The Frobenius-Schur Indicator and the Finite Rotation Groups
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Lecture 3: Spinor Representations
Spin 2010 (jmf) 19 Lecture 3: Spinor representations Yes now I’ve met me another spinor... — Suzanne Vega (with apologies) It was Élie Cartan, in his study of representations of simple Lie algebras, who came across repres- entations of the orthogonal Lie algebra which were not tensorial; that is, not contained in any tensor product of the fundamental (vector) representation. These are the so-called spinorial representations. His description [Car38] of the spinorial representations was quite complicated (“fantastic” according to Dieudonné’s review of Chevalley’s book below) and it was Brauer and Weyl [BW35] who in 1935 de- scribed these representations in terms of Clifford algebras. This point of view was further explored in Chevalley’s book [Che54] which is close to the modern treatment. This lecture is devoted to the Pin and Spin groups and to a discussion of their (s)pinorial representations. 3.1 The orthogonal group and its Lie algebra Throughout this lecture we will let (V,Q) be a real finite-dimensional quadratic vector space with Q nondegenerate. We will drop explicit mention of Q, whence the Clifford algebra shall be denoted C(V) and similarly for other objects which depend on Q. We will let B denote the bilinear form defining Q. We start by defining the group O(V) of orthogonal transformations of V: (51) O(V) {a :V V Q(av) Q(v) v V} . = → | = ∀ ∈ We write O(Rs,t ) O(s,t) and O(n) for O(n,0). If a O(V), then deta 1. Those a O(V) with deta = ∈ =± ∈ = 1 define the special orthogonal group SO(V). -
Arxiv:2009.14613V5 [Math.GR] 20 Dec 2020
A GROUP-THEORIST’S PERSPECTIVE ON SYMMETRY GROUPS IN PHYSICS ROBERT ARNOTT WILSON Abstract. There are many Lie groups used in physics, including the Lorentz group of special relativity, the spin groups (relativistic and non-relativistic) and the gauge groups of quantum electrodynamics and the weak and strong nuclear forces. Various grand unified theories use larger Lie groups in different attempts to unify some of these groups into something more fundamental. There are also a number of finite symmetry groups that are related to the finite number of distinct elementary particle types. I offer a group-theorist’s perspective on these groups, and suggest some ways in which a deeper use of group theory might in principle be useful. These suggestions include a number of options that seem not to be under active investigation at present. I leave open the question of whether they can be implemented in physical theories. 1. Introduction 1.1. The status quo. The most important Lie group in macroscopic physics is surely the Lorentz group SO(3, 1), that describes the coordinate transformations on spacetime that are necessary to incorporate the experimental fact that the speed of light in a vacuum is independent of the relative velocity of the source and the observer. This group is the cornerstone of the theory of special relativity [1], and modern physics is almost inconceivable without it. The Lorentz group is also used as a foundation for the theory of general relativity [2, 3, 4], but it is also possible to use the larger group SL(4, R), that is the special linear group of degree 4, consisting of all 4 4 real matrices with determinant 1. -
Spinor Algebras
CERN-TH/2000-260 SPINOR ALGEBRAS R. D’Auria†, S. Ferrara•, M. A. Lled´o† and V. S. Varadarajan?. † Dipartimento di Fisica, Politecnico di Torino, Corso Duca degli Abruzzi 24, I-10129 Torino, Italy, and INFN, Sezione di Torino, Italy. • CERN, Theory Division, CH 1211 Geneva 23, Switzerland, and Laboratori Nazionali di Frascati, INFN, Italy. ? Department of Mathematics, University of California, Los Angeles, Los Angeles, CA 90095-1555, USA. Abstract We consider supersymmetry algebras in space-times with arbitrary signature and minimal number of spinor generators. The interrelation between super Poincar´eand super conformal algebras is elucidated. Minimal super conformal algebras are seen to have as bosonic part a classical semimisimple algebra naturally associated to the spin group. This algebra, the Spin(s,t)-algebra, depends both on the dimension and on the signature of space time. We also consider maximal su- per conformal algebras, which are classified by the orthosymplectic algebras. 1 1 Introduction In recent times the extension of Poincar´eand conformal superalgebras to orthosymplectic algebras has been considered with a variety of purposes. In particular the role of osp(1 32, R) and osp(1 64, R) as minimal superalgebras containing the conformal algebras| in 10 and| 11 dimensions (or the anti de Sitter algebra in 11 and 12 dimensions) has been considered in view of possi- ble generalizations of M theory [1, 2, 3, 7, 8, 17, 18, 16, 20, 21] and of string theory to F-theory [9]. The contractions of orthosymplectic algebras are used in the study of BPS branes [35, 7, 19, 34, 12].