. Kusuoka, T. Maruyama (Eds) two at the University of Florida and one at the caution. The aim of this book is to explain the Arizona Winter School. DFT and its various artifacts and pitfalls and to Advances in Mathematical show how to avoid these (whenever possible), or Economics Volume 17 Features at least how to recognize them in order to avoid 7 Provides survey lectures, also accessible to non- misinterpretations. A lot of economic problems can be formulated experts 7 Introduction summarizes current as constrained optimizations and equilibration research on quadratic and higher degree forms Features of their solutions. -
A Survey on Recent Advances and Future Challenges in the Computation of Asymptotes
A Survey on Recent Advances and Future Challenges in the Computation of Asymptotes Angel Blasco and Sonia P´erez-D´ıaz Dpto. de F´ısica y Matem´aticas Universidad de Alcal´a E-28871 Madrid, Spain [email protected], [email protected] Abstract In this paper, we summarize two algorithms for computing all the gener- alized asymptotes of a plane algebraic curve implicitly or parametrically de- fined. The approach is based on the notion of perfect curve introduced from the concepts and results presented in [Blasco and P´erez-D´ıaz(2014)], [Blasco and P´erez-D´ıaz(2014-b)] and [Blasco and P´erez-D´ıaz(2015)]. From these results, we derive a new method that allow to easily compute horizontal and vertical asymptotes. Keywords: Implicit Algebraic Plane Curve; Parametric Plane Curve; Infinity Branches; Asymptotes; Perfect Curves; Approaching Curves. 1 Introduction In this paper, we deal with the problem of computing the asymptotes of the infinity branches of a plane algebraic curve. This question is very important in the study of real plane algebraic curves because asymptotes contain much of the information about the behavior of the curves in the large. For instance, determining the asymptotes of a curve is an important step in sketching its graph. Intuitively speaking, the asymptotes of some branch, B, of a real plane algebraic curve, C, reflect the status of B at the points with sufficiently large coordinates. In analytic geometry, an asymptote of a curve is a line such that the distance between the curve and the line approaches zero as they tend to infinity. -
Arxiv:Math/9404219V1
A Package on Formal Power Series Wolfram Koepf Konrad-Zuse-Zentrum f¨ur Informationstechnik Heilbronner Str. 10 D-10711 Berlin [email protected] Mathematica Journal 4, to appear in May, 1994 Abstract: Formal Laurent-Puiseux series are important in many branches of mathemat- ics. This paper presents a Mathematica implementation of algorithms devel- oped by the author for converting between certain classes of functions and their equivalent representing series. The package PowerSeries handles func- tions of rational, exponential, and hypergeometric type, and enables the user to reproduce most of the results of Hansen’s extensive table of series. Subal- gorithms of independent significance generate differential equations satisfied by a given function and recurrence equations satisfied by a given sequence. Scope of the Algorithms A common problem in mathematics is to convert an expression involving el- ementary or special functions into its corresponding formal Laurent-Puiseux series of the form ∞ k/n f(x)= akx . (1) kX=k0 Expressions created from algebraic operations on series, such as addition, arXiv:math/9404219v1 [math.CA] 19 Apr 1994 multiplication, division, and substitution, can be handled by finite algo- rithms if one truncates the resulting series. These algorithms are imple- mented in Mathematica’s Series command. For example: In[1]:= Series[Sin[x] Exp[x], {x, 0, 5}] 3 5 2xx 6 Out[1]= x + x + -- - -- + O[x] 3 30 It is usually much more difficult to find the exact formal result, that is, an explicit formula for the coefficients ak. 1 This -
Formulae and Asymptotics for Coefficients of Algebraic Functions
FORMULAE AND ASYMPTOTICS FOR COEFFICIENTS OF ALGEBRAIC FUNCTIONS CYRIL BANDERIER AND MICHAEL DRMOTA UUUWe dedicate this article to the memory of Philippe Flajolet, who was and will remain a guide and a wonderful source of inspiration for so many of us. UUU [ This article will appear in Combinatorics, Probability, and Computing, in the special volume dedicated to Philippe Flajolet. ] Cyril Banderier, CNRS/Univ. Paris 13, Villetaneuse (France). Cyril.Banderier at lipn.univ-paris13.fr, http://lipn.univ-paris13.fr/∼banderier Michael Drmota, TU Wien (Austria). drmota at dmg.tuwien.ac.at, http://dmg.tuwien.ac.at/drmota/ Date: March 22, 2013 (revised March 22, 2014). Key words and phrases. analytic combinatorics, generating function, algebraic function, singu- larity analysis, context-free grammars, critical exponent, non-strongly connected positive systems, Gaussian limit laws, N-algebraic function. 1 2 FORMULAE AND ASYMPTOTICS FOR COEFFICIENTS OF ALGEBRAIC FUNCTIONS P n Abstract. We study the coefficients of algebraic functions n≥0 fnz . First, we recall the too-little-known fact that these coefficients fn always admit a closed form. Then we study their asymptotics, known to be of the type n α fn ∼ CA n . When the function is a power series associated to a context- free grammar, we solve a folklore conjecture: the critical exponents α can- not be 1=3 or −5=2; they in fact belong to a proper subset of the dyadic numbers. We initiate the study of the set of possible values for A. We ex- tend what Philippe Flajolet called the Drmota{Lalley{Woods theorem (which states that α = −3=2 when the dependency graph associated to the algebraic system defining the function is strongly connected). -
A Proof of Saari's Conjecture for the Three-Body
A PROOF OF SAARI’S CONJECTURE FOR THE THREE-BODY PROBLEM IN Rd RICHARD MOECKEL Abstract. The well-known central configurations of the three-body problem give rise to periodic solutions where the bodies rotate rigidly around their center of mass. For these solutions, the moment of inertia of the bodies with respect to the center of mass is clearly constant. Saari conjectured that such rigid motions, called relative equilibrium solutions, are the only solutions with constant moment of inertia. This result will be proved here for the Newtonian three-body problem in Rd with three positive masses. The proof makes use of some computational algebra and geometry. When d ≤ 3, the rigid motions are the planar, periodic solutions arising from the five central configurations, but for d ≥ 4 there are other possibilities. 1. Introduction It is a well-known property of the Newtonian n-body problem that the center of mass of the bodies moves along a line with constant velocity. Making a change of coordinates, one may assume that the center of mass is actually constant and remains at the origin. Once this is done, the moment of inertia with respect to the origin provides a natural measure of the size of the configuration. The familiar rigidly rotating periodic solutions of Lagrange provide examples of solutions with constant moment of inertia. Saari conjectured that these are in fact the only such solutions [11]. The goal of this paper is to provide a proof for the three-body problem in Rd. This corresponding result for the planar problem was presented in [9]. -
Trigonometric Functions
72 Chapter 4 Trigonometric Functions To define the radian measurement system, we consider the unit circle in the xy-plane: ........................ ....... ....... ...... ....................... .............. ............... ......... ......... ....... ....... ....... ...... ...... ...... ..... ..... ..... ..... ..... ..... .... ..... ..... .... .... .... .... ... (cos x, sin x) ... ... 4 ... A ..... .. ... ....... ... ... ....... ... .. ....... .. .. ....... .. .. ....... .. .. ....... .. .. ....... .. .. ....... ...... ....... ....... ...... ....... x . ....... Trigonometric Functions . ...... ....y . ....... (1, 0) . ....... ....... .. ...... .. .. ....... .. .. ....... .. .. ....... .. .. ....... .. ... ...... ... ... ....... ... ... .......... ... ... ... ... .... B... .... .... ..... ..... ..... ..... ..... ..... ..... ..... ...... ...... ...... ...... ....... ....... ........ ........ .......... .......... ................................................................................... An angle, x, at the center of the circle is associated with an arc of the circle which is said to subtend the angle. In the figure, this arc is the portion of the circle from point (1, 0) So far we have used only algebraic functions as examples when finding derivatives, that is, to point A. The length of this arc is the radian measure of the angle x; the fact that the functions that can be built up by the usual algebraic operations of addition, subtraction, radian measure is an actual geometric length is largely responsible for the usefulness of -
Fractional-Order Phase Transition of Charged Ads Black Holes
Physics Letters B 795 (2019) 490–495 Contents lists available at ScienceDirect Physics Letters B www.elsevier.com/locate/physletb Fractional-order phase transition of charged AdS black holes ∗ Meng-Sen Ma a,b, a Institute of Theoretical Physics, Shanxi Datong University, Datong 037009, China b Department of Physics, Shanxi Datong University, Datong 037009, China a r t i c l e i n f o a b s t r a c t Article history: Employing the fractional derivatives, one can construct a more elaborate classification of phase transitions Received 23 May 2019 compared to the original Ehrenfest classification. In this way, a thermodynamic system can even undergo Received in revised form 26 June 2019 a fractional-order phase transition. We use this method to restudy the charged AdS black hole and Van Accepted 28 June 2019 der Waals fluids and find that at the critical point they both have a 4/3-order phase transition, but not Available online 2 July 2019 the previously recognized second-order one. Editor: M. Cveticˇ © 2019 The Author(s). Published by Elsevier B.V. This is an open access article under the CC BY license 3 (http://creativecommons.org/licenses/by/4.0/). Funded by SCOAP . 1. Introduction The generalized classification can work in any thermodynamic systems that having phase structures. Black holes, being charac- In many thermodynamic systems there exist phase transitions terized by only three parameters, are the simplest thermodynamic and critical phenomena. The original classification of phase tran- system. In particular, it has been found that AdS black holes have sitions was proposed by Ehrenfest. -
Complex Algebraic Geometry
Complex Algebraic Geometry Jean Gallier∗ and Stephen S. Shatz∗∗ ∗Department of Computer and Information Science University of Pennsylvania Philadelphia, PA 19104, USA e-mail: [email protected] ∗∗Department of Mathematics University of Pennsylvania Philadelphia, PA 19104, USA e-mail: [email protected] February 25, 2011 2 Contents 1 Complex Algebraic Varieties; Elementary Theory 7 1.1 What is Geometry & What is Complex Algebraic Geometry? . .......... 7 1.2 LocalStructureofComplexVarieties. ............ 14 1.3 LocalStructureofComplexVarieties,II . ............. 28 1.4 Elementary Global Theory of Varieties . ........... 42 2 Cohomologyof(Mostly)ConstantSheavesandHodgeTheory 73 2.1 RealandComplex .................................... ...... 73 2.2 Cohomology,deRham,Dolbeault. ......... 78 2.3 Hodge I, Analytic Preliminaries . ........ 89 2.4 Hodge II, Globalization & Proof of Hodge’s Theorem . ............ 107 2.5 HodgeIII,TheK¨ahlerCase . .......... 131 2.6 Hodge IV: Lefschetz Decomposition & the Hard Lefschetz Theorem............... 147 2.7 ExtensionsofResultstoVectorBundles . ............ 162 3 The Hirzebruch-Riemann-Roch Theorem 165 3.1 Line Bundles, Vector Bundles, Divisors . ........... 165 3.2 ChernClassesandSegreClasses . .......... 179 3.3 The L-GenusandtheToddGenus .............................. 215 3.4 CobordismandtheSignatureTheorem. ........... 227 3.5 The Hirzebruch–Riemann–Roch Theorem (HRR) . ............ 232 3 4 CONTENTS Preface This manuscript is based on lectures given by Steve Shatz for the course Math 622/623–Complex Algebraic Geometry, during Fall 2003 and Spring 2004. The process for producing this manuscript was the following: I (Jean Gallier) took notes and transcribed them in LATEX at the end of every week. A week later or so, Steve reviewed these notes and made changes and corrections. After the course was over, Steve wrote up additional material that I transcribed into LATEX. The following manuscript is thus unfinished and should be considered as work in progress. -
FPS a Package for the Automatic Calculation of Formal Power Series
FPS A Package for the Automatic Calculation of Formal Power Series Wolfram Koepf ZIB Berlin Email: [email protected] Present REDUCE form by Winfried Neun ZIB Berlin Email: [email protected] 1 Introduction This package can expand functions of certain type into their corresponding Laurent-Puiseux series as a sum of terms of the form X1 mk=n+s ak(x − x0) k=0 where m is the ‘symmetry number’, s is the ‘shift number’, n is the ‘Puiseux number’, and x0 is the ‘point of development’. The following types are supported: • functions of ‘rational type’, which are either rational or have a rational derivative of some order; • functions of ‘hypergeometric type’ where a(k + m)=a(k) is a ra- tional function for some integer m; • functions of ‘explike type’ which satisfy a linear homogeneous dif- ferential equation with constant coefficients. 1 2 REDUCE OPERATOR FPS 2 The FPS package is an implementation of the method presented in [2]. The implementations of this package for Maple (by D. Gruntz) and Mathe- matica (by W. Koepf) served as guidelines for this one. Numerous examples can be found in [3]–[4], most of which are contained in the test file fps.tst. Many more examples can be found in the extensive bibliography of Hansen [1]. 2 REDUCE operator FPS The FPS Package must be loaded first by: load FPS; FPS(f,x,x0) tries to find a formal power series expansion for f with respect to the variable x at the point of development x0. It also works for formal Laurent (negative exponents) and Puiseux series (fractional exponents).