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2009, arXiv (Cornell University)
In "A note on generalized Clifford algebras and representations" (Caenepeel, S.; Van Oystaeyen, F., Comm. Algebra 17 (1989) no. 1, 93--102.) generalized Clifford algebras were introduced via Clifford representations; these correspond to projective representations of a finite group (Abelian), $G$ say, such that the corresponding twisted group ring has minimal center. The latter then translates to the fact that the corresponding 2-cocycle allows a minimal (none!) number of ray classes and this forces a decomposition of $G$ in cyclic components in a suitable way, cf. Zmud, M., Symplectic geometries and projective representations of finite Abelian groups, (Russian) Mat. Sb. (N.S.) 87(129) (1972), 3--17.. In this small paper, I will provide a way to represent an Abelian Group Clifford Algebra using a matrix, and then give a way to calculate whether or not the center is trivial.
Quart. J. Math. Oxford, 1991
Reports on Mathematical Physics, 1974
It is shown that using the basis elements of the generalized Chfford algebra C." we can construct a group 57 called the generalized Clifford group (G.C.G.) which is a generalization of the Dirac group of the 16 Dirac matrices and their negative counterparts. We have studied the irreducible representations of G.C.G. and we have found the connection with the group of linear transformations leaving invariant the expression 1 (x')" for m22. InI
2008
Since the spinor groups are certain well chosen subgroups of units of Clifford algebras, it is necessary to investigate Clifford algebras to get a firm understanding of spinor groups. These notes provide a tutorial on Clifford algebra and the groups Spin and Pin, including a study of the structure of the Clifford algebra Cl_{p, q} associated with a nondegenerate symmetric bilinear form of signature (p, q) and culminating in the beautiful "8-periodicity theorem" of Elie Cartan and Raoul Bott (with proofs).
Geometry and computing, 2020
The main goal of this chapter is to explain how rotations in R n are induced by the action of a certain group Spin(n) on R n , in a way that generalizes the action of the unit complex numbers U(1) on R 2 , and the action of the unit quaternions SU(2) on R 3 (i.e., the action is defined in terms of multiplication in a larger algebra containing both the group Spin(n) and R n). The group Spin(n), called a spinor group, is defined as a certain subgroup of units of an algebra Cl n , the Clifford algebra associated with R n. Furthermore, for n ≥ 3, we are lucky, because the group Spin(n) is topologically simpler than the group SO(n). Indeed, for n ≥ 3, the group Spin(n) is simply connected (a fact that it is not so easy to prove without some machinery), whereas SO(n) is not simply connected. Intuitively speaking, SO(n) is more twisted than Spin(n). In fact, we will see that Spin(n) is a double cover of SO(n). Since the spinor groups are certain well-chosen subgroups of units of Clifford algebras, it is necessary to investigate Clifford algebras to get a firm understanding of spinor groups. This chapter provides a tutorial on Clifford algebra and the groups Spin and Pin, including a study of the structure of the Clifford algebra Cl p,q associated with a nondegenerate symmetric bilinear form of signature (p, q) and culminating in the beautiful "8-periodicity theorem" of Élie Cartan and Raoul Bott (with proofs). We also explain when Spin(p, q) is a double-cover of SO(p, q). The reader should be warned that a certain amount of algebraic (and topological) background is expected. This being said, perseverant readers will be rewarded by being exposed to some beautiful and nontrivial concepts and results, including Élie Cartan and Raoul Bott "8-periodicity theorem." Going back to rotations as transformations induced by group actions, recall that if V is a vector space, a linear action (on the left) of a group G on V is a map α : G× V → V satisfying the following conditions, where, for simplicity of notation, we denote α(g, v) by g • v:
Advances in Applied Clifford Algebras, 2011
The structure of a complex Clifford algebra is studied by direct sum decompositions into eigenspaces of specific linear operators.
Journal of Algebra, 1989
2004
CLIFFORD performs various computations in Graßmann and Clifford algebras. It can compute with quaternions, octonions, and matrices with entries in C (B) -the Clifford algebra of a vector space V endowed with an arbitrary bilinear form B. Two user-selectable algorithms for the Clifford product are implemented: cmulNUMbased on Chevalley's recursive formula, and cmulRS -based on a non-recursive Rota-Stein sausage. Graßmann and Clifford bases can be used. Properties of reversion in undotted and dotted wedge bases are discussed.
2015
We are concerned with matrices over nondivision algebras and show by an example from an R algebra that these matrices do not necessarily have eigenvalues, even if these matrices are invertible. The standard condition for eigenvectors x = 0 will be replaced by the condition that x contains at least one invertible component which is the same as x = 0 for division algebras. The topic is of principal interest, and leads to the question what qualifies a matrix over a nondivision algebra to have eigenvalues. And connected with this problem is the question, whether these matrices are diagonalizable or triangulizable and allow a Schur decomposition. There is a last section where the question whether a specific matrix A has eigenvalues is extended to all eight R algebras by applying numerical means. As a curiosity we found that the considered matrix A over the algebra of tessarines, which is a commutative algebra, introduced by Cockle (Phil Mag 35(3):434–437, 1849; http:// www.oocities.org/c...
Russian Mathematics
Considering tensor products of special commutative algebras and general real Clifford algebras, we arrive at extended Clifford algebras. We have found that there are five types of extended Clifford algebras. The class of extended Clifford algebras is closed with respect to the tensor product.
2011
The finite Heisenberg group knows when the dimension of Hilbert space is a square number. Remarkably, it then admits a representation such that the entire Clifford group-the automorphism group of the Heisenberg group-is represented by monomial phase-permutation matrices. This has a beneficial influence on the amount of calculation that must be done to find Symmetric Informationally Complete POVMs. I make some comments on the equations obeyed by the absolute values of the components of the SIC vectors, and on the fact that the representation partly suggests a preferred tensor product structure.
2001
One of the main goals of these notes is to explain how rotations in R n are induced by the action of a certain group, Spin(n), on R n , in a way that generalizes the action of the unit complex numbers, U(1), on R 2 , and the action of the unit quaternions, SU(2), on R 3
International Journal of Theoretical Physics, 2001
The history and immediate future of the International Conferences on Clifford Algebras and Their Applications.
2007
Abstract One of the main goals of these notes is to explain how rotations in R n are induced by the action of a certain group, Spin (n), on R n, in a way that generalizes the action of the unit complex numbers, U (1), on R 2, and the action of the unit quaternions, SU (2), on R�� (ie, the action is defined in terms of multiplication in a larger algebra containing both the group Spin (n) and R n). The group Spin (n), called a spinor group, is defined as a certain subgroup of units of an algebra, Cl n, the Clifford algebra associated with R n.
Journal of Algebra, 2000
In this paper a Clifford theory for semisimple G-groups is developed, as a particular case of an abstract Clifford theory for G-functors. ᮊ
2003
Given a finite group G, a set of basis vectors B = {ip|p 2 G} and a 'sign function' or 'twist' α : G × G ! { 1,1}, there is a 'twisted group algebra' defined on the set V of all linear combinations of elements of B over a field F such that if p, q 2 G, then ipiq = α(p, q)ipq. This product is extended to V by distribution. Examples of such twisted group algebras are the Cayley-Dickson algebras and Clifford algebras. It is conjectured that the Hilbert Space l 2 of square summable sequences is a Cayley-Dickson algebra.
The Legacy of Alladi Ramakrishnan in the Mathematical Sciences, 2010
Generalized Clifford algebras (GCAs) and their physical applications were extensively studied for about a decade from 1967 by Alladi Ramakrishnan and his collaborators under the name of L-matrix theory. Some aspects of GCAs and their physical applications are outlined here. The topics dealt with include: GCAs and projective representations of finite abelian groups, Alladi Ramakrishnan's σ-operation approach to the representation theory of Clifford algebra and GCAs, Dirac's positive energy relativistic wave equation, Weyl-Schwinger unitary basis for matrix algebra and Alladi Ramakrishnan's matrix decomposition theorem, finite-dimensional Wigner function, finite-dimensional canonical transformations, magnetic Bloch functions, finite-dimensional quantum mechanics, and the relation between GCAs and quantum groups.
Arxiv preprint arXiv:1107.1375, 2011
Given a finite group G, a set of basis vectors B = {ip|p ∈ G} and a 'sign function' or 'twist' α : G × G → {−1, 1}, there is a 'twisted group algebra' defined on the set V of all linear combinations of elements of B over a field F such that if p, q ∈ G, then ipiq = α(p, q)ipq. This product is extended to V by distribution. Examples of such twisted group algebras are the Cayley-Dickson algebras and Clifford algebras. It is conjectured that the Hilbert Space ℓ 2 of square summable sequences is a Cayley-Dickson algebra.
Linear Algebra and its Applications, 1990
As is well known, Clifford algebras can 'be faithfully realized as certain matrix algebras, the matrix entries betig real numbers, complex numbers, or wternions, nding on the particular Clifford algebra. We show that the matrix representations of the basis elements of a Clifford algebra can be chosen to satisfy a certain additional trace condition; we then use this trace condition to establish optimal ineqz&ties involving norms in Clifford algebras.
Developments in Mathematics
We discuss a certain class of absolutely irreducible group representations that behave nicely under the restriction to normal subgroups and subalgebras.
Journal of Mathematical Physics, 2009
In this paper we address the problem of constructing a class of representations of Clifford algebras that can be named "alphabetic (re)presentations". The Clifford algebras generators are expressed as m-letter words written with a 3-character or a 4-character alphabet. We formulate the problem of the alphabetic presentations, deriving the main properties and some general results. At the end we briefly discuss the motivations of this work and outline some possible applications.