Orders of Quaternion Algebras Over Number Fields
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The Class Number One Problem for Imaginary Quadratic Fields
MODULAR CURVES AND THE CLASS NUMBER ONE PROBLEM JEREMY BOOHER Gauss found 9 imaginary quadratic fields with class number one, and in the early 19th century conjectured he had found all of them. It turns out he was correct, but it took until the mid 20th century to prove this. Theorem 1. Let K be an imaginary quadratic field whose ring of integers has class number one. Then K is one of p p p p p p p p Q(i); Q( −2); Q( −3); Q( −7); Q( −11); Q( −19); Q( −43); Q( −67); Q( −163): There are several approaches. Heegner [9] gave a proof in 1952 using the theory of modular functions and complex multiplication. It was dismissed since there were gaps in Heegner's paper and the work of Weber [18] on which it was based. In 1967 Stark gave a correct proof [16], and then noticed that Heegner's proof was essentially correct and in fact equiv- alent to his own. Also in 1967, Baker gave a proof using lower bounds for linear forms in logarithms [1]. Later, Serre [14] gave a new approach based on modular curve, reducing the class number + one problem to finding special points on the modular curve Xns(n). For certain values of n, it is feasible to find all of these points. He remarks that when \N = 24 An elliptic curve is obtained. This is the level considered in effect by Heegner." Serre says nothing more, and later writers only repeat this comment. This essay will present Heegner's argument, as modernized in Cox [7], then explain Serre's strategy. -
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). -
MAXIMAL and NON-MAXIMAL ORDERS 1. Introduction Let K Be A
MAXIMAL AND NON-MAXIMAL ORDERS LUKE WOLCOTT Abstract. In this paper we compare and contrast various prop- erties of maximal and non-maximal orders in the ring of integers of a number field. 1. Introduction Let K be a number field, and let OK be its ring of integers. An order in K is a subring R ⊆ OK such that OK /R is finite as a quotient of abelian groups. From this definition, it’s clear that there is a unique maximal order, namely OK . There are many properties that all orders in K share, but there are also differences. The main difference between a non-maximal order and the maximal order is that OK is integrally closed, but every non-maximal order is not. The result is that many of the nice properties of Dedekind domains do not hold in arbitrary orders. First we describe properties common to both maximal and non-maximal orders. In doing so, some useful results and constructions given in class for OK are generalized to arbitrary orders. Then we de- scribe a few important differences between maximal and non-maximal orders, and give proofs or counterexamples. Several proofs covered in lecture or the text will not be reproduced here. Throughout, all rings are commutative with unity. 2. Common Properties Proposition 2.1. The ring of integers OK of a number field K is a Noetherian ring, a finitely generated Z-algebra, and a free abelian group of rank n = [K : Q]. Proof: In class we showed that OK is a free abelian group of rank n = [K : Q], and is a ring. -
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. -
Artinian Subrings of a Commutative Ring
transactions of the american mathematical society Volume 336, Number 1, March 1993 ARTINIANSUBRINGS OF A COMMUTATIVERING ROBERT GILMER AND WILLIAM HEINZER Abstract. Given a commutative ring R, we investigate the structure of the set of Artinian subrings of R . We also consider the family of zero-dimensional subrings of R. Necessary and sufficient conditions are given in order that every zero-dimensional subring of a ring be Artinian. We also consider closure properties of the set of Artinian subrings of a ring with respect to intersection or finite intersection, and the condition that the set of Artinian subrings of a ring forms a directed family. 1. Introduction Suppose R is a commutative ring with unity element. We consider here various properties of the family sf of Artinian subrings of R and the family Z of zero-dimensional subrings of R . We remark that the inclusion s? ç Z may be proper, even if R is Noetherian; for example, Corollary 3.4 implies that if K is an infinite field of positive characteristic, then the local principal ideal ring K[X]/(X2) contains a zero-dimensional subring that is not Artinian. Of course, if every subring of R were Noetherian, the families sf and Z would be identical. Thus one source of motivation for this work comes from papers such as [Gi, Wi, W2, GHi, GH3] that deal with Noetherian and zero- dimensional pairs of rings, hereditarily Noetherian rings, and hereditarily zero- dimensional rings. Another source of motivation is related to our work in [GH3], where we considered several problems concerning a direct product of zero-dimensional rings. -
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. -
Maximal Orders of Quaternions
Maximal Orders of Quaternions Alyson Deines Quaternion Algebras Maximal Orders of Quaternions Maximal Orders Norms, Traces, and Alyson Deines Integrality Local Fields and Hilbert Symbols December 8th Math 581b Final Project Uses A non-commutative analogue of Rings of Integers of Number Field Abstract Maximal Orders of Quaternions Alyson Deines Abstract Quaternion I will define maximal orders of quaternion algebras, give Algebras Maximal examples, discuss how they are similar to and differ from rings Orders of integers, and then I will discuss one of their applications . Norms, Traces, and Integrality Local Fields and Hilbert Symbols Uses Quaternion Algebras over Number Fields Maximal Orders of Definition Quaternions Alyson Deines Let F be a field and a; b 2 F . A quaternion algebra over F is an F -algebra B = a;b Quaternion F Algebras with basis Maximal 2 2 Orders i = a; j = b; and ij = −ji: Norms, Traces, and Integrality Examples: Local Fields −1;−1 and Hilbert = Symbols H R p Uses −1;−1 F = Q( 5), B = F 1;b ∼ Let F be any number field, F = M2(F ) via 1 0 0 b i 7! and j 7! 0 −1 1 0 Maximal Orders Maximal Orders of Quaternions Lattices Alyson Deines Let F be a number field with ring of integers R and let V Quaternion be a finite dimensional F -vector space. Algebras An R-lattice of V is a finitely generated R-submodule Maximal Orders O ⊂ V such that OF = V . Norms, Traces, and Integrality Orders Local Fields and Hilbert Let F be a number field with ring of integers R and let B Symbols be a finite dimensional F -algebra. -
Ring (Mathematics) 1 Ring (Mathematics)
Ring (mathematics) 1 Ring (mathematics) In mathematics, a ring is an algebraic structure consisting of a set together with two binary operations usually called addition and multiplication, where the set is an abelian group under addition (called the additive group of the ring) and a monoid under multiplication such that multiplication distributes over addition.a[›] In other words the ring axioms require that addition is commutative, addition and multiplication are associative, multiplication distributes over addition, each element in the set has an additive inverse, and there exists an additive identity. One of the most common examples of a ring is the set of integers endowed with its natural operations of addition and multiplication. Certain variations of the definition of a ring are sometimes employed, and these are outlined later in the article. Polynomials, represented here by curves, form a ring under addition The branch of mathematics that studies rings is known and multiplication. as ring theory. Ring theorists study properties common to both familiar mathematical structures such as integers and polynomials, and to the many less well-known mathematical structures that also satisfy the axioms of ring theory. The ubiquity of rings makes them a central organizing principle of contemporary mathematics.[1] Ring theory may be used to understand fundamental physical laws, such as those underlying special relativity and symmetry phenomena in molecular chemistry. The concept of a ring first arose from attempts to prove Fermat's last theorem, starting with Richard Dedekind in the 1880s. After contributions from other fields, mainly number theory, the ring notion was generalized and firmly established during the 1920s by Emmy Noether and Wolfgang Krull.[2] Modern ring theory—a very active mathematical discipline—studies rings in their own right. -
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. -
On the Tensor Product of Two Composition Algebras
On The Tensor Product of Two Composition Algebras Patrick J. Morandi S. Pumplun¨ 1 Introduction Let C1 F C2 be the tensor product of two composition algebras over a field F with char(F ) =¡ 2. R. Brauer [7] and A. A. Albert [1], [2], [3] seemed to be the first math- ematicians who investigated the tensor product of two quaternion algebras. Later their results were generalized to this more general situation by B. N. Allison [4], [5], [6] and to biquaternion algebras over rings by Knus [12]. In the second section we give some new results on the Albert form of these algebras. We also investigate the F -quadric defined by this Albert form, generalizing a result of Knus ([13]). £ £ Since Allison regarded the involution ¢ = 1 2 as an essential part of the algebra C = C1 C2, he only studied automorphisms of C which are compatible with ¢ . In the last section we show that any automorphism of C that preserves a certain biquaternion subalgebra also is compatible with ¢ . As a consequence, if C is the tensor product of two octonion algebras, we show that C does not satisfy the Skolem-Noether Theorem. Let F be a field and C a unital, nonassociative F -algebra. Then C is a composition algebra if there exists a nondegenerate quadratic form n : C ¤ F such that n(x · y) = n(x)n(y) for all x, y ¥ C. The form n is uniquely determined by these conditions and is called the norm of C. We will write n = nC . Composition algebras only exist in ranks 1, 2, 4 or 8 (see [10]). -
The Arithmetic Hyperbolic 3-Manifold of Smallest Volume
THE ARITHMETIC HYPERBOLIC 3-MANIFOLD OF SMALLEST VOLUME Ted Chinburg * Eduardo Friedman ** Kerry N. Jones y Alan W. Reid yy Abstract. We show that the arithmetic hyperbolic 3-manifold of smallest volume is the Weeks manifold. The next smallest one is the Meyerhoff manifold. 0. Introduction x A hyperbolic 3-manifold is a 3-manifold admitting a complete Riemannian metric all of whose sectional curvatures are 1. The universal cover of such a manifold can therefore be identified with the hyperbolic− 3-space, that is, the unique connected and simply connected hyperbolic 3-manifold. We denote by H3 = (z; t) C R t > 0 ; f 2 ⊕ j g the upper half space model of hyperbolic 3-space. With this convention, the full group of orientation-preserving isometries of H3 is simply PGL(2; C). A Kleinian group Γ is a discrete subgroup of PGL(2; C). Hence an orientable hyperbolic 3- manifold is the quotient of H3 by a torsion-free Kleinian group, since this acts properly discontinuously and freely on H3. If we relax the condition that Γ act freely, allowing Γ to contain torsion elements, we obtain a complete orientable hyperbolic 3-orbifold (cf. [Th] for further details). We will only be concerned with the case that M = H3=Γ has a hyperbolic structure of finite volume (we say Γ has finite covolume). Therefore in what follows, by a hyperbolic 3-manifold or 3-orbifold we shall always mean a complete orientable hyperbolic 3-manifold or 3-orbifold of finite volume. By the Mostow and Prasad Rigidity Theorems [Mo] [Pr], hyperbolic volume is a topological invariant of a hyperbolic 3-orbifold and is therefore a natural object to study.