Algebraic Groups and Discontinuous Subgroups
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Arxiv:1006.1489V2 [Math.GT] 8 Aug 2010 Ril.Ias Rfie Rmraigtesre Rils[14 Articles Survey the Reading from Profited Also I Article
Pure and Applied Mathematics Quarterly Volume 8, Number 1 (Special Issue: In honor of F. Thomas Farrell and Lowell E. Jones, Part 1 of 2 ) 1—14, 2012 The Work of Tom Farrell and Lowell Jones in Topology and Geometry James F. Davis∗ Tom Farrell and Lowell Jones caused a paradigm shift in high-dimensional topology, away from the view that high-dimensional topology was, at its core, an algebraic subject, to the current view that geometry, dynamics, and analysis, as well as algebra, are key for classifying manifolds whose fundamental group is infinite. Their collaboration produced about fifty papers over a twenty-five year period. In this tribute for the special issue of Pure and Applied Mathematics Quarterly in their honor, I will survey some of the impact of their joint work and mention briefly their individual contributions – they have written about one hundred non-joint papers. 1 Setting the stage arXiv:1006.1489v2 [math.GT] 8 Aug 2010 In order to indicate the Farrell–Jones shift, it is necessary to describe the situation before the onset of their collaboration. This is intimidating – during the period of twenty-five years starting in the early fifties, manifold theory was perhaps the most active and dynamic area of mathematics. Any narrative will have omissions and be non-linear. Manifold theory deals with the classification of ∗I thank Shmuel Weinberger and Tom Farrell for their helpful comments on a draft of this article. I also profited from reading the survey articles [14] and [4]. 2 James F. Davis manifolds. There is an existence question – when is there a closed manifold within a particular homotopy type, and a uniqueness question, what is the classification of manifolds within a homotopy type? The fifties were the foundational decade of manifold theory. -
Stable Real Cohomology of Arithmetic Groups
ANNALES SCIENTIFIQUES DE L’É.N.S. ARMAND BOREL Stable real cohomology of arithmetic groups Annales scientifiques de l’É.N.S. 4e série, tome 7, no 2 (1974), p. 235-272 <http://www.numdam.org/item?id=ASENS_1974_4_7_2_235_0> © Gauthier-Villars (Éditions scientifiques et médicales Elsevier), 1974, tous droits réservés. L’accès aux archives de la revue « Annales scientifiques de l’É.N.S. » (http://www. elsevier.com/locate/ansens) implique l’accord avec les conditions générales d’utilisation (http://www.numdam.org/conditions). Toute utilisation commerciale ou impression systé- matique est constitutive d’une infraction pénale. Toute copie ou impression de ce fi- chier doit contenir la présente mention de copyright. Article numérisé dans le cadre du programme Numérisation de documents anciens mathématiques http://www.numdam.org/ Ann. sclent. EC. Norm. Sup., 46 serie, t. 7, 1974, p. 235 a 272. STABLE REAL COHOMOLOGY OF ARITHMETIC GROUPS BY ARMAND BOREL A Henri Cartan, a Poccasion de son 70® anniversaire Let r be an arithmetic subgroup of a semi-simple group G defined over the field of rational numbers Q. The real cohomology H* (T) of F may be identified with the coho- mology of the complex Q^ of r-invariant smooth differential forms on the symmetric space X of maximal compact subgroups of the group G (R) of real points of G. Let 1^ be the space of differential forms on X which are invariant under the identity component G (R)° of G (R). It is well-known to consist of closed (in fact harmonic) forms, whence a natural homomorphism^* : 1^ —> H* (T). -
Algebraic D-Modules and Representation Theory Of
Contemporary Mathematics Volume 154, 1993 Algebraic -modules and Representation TheoryDof Semisimple Lie Groups Dragan Miliˇci´c Abstract. This expository paper represents an introduction to some aspects of the current research in representation theory of semisimple Lie groups. In particular, we discuss the theory of “localization” of modules over the envelop- ing algebra of a semisimple Lie algebra due to Alexander Beilinson and Joseph Bernstein [1], [2], and the work of Henryk Hecht, Wilfried Schmid, Joseph A. Wolf and the author on the localization of Harish-Chandra modules [7], [8], [13], [17], [18]. These results can be viewed as a vast generalization of the classical theorem of Armand Borel and Andr´e Weil on geometric realiza- tion of irreducible finite-dimensional representations of compact semisimple Lie groups [3]. 1. Introduction Let G0 be a connected semisimple Lie group with finite center. Fix a maximal compact subgroup K0 of G0. Let g be the complexified Lie algebra of G0 and k its subalgebra which is the complexified Lie algebra of K0. Denote by σ the corresponding Cartan involution, i.e., σ is the involution of g such that k is the set of its fixed points. Let K be the complexification of K0. The group K has a natural structure of a complex reductive algebraic group. Let π be an admissible representation of G0 of finite length. Then, the submod- ule V of all K0-finite vectors in this representation is a finitely generated module over the enveloping algebra (g) of g, and also a direct sum of finite-dimensional U irreducible representations of K0. -
Construction of Free Subgroups in the Group of Units of Modular Group Algebras
CONSTRUCTION OF FREE SUBGROUPS IN THE GROUP OF UNITS OF MODULAR GROUP ALGEBRAS Jairo Z. Gon¸calves1 Donald S. Passman2 Department of Mathematics Department of Mathematics University of S~ao Paulo University of Wisconsin-Madison 66.281-Ag Cidade de S. Paulo Van Vleck Hall 05389-970 S. Paulo 480 Lincoln Drive S~ao Paulo, Brazil Madison, WI 53706, U.S.A [email protected] [email protected] Abstract. Let KG be the group algebra of a p0-group G over a field K of characteristic p > 0; and let U(KG) be its group of units. If KG contains a nontrivial bicyclic unit and if K is not algebraic over its prime field, then we prove that the free product Zp ∗ Zp ∗ Zp can be embedded in U(KG): 1. Introduction Let KG be the group algebra of the group G over the field K; and let U(KG) be its group of units. Motivated by the work of Pickel and Hartley [4], and Sehgal ([7, pg. 200]) on the existence of free subgroups in the inte- gral group ring ZG; analogous conditions for U(KG) have been intensively investigated in [1], [2] and [3]. Recently Marciniak and Sehgal [5] gave a constructive method for produc- ing free subgroups in U(ZG); provided ZG contains a nontrivial bicyclic unit. In this paper we prove an analogous result for the modular group algebra KG; whenever K is not algebraic over its prime field GF (p): Specifically, if Zp denotes the cyclic group of order p, then we prove: 1- Research partially supported by CNPq - Brazil. -
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). -
Chapter 1 GENERAL STRUCTURE and PROPERTIES
Chapter 1 GENERAL STRUCTURE AND PROPERTIES 1.1 Introduction In this Chapter we would like to introduce the main de¯nitions and describe the main properties of groups, providing examples to illustrate them. The detailed discussion of representations is however demanded to later Chapters, and so is the treatment of Lie groups based on their relation with Lie algebras. We would also like to introduce several explicit groups, or classes of groups, which are often encountered in Physics (and not only). On the one hand, these \applications" should motivate the more abstract study of the general properties of groups; on the other hand, the knowledge of the more important and common explicit instances of groups is essential for developing an e®ective understanding of the subject beyond the purely formal level. 1.2 Some basic de¯nitions In this Section we give some essential de¯nitions, illustrating them with simple examples. 1.2.1 De¯nition of a group A group G is a set equipped with a binary operation , the group product, such that1 ¢ (i) the group product is associative, namely a; b; c G ; a (b c) = (a b) c ; (1.2.1) 8 2 ¢ ¢ ¢ ¢ (ii) there is in G an identity element e: e G such that a e = e a = a a G ; (1.2.2) 9 2 ¢ ¢ 8 2 (iii) each element a admits an inverse, which is usually denoted as a¡1: a G a¡1 G such that a a¡1 = a¡1 a = e : (1.2.3) 8 2 9 2 ¢ ¢ 1 Notice that the axioms (ii) and (iii) above are in fact redundant. -
Issue 118 ISSN 1027-488X
NEWSLETTER OF THE EUROPEAN MATHEMATICAL SOCIETY S E European M M Mathematical E S Society December 2020 Issue 118 ISSN 1027-488X Obituary Sir Vaughan Jones Interviews Hillel Furstenberg Gregory Margulis Discussion Women in Editorial Boards Books published by the Individual members of the EMS, member S societies or societies with a reciprocity agree- E European ment (such as the American, Australian and M M Mathematical Canadian Mathematical Societies) are entitled to a discount of 20% on any book purchases, if E S Society ordered directly at the EMS Publishing House. Recent books in the EMS Monographs in Mathematics series Massimiliano Berti (SISSA, Trieste, Italy) and Philippe Bolle (Avignon Université, France) Quasi-Periodic Solutions of Nonlinear Wave Equations on the d-Dimensional Torus 978-3-03719-211-5. 2020. 374 pages. Hardcover. 16.5 x 23.5 cm. 69.00 Euro Many partial differential equations (PDEs) arising in physics, such as the nonlinear wave equation and the Schrödinger equation, can be viewed as infinite-dimensional Hamiltonian systems. In the last thirty years, several existence results of time quasi-periodic solutions have been proved adopting a “dynamical systems” point of view. Most of them deal with equations in one space dimension, whereas for multidimensional PDEs a satisfactory picture is still under construction. An updated introduction to the now rich subject of KAM theory for PDEs is provided in the first part of this research monograph. We then focus on the nonlinear wave equation, endowed with periodic boundary conditions. The main result of the monograph proves the bifurcation of small amplitude finite-dimensional invariant tori for this equation, in any space dimension. -
Armand Borel (1923–2003), Volume 51, Number 5
Armand Borel (1923–2003) James Arthur, Enrico Bombieri, Komaravolu Chandrasekharan, Friedrich Hirzebruch, Gopal Prasad, Jean-Pierre Serre, Tonny A. Springer, and Jacques Tits Citations within this article. Borel’s Collected Papers are [Œ], and his 17 books are referred to as [1] through [17]. These are all listed in a sidebar on page 501. An item like [Œ 23] is Borel paper number 23 in [Œ]. Ci- tations of work by people other than Borel are by letter combinations such as [Che], and the de- tails appear at the end of the article. their root systems. He spent the year 1949–50 in 1 Institute for Advanced Study, 1999. Paris, with a grant from the CNRS . A good choice Armand Borel (for us, as well as for him), Paris being the very spot where what Americans have called “French Topol- Jean-Pierre Serre ogy” was being created, with the courses from The Swiss mathematician Armand Borel died Leray at the Collège de France and the Cartan sem- August 11, 2003, in Princeton from a rapidly evolv- inar at the École Normale Supérieure. Borel was an ing cancer. Few foreign mathematicians had as active participant in the Cartan seminar while many connections with France. He was a student closely following Leray’s courses. He managed to of Leray, he took part in the Cartan seminar, and understand the famous “spectral sequence”, not an he published more than twenty papers in collabo- easy task, and he explained it to me so well that I ration with our colleagues Lichnerowicz and Tits, have not stopped using it since. -
Lie Groups and Linear Algebraic Groups I. Complex and Real Groups Armand Borel
Lie Groups and Linear Algebraic Groups I. Complex and Real Groups Armand Borel 1. Root systems x 1.1. Let V be a finite dimensional vector space over Q. A finite subset of V is a root system if it satisfies: RS 1. Φ is finite, consists of non-zero elements and spans V . RS 2. Given a Φ, there exists an automorphism ra of V preserving Φ 2 ra such that ra(a) = a and its fixed point set V has codimension 1. [Such a − transformation is unique, of order 2.] The Weyl group W (Φ) or W of Φ is the subgroup of GL(V ) generated by the ra (a Φ). It is finite. Fix a positive definite scalar product ( , ) on V invariant 2 under W . Then ra is the reflection to the hyperplane a. ? 1 RS 3. Given u; v V , let nu;v = 2(u; v) (v; v)− . We have na;b Z for all 2 · 2 a; b Φ. 2 1.2. Some properties. (a) If a and c a (c > 0) belong to Φ, then c = 1; 2. · The system Φ is reduced if only c = 1 occurs. (b) The reflection to the hyperplane a = 0 (for any a = 0) is given by 6 (1) ra(v) = v nv;aa − therefore if a; b Φ are linearly independent, and (a; b) > 0 (resp. (a; b) < 0), 2 then a b (resp. a + b) is a root. On the other hand, if (a; b) = 0, then either − a + b and a b are roots, or none of them is (in which case a and b are said to be − strongly orthogonal). -
MODULAR GROUP IMAGES ARISING from DRINFELD DOUBLES of DIHEDRAL GROUPS Deepak Naidu 1. Introduction the Modular Group SL(2, Z) Is
International Electronic Journal of Algebra Volume 28 (2020) 156-174 DOI: 10.24330/ieja.768210 MODULAR GROUP IMAGES ARISING FROM DRINFELD DOUBLES OF DIHEDRAL GROUPS Deepak Naidu Received: 28 October 2019; Revised: 30 May 2020; Accepted: 31 May 2020 Communicated by A. C¸i˘gdem Ozcan¨ Abstract. We show that the image of the representation of the modular group SL(2; Z) arising from the representation category Rep(D(G)) of the Drinfeld double D(G) is isomorphic to the group PSL(2; Z=nZ) × S3, when G is either the dihedral group of order 2n or the dihedral group of order 4n for some odd integer n ≥ 3. Mathematics Subject Classification (2020): 18M20 Keywords: Drinfeld double, modular tensor category, modular group, con- gruence subgroup 1. Introduction The modular group SL(2; Z) is the group of all 2 × 2 matrices of determinant 1 whose entries belong to the ring Z of integers. The modular group is known to play a significant role in conformal field theory [3]. Every two-dimensional rational con- formal field theory gives rise to a finite-dimensional representation of the modular group, and the kernel of this representation has been of much interest. In particu- lar, the question whether the kernel is a congruence subgroup of SL(2; Z) has been investigated by several authors. For example, A. Coste and T. Gannon in their paper [4] showed that under certain assumptions the kernel is indeed a congruence subgroup. In the present paper, we consider the kernel of the representation of the modular group arising from Drinfeld doubles of dihedral groups. -
The Modular Group Action on Real SL(2)–Characters of a One-Holed Torus
ISSN 1364-0380 (on line) 1465-3060 (printed) 443 Geometry & Topology G T T G G T T Volume 7 (2003) 443–486 G T G T T G T Published: 18 July 2003 G T G T G Republished with corrections: 21 August 2003 T G T G G T G G G T T The modular group action on real SL(2)–characters of a one-holed torus William M Goldman Mathematics Department, University of Maryland College Park, MD 20742 USA Email: [email protected] Abstract The group Γ of automorphisms of the polynomial κ(x,y,z)= x2 + y2 + z2 − xyz − 2 is isomorphic to PGL(2, Z) ⋉ (Z/2 ⊕ Z/2). For t ∈ R, the Γ-action on κ−1(t) ∩ R3 displays rich and varied dynamics. The action of Γ preserves a Poisson structure defining a Γ–invariant area form on each κ−1(t) ∩ R3 . For t < 2, the action of Γ is properly discontinuous on the four con- tractible components of κ−1(t) ∩ R3 and ergodic on the compact component (which is empty if t < −2). The contractible components correspond to Teichm¨uller spaces of (possibly singular) hyperbolic structures on a torus M¯ . For t = 2, the level set κ−1(t) ∩ R3 consists of characters of reducible representations and comprises two er- godic components corresponding to actions of GL(2, Z) on (R/Z)2 and R2 respectively. For 2 <t ≤ 18, the action of Γ on κ−1(t) ∩ R3 is ergodic. Corresponding to the Fricke space of a three-holed sphere is a Γ–invariant open subset Ω ⊂ R3 whose components are permuted freely by a subgroup of index 6 in Γ. -
Notes on Modular Forms
Notes on Modular Forms Dan Schultz August 20, 2015 Contents 0.1 Notation . .2 1 Introduction 4 1.1 Partitions and the η function . .4 1.2 Sums of squares and the θ function . .4 1.3 Ramanujan's τ Function . .5 1.4 Mock Modular Forms . .5 1.5 Special Values of the j Function . .6 2 Elliptic Functions and Basic Modular Forms on SL2(Z) 7 2.1 Theory of Elliptic Functions . .7 2.2 The Weierstrass } Function . .8 2.3 Eisenstein Series . .9 2.4 Modular Discriminant ∆(τ) and Klein's Absolute Invariant j(τ)............ 10 2.5 Basic Properties of SL2(Z)................................. 11 2.6 The η function and E2 ................................... 12 2.7 Recursions for the Eisenstein Series . 15 2.8 Elliptic Θ Functions . 15 2.9 Γ(2) and the Asymptotic of Θ Near the Cusps . 19 2.10 Addition Formulas . 23 2.11 Γ(3) and the Asymptotic of η Near the Cusps . 24 2.12 Exercises . 28 3 Theory of Modular Forms on SL2(Z) 31 3.1 Definition of a Modular Form . 31 3.2 Valence Formula . 32 3.3 Dimension Formulas and Generators . 33 3.4 Applications to Identities . 34 3.5 Exercises . 35 4 Theory of Modular Forms on Congruence Subgroups of SL2(Z) 36 4.1 Definition of modular forms on Γ with [Γ(1) : Γ] < 1 .................. 36 4.2 Dimension formulas . 38 4.3 Counting i for Γ(N) and Γ1(N) and Γ0(N)....................... 40 4.4 General properties of Ak(Γ) ................................ 42 4.5 Working with finite index subgroups of Γ(1) .