Remarks on Classical Invariant Theory 549
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http://dx.doi.org/10.1090/gsm/039 Selected Titles in This Series 39 Larry C. Grove, Classical groups and geometric algebra, 2002 38 Elton P. Hsu, Stochastic analysis on manifolds, 2001 37 Hershel M. Farkas and Irwin Kra, Theta constants, Riemann surfaces and the modular group, 2001 36 Martin Schechter, Principles of functional analysis, second edition, 2001 35 James F. Davis and Paul Kirk, Lecture notes in algebraic topology, 2001 34 Sigurdur Helgason, Differential geometry, Lie groups, and symmetric spaces, 2001 33 Dmitri Burago, Yuri Burago, and Sergei Ivanov, A course in metric geometry, 2001 32 Robert G. Bartle, A modern theory of integration, 2001 31 Ralf Korn and Elke Korn, Option pricing and portfolio optimization: Modern methods of financial mathematics, 2001 30 J. C. McConnell and J. C. Robson, Noncommutative Noetherian rings, 2001 29 Javier Duoandikoetxea, Fourier analysis, 2001 28 Liviu I. Nicolaescu, Notes on Seiberg-Witten theory, 2000 27 Thierry Aubin, A course in differential geometry, 2001 26 Rolf Berndt, An introduction to symplectic geometry, 2001 25 Thomas Friedrich, Dirac operators in Riemannian geometry, 2000 24 Helmut Koch, Number theory: Algebraic numbers and functions, 2000 23 Alberto Candel and Lawrence Conlon, Foliations I, 2000 22 Giinter R. Krause and Thomas H. Lenagan, Growth of algebras and Gelfand-Kirillov dimension, 2000 21 John B. Conway, A course in operator theory, 2000 20 Robert E. Gompf and Andras I. Stipsicz, 4-manifolds and Kirby calculus, 1999 19 Lawrence C. Evans, Partial differential equations, 1998 18 Winfried Just and Martin Weese, Discovering modern set theory. II: Set-theoretic tools for every mathematician, 1997 17 Henryk Iwaniec, Topics in classical automorphic forms, 1997 16 Richard V. -
[Math.GR] 9 Jul 2003 Buildings and Classical Groups
Buildings and Classical Groups Linus Kramer∗ Mathematisches Institut, Universit¨at W¨urzburg Am Hubland, D–97074 W¨urzburg, Germany email: [email protected] In these notes we describe the classical groups, that is, the linear groups and the orthogonal, symplectic, and unitary groups, acting on finite dimen- sional vector spaces over skew fields, as well as their pseudo-quadratic gen- eralizations. Each such group corresponds in a natural way to a point-line geometry, and to a spherical building. The geometries in question are pro- jective spaces and polar spaces. We emphasize in particular the rˆole played by root elations and the groups generated by these elations. The root ela- tions reflect — via their commutator relations — algebraic properties of the underlying vector space. We also discuss some related algebraic topics: the classical groups as per- mutation groups and the associated simple groups. I have included some remarks on K-theory, which might be interesting for applications. The first K-group measures the difference between the classical group and its subgroup generated by the root elations. The second K-group is a kind of fundamental group of the group generated by the root elations and is related to central extensions. I also included some material on Moufang sets, since this is an in- arXiv:math/0307117v1 [math.GR] 9 Jul 2003 teresting topic. In this context, the projective line over a skew field is treated in some detail, and possibly with some new results. The theory of unitary groups is developed along the lines of Hahn & O’Meara [15]. -
Hartley's Theorem on Representations of the General Linear Groups And
Turk J Math 31 (2007) , Suppl, 211 – 225. c TUB¨ ITAK˙ Hartley’s Theorem on Representations of the General Linear Groups and Classical Groups A. E. Zalesski To the memory of Brian Hartley Abstract We suggest a new proof of Hartley’s theorem on representations of the general linear groups GLn(K)whereK is a field. Let H be a subgroup of GLn(K)andE the natural GLn(K)-module. Suppose that the restriction E|H of E to H contains aregularKH-module. The theorem asserts that this is then true for an arbitrary GLn(K)-module M provided dim M>1andH is not of exponent 2. Our proof is based on the general facts of representation theory of algebraic groups. In addition, we provide partial generalizations of Hartley’s theorem to other classical groups. Key Words: subgroups of classical groups, representation theory of algebraic groups 1. Introduction In 1986 Brian Hartley [4] obtained the following interesting result: Theorem 1.1 Let K be a field, E the standard GLn(K)-module, and let M be an irre- ducible finite-dimensional GLn(K)-module over K with dim M>1. For a finite subgroup H ⊂ GLn(K) suppose that the restriction of E to H contains a regular submodule, that ∼ is, E = KH ⊕ E1 where E1 is a KH-module. Then M contains a free KH-submodule, unless H is an elementary abelian 2-groups. His proof is based on deep properties of the duality between irreducible representations of the general linear group GLn(K)and the symmetric group Sn. -
Symmetry Breaking Operators for Dual Pairs with One Member Compact M Mckee, Angela Pasquale, T Przebinda
Symmetry breaking operators for dual pairs with one member compact M Mckee, Angela Pasquale, T Przebinda To cite this version: M Mckee, Angela Pasquale, T Przebinda. Symmetry breaking operators for dual pairs with one member compact. 2021. hal-03293407 HAL Id: hal-03293407 https://hal.archives-ouvertes.fr/hal-03293407 Preprint submitted on 21 Jul 2021 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. SYMMETRY BREAKING OPERATORS FOR DUAL PAIRS WITH ONE MEMBER COMPACT M. MCKEE, A. PASQUALE, AND T. PRZEBINDA Abstract. We consider a dual pair (G; G0), in the sense of Howe, with G compact acting on L2(Rn), for an appropriate n, via the Weil representation !. Let Ge be the preimage of G in the metaplectic group. Given a genuine irreducible unitary representation Π of G,e let Π0 be the corresponding irreducible unitary representation of Ge 0 in the Howe duality. 2 n The orthogonal projection onto L (R )Π, the Π-isotypic component, is the essentially 1 1 1 unique symmetry breaking operator in Hom (H ; H ⊗H 0 ). We study this operator GeGf0 ! Π Π by computing its Weyl symbol. -
Spacetime May Have Fractal Properties on a Quantum Scale 25 March 2009, by Lisa Zyga
Spacetime May Have Fractal Properties on a Quantum Scale 25 March 2009, By Lisa Zyga values at short scales. More than being just an interesting idea, this phenomenon might provide insight into a quantum theory of relativity, which also has been suggested to have scale-dependent dimensions. Benedetti’s study is published in a recent issue of Physical Review Letters. “It is an old idea in quantum gravity that at short scales spacetime might appear foamy, fuzzy, fractal or similar,” Benedetti told PhysOrg.com. “In my work, I suggest that quantum groups are a valid candidate for the description of such a quantum As scale decreases, the number of dimensions of k- spacetime. Furthermore, computing the spectral Minkowski spacetime (red line), which is an example of a dimension, I provide for the first time a link between space with quantum group symmetry, decreases from four to three. In contrast, classical Minkowski spacetime quantum groups/noncommutative geometries and (blue line) is four-dimensional on all scales. This finding apparently unrelated approaches to quantum suggests that quantum groups are a valid candidate for gravity, such as Causal Dynamical Triangulations the description of a quantum spacetime, and may have and Exact Renormalization Group. And establishing connections with a theory of quantum gravity. Image links between different topics is often one of the credit: Dario Benedetti. best ways we have to understand such topics.” In his study, Benedetti explains that a spacetime with quantum group symmetry has in general a (PhysOrg.com) -- Usually, we think of spacetime scale-dependent dimension. Unlike classical as being four-dimensional, with three dimensions groups, which act on commutative spaces, of space and one dimension of time. -
Dual Pairs in the Pin-Group and Duality for the Corresponding Spinorial
DUAL PAIRS IN THE PIN-GROUP AND DUALITY FOR THE CORRESPONDING SPINORIAL REPRESENTATION CLÉMENT GUÉRIN, GANG LIU, AND ALLAN MERINO Abstract. In this paper, we give a complete picture of Howe correspondence for the setting (O(E, b), Pin(E, b), Π), where O(E, b) is an orthogonal group (real or complex), Pin(E, b) is the two-fold Pin-covering of O(E, b), and Π is the spinorial representation of Pin(E, b). More pre- cisely, for a dual pair (G, G′) in O(E, b), we determine explicitly the nature of its preimages (G, G′) in Pin(E, b), and prove that apart from some exceptions, (G, G′) is always a dual pair in e f e f Pin(E, b); then we establish the Howe correspondence for Π with respect to (G, G′). e f Contents 1. Introduction 1 2. Preliminaries 3 3. Dual pairs in the Pin-group 6 3.1. Pull-back of dual pairs 6 3.2. Identifyingtheisomorphismclassofpull-backs 8 4. Duality for the spinorial representation 14 References 21 1. Introduction The first duality phenomenon has been discovered by H. Weyl who pointed out a correspon- dence between some irreducible finite dimensional representations of the general linear group GL(V) and the symmetric group Sk where V is a finite dimensional vector space over C. In- d deed, considering the joint action of GL(V) and Sd on the space V⊗ , we get the following decomposition: arXiv:1907.09093v1 [math.RT] 22 Jul 2019 d λ V⊗ = M λ σ , [ ⊗ (Vλ,λ) GL(V) ∈ π [ where GL(V)π is the set of equivalence classes of irreducible finite dimensional representations d of GL(V) such that Hom (V , V⊗ ) , 0 and σ is an irreducible representation of S . -
Special Unitary Group - Wikipedia
Special unitary group - Wikipedia https://en.wikipedia.org/wiki/Special_unitary_group Special unitary group In mathematics, the special unitary group of degree n, denoted SU( n), is the Lie group of n×n unitary matrices with determinant 1. (More general unitary matrices may have complex determinants with absolute value 1, rather than real 1 in the special case.) The group operation is matrix multiplication. The special unitary group is a subgroup of the unitary group U( n), consisting of all n×n unitary matrices. As a compact classical group, U( n) is the group that preserves the standard inner product on Cn.[nb 1] It is itself a subgroup of the general linear group, SU( n) ⊂ U( n) ⊂ GL( n, C). The SU( n) groups find wide application in the Standard Model of particle physics, especially SU(2) in the electroweak interaction and SU(3) in quantum chromodynamics.[1] The simplest case, SU(1) , is the trivial group, having only a single element. The group SU(2) is isomorphic to the group of quaternions of norm 1, and is thus diffeomorphic to the 3-sphere. Since unit quaternions can be used to represent rotations in 3-dimensional space (up to sign), there is a surjective homomorphism from SU(2) to the rotation group SO(3) whose kernel is {+ I, − I}. [nb 2] SU(2) is also identical to one of the symmetry groups of spinors, Spin(3), that enables a spinor presentation of rotations. Contents Properties Lie algebra Fundamental representation Adjoint representation The group SU(2) Diffeomorphism with S 3 Isomorphism with unit quaternions Lie Algebra The group SU(3) Topology Representation theory Lie algebra Lie algebra structure Generalized special unitary group Example Important subgroups See also 1 of 10 2/22/2018, 8:54 PM Special unitary group - Wikipedia https://en.wikipedia.org/wiki/Special_unitary_group Remarks Notes References Properties The special unitary group SU( n) is a real Lie group (though not a complex Lie group). -
Sylow P -Subgroups of the Classical Groups Over Finite Fields with Characteristic Prime to P
SYLOW /--SUBGROUPS OF THE CLASSICAL GROUPS OVER FINITE FIELDS WITH CHARACTERISTIC PRIME TO p A. J. WEIR If Sn is a Sylow /--subgroup of the symmetric group of degree pn, then any group of order pn may be imbedded in 5„. We may express Sn as the complete product1 C o C o • • • o C of « cyclic groups of order p and the purpose of this paper is to show that any Sylow p- subgroup of a classical group (see §1) over the finite field GF(q) with q elements, where (q, p) = 1, is expressible as a direct product of basic subgroups 5„= C o C o • • • o C (n factors), where C is cyclic of order pT. (We assume always that p7£2.) Since C may be imbedded in ST, we see that Sn is imbedded in Sn+r-i in a particularly simple way. The above r is defined by the equation q*— \ =pT * where g* is the first power of q which is congruent to 1 mod p and * denotes some unspecified number prime to p. The case r = 1 is therefore of frequent occurrence, and then clearly Sn=Sn. Professor Philip Hall was my research supervisor in Cambridge (England) during the years 1949-1952 and it is a pleasure to acknowl- edge here my indebtedness to him for his generous encouragement. 1. We shall refer to the following groups as the Classical Groups:* I. The general linear group GL(n, q) is the group of all nonsingular (nXn) matrices with coefficients in GF(q). The order of GL(n, q) is qn(n-l)l2fq _ 1)(?2 _ J) . -
Two Topics on Local Theta Correspondence Ma Jia
TWO TOPICS ON LOCAL THETA CORRESPONDENCE MA JIA JUN (B.Sc., Soochow University) A THESIS SUBMITTED FOR THE DEGREE OF DOCTOR OF PHILOSOPHY DEPARTMENT OF MATHEMATICS NATIONAL UNIVERSITY OF SINGAPORE 2012 Declaration I hereby declare that this thesis is my original work and it has been written by me in its entirety. I have duly acknowledged all the sources of information which have been used in the thesis. This thesis has also not been submitted for any degree in any university previously. Ma Jia Jun 20 February 2013 ACKNOWLEDGEMENTS I would like to take this opportunity to acknowledge and thank those who made this work possible. I would like to express my deep gratitude to Prof. Chengbo Zhu, my supervisor for his supervision and constant support. Prof. Zhu leads me to this exciting research area, proposes interesting questions and always provides illuminating suggestions to me during my study. I am sincerely grateful to Prof. Hung Yean Loke, who have spent enor- mous of time in patient discussion with me and given me lots of inspiring advices. In the collaboration with Prof. Loke, I learnt many mathematics from him. I am profoundly indebted to Prof. Soo Teck Lee, who launched instructive seminars which deeply influenced this work. I express my sincere thanks to Prof. CheeWhye Chin and Prof. De-Qi Zhang, who patiently explained lots of concepts in algebraic geometry to me. I also would like to thank Prof. Michel Brion, Prof. Wee Teck Gan, Prof. Roger Howe, Prof. Jingsong Huang, Prof. Kyo Nishiyama, Prof. Gordan Savin and Prof. Binyong Sun, for their stimulating conversations and suggestions. -
The Theta Correspondence Over R
The Theta Correspondence over R Jeffrey Adams May 3, 2007 1 Introduction These notes were written for the workshop on the Theta correspondence held at the University of Maryland, May 1994. They have circulated informally for many years. Except for minor changes and some improvements to the references they have not been changed. There have been too many develop- ments in the field since 1994 to try to bring them up to date. This is dedicated to Roger Howe, who introduced me to representation theory in graduate school in 1977. 2 Fock model: complex Lie algebra The Fock model is the algebraic oscillator representation: it is the (g; K) module of the oscillator representation of Sp(2n; R). The basic references e are [6],[7], and [47]. See also [11],[17] and [18]. The presentation here is due f to Steve Kudla (unpublished); a similar treatment is found in [49], as well as [51]. In this section we define the oscillator representation of the complex Heisenberg and symplectic Lie algebras. Let be a non{trivial linear form on C, i.e. fix λ 2 C× and let (z) = λz (z 2 C). Definition 2.1 Let W be a vector space with a symplectic form h; i, possibly degenerate. Let Ω(W ) = T (W )=I 1 where T is the tensor algebra of W and I is the two{sided ideal generated by elements of the form v ⊗ w − w ⊗ v − hv; wi (v; w 2 W ): This is an associative algebra, sometimes referred to as the quantum algebra. For example if hv; wi = 0 for all v; w, then Ω(W ) is isomorphic to the polynomial algebra on W . -
Representations and Invariants of the Classical Groups, by Roe Goodman and Nolan R
BULLETIN (New Series) OF THE AMERICAN MATHEMATICAL SOCIETY Volume 36, Number 4, Pages 533{538 S 0273-0979(99)00795-8 Article electronically published on July 28, 1999 Representations and invariants of the classical groups, by Roe Goodman and Nolan R. Wallach, Cambridge Univ. Press, Cambridge, 1998, xvi + 685 pp., $100.00, ISBN 0-521-58273-3, paperback, $39.95, ISBN 0-521-66348-2 This 685-page text by Goodman and Wallach constitutes a carefully organized exposition, not indeed of the entire finite-dimensional representation-theory over R or C of the classical groups (which would be hard to imagine in a single text three times the size of this one), but rather of a selection of some key topics therein. This selection of topics, especially as concerns invariant-theory, seems (as Goodman and Wallach indicate in the preface to their text) to have been in many ways inspired by the contents of H. Weyl’s The Classical Groups, Their Invariants and Representations [31]. Approximately half of the text under review is purely introductory; the remaining half then utilizes this introductory material to develop the main themes. The introductory material, covered in a total of approximately 280 pages in the first three chapters and in four appendices, introduces the reader to some necessary topics in elementary algebraic and differential geometry and to such basic concepts of representation theory as: linear algebraic groups and Lie groups, Lie algebras associated to such, Jordan decomposition, maximal tori, roots and weights, real forms of classical groups, the PBW theorem, invariant integration over compact Lie groups, etc. -
Representation Models for Classical Groups and Their Higher Symmetries Astérisque, Tome S131 (1985), P
Astérisque I. M. GELFAND A. V. ZELEVINSKY Representation models for classical groups and their higher symmetries Astérisque, tome S131 (1985), p. 117-128 <http://www.numdam.org/item?id=AST_1985__S131__117_0> © Société mathématique de France, 1985, tous droits réservés. L’accès aux archives de la collection « Astérisque » (http://smf4.emath.fr/ Publications/Asterisque/) implique l’accord avec les conditions générales d’uti- lisation (http://www.numdam.org/conditions). Toute utilisation commerciale ou impression systématique est constitutive d’une infraction pénale. Toute copie ou impression de ce fichier doit contenir la présente mention de copyright. Article numérisé dans le cadre du programme Numérisation de documents anciens mathématiques http://www.numdam.org/ Société Mathématique de France Astérisque, hors série, 1985, p. 117-128 REPRESENTATION MODELS FOR CLASSICAL GROUPS AND THEIR HIGHER SYMMETRIES BY I.M. GELFAND and A.V. ZELEVINSKY The main results presented in this talk are published with complete proofs in [1]. We give also some new results obtained by the authors jointly with V.V. SERGANOVA. The conversations with V.V. SERGANOVA enable us also to clarify the formulations of [1] related to supermanifolds. We are very grateful to her. Let G be a reductive algebraic group over C. A representation of G which decomposes into the direct sum of all its (finite dimensional) irreducible al gebraic representations each occurring exactly once is called a representation model for G. The H. WeyPs unitary trick shows that the construction of such a model is equivalent to the construction of a representation model for the compact form of G ; the language of complex groups is more convenient for us here.