The Severi-Brauer Variety Associated to a Central Simple Algebra
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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). -
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. -
Algebraic Groups I. Homework 8 1. Let a Be a Central Simple Algebra Over a field K, T a K-Torus in A×
Algebraic Groups I. Homework 8 1. Let A be a central simple algebra over a field k, T a k-torus in A×. (i) Adapt Exercise 5 in HW5 to make an ´etalecommutative k-subalgebra AT ⊆ A such that (AT )ks is × generated by T (ks), and establish a bijection between the sets of maximal k-tori in A and maximal ´etale commutative k-subalgebras of A. Deduce that SL(A) is k-anisotropic if and only if A is a division algebra. (ii) For an ´etalecommutative k-subalgebra C ⊆ A, prove ZA(C) is a semisimple k-algebra with center C. × (iv) If T is maximal as a k-split subtorus of A prove T is the k-group of units in AT and that the (central!) simple factors Bi of BT := ZA(AT ) are division algebras. (v) Fix A ' EndD(V ) for a right module V over a central division algebra D, so V is a left A-module and Q × V = Vi with nonzero left Bi-modules Vi. If T is maximal as a k-split torus in A , prove Vi has rank 1 × × over Bi and D, so Bi ' D. Using D-bases, deduce that all maximal k-split tori in A are A (k)-conjugate. 2. For a torus T over a local field k (allow R, C), prove T is k-anisotropic if and only if T (k) is compact. 3. Let Y be a smooth separated k-scheme locally of finite type, and T a k-torus with a left action on Y . -
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. -
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]). -
Differential Central Simple Algebras and Picard–Vessiot
Differential Central Simple Algebras and Picard–Vessiot Representations Lourdes Juan Department of Mathematics Texas Tech University Lubbock TX 79409 Andy R. Magid Department of Mathematics University of Oklahoma Norman OK 73019 March 7, 2007 Abstract A differential central simple algebra, and in particular a differential matrix algebra, over a differential field K with constants C can be trivial- ized by a Picard–Vessiot (differential Galois) extension E. In the matrix algebra case, there is a correspondence between K algebras trivialized by E and representations of the Galois group of E over K in P GLn(C), which can be interpreted as cocyles equivalent up to coboundaries. 1 Introduction Let K be a differential field with algebraically closed characteristic zero field of constants C and derivation D = DK . By a differential central simple al- gebra (DCSA) over K we mean a pair (A, D) where A is a central simple K algebra and D is a derivation of A extending the derivation D of its center K. Given two such pairs (A1, D1) and (A2, D2), we can form the differential algebra (A1 ⊗ A2, D1 ⊗ D2), where the derivation D1 ⊗ D2 is given by D1 ⊗ 1 + 1 ⊗ D2. Morphisms of DCSA’s over K are K algebra homomorphisms preserving deriva- tions. We denote the isomorphism class of (A, D) by [A, D]. The above tensor product defines a monoid operation on the isomorphism classes (the identity being the class [K, DK ]), and hence we can form the corresponding universal diff group K0 Az(K). (A central simple algebra (CSA) over a field is a special case of Azumaya, or central separable, algebras over rings; Az is an abbre- viation for Azumaya.) The corresponding object for K when derivations are not considered is the familiar K0Az(K) as defined by Bass in [1, Chapter III]. -
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.