Composition Algebras Over Algebraic Curves of Genus Zero
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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). -
Center and Composition Conditions for Abel Equation
Center and Comp osition conditions for Ab el Equation Thesis for the degree of Do ctor of Philosophy by Michael Blinov Under the Sup ervision of professor Yosef Yomdin Department of Theoretical Mathematics The Weizmann Institute of Science Submitted to the Feinb erg Graduate Scho ol of the Weizmann Institute of Science Rehovot Israel June Acknowledgments I would like to thank my advisor Professor Yosef Yomdin for his great sup ervision constant supp ort and encouragement for guiding and stimulat ing my mathematical work I should also mention that my trips to scien tic meetings were supp orted from Y Yomdins Minerva Science Foundation grant I am grateful to JP Francoise F Pakovich E Shulman S Yakovenko and V Katsnelson for interesting discussions I thank Carla Scapinello Uruguay Jonatan Gutman Israel Michael Kiermaier Germany and Oleg Lavrovsky Canada for their results obtained during summer pro jects that I sup ervised I am also grateful to my mother for her patience supp ort and lo ve I wish to thank my mathematical teacher V Sap ozhnikov who gave the initial push to my mathematical research Finally I wish to thank the following for their friendship and in some cases love Lili Eugene Bom Elad Younghee Ira Rimma Yulia Felix Eduard Lena Dima Oksana Olga Alex and many more Abstract We consider the real vector eld f x y gx y on the real plane IR This vector eld describ es the dynamical system x f x y y g x y A classical CenterFo cus problem whichwas stated byHPoincare in s is nd conditions on f g under which all tra jectories -
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. -
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. -
Arxiv:1711.00219V2 [Math.OA] 9 Aug 2019 R,Fe Rbblt,Glbr Coefficients
CUMULANTS, SPREADABILITY AND THE CAMPBELL-BAKER-HAUSDORFF SERIES TAKAHIRO HASEBE AND FRANZ LEHNER Abstract. We define spreadability systems as a generalization of exchangeability systems in order to unify various notions of independence and cumulants known in noncommutative probability. In particular, our theory covers monotone independence and monotone cumulants which do not satisfy exchangeability. To this end we study generalized zeta and M¨obius functions in the context of the incidence algebra of the semilattice of ordered set partitions and prove an appropriate variant of Faa di Bruno’s theorem. With the aid of this machinery we show that our cumulants cover most of the previously known cumulants. Due to noncommutativity of independence the behaviour of these cumulants with respect to independent random variables is more complicated than in the exchangeable case and the appearance of Goldberg coefficients exhibits the role of the Campbell-Baker-Hausdorff series in this context. In a final section we exhibit an interpretation of the Campbell-Baker-Hausdorff series as a sum of cumulants in a particular spreadability system, thus providing a new derivation of the Goldberg coefficients. Contents 1. Introduction 2 2. Ordered set partitions 4 2.1. Set partitions 4 2.2. Ordered set partitions 5 2.3. Incidence algebras and multiplicative functions 8 2.4. Special functions in the poset of ordered set partitions 10 3. A generalized notion of independence related to spreadability systems 11 3.1. Notation and terminology 11 3.2. Spreadability systems 13 3.3. Examples from natural products of linear maps 14 3.4. E-independence 15 3.5. -
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. -
Arxiv:1103.4922V1 [Math.NT] 25 Mar 2011 Hoyo Udai Om.Let Forms
QUATERNION ORDERS AND TERNARY QUADRATIC FORMS STEFAN LEMURELL Introduction The main purpose of this paper is to provide an introduction to the arith- metic theory of quaternion algebras. However, it also contains some new results, most notably in Section 5. We will emphasise on the connection between quaternion algebras and quadratic forms. This connection will pro- vide us with an efficient tool to consider arbitrary orders instead of having to restrict to special classes of them. The existing results are mostly restricted to special classes of orders, most notably to so called Eichler orders. The paper is organised as follows. Some notations and background are provided in Section 1, especially on the theory of quadratic forms. Section 2 contains the basic theory of quaternion algebras. Moreover at the end of that section, we give a quite general solution to the problem of representing a quaternion algebra with given discriminant. Such a general description seems to be lacking in the literature. Section 3 gives the basic definitions concerning orders in quaternion alge- bras. In Section 4, we prove an important correspondence between ternary quadratic forms and quaternion orders. Section 5 deals with orders in quaternion algebras over p-adic fields. The major part is an investigation of the isomorphism classes in the non-dyadic and 2-adic cases. The starting- point is the correspondence with ternary quadratic forms and known classi- fications of such forms. From this, we derive representatives of the isomor- phism classes of quaternion orders. These new results are complements to arXiv:1103.4922v1 [math.NT] 25 Mar 2011 existing more ring-theoretic descriptions of orders. -
Algebraic Foundations of Split Hypercomplex Nonlinear Adaptive
Mathematical Methods in the Research Article Applied Sciences Received XXXX (www.interscience.wiley.com) DOI: 10.1002/sim.0000 MOS subject classification: 60G35; 15A66 Algebraic foundations of split hypercomplex nonlinear adaptive filtering E. Hitzer∗ A split hypercomplex learning algorithm for the training of nonlinear finite impulse response adaptive filters for the processing of hypercomplex signals of any dimension is proposed. The derivation strictly takes into account the laws of hypercomplex algebra and hypercomplex calculus, some of which have been neglected in existing learning approaches (e.g. for quaternions). Already in the case of quaternions we can predict improvements in performance of hypercomplex processes. The convergence of the proposed algorithms is rigorously analyzed. Copyright c 2011 John Wiley & Sons, Ltd. Keywords: Quaternionic adaptive filtering, Hypercomplex adaptive filtering, Nonlinear adaptive filtering, Hypercomplex Multilayer Perceptron, Clifford geometric algebra 1. Introduction Split quaternion nonlinear adaptive filtering has recently been treated by [23], who showed its superior performance for Saito’s Chaotic Signal and for wind forecasting. The quaternionic methods constitute a generalization of complex valued adaptive filters, treated in detail in [19]. A method of quaternionic least mean square algorithm for adaptive quaternionic has previously been developed in [22]. Additionally, [24] successfully proposes the usage of local analytic fully quaternionic functions in the Quaternion Nonlinear Gradient Descent (QNGD). Yet the unconditioned use of analytic fully quaternionic activation functions in neural networks faces problems with poles due to the Liouville theorem [3]. The quaternion algebra of Hamilton is a special case of the higher dimensional Clifford algebras [10]. The problem with poles in nonlinear analytic functions does not generally occur for hypercomplex activation functions in Clifford algebras, where the Dirac and the Cauchy-Riemann operators are not elliptic [21], as shown, e.g., for hyperbolic numbers in [17]. -
Quaternion Algebras Applications of Quaternion Algebras
Quaternion Algebras Applications of Quaternion Algebras Quaternion Algebras Properties and Applications Rob Eimerl 1Department of Mathematics University of Puget Sound May 5th, 2015 Quaternion Algebras Applications of Quaternion Algebras Quaternion Algebra • Definition: Let F be a field and A be a vector space over a over F with an additional operation (∗) from A × A to A. Then A is an algebra over F , if the following expressions hold for any three elements x; y; z 2 F , and any a; b 2 F : 1. Right Distributivity: (x + y) ∗ z = x ∗ z + y ∗ z 2. Left Distributivity: x*(y+z) = (x * y) + (x * z) 3. Compatability with Scalers: (ax)*(by) = (ab)(x * y) • Definition: A quaternion algebra is a 4-dimensional algebra over a field F with a basis f1; i; j; kg such that i 2 = a; j2 = b; ij = −ji = k for some a; b 2 F x . F x is the set of units in F . a;b • For q 2 F , q = α + βi + γj + δk, where α; β; γ; δ 2 F Quaternion Algebras Applications of Quaternion Algebras Existence of Quaternion Algebras x a;b Theorem 1: Let a; b 2 F , then F exists. Proof : Grab α; β in an algebra E of F such that α2 = a and β2 = −b. Let α 0 0 β i = ; j = 0 −α −β 0 Then 0 αβ i 2 = a; j2 = b; ij = = −ji: αβ 0 Since fI2; i; j; ijg is linearly independent over E it is also linearly independent over F . Therefore F -span of fI2; i; j; ijg is a a;b 4-dimensional algebra Q over F , and Q = F Quaternion Algebras Applications of Quaternion Algebras Associated Quantities of Quaternion Algebras Pure Quaternions: Let f1; i; j; kg be a standard basis for a quaternion algebra Q. -
Dynatomic Polynomials, Necklace Operators, and Universal Relations for Dynamical Units
DYNATOMIC POLYNOMIALS, NECKLACE OPERATORS, AND UNIVERSAL RELATIONS FOR DYNAMICAL UNITS JOHN R. DOYLE, PAUL FILI, AND TREVOR HYDE 1. INTRODUCTION Let f(x) 2 K[x] be a polynomial with coefficients in a field K. For an integer k ≥ 0, we denote by f k(x) the k-fold iterated composition of f with itself. The dth dynatomic polynomial Φf;d(x) 2 K[x] of f is defined by the product Y d=e µ(e) Φf;d(x) := (f (x) − x) ; ejd where µ is the standard number-theoretic Möbius function on N. We refer the reader to [12, §4.1] for background on dynatomic polynomials. For generic f(x), the dth dynatomic polyno- mial Φf;d(x) vanishes at precisely the periodic points of f with primitive period d. In this paper we consider the polynomial equation Φf;d(x) = 1 and show that it often has f-preperiodic solu- tions determined by arithmetic properties of d, independent of f. Moreover, these f-preperiodic solutions are detected by cyclotomic factors of the dth necklace polynomial: 1 X M (x) = µ(e)xd=e 2 [x]: d d Q ejd Our results extend earlier work of Morton and Silverman [8], but our techniques are quite dif- ferent and apply more broadly. We begin by recalling some notation and terminology. The cocore of a positive integer d is d=d0 where d0 is the largest squarefree factor of d. If m ≥ 0 and n ≥ 1, then the (m; n)th generalized dynatomic polynomial Φf;m;n(x) of f(x) is defined by Φf;0;n(x) := Φf;n(x) and m Φf;n(f (x)) Φf;m;n(x) := m−1 Φf;n(f (x)) for m ≥ 1.