RATIONAL POINTS Contents Introduction 1 1. Conics, Quaternion
Total Page:16
File Type:pdf, Size:1020Kb
Load more
Recommended publications
-
Quaternions and Cli Ord Geometric Algebras
Quaternions and Cliord Geometric Algebras Robert Benjamin Easter First Draft Edition (v1) (c) copyright 2015, Robert Benjamin Easter, all rights reserved. Preface As a rst rough draft that has been put together very quickly, this book is likely to contain errata and disorganization. The references list and inline citations are very incompete, so the reader should search around for more references. I do not claim to be the inventor of any of the mathematics found here. However, some parts of this book may be considered new in some sense and were in small parts my own original research. Much of the contents was originally written by me as contributions to a web encyclopedia project just for fun, but for various reasons was inappropriate in an encyclopedic volume. I did not originally intend to write this book. This is not a dissertation, nor did its development receive any funding or proper peer review. I oer this free book to the public, such as it is, in the hope it could be helpful to an interested reader. June 19, 2015 - Robert B. Easter. (v1) [email protected] 3 Table of contents Preface . 3 List of gures . 9 1 Quaternion Algebra . 11 1.1 The Quaternion Formula . 11 1.2 The Scalar and Vector Parts . 15 1.3 The Quaternion Product . 16 1.4 The Dot Product . 16 1.5 The Cross Product . 17 1.6 Conjugates . 18 1.7 Tensor or Magnitude . 20 1.8 Versors . 20 1.9 Biradials . 22 1.10 Quaternion Identities . 23 1.11 The Biradial b/a . -
Arxiv:1001.0240V1 [Math.RA]
Fundamental representations and algebraic properties of biquaternions or complexified quaternions Stephen J. Sangwine∗ School of Computer Science and Electronic Engineering, University of Essex, Wivenhoe Park, Colchester, CO4 3SQ, United Kingdom. Email: [email protected] Todd A. Ell† 5620 Oak View Court, Savage, MN 55378-4695, USA. Email: [email protected] Nicolas Le Bihan GIPSA-Lab D´epartement Images et Signal 961 Rue de la Houille Blanche, Domaine Universitaire BP 46, 38402 Saint Martin d’H`eres cedex, France. Email: [email protected] October 22, 2018 Abstract The fundamental properties of biquaternions (complexified quaternions) are presented including several different representations, some of them new, and definitions of fundamental operations such as the scalar and vector parts, conjugates, semi-norms, polar forms, and inner and outer products. The notation is consistent throughout, even between representations, providing a clear account of the many ways in which the component parts of a biquaternion may be manipulated algebraically. 1 Introduction It is typical of quaternion formulae that, though they be difficult to find, once found they are immediately verifiable. J. L. Synge (1972) [43, p34] arXiv:1001.0240v1 [math.RA] 1 Jan 2010 The quaternions are relatively well-known but the quaternions with complex components (complexified quaternions, or biquaternions1) are less so. This paper aims to set out the fundamental definitions of biquaternions and some elementary results, which, although elementary, are often not trivial. The emphasis in this paper is on the biquaternions as an applied algebra – that is, a tool for the manipulation ∗This paper was started in 2005 at the Laboratoire des Images et des Signaux (now part of the GIPSA-Lab), Grenoble, France with financial support from the Royal Academy of Engineering of the United Kingdom and the Centre National de la Recherche Scientifique (CNRS). -
Gauging the Octonion Algebra
UM-P-92/60_» Gauging the octonion algebra A.K. Waldron and G.C. Joshi Research Centre for High Energy Physics, University of Melbourne, Parkville, Victoria 8052, Australia By considering representation theory for non-associative algebras we construct the fundamental and adjoint representations of the octonion algebra. We then show how these representations by associative matrices allow a consistent octonionic gauge theory to be realized. We find that non-associativity implies the existence of new terms in the transformation laws of fields and the kinetic term of an octonionic Lagrangian. PACS numbers: 11.30.Ly, 12.10.Dm, 12.40.-y. Typeset Using REVTEX 1 L INTRODUCTION The aim of this work is to genuinely gauge the octonion algebra as opposed to relating properties of this algebra back to the well known theory of Lie Groups and fibre bundles. Typically most attempts to utilise the octonion symmetry in physics have revolved around considerations of the automorphism group G2 of the octonions and Jordan matrix representations of the octonions [1]. Our approach is more simple since we provide a spinorial approach to the octonion symmetry. Previous to this work there were already several indications that this should be possible. To begin with the statement of the gauge principle itself uno theory shall depend on the labelling of the internal symmetry space coordinates" seems to be independent of the exact nature of the gauge algebra and so should apply equally to non-associative algebras. The octonion algebra is an alternative algebra (the associator {x-1,y,i} = 0 always) X -1 so that the transformation law for a gauge field TM —• T^, = UY^U~ — ^(c^C/)(/ is well defined for octonionic transformations U. -
Arithmetic of Hyperbolic 3-Manifolds
Arithmetic of Hyperbolic 3-Manifolds Alan Reid Rice University Hyperbolic 3-Manifolds and Discrete Groups Hyperbolic 3-space can be defined as 3 H = f(z; t) 2 C × R : t > 0g dsE and equipped with the metric ds = t . Geodesics are vertical lines perpendicular to C or semi-circles perpendicular to C. Codimension 1 geodesic submanifolds are Euclidean planes in 3 H orthogonal to C or hemispheres centered on C. 3 The full group of orientation-preserving isometries of H can be identified with PSL(2; C). Abuse of notation We will often view Kleinian groups as groups of matrices! A discrete subgroup of PSL(2; C) is called a Kleinian group. 3 Such a group acts properly discontinuously on H . If Γ is torsion-free (does not contain elements of finite order) then Γ acts freely. 3 In this latter case we get a quotient manifold H =Γ and a 3 3 covering map H ! H =Γ which is a local isometry. 3 We will be interested in the case when H =Γ has finite volume. Note: If Γ is a finitely generated subgroup of PSL(2; C) there is always a finite index subgroup that is torsion-free. Examples 1. Let d be a square-freep positive integer, and Od the ring of algebraic integers in Q( −d). Then PSL(2; Od) is a Kleinian group. 3 Indeed H =PSL(2; Od) has finite volume but is non-compact. These are known as the Bianchi groups. d = 1 (picture by Jos Leys) 2. Reflection groups. Tessellation by all right dodecahedra (from the Not Knot video) 3.Knot Complements The Figure-Eight Knot Thurston's hyperbolization theorem shows that many knots have complements that are hyperbolic 3-manifolds of finite volume. -
Division Rings and V-Domains [4]
PROCEEDINGS OF THE AMERICAN MATHEMATICAL SOCIETY Volume 99, Number 3, March 1987 DIVISION RINGS AND V-DOMAINS RICHARD RESCO ABSTRACT. Let D be a division ring with center k and let fc(i) denote the field of rational functions over k. A square matrix r 6 Mn(D) is said to be totally transcendental over fc if the evaluation map e : k[x] —>Mn(D), e(f) = }(r), can be extended to fc(i). In this note it is shown that the tensor product D®k k(x) is a V-domain which has, up to isomorphism, a unique simple module iff any two totally transcendental matrices of the same order over D are similar. The result applies to the class of existentially closed division algebras and gives a partial solution to a problem posed by Cozzens and Faith. An associative ring R is called a right V-ring if every simple right fi-module is injective. While it is easy to see that any prime Goldie V-ring is necessarily simple [5, Lemma 5.15], the first examples of noetherian V-domains which are not artinian were constructed by Cozzens [4]. Now, if D is a division ring with center k and if k(x) is the field of rational functions over k, then an observation of Jacobson [7, p. 241] implies that the simple noetherian domain D (g)/.k(x) is a division ring iff the matrix ring Mn(D) is algebraic over k for every positive integer n. In their monograph on simple noetherian rings, Cozzens and Faith raise the question of whether this tensor product need be a V-domain [5, Problem (13), p. -
The Geometry and Topology of Arithmetic Hyperbolic 3-Manifolds
The geometry and topology of arithmetic hyperbolic 3-manifolds Alan W. Reid∗ May 12, 2007 1 Introduction This paper is based on three lectures given by the author at the RIMS Symposium, “Topology, Com- plex Analysis and Arithmetic of Hyperbolic Spaces” held at the Research Institute for Mathematical Sciences, Kyoto University, in December 2006. The goal of the lectures was to describe recent work on understanding topological and geometric properties of arithmetic hyperbolic 3-manifolds, and the connections with number theory. This is the theme of the paper. Our discussion of topological aspects of arithmetic hyperbolic 3-orbifolds is motivated by the following central conjectures from 3-manifold topology: Conjecture 1.1. Let M be a closed hyperbolic 3-manifold, then M is virtually Haken; ie M has a finite sheeted cover N which contains embedded incompressible surface (necessarily of genus at least 2). Conjecture 1.2. Let M be a closed hyperbolic 3-manifold, then M has a finite sheeted cover N for which b1(N) > 0 (where b1(N) is the first Betti number of N). We can also rephrase Conjecture 1.2 to say that vb1(M) > 0 where vb1(M) is defined by vb1(M) = sup{b1(N) : N is a finite cover of M}, and is called the virtual first Betti number of M. Conjecture 1.3. Let M be a closed hyperbolic 3-manifold, then vb1(M) = ∞. Conjecture 1.4. Let M be a closed hyperbolic 3-manifold, then π1(M) is large; that is to say, some finite index subgroup of π1(M) admits a surjective homomorphism onto a non-abelian free group. -
An Introduction to Central Simple Algebras and Their Applications to Wireless Communication
Mathematical Surveys and Monographs Volume 191 An Introduction to Central Simple Algebras and Their Applications to Wireless Communication Grégory Berhuy Frédérique Oggier American Mathematical Society http://dx.doi.org/10.1090/surv/191 An Introduction to Central Simple Algebras and Their Applications to Wireless Communication Mathematical Surveys and Monographs Volume 191 An Introduction to Central Simple Algebras and Their Applications to Wireless Communication Grégory Berhuy Frédérique Oggier American Mathematical Society Providence, Rhode Island EDITORIAL COMMITTEE Ralph L. Cohen, Chair Benjamin Sudakov Robert Guralnick MichaelI.Weinstein MichaelA.Singer 2010 Mathematics Subject Classification. Primary 12E15; Secondary 11T71, 16W10. For additional information and updates on this book, visit www.ams.org/bookpages/surv-191 Library of Congress Cataloging-in-Publication Data Berhuy, Gr´egory. An introduction to central simple algebras and their applications to wireless communications /Gr´egory Berhuy, Fr´ed´erique Oggier. pages cm. – (Mathematical surveys and monographs ; volume 191) Includes bibliographical references and index. ISBN 978-0-8218-4937-8 (alk. paper) 1. Division algebras. 2. Skew fields. I. Oggier, Fr´ed´erique. II. Title. QA247.45.B47 2013 512.3–dc23 2013009629 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. -
Subfields of Central Simple Algebras
The Brauer Group Subfields of Algebras Subfields of Central Simple Algebras Patrick K. McFaddin University of Georgia Feb. 24, 2016 Patrick K. McFaddin University of Georgia Subfields of Central Simple Algebras The Brauer Group Subfields of Algebras Introduction Central simple algebras and the Brauer group have been well studied over the past century and have seen applications to class field theory, algebraic geometry, and physics. Since higher K-theory defined in '72, the theory of algebraic cycles have been utilized to study geometric objects associated to central simple algebras (with involution). This new machinery has provided a functorial viewpoint in which to study questions of arithmetic. Patrick K. McFaddin University of Georgia Subfields of Central Simple Algebras The Brauer Group Subfields of Algebras Central Simple Algebras Let F be a field. An F -algebra A is a ring with identity 1 such that A is an F -vector space and α(ab) = (αa)b = a(αb) for all α 2 F and a; b 2 A. The center of an algebra A is Z(A) = fa 2 A j ab = ba for every b 2 Ag: Definition A central simple algebra over F is an F -algebra whose only two-sided ideals are (0) and (1) and whose center is precisely F . Examples An F -central division algebra, i.e., an algebra in which every element has a multiplicative inverse. A matrix algebra Mn(F ) Patrick K. McFaddin University of Georgia Subfields of Central Simple Algebras The Brauer Group Subfields of Algebras Why Central Simple Algebras? Central simple algebras are a natural generalization of matrix algebras. -
A Brief History of Ring Theory
A Brief History of Ring Theory by Kristen Pollock Abstract Algebra II, Math 442 Loyola College, Spring 2005 A Brief History of Ring Theory Kristen Pollock 2 1. Introduction In order to fully define and examine an abstract ring, this essay will follow a procedure that is unlike a typical algebra textbook. That is, rather than initially offering just definitions, relevant examples will first be supplied so that the origins of a ring and its components can be better understood. Of course, this is the path that history has taken so what better way to proceed? First, it is important to understand that the abstract ring concept emerged from not one, but two theories: commutative ring theory and noncommutative ring the- ory. These two theories originated in different problems, were developed by different people and flourished in different directions. Still, these theories have much in com- mon and together form the foundation of today's ring theory. Specifically, modern commutative ring theory has its roots in problems of algebraic number theory and algebraic geometry. On the other hand, noncommutative ring theory originated from an attempt to expand the complex numbers to a variety of hypercomplex number systems. 2. Noncommutative Rings We will begin with noncommutative ring theory and its main originating ex- ample: the quaternions. According to Israel Kleiner's article \The Genesis of the Abstract Ring Concept," [2]. these numbers, created by Hamilton in 1843, are of the form a + bi + cj + dk (a; b; c; d 2 R) where addition is through its components 2 2 2 and multiplication is subject to the relations i =pj = k = ijk = −1. -
Some Notes on the Real Numbers and Other Division Algebras
Some Notes on the Real Numbers and other Division Algebras August 21, 2018 1 The Real Numbers Here is the standard classification of the real numbers (which I will denote by R). Q Z N Irrationals R 1 I personally think of the natural numbers as N = f0; 1; 2; 3; · · · g: Of course, not everyone agrees with this particular definition. From a modern perspective, 0 is the \most natural" number since all other numbers can be built out of it using machinery from set theory. Also, I have never used (or even seen) a symbol for the whole numbers in any mathematical paper. No one disagrees on the definition of the integers Z = f0; ±1; ±2; ±3; · · · g: The fancy Z stands for the German word \Zahlen" which means \numbers." To avoid the controversy over what exactly constitutes the natural numbers, many mathematicians will use Z≥0 to stand for the non-negative integers and Z>0 to stand for the positive integers. The rational numbers are given the fancy symbol Q (for Quotient): n a o = a; b 2 ; b > 0; a and b share no common prime factors : Q b Z The set of irrationals is not given any special symbol that I know of and is rather difficult to define rigorously. The usual notion that a number is irrational if it has a non-terminating, non-repeating decimal expansion is the easiest characterization, but that actually entails a lot of baggage about representations of numbers. For example, if a number has a non-terminating, non-repeating decimal expansion, will its expansion in base 7 also be non- terminating and non-repeating? The answer is yes, but it takes some work to prove that. -
1. Introduction 2. Real Octonion Division Algebra
Pr´e-Publica¸c~oesdo Departamento de Matem´atica Universidade de Coimbra Preprint Number 19{02 EIGENVALUES OF MATRICES RELATED TO THE OCTONIONS ROGERIO´ SERODIO,^ PATR´ICIA DAMAS BEITES AND JOSE´ VITORIA´ Abstract: A pseudo real matrix representation of an octonion, which is based on two real matrix representations of a quaternion, is considered. We study how some operations defined on the octonions change the set of eigenvalues of the matrix obtained if these operations are performed after or before the matrix representation. The established results could be of particular interest to researchers working on estimation algorithms involving such operations. Keywords: Octonions, quaternions, real matrix representations, eigenvalues. Math. Subject Classification (2010): 11R52, 15A18. 1. Introduction Due to nonassociativity, the real octonion division algebra is not alge- braically isomorphic to a real matrix algebra. Despite this fact, pseudo real matrix representations of an octonion may be introduced, as in [1], through real matrix representations of a quaternion. In this work, the left matrix representation of an octonion over R, as called by Tian in [1], is considered. For the sake of completeness, some definitions and results, in particular on this pseudo representation, are recalled in Section 2. Using the mentioned representation, results concerning eigenvalues of ma- trices related to the octonions are established in Section 3. Previous research on this subject, although not explicitly applying real matrix representations of a quaternion, can be seen in [2]. 2. Real octonion division algebra Consider the real octonion division algebra O, that is, the usual real vector 8 space R , with canonical basis fe0; : : : ; e7g, equipped with the multiplication given by the relations eiej = −δije0 + "ijkek; Received January 28, 2019. -
1 Introduction 2 Central Simple Algebras
Alexandre Puttick Etale´ Cohomology December 13, 2018 Brauer groups and Galois Cohomology 1 Introduction The main goal of the next talks is to prove the following theorem: Theorem 1.1. Let K be a field extension of transcendence degree 1 over an algebraically 2 closed field k. Then Het´ (Spec K; Gm) = 0. sep Let k be an arbitrary field, and fix a separable closure k of k, and let Gk := Gal(ksep=k). The first step is to show Theorem 1.2 (Corollary 4.10). There is a natural bijection 2 sep × ∼ H Gk; (k ) = Br(k); (1.1) where Br(k) is the Brauer group of k. This is aim of the current talk. The main references are [1, Chapter IV] and [2, Tag 073W]. 2 Central simple algebras 2.1 Basic definitions and properties Let k be a field. In what follows, we use the term k-algebra to refer to an associative unital k-algebra which is finite dimensional as a k-vector space. In particular, we do not assume that k-algebras are commutative. Definition 2.1. A k-algebra is called simple if it contains no proper two sided ideals other than (0). Definition 2.2. A k-algebra A is said to be central if its center Z(A) is equal to k. If A is also simple, we say that it is central simple. We say a k-algebra D is a division algebra if every non-zero element has a multi- plicative inverse, i.e., for every a 2 D r f0g, there exists a b 2 D such that ab = 1 = ba.