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Lie Algebras Associated with Generalized Cartan Matrices
LIE ALGEBRAS ASSOCIATED WITH GENERALIZED CARTAN MATRICES BY R. V. MOODY1 Communicated by Charles W. Curtis, October 3, 1966 1. Introduction. If 8 is a finite-dimensional split semisimple Lie algebra of rank n over a field $ of characteristic zero, then there is associated with 8 a unique nXn integral matrix (Ay)—its Cartan matrix—which has the properties Ml. An = 2, i = 1, • • • , n, M2. M3. Ay = 0, implies An = 0. These properties do not, however, characterize Cartan matrices. If (Ay) is a Cartan matrix, it is known (see, for example, [4, pp. VI-19-26]) that the corresponding Lie algebra, 8, may be recon structed as follows: Let e y fy hy i = l, • • • , n, be any Zn symbols. Then 8 is isomorphic to the Lie algebra 8 ((A y)) over 5 defined by the relations Ml = 0, bifj] = dyhy If or all i and j [eihj] = Ajid [f*,] = ~A„fy\ «<(ad ej)-A>'i+l = 0,1 /,(ad fà-W = (J\ii i 7* j. In this note, we describe some results about the Lie algebras 2((Ay)) when (Ay) is an integral square matrix satisfying Ml, M2, and M3 but is not necessarily a Cartan matrix. In particular, when the further condition of §3 is imposed on the matrix, we obtain a reasonable (but by no means complete) structure theory for 8(04t/)). 2. Preliminaries. In this note, * will always denote a field of char acteristic zero. An integral square matrix satisfying Ml, M2, and M3 will be called a generalized Cartan matrix, or g.c.m. -
Matroid Automorphisms of the F4 Root System
∗ Matroid automorphisms of the F4 root system Stephanie Fried Aydin Gerek Gary Gordon Dept. of Mathematics Dept. of Mathematics Dept. of Mathematics Grinnell College Lehigh University Lafayette College Grinnell, IA 50112 Bethlehem, PA 18015 Easton, PA 18042 [email protected] [email protected] Andrija Peruniˇci´c Dept. of Mathematics Bard College Annandale-on-Hudson, NY 12504 [email protected] Submitted: Feb 11, 2007; Accepted: Oct 20, 2007; Published: Nov 12, 2007 Mathematics Subject Classification: 05B35 Dedicated to Thomas Brylawski. Abstract Let F4 be the root system associated with the 24-cell, and let M(F4) be the simple linear dependence matroid corresponding to this root system. We determine the automorphism group of this matroid and compare it to the Coxeter group W for the root system. We find non-geometric automorphisms that preserve the matroid but not the root system. 1 Introduction Given a finite set of vectors in Euclidean space, we consider the linear dependence matroid of the set, where dependences are taken over the reals. When the original set of vectors has `nice' symmetry, it makes sense to compare the geometric symmetry (the Coxeter or Weyl group) with the group that preserves sets of linearly independent vectors. This latter group is precisely the automorphism group of the linear matroid determined by the given vectors. ∗Research supported by NSF grant DMS-055282. the electronic journal of combinatorics 14 (2007), #R78 1 For the root systems An and Bn, matroid automorphisms do not give any additional symmetry [4]. One can interpret these results in the following way: combinatorial sym- metry (preserving dependence) and geometric symmetry (via isometries of the ambient Euclidean space) are essentially the same. -
Platonic Solids Generate Their Four-Dimensional Analogues
1 Platonic solids generate their four-dimensional analogues PIERRE-PHILIPPE DECHANT a;b;c* aInstitute for Particle Physics Phenomenology, Ogden Centre for Fundamental Physics, Department of Physics, University of Durham, South Road, Durham, DH1 3LE, United Kingdom, bPhysics Department, Arizona State University, Tempe, AZ 85287-1604, United States, and cMathematics Department, University of York, Heslington, York, YO10 5GG, United Kingdom. E-mail: [email protected] Polytopes; Platonic Solids; 4-dimensional geometry; Clifford algebras; Spinors; Coxeter groups; Root systems; Quaternions; Representations; Symmetries; Trinities; McKay correspondence Abstract In this paper, we show how regular convex 4-polytopes – the analogues of the Platonic solids in four dimensions – can be constructed from three-dimensional considerations concerning the Platonic solids alone. Via the Cartan-Dieudonne´ theorem, the reflective symmetries of the arXiv:1307.6768v1 [math-ph] 25 Jul 2013 Platonic solids generate rotations. In a Clifford algebra framework, the space of spinors gen- erating such three-dimensional rotations has a natural four-dimensional Euclidean structure. The spinors arising from the Platonic Solids can thus in turn be interpreted as vertices in four- dimensional space, giving a simple construction of the 4D polytopes 16-cell, 24-cell, the F4 root system and the 600-cell. In particular, these polytopes have ‘mysterious’ symmetries, that are almost trivial when seen from the three-dimensional spinorial point of view. In fact, all these induced polytopes are also known to be root systems and thus generate rank-4 Coxeter PREPRINT: Acta Crystallographica Section A A Journal of the International Union of Crystallography 2 groups, which can be shown to be a general property of the spinor construction. -
Hyperbolic Weyl Groups and the Four Normed Division Algebras
Hyperbolic Weyl Groups and the Four Normed Division Algebras Alex Feingold1, Axel Kleinschmidt2, Hermann Nicolai3 1 Department of Mathematical Sciences, State University of New York Binghamton, New York 13902–6000, U.S.A. 2 Physique Theorique´ et Mathematique,´ Universite´ Libre de Bruxelles & International Solvay Institutes, Boulevard du Triomphe, ULB – CP 231, B-1050 Bruxelles, Belgium 3 Max-Planck-Institut fur¨ Gravitationsphysik, Albert-Einstein-Institut Am Muhlenberg¨ 1, D-14476 Potsdam, Germany – p. Introduction Presented at Illinois State University, July 7-11, 2008 Vertex Operator Algebras and Related Areas Conference in Honor of Geoffrey Mason’s 60th Birthday – p. Introduction Presented at Illinois State University, July 7-11, 2008 Vertex Operator Algebras and Related Areas Conference in Honor of Geoffrey Mason’s 60th Birthday – p. Introduction Presented at Illinois State University, July 7-11, 2008 Vertex Operator Algebras and Related Areas Conference in Honor of Geoffrey Mason’s 60th Birthday “The mathematical universe is inhabited not only by important species but also by interesting individuals” – C. L. Siegel – p. Introduction (I) In 1983 Feingold and Frenkel studied the rank 3 hyperbolic Kac–Moody algebra = A++ with F 1 y y @ y Dynkin diagram @ 1 0 1 − Weyl Group W ( )= w , w , w wI = 2, wI wJ = mIJ F h 1 2 3 || | | | i 2 1 0 − 2(αI , αJ ) Cartan matrix [AIJ ]= 1 2 2 = − − (αJ , αJ ) 0 2 2 − 2 3 2 Coxeter exponents [mIJ ]= 3 2 ∞ 2 2 ∞ – p. Introduction (II) The simple roots, α 1, α0, α1, span the − 1 Root lattice Λ( )= α = nI αI n 1,n0,n1 Z F − ∈ ( I= 1 ) X− – p. -
Matrix Lie Groups
Maths Seminar 2007 MATRIX LIE GROUPS Claudiu C Remsing Dept of Mathematics (Pure and Applied) Rhodes University Grahamstown 6140 26 September 2007 RhodesUniv CCR 0 Maths Seminar 2007 TALK OUTLINE 1. What is a matrix Lie group ? 2. Matrices revisited. 3. Examples of matrix Lie groups. 4. Matrix Lie algebras. 5. A glimpse at elementary Lie theory. 6. Life beyond elementary Lie theory. RhodesUniv CCR 1 Maths Seminar 2007 1. What is a matrix Lie group ? Matrix Lie groups are groups of invertible • matrices that have desirable geometric features. So matrix Lie groups are simultaneously algebraic and geometric objects. Matrix Lie groups naturally arise in • – geometry (classical, algebraic, differential) – complex analyis – differential equations – Fourier analysis – algebra (group theory, ring theory) – number theory – combinatorics. RhodesUniv CCR 2 Maths Seminar 2007 Matrix Lie groups are encountered in many • applications in – physics (geometric mechanics, quantum con- trol) – engineering (motion control, robotics) – computational chemistry (molecular mo- tion) – computer science (computer animation, computer vision, quantum computation). “It turns out that matrix [Lie] groups • pop up in virtually any investigation of objects with symmetries, such as molecules in chemistry, particles in physics, and projective spaces in geometry”. (K. Tapp, 2005) RhodesUniv CCR 3 Maths Seminar 2007 EXAMPLE 1 : The Euclidean group E (2). • E (2) = F : R2 R2 F is an isometry . → | n o The vector space R2 is equipped with the standard Euclidean structure (the “dot product”) x y = x y + x y (x, y R2), • 1 1 2 2 ∈ hence with the Euclidean distance d (x, y) = (y x) (y x) (x, y R2). -
Introduction to Lie Theory Homework #6 1. Let G = G 1 ⊕ G2 Be a Direct
Introduction to Lie Theory Homework #6 1. Let g = g1 ⊕ g2 be a direct sum of two Lie algebras. Let V be a finite-dimensional g-module. Prove that V is completely reducible as a g-module if and only it is completely reducible both as a g1-module and as a g2-module. (Hint. Consider the finite-dimensional algebra A that is the image of U(g) under the induced algebra homomorphism ρ : U(g) ! EndC(V ), use Wedderburn theorem.) 2. Let g be a finite-dimensional semisimple Lie algebra with Killing form κ. We showed in L6-2 that g is the direct sum g1 ⊕· · ·⊕gn of its simple ideals, with gi ?κ gj for i 6= j. Let β be some other invariant bilinear form on g. Prove: (a) βjgi is a multiple of the Killing form κjgi for each i = 1; : : : ; n. (b) gi ?β gi for i 6= j. (c) β is a symmetric bilinear form. The remaining questions require the notion of a toral subalgebra t of a finite- dimensional semisimple Lie algebra g. Recall that this is a subalgebra con- sisting entirely of semisimple elements of g. As established in L7-1, such a subalgebra is necessarily Abelian. Hence, there is a root space decomposition M g = g0 ⊕ gα α2R ∗ where R = f0 6= α 2 t j gα 6= 0g is the set of roots of g with respect to t. Here, gα = fx 2 t j [t; x] = α(t)x for all t 2 tg for any α 2 t∗. -
Expansion in Finite Simple Groups of Lie Type
Expansion in finite simple groups of Lie type Terence Tao Department of Mathematics, UCLA, Los Angeles, CA 90095 E-mail address: [email protected] In memory of Garth Gaudry, who set me on the road Contents Preface ix Notation x Acknowledgments xi Chapter 1. Expansion in Cayley graphs 1 x1.1. Expander graphs: basic theory 2 x1.2. Expansion in Cayley graphs, and Kazhdan's property (T) 20 x1.3. Quasirandom groups 54 x1.4. The Balog-Szemer´edi-Gowers lemma, and the Bourgain- Gamburd expansion machine 81 x1.5. Product theorems, pivot arguments, and the Larsen-Pink non-concentration inequality 94 x1.6. Non-concentration in subgroups 127 x1.7. Sieving and expanders 135 Chapter 2. Related articles 157 x2.1. Cayley graphs and the algebra of groups 158 x2.2. The Lang-Weil bound 177 x2.3. The spectral theorem and its converses for unbounded self-adjoint operators 191 x2.4. Notes on Lie algebras 214 x2.5. Notes on groups of Lie type 252 Bibliography 277 Index 285 vii Preface Expander graphs are a remarkable type of graph (or more precisely, a family of graphs) on finite sets of vertices that manage to simultaneously be both sparse (low-degree) and \highly connected" at the same time. They enjoy very strong mixing properties: if one starts at a fixed vertex of an (two-sided) expander graph and randomly traverses its edges, then the distribution of one's location will converge exponentially fast to the uniform distribution. For this and many other reasons, expander graphs are useful in a wide variety of areas of both pure and applied mathematics. -
CHAPTER 4 Representations of Finite Groups of Lie Type Let Fq Be a Finite
CHAPTER 4 Representations of finite groups of Lie type Let Fq be a finite field of order q and characteristic p. Let G be a finite group of Lie type, that is, G is the Fq-rational points of a connected reductive group G defined over Fq. For example, if n is a positive integer GLn(Fq) and SLn(Fq) are finite groups of Lie type. 0 In Let J = , where In is the n × n identity matrix. Let −In 0 t Sp2n(Fq) = { g ∈ GL2n(Fq) | gJg = J }. Then Sp2n(Fq) is a symplectic group of rank n and is a finite group of Lie type. For G = GLn(Fq) or SLn(Fq) (and some other examples), the standard Borel subgroup B of G is the subgroup of G consisting of the upper triangular elements in G.A standard parabolic subgroup of G is a subgroup of G which contains the standard Borel subgroup B. If P is a standard parabolic subgroup of GLn(Fq), then there exists a partition (n1, . , nr) of n (a set of positive integers nj such that n1 + ··· + nr = n) such that P = P(n1,...,nr ) = M n N, where M ' GLn1 (Fq) × · · · × GLnr (Fq) has the form A 0 ··· 0 1 0 A2 ··· 0 M = | A ∈ GL ( ), 1 ≤ j ≤ r . . .. .. j nj Fq . 0 ··· 0 Ar and In1 ∗ · · · ∗ 0 In2 · · · ∗ N = , . .. .. . 0 ··· 0 Inr where ∗ denotes arbitary entries in Fq. The subgroup M is called a (standard) Levi sub- group of P , and N is called the unipotent radical of P . Note that the partition (1, 1,..., 1) corresponds to B and (n) corresponds to G. -
Classifying the Representation Type of Infinitesimal Blocks of Category
Classifying the Representation Type of Infinitesimal Blocks of Category OS by Kenyon J. Platt (Under the Direction of Brian D. Boe) Abstract Let g be a simple Lie algebra over the field C of complex numbers, with root system Φ relative to a fixed maximal toral subalgebra h. Let S be a subset of the simple roots ∆ of Φ, which determines a standard parabolic subalgebra of g. Fix an integral weight ∗ µ µ ∈ h , with singular set J ⊆ ∆. We determine when an infinitesimal block O(g,S,J) := OS of parabolic category OS is nonzero using the theory of nilpotent orbits. We extend work of Futorny-Nakano-Pollack, Br¨ustle-K¨onig-Mazorchuk, and Boe-Nakano toward classifying the representation type of the nonzero infinitesimal blocks of category OS by considering arbitrary sets S and J, and observe a strong connection between the theory of nilpotent orbits and the representation type of the infinitesimal blocks. We classify certain infinitesimal blocks of category OS including all the semisimple infinitesimal blocks in type An, and all of the infinitesimal blocks for F4 and G2. Index words: Category O; Representation type; Verma modules Classifying the Representation Type of Infinitesimal Blocks of Category OS by Kenyon J. Platt B.A., Utah State University, 1999 M.S., Utah State University, 2001 M.A, The University of Georgia, 2006 A Thesis Submitted to the Graduate Faculty of The University of Georgia in Partial Fulfillment of the Requirements for the Degree Doctor of Philosophy Athens, Georgia 2008 c 2008 Kenyon J. Platt All Rights Reserved Classifying the Representation Type of Infinitesimal Blocks of Category OS by Kenyon J. -
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. -
Shtukas for Reductive Groups and Langlands Correspondence for Functions Fields
SHTUKAS FOR REDUCTIVE GROUPS AND LANGLANDS CORRESPONDENCE FOR FUNCTIONS FIELDS VINCENT LAFFORGUE This text gives an introduction to the Langlands correspondence for function fields and in particular to some recent works in this subject. We begin with a short historical account (all notions used below are recalled in the text). The Langlands correspondence [49] is a conjecture of utmost impor- tance, concerning global fields, i.e. number fields and function fields. Many excellent surveys are available, for example [39, 14, 13, 79, 31, 5]. The Langlands correspondence belongs to a huge system of conjectures (Langlands functoriality, Grothendieck’s vision of motives, special val- ues of L-functions, Ramanujan-Petersson conjecture, generalized Rie- mann hypothesis). This system has a remarkable deepness and logical coherence and many cases of these conjectures have already been es- tablished. Moreover the Langlands correspondence over function fields admits a geometrization, the “geometric Langlands program”, which is related to conformal field theory in Theoretical Physics. Let G be a connected reductive group over a global field F . For the sake of simplicity we assume G is split. The Langlands correspondence relates two fundamental objects, of very different nature, whose definition will be recalled later, • the automorphic forms for G, • the global Langlands parameters , i.e. the conjugacy classes of morphisms from the Galois group Gal(F =F ) to the Langlands b dual group G(Q`). b For G = GL1 we have G = GL1 and this is class field theory, which describes the abelianization of Gal(F =F ) (one particular case of it for Q is the law of quadratic reciprocity, which dates back to Euler, Legendre and Gauss). -
LIE GROUPS and ALGEBRAS NOTES Contents 1. Definitions 2
LIE GROUPS AND ALGEBRAS NOTES STANISLAV ATANASOV Contents 1. Definitions 2 1.1. Root systems, Weyl groups and Weyl chambers3 1.2. Cartan matrices and Dynkin diagrams4 1.3. Weights 5 1.4. Lie group and Lie algebra correspondence5 2. Basic results about Lie algebras7 2.1. General 7 2.2. Root system 7 2.3. Classification of semisimple Lie algebras8 3. Highest weight modules9 3.1. Universal enveloping algebra9 3.2. Weights and maximal vectors9 4. Compact Lie groups 10 4.1. Peter-Weyl theorem 10 4.2. Maximal tori 11 4.3. Symmetric spaces 11 4.4. Compact Lie algebras 12 4.5. Weyl's theorem 12 5. Semisimple Lie groups 13 5.1. Semisimple Lie algebras 13 5.2. Parabolic subalgebras. 14 5.3. Semisimple Lie groups 14 6. Reductive Lie groups 16 6.1. Reductive Lie algebras 16 6.2. Definition of reductive Lie group 16 6.3. Decompositions 18 6.4. The structure of M = ZK (a0) 18 6.5. Parabolic Subgroups 19 7. Functional analysis on Lie groups 21 7.1. Decomposition of the Haar measure 21 7.2. Reductive groups and parabolic subgroups 21 7.3. Weyl integration formula 22 8. Linear algebraic groups and their representation theory 23 8.1. Linear algebraic groups 23 8.2. Reductive and semisimple groups 24 8.3. Parabolic and Borel subgroups 25 8.4. Decompositions 27 Date: October, 2018. These notes compile results from multiple sources, mostly [1,2]. All mistakes are mine. 1 2 STANISLAV ATANASOV 1. Definitions Let g be a Lie algebra over algebraically closed field F of characteristic 0.