The Group Sk 2 of a Biquaternion Algebra
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Hypercomplex Algebras and Their Application to the Mathematical
Hypercomplex Algebras and their application to the mathematical formulation of Quantum Theory Torsten Hertig I1, Philip H¨ohmann II2, Ralf Otte I3 I tecData AG Bahnhofsstrasse 114, CH-9240 Uzwil, Schweiz 1 [email protected] 3 [email protected] II info-key GmbH & Co. KG Heinz-Fangman-Straße 2, DE-42287 Wuppertal, Deutschland 2 [email protected] March 31, 2014 Abstract Quantum theory (QT) which is one of the basic theories of physics, namely in terms of ERWIN SCHRODINGER¨ ’s 1926 wave functions in general requires the field C of the complex numbers to be formulated. However, even the complex-valued description soon turned out to be insufficient. Incorporating EINSTEIN’s theory of Special Relativity (SR) (SCHRODINGER¨ , OSKAR KLEIN, WALTER GORDON, 1926, PAUL DIRAC 1928) leads to an equation which requires some coefficients which can neither be real nor complex but rather must be hypercomplex. It is conventional to write down the DIRAC equation using pairwise anti-commuting matrices. However, a unitary ring of square matrices is a hypercomplex algebra by definition, namely an associative one. However, it is the algebraic properties of the elements and their relations to one another, rather than their precise form as matrices which is important. This encourages us to replace the matrix formulation by a more symbolic one of the single elements as linear combinations of some basis elements. In the case of the DIRAC equation, these elements are called biquaternions, also known as quaternions over the complex numbers. As an algebra over R, the biquaternions are eight-dimensional; as subalgebras, this algebra contains the division ring H of the quaternions at one hand and the algebra C ⊗ C of the bicomplex numbers at the other, the latter being commutative in contrast to H. -
K-Theory and Algebraic Geometry
http://dx.doi.org/10.1090/pspum/058.2 Recent Titles in This Series 58 Bill Jacob and Alex Rosenberg, editors, ^-theory and algebraic geometry: Connections with quadratic forms and division algebras (University of California, Santa Barbara) 57 Michael C. Cranston and Mark A. Pinsky, editors, Stochastic analysis (Cornell University, Ithaca) 56 William J. Haboush and Brian J. Parshall, editors, Algebraic groups and their generalizations (Pennsylvania State University, University Park, July 1991) 55 Uwe Jannsen, Steven L. Kleiman, and Jean-Pierre Serre, editors, Motives (University of Washington, Seattle, July/August 1991) 54 Robert Greene and S. T. Yau, editors, Differential geometry (University of California, Los Angeles, July 1990) 53 James A. Carlson, C. Herbert Clemens, and David R. Morrison, editors, Complex geometry and Lie theory (Sundance, Utah, May 1989) 52 Eric Bedford, John P. D'Angelo, Robert E. Greene, and Steven G. Krantz, editors, Several complex variables and complex geometry (University of California, Santa Cruz, July 1989) 51 William B. Arveson and Ronald G. Douglas, editors, Operator theory/operator algebras and applications (University of New Hampshire, July 1988) 50 James Glimm, John Impagliazzo, and Isadore Singer, editors, The legacy of John von Neumann (Hofstra University, Hempstead, New York, May/June 1988) 49 Robert C. Gunning and Leon Ehrenpreis, editors, Theta functions - Bowdoin 1987 (Bowdoin College, Brunswick, Maine, July 1987) 48 R. O. Wells, Jr., editor, The mathematical heritage of Hermann Weyl (Duke University, Durham, May 1987) 47 Paul Fong, editor, The Areata conference on representations of finite groups (Humboldt State University, Areata, California, July 1986) 46 Spencer J. Bloch, editor, Algebraic geometry - Bowdoin 1985 (Bowdoin College, Brunswick, Maine, July 1985) 45 Felix E. -
Generic Splitting Fields of Central Simple Algebras: Galois Cohomology and Non-Excellence
GENERIC SPLITTING FIELDS OF CENTRAL SIMPLE ALGEBRAS: GALOIS COHOMOLOGY AND NON-EXCELLENCE OLEG T. IZHBOLDIN AND NIKITA A. KARPENKO Abstract. A field extension L=F is called excellent, if for any quadratic form ϕ over F the anisotropic part (ϕL)an of ϕ over L is defined over F ; L=F is called universally excellent, if L · E=E is excellent for any field ex- tension E=F . We study the excellence property for a generic splitting field of a central simple F -algebra. In particular, we show that it is universally excellent if and only if the Schur index of the algebra is not divisible by 4. We begin by studying the torsion in the second Chow group of products of Severi-Brauer varieties and its relationship with the relative Galois co- homology group H3(L=F ) for a generic (common) splitting field L of the corresponding central simple F -algebras. Let F be a field and let A1;:::;An be central simple F -algebras. A splitting field of this collection of algebras is a field extension L of F such that all the def algebras (Ai)L = Ai ⊗F L (i = 1; : : : ; n) are split. A splitting field L=F of 0 A1;:::;An is called generic (cf. [41, Def. C9]), if for any splitting field L =F 0 of A1;:::;An, there exists an F -place of L to L . Clearly, generic splitting field of A1;:::;An is not unique, however it is uniquely defined up to equivalence over F in the sense of [24, x3]. Therefore, working on problems (Q1) and (Q2) discussed below, we may choose any par- ticular generic splitting field L of the algebras A1;:::;An (cf. -
Hyperbolicity of Hermitian Forms Over Biquaternion Algebras
HYPERBOLICITY OF HERMITIAN FORMS OVER BIQUATERNION ALGEBRAS NIKITA A. KARPENKO Abstract. We show that a non-hyperbolic hermitian form over a biquaternion algebra over a field of characteristic 6= 2 remains non-hyperbolic over a generic splitting field of the algebra. Contents 1. Introduction 1 2. Notation 2 3. Krull-Schmidt principle 3 4. Splitting off a motivic summand 5 5. Rost correspondences 7 6. Motivic decompositions of some isotropic varieties 12 7. Proof of Main Theorem 14 References 16 1. Introduction Throughout this note (besides of x3 and x4) F is a field of characteristic 6= 2. The basic reference for the staff related to involutions on central simple algebras is [12].p The degree deg A of a (finite dimensional) central simple F -algebra A is the integer dimF A; the index ind A of A is the degree of a central division algebra Brauer-equivalent to A. Conjecture 1.1. Let A be a central simple F -algebra endowed with an orthogonal invo- lution σ. If σ becomes hyperbolic over the function field of the Severi-Brauer variety of A, then σ is hyperbolic (over F ). In a stronger version of Conjecture 1.1, each of two words \hyperbolic" is replaced by \isotropic", cf. [10, Conjecture 5.2]. Here is the complete list of indices ind A and coindices coind A = deg A= ind A of A for which Conjecture 1.1 is known (over an arbitrary field of characteristic 6= 2), given in the chronological order: • ind A = 1 | trivial; Date: January 2008. Key words and phrases. -
The Descent of Biquaternion Algebras in Characteristic
The descent of biquaternion algebras in characteristic two Demba Barrya,b, Adam Chapmanc, Ahmed Laghribid aFacult´edes Sciences et Techniques de Bamako, BP: E3206 Bamako, Mali bDepartement Wiskunde–Informatica, Universiteit Antwerpen, Belgium cDepartment of Computer Science, Tel-Hai College, Upper Galilee, 12208 Israel dUniversit´ed’Artois, Facult´edes Sciences Jean Perrin, Laboratoire de math´ematiques de Lens EA 2462, rue Jean Souvraz - SP18, 62307 Lens, France Abstract In this paper we associate an invariant to a biquaternion algebra B over a field K with a subfield F such that K/F is a quadratic separable extension and char(F) = 2. We show that this invariant is trivial exactly when B B0 ⊗ K for some biquaternion algebra B0 over F. We also study the behavior of this invariant under certain field extensions and provide several interesting examples. Keywords: Kato-Milne Cohomology, Cohomological invariants, Algebras with involution, Biquaternion algebras 2010 MSC: primary 11E81; secondary 11E04, 16K20, 19D45 1. Introduction Given a central simple algebra C over a field K with a subfield F, we say that C has a descent to F if there exists a central simple algebra C0 over F such that C C0 ⊗ K. When [K : F] = exp(C), one necessary condition for C to have a descent to F is that corK/F(C) ∼Br F, because if C C0⊗K ⊗[K:F] then corK/F(C) = corK/F(C0 ⊗ K) = C0 ∼Br F, where ∼Br denotes the Brauer equivalence. If K/F is a separable quadratic extension and Q is a quaternion algebra over K, then corK/F(Q) ∼Br F is a necessary and sufficient condition for Q to have a descent to F by [1, Chapter X, Theorem 21]. -
Issue 2006 Volume 4
ISSUE 2006 PROGRESS IN PHYSICS VOLUME 4 ISSN 1555-5534 The Journal on Advanced Studies in Theoretical and Experimental Physics, including Related Themes from Mathematics PROGRESS IN PHYSICS A quarterly issue scientific journal, registered with the Library of Congress (DC, USA). This journal is peer reviewed and includedinthe abstracting and indexing coverage of: Mathematical Reviews and MathSciNet (AMS, USA), DOAJ of Lund University (Sweden), Zentralblatt MATH (Germany), Referativnyi Zhurnal VINITI (Russia), etc. Electronic version of this journal: OCTOBER 2006 VOLUME 4 http://www.ptep-online.com http://www.geocities.com/ptep_online CONTENTS To order printed issues of this journal, con- tact the Editor in Chief. D. Rabounski New Effect of General Relativity: Thomson Dispersion of Light in Stars as a Machine Producing Stellar Energy. .3 Chief Editor A. N. Mina and A. H. Phillips Frequency Resolved Detection over a Large Dmitri Rabounski Frequency Range of the Fluctuations in an Array of Quantum Dots . 11 [email protected] C. Y. Lo Completing Einstein’s Proof of E = mc2 ..........................14 Associate Editors Prof. Florentin Smarandache D. Rabounski A Source of Energy for Any Kind of Star . 19 [email protected] Dr. Larissa Borissova J. Dunning-Davies The Thermodynamics Associated with Santilli’s Hadronic [email protected] Mechanics . 24 Stephen J. Crothers F. Smarandache and V.Christianto A Note on Geometric and Information [email protected] Fusion Interpretation of Bell’s Theorem and Quantum Measurement . 27 Department of Mathematics, University of J. X. Zheng-Johansson and P.-I. Johansson Developing de Broglie Wave . 32 New Mexico, 200 College Road, Gallup, NM 87301, USA The Classical Theory of Fields Revision Project (CTFRP): Collected Papers Treating of Corrections to the Book “The Classical Theory of Fields” by L. -
Witt Kernels and Brauer Kernels for Quartic Extensions in Characteristic
WITT KERNELS AND BRAUER KERNELS FOR QUARTIC EXTENSIONS IN CHARACTERISTIC TWO DETLEV W. HOFFMANN AND MARCO SOBIECH Abstract. Let F be a field of characteristic 2 and let E/F be a field extension of degree 4. We determine the kernel Wq(E/F ) of the restriction map WqF → WqE between the Witt groups of nondegenerate quadratic forms over F and over E, completing earlier partial results by Ahmad, Baeza, Mammone and Moresi. We also deduct the corresponding result for the Witt kernel W (E/F ) of the restriction map WF → WE between the Witt rings of nondegenerate symmetric bilinear forms over F and over E from earlier results by the first author. As application, we describe the 2-torsion part of the Brauer kernel for such extensions. 1. Introduction When considering algebraic objects defined over fields such as quadratic forms or central simple algebras, an important problem is to characterize their behavior under field extensions, for example to determine which quadratic forms become hyperbolic or which central simple algebras split over a given extension, in other words to compute the Witt kernel or the Brauer kernel for that extension. The purpose of the present paper is to determine Witt kernels for quartic extensions in characteristic 2 completing earlier results by various authors, and to apply this to the determination of the 2-torsion part of the Brauer kernel. These kernels have been previously computed in characteristic not 2. Also, in all characteristics the kernels have been known for quite some time in the case of quadratic extensions, and they are trivial for odd degree extensions due to Springer’s theorem, so quartic extensions in characteristic 2 are the first case where the determination of these kernels was still incomplete. -
In Praise of Quaternions
IN PRAISE OF QUATERNIONS JOACHIM LAMBEK With an appendix on the algebra of biquaternions Michael Barr Abstract. This is a survey of some of the applications of quaternions to physics in the 20th century. In the first half century, an elegant presentation of Maxwell's equations and special relativity was achieved with the help of biquaternions, that is, quaternions with complex coefficients. However, a quaternionic derivation of Dirac's celebrated equation of the electron depended on the observation that all 4 × 4 real matrices can be generated by quaternions and their duals. On examine quelques applications des quaternions `ala physique du vingti`emesi`ecle.Le premier moiti´edu si`ecleavait vu une pr´esentation ´el´egantes des equations de Maxwell et de la relativit´e specialle par les quaternions avec des coefficients complexes. Cependant, une d´erivation de l'´equationc´el`ebrede Dirac d´ependait sur l'observation que toutes les matrices 4 × 4 r´eelles peuvent ^etre gener´eespar les representations reguli`eresdes quaternions. 1. Prologue. This is an expository article attempting to acquaint algebraically inclined readers with some basic notions of modern physics, making use of Hamilton's quaternions rather than the more sophisticated spinor calculus. While quaternions play almost no r^olein mainstream physics, they afford a quick entry into the world of special relativity and allow one to formulate the Maxwell-Lorentz theory of electro-magnetism and the Dirac equation of the electron with a minimum of mathematical prerequisites. Marginally, quaternions even give us a glimpse of the Feynman diagrams appearing in the standard model. As everyone knows, quaternions were invented (discovered?) by William Rowan Hamilton. -
Geometric Algebra Techniques
Geometric Algebra Techniques in Mathematics, Physics and Engineering S. Xamb´o UPC IMUVA 16-19 Nov 2015 · · S. Xamb´o (UPC) GAT 04 Space-time GA IMUVA · 16-19 Nov · 2015 1 / 47 Index Main points Background. Lorentz transformations. Introduction. Definitions, notations and conventions. The Dirac representation of . D + Lorentzian GA. = 1;3 = ΛηE. Involutions and . Complex structure. G G G The nature of the even subalgebra. Inner products in and . Relative P D involutions. Space-time kinematics. Space-time paths. Timelike paths and proper time. Instantaneous rest frame. Relative velocity. Lorentz transformations. Lorentz spinors. Rotations. Lorentz boosts. Relativistic addition of velocities. General boosts. Lorentz group. Appendix A. Appendix B. EM field. Maxwell's equations. Gradient operator. Riesz form of Maxwell's equations. GA form of Dirac's equation. References. S. Xamb´o (UPC) GAT 04 Space-time GA IMUVA · 16-19 Nov · 2015 2 / 47 Background Lorentz transformations The Lorentz boost for speed v is given by t0 = γ(t βx); x 0 = γ(x βt) − p − where β = v=c and γ = 1= 1 β2. − This transformation leaves invariant the Lorentz quadratic form (ct)2 x 2 y 2 z 2. − − − S. Xamb´o (UPC) GAT 04 Space-time GA IMUVA · 16-19 Nov · 2015 3 / 47 Background Lorentz transformations Let γx ; γy ; γz ; γt be the unit vectors on the axes of the reference S 0 0 0 0 0 and γx ; γy ; γz ; γt be the unit vectors on the axes of the reference S . Then the above Lorentz boost is equivalent to the linear transformation 0 0 0 0 γt = γ(γt + βγx ); γx = γ(γx + βγt ); γy = γy ; γz = γz ; which is a Lorentz isometry. -
The Descent of Biquaternion Algebras in Characteristic Two
The descent of biquaternion algebras in characteristic two Demba Barrya,b, Adam Chapmanc, Ahmed Laghribid aFacult´edes Sciences et Techniques de Bamako, BP: E3206 Bamako, Mali bDepartement Wiskunde–Informatica, Universiteit Antwerpen, Belgium cDepartment of Computer Science, Tel-Hai College, Upper Galilee, 12208 Israel dUniversit´ed’Artois, Facult´edes Sciences Jean Perrin, Laboratoire de math´ematiquesde Lens EA 2462, rue Jean Souvraz - SP18, 62307 Lens, France Abstract In this paper we associate an invariant to a biquaternion algebra B over a field K with a subfield F such that K=F is a quadratic separable extension and char(F) = 2. We show that this invariant is trivial exactly when B B0 ⊗ K for some biquaternion algebra B0 over F. We also study the behavior of this invariant under certain field extensions and provide several interesting examples. Keywords: Kato-Milne Cohomology, Cohomological invariants, Algebras with involution, Biquaternion algebras 2010 MSC: primary 11E81; secondary 11E04, 16K20, 19D45 1. Introduction Given a central simple algebra C over a field K with a subfield F, we say that C has a descent to F if there exists a central simple algebra C0 over F such that C C0 ⊗ K. When [K : F] = exp(C), one necessary condition for C to have a descent to F is that corK=F(C) ∼Br F, because if C C0⊗K ⊗ ⊗[K:F] ∼ ∼ then corK=F(C) = corK=F(C0 K) = C0 Br F, where Br denotes the Brauer equivalence. If K=F is a separable quadratic extension and Q is a quaternion algebra over K, then corK=F(Q) ∼Br F is a necessary and sufficient condition for Q to have a descent to F by [1, Chapter X, Theorem 21]. -
Scaled Trace Forms of Central Simple Algebras
Scaled trace forms of central simple algebras D. W. Lewis Introduction Any central simple algebra over a field of characteristic not two has a well-defined non-singular quadratic form called the trace form attached to it. This quadratic form was studied in [6] from the viewpoint of the algebraic theory of quadratic forms. In this article we examine a generalization of trace forms to \scaled trace forms" which are defined via the reduced trace map together with scaling by a non-zero element of the algebra. In section 1 of the paper we give our basic definitions and obtain necessary and sufficient conditions for the scaled trace forms to be non-singular. In section 2 we deal with the \split" case, i.e. the case when the algebra is a full matrix algebra over the field. In section 3 we investigate the algebraic invariants of scaled trace forms. We show that the determinant of a scaled trace form is, up to sign, equal to the reduced norm of the scaling element. Also we give formulae for the signature at each ordering when the underlying field is formally real. We cannot calculate the Hasse-Witt invariant in general but we determine it in two special cases only. In sections 4 and 5 we relate scaled trace forms to the transfer homomorphism of quadratic form theory and use them to obtain information about the kernel and image of the extension of scalars homomorphism of Witt rings. We use the terminology and notation of the book of Scharlau [9] and refer the reader to this book for any further background information on quadratic form theory. -
The Four Dimensional Dirac Equation in Five Dimensions
The Four Dimensional Dirac Equation in Five Dimensions Romulus Breban Institut Pasteur, Paris, France Abstract The Dirac equation may be thought as originating from a theory of five-dimensional (5D) space- time. We define a special 5D Clifford algebra and introduce a spin-1/2 constraint equation to describe null propagation in a 5D space-time manifold. We explain how the 5D null formalism breaks down to four dimensions to recover two single-particle theories. Namely, we obtain Dirac’s relativistic quantum mechanics and a formulation of statistical mechanics. Exploring the non-relativistic limit in five and four dimensions, we identify a new spin-electric interaction with possible applications to magnetic resonance spectroscopy (within quantum mechanics) and superconductivity (within statistical mechanics). 1 Introduction The Dirac equation [1, 2] established itself as a fundamental tool in four dimensional (4D) physics. With increasing popularity of 5D physics, many authors generalized it from four to five dimensions [3–12]. A different approach was that of Barut [13] who recognized that the Dirac matrices αj (j, k, ... =1, 2, 3) and β close under commutation to provide a representation of so(1,4), thus establishing an intrinsic 5D symmetry of the Dirac equation. Later, Bracken and Cohen [14] introduced an algebraic formalism, for the Dirac equation, based on so(1,4). In this paper, we present a curved geometry for 5D space-times compatible to the Dirac equation, where the electromagnetic field enters according to the minimal coupling recipe. Furthermore, we reconsider the non-relativistic limit of the Dirac equation using 5D-based approximations.