14.2 Covers of Symmetric and Alternating Groups
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Math 411 Midterm 2, Thursday 11/17/11, 7PM-8:30PM. Instructions: Exam Time Is 90 Mins
Math 411 Midterm 2, Thursday 11/17/11, 7PM-8:30PM. Instructions: Exam time is 90 mins. There are 7 questions for a total of 75 points. Calculators, notes, and textbook are not allowed. Justify all your answers carefully. If you use a result proved in the textbook or class notes, state the result precisely. 1 Q1. (10 points) Let σ 2 S9 be the permutation 1 2 3 4 5 6 7 8 9 5 8 7 2 3 9 1 4 6 (a) (2 points) Write σ as a product of disjoint cycles. (b) (2 points) What is the order of σ? (c) (2 points) Write σ as a product of transpositions. (d) (4 points) Compute σ100. Q2. (8 points) (a) (3 points) Find an element of S5 of order 6 or prove that no such element exists. (b) (5 points) Find an element of S6 of order 7 or prove that no such element exists. Q3. (12 points) (a) (4 points) List all the elements of the alternating group A4. (b) (8 points) Find the left cosets of the subgroup H of A4 given by H = fe; (12)(34); (13)(24); (14)(23)g: Q4. (10 points) (a) (3 points) State Lagrange's theorem. (b) (7 points) Let p be a prime, p ≥ 3. Let Dp be the dihedral group of symmetries of a regular p-gon (a polygon with p sides of equal length). What are the possible orders of subgroups of Dp? Give an example in each case. 2 Q5. (13 points) (a) (3 points) State a theorem which describes all finitely generated abelian groups. -
Generating the Mathieu Groups and Associated Steiner Systems
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Elsevier - Publisher Connector Discrete Mathematics 112 (1993) 41-47 41 North-Holland Generating the Mathieu groups and associated Steiner systems Marston Conder Department of Mathematics and Statistics, University of Auckland, Private Bag 92019, Auckland, New Zealand Received 13 July 1989 Revised 3 May 1991 Abstract Conder, M., Generating the Mathieu groups and associated Steiner systems, Discrete Mathematics 112 (1993) 41-47. With the aid of two coset diagrams which are easy to remember, it is shown how pairs of generators may be obtained for each of the Mathieu groups M,,, MIz, Mz2, M,, and Mz4, and also how it is then possible to use these generators to construct blocks of the associated Steiner systems S(4,5,1 l), S(5,6,12), S(3,6,22), S(4,7,23) and S(5,8,24) respectively. 1. Introduction Suppose you land yourself in 24-dimensional space, and are faced with the problem of finding the best way to pack spheres in a box. As is well known, what you really need for this is the Leech Lattice, but alas: you forgot to bring along your Miracle Octad Generator. You need to construct the Leech Lattice from scratch. This may not be so easy! But all is not lost: if you can somehow remember how to define the Mathieu group Mz4, you might be able to produce the blocks of a Steiner system S(5,8,24), and the rest can follow. In this paper it is shown how two coset diagrams (which are easy to remember) can be used to obtain pairs of generators for all five of the Mathieu groups M,,, M12, M22> Mz3 and Mz4, and also how blocks may be constructed from these for each of the Steiner systems S(4,5,1 I), S(5,6,12), S(3,6,22), S(4,7,23) and S(5,8,24) respectively. -
The Unitary Representations of the Poincaré Group in Any Spacetime
The unitary representations of the Poincar´e group in any spacetime dimension Xavier Bekaert a and Nicolas Boulanger b a Institut Denis Poisson, Unit´emixte de Recherche 7013, Universit´ede Tours, Universit´ed’Orl´eans, CNRS, Parc de Grandmont, 37200 Tours (France) [email protected] b Service de Physique de l’Univers, Champs et Gravitation Universit´ede Mons – UMONS, Place du Parc 20, 7000 Mons (Belgium) [email protected] An extensive group-theoretical treatment of linear relativistic field equa- tions on Minkowski spacetime of arbitrary dimension D > 2 is presented in these lecture notes. To start with, the one-to-one correspondence be- tween linear relativistic field equations and unitary representations of the isometry group is reviewed. In turn, the method of induced representa- tions reduces the problem of classifying the representations of the Poincar´e group ISO(D 1, 1) to the classification of the representations of the sta- − bility subgroups only. Therefore, an exhaustive treatment of the two most important classes of unitary irreducible representations, corresponding to massive and massless particles (the latter class decomposing in turn into the “helicity” and the “infinite-spin” representations) may be performed via the well-known representation theory of the orthogonal groups O(n) (with D 4 <n<D ). Finally, covariant field equations are given for each − unitary irreducible representation of the Poincar´egroup with non-negative arXiv:hep-th/0611263v2 13 Jun 2021 mass-squared. Tachyonic representations are also examined. All these steps are covered in many details and with examples. The present notes also include a self-contained review of the representation theory of the general linear and (in)homogeneous orthogonal groups in terms of Young diagrams. -
Arxiv:Math/0511624V1
Automorphism groups of polycyclic-by-finite groups and arithmetic groups Oliver Baues ∗ Fritz Grunewald † Mathematisches Institut II Mathematisches Institut Universit¨at Karlsruhe Heinrich-Heine-Universit¨at D-76128 Karlsruhe D-40225 D¨usseldorf May 18, 2005 Abstract We show that the outer automorphism group of a polycyclic-by-finite group is an arithmetic group. This result follows from a detailed structural analysis of the automorphism groups of such groups. We use an extended version of the theory of the algebraic hull functor initiated by Mostow. We thus make applicable refined methods from the theory of algebraic and arithmetic groups. We also construct examples of polycyclic-by-finite groups which have an automorphism group which does not contain an arithmetic group of finite index. Finally we discuss applications of our results to the groups of homotopy self-equivalences of K(Γ, 1)-spaces and obtain an extension of arithmeticity results of Sullivan in rational homo- topy theory. 2000 Mathematics Subject Classification: Primary 20F28, 20G30; Secondary 11F06, 14L27, 20F16, 20F34, 22E40, 55P10 arXiv:math/0511624v1 [math.GR] 25 Nov 2005 ∗e-mail: [email protected] †e-mail: [email protected] 1 Contents 1 Introduction 4 1.1 Themainresults ........................... 4 1.2 Outlineoftheproofsandmoreresults . 6 1.3 Cohomologicalrepresentations . 8 1.4 Applications to the groups of homotopy self-equivalences of spaces 9 2 Prerequisites on linear algebraic groups and arithmetic groups 12 2.1 Thegeneraltheory .......................... 12 2.2 Algebraicgroupsofautomorphisms. 15 3 The group of automorphisms of a solvable-by-finite linear algebraic group 17 3.1 The algebraic structure of Auta(H)................ -
On Some Generation Methods of Finite Simple Groups
Introduction Preliminaries Special Kind of Generation of Finite Simple Groups The Bibliography On Some Generation Methods of Finite Simple Groups Ayoub B. M. Basheer Department of Mathematical Sciences, North-West University (Mafikeng), P Bag X2046, Mmabatho 2735, South Africa Groups St Andrews 2017 in Birmingham, School of Mathematics, University of Birmingham, United Kingdom 11th of August 2017 Ayoub Basheer, North-West University, South Africa Groups St Andrews 2017 Talk in Birmingham Introduction Preliminaries Special Kind of Generation of Finite Simple Groups The Bibliography Abstract In this talk we consider some methods of generating finite simple groups with the focus on ranks of classes, (p; q; r)-generation and spread (exact) of finite simple groups. We show some examples of results that were established by the author and his supervisor, Professor J. Moori on generations of some finite simple groups. Ayoub Basheer, North-West University, South Africa Groups St Andrews 2017 Talk in Birmingham Introduction Preliminaries Special Kind of Generation of Finite Simple Groups The Bibliography Introduction Generation of finite groups by suitable subsets is of great interest and has many applications to groups and their representations. For example, Di Martino and et al. [39] established a useful connection between generation of groups by conjugate elements and the existence of elements representable by almost cyclic matrices. Their motivation was to study irreducible projective representations of the sporadic simple groups. In view of applications, it is often important to exhibit generating pairs of some special kind, such as generators carrying a geometric meaning, generators of some prescribed order, generators that offer an economical presentation of the group. -
Janko's Sporadic Simple Groups
Janko’s Sporadic Simple Groups: a bit of history Algebra, Geometry and Computation CARMA, Workshop on Mathematics and Computation Terry Gagen and Don Taylor The University of Sydney 20 June 2015 Fifty years ago: the discovery In January 1965, a surprising announcement was communicated to the international mathematical community. Zvonimir Janko, working as a Research Fellow at the Institute of Advanced Study within the Australian National University had constructed a new sporadic simple group. Before 1965 only five sporadic simple groups were known. They had been discovered almost exactly one hundred years prior (1861 and 1873) by Émile Mathieu but the proof of their simplicity was only obtained in 1900 by G. A. Miller. Finite simple groups: earliest examples É The cyclic groups Zp of prime order and the alternating groups Alt(n) of even permutations of n 5 items were the earliest simple groups to be studied (Gauss,≥ Euler, Abel, etc.) É Evariste Galois knew about PSL(2,p) and wrote about them in his letter to Chevalier in 1832 on the night before the duel. É Camille Jordan (Traité des substitutions et des équations algébriques,1870) wrote about linear groups defined over finite fields of prime order and determined their composition factors. The ‘groupes abéliens’ of Jordan are now called symplectic groups and his ‘groupes hypoabéliens’ are orthogonal groups in characteristic 2. É Émile Mathieu introduced the five groups M11, M12, M22, M23 and M24 in 1861 and 1873. The classical groups, G2 and E6 É In his PhD thesis Leonard Eugene Dickson extended Jordan’s work to linear groups over all finite fields and included the unitary groups. -
Representations of the Infinite Symmetric Group
Representations of the infinite symmetric group Alexei Borodin1 Grigori Olshanski2 Version of February 26, 2016 1 Department of Mathematics, Massachusetts Institute of Technology, Cambridge, MA, USA Institute for Information Transmission Problems of the Russian Academy of Sciences, Moscow, Russia 2 Institute for Information Transmission Problems of the Russian Academy of Sciences, Moscow, Russia National Research University Higher School of Economics, Moscow, Russia Contents 0 Introduction 4 I Symmetric functions and Thoma's theorem 12 1 Symmetric group representations 12 Exercises . 19 2 Theory of symmetric functions 20 Exercises . 31 3 Coherent systems on the Young graph 37 The infinite symmetric group and the Young graph . 37 Coherent systems . 39 The Thoma simplex . 41 1 CONTENTS 2 Integral representation of coherent systems and characters . 44 Exercises . 46 4 Extreme characters and Thoma's theorem 47 Thoma's theorem . 47 Multiplicativity . 49 Exercises . 52 5 Pascal graph and de Finetti's theorem 55 Exercises . 60 6 Relative dimension in Y 61 Relative dimension and shifted Schur polynomials . 61 The algebra of shifted symmetric functions . 65 Modified Frobenius coordinates . 66 The embedding Yn ! Ω and asymptotic bounds . 68 Integral representation of coherent systems: proof . 71 The Vershik{Kerov theorem . 74 Exercises . 76 7 Boundaries and Gibbs measures on paths 82 The category B ............................. 82 Projective chains . 83 Graded graphs . 86 Gibbs measures . 88 Examples of path spaces for branching graphs . 91 The Martin boundary and Vershik{Kerov's ergodic theorem . 92 Exercises . 94 II Unitary representations 98 8 Preliminaries and Gelfand pairs 98 Exercises . 108 9 Spherical type representations 111 10 Realization of spherical representations 118 Exercises . -
THE CONJUGACY CLASS RANKS of M24 Communicated by Robert Turner Curtis 1. Introduction M24 Is the Largest Mathieu Sporadic Simple
International Journal of Group Theory ISSN (print): 2251-7650, ISSN (on-line): 2251-7669 Vol. 6 No. 4 (2017), pp. 53-58. ⃝c 2017 University of Isfahan ijgt.ui.ac.ir www.ui.ac.ir THE CONJUGACY CLASS RANKS OF M24 ZWELETHEMBA MPONO Dedicated to Professor Jamshid Moori on the occasion of his seventieth birthday Communicated by Robert Turner Curtis 10 3 Abstract. M24 is the largest Mathieu sporadic simple group of order 244823040 = 2 ·3 ·5·7·11·23 and contains all the other Mathieu sporadic simple groups as subgroups. The object in this paper is to study the ranks of M24 with respect to the conjugacy classes of all its nonidentity elements. 1. Introduction 10 3 M24 is the largest Mathieu sporadic simple group of order 244823040 = 2 ·3 ·5·7·11·23 and contains all the other Mathieu sporadic simple groups as subgroups. It is a 5-transitive permutation group on a set of 24 points such that: (i) the stabilizer of a point is M23 which is 4-transitive (ii) the stabilizer of two points is M22 which is 3-transitive (iii) the stabilizer of a dodecad is M12 which is 5-transitive (iv) the stabilizer of a dodecad and a point is M11 which is 4-transitive M24 has a trivial Schur multiplier, a trivial outer automorphism group and it is the automorphism group of the Steiner system of type S(5,8,24) which is used to describe the Leech lattice on which M24 acts. M24 has nine conjugacy classes of maximal subgroups which are listed in [4], its ordinary character table is found in [4], its blocks and its Brauer character tables corresponding to the various primes dividing its order are found in [9] and [10] respectively and its complete prime spectrum is given by 2; 3; 5; 7; 11; 23. -
6 Permutation Groups
Arkansas Tech University MATH 4033: Elementary Modern Algebra Dr. Marcel B. Finan 6 Permutation Groups Let S be a nonempty set and M(S) be the collection of all mappings from S into S. In this section, we will emphasize on the collection of all invertible mappings from S into S. The elements of this set will be called permutations because of Theorem 2.4 and the next definition. Definition 6.1 Let S be a nonempty set. A one-to-one mapping from S onto S is called a permutation. Consider the collection of all permutations on S. Then this set is a group with respect to composition. Theorem 6.1 The set of all permutations of a nonempty set S is a group with respect to composition. This group is called the symmetric group on S and will be denoted by Sym(S). Proof. By Theorem 2.4, the set of all permutations on S is just the set I(S) of all invertible mappings from S to S. According to Theorem 4.3, this set is a group with respect to composition. Definition 6.2 A group of permutations , with composition as the operation, is called a permutation group on S. Example 6.1 1. Sym(S) is a permutation group. 2. The collection L of all invertible linear functions from R to R is a permu- tation group with respect to composition.(See Example 4.4.) Note that L is 1 a proper subset of Sym(R) since we can find a function in Sym(R) which is not in L, namely, the function f(x) = x3. -
Outer Automorphism Group of the Ergodic Equivalence Relation Generated by Translations of Dense Subgroup of Compact Group on Its Homogeneous Space
Publ. RIMS, Kyoto Univ. 32 (1996), 517-538 Outer Automorphism Group of the Ergodic Equivalence Relation Generated by Translations of Dense Subgroup of Compact Group on its Homogeneous Space By Sergey L. GEFTER* Abstract We study the outer automorphism group OutRr of the ergodic equivalence relation Rr generated by the action of a lattice F in a semisimple Lie group on the homogeneos space of a compact group K. It is shown that OutRr is locally compact. If K is a connected simple Lie group, we prove the compactness of 0\itRr using the D. Witte's rigidity theorem. Moreover, an example of an equivalence relation without outer automorphisms is constructed. Introduction An important problem in the theory of full factors [Sak], [Con 1] and in the orbit theory for groups with the T-property [Kaz] is that of studying the group of outer automorphisms of the corresponding object as a topological group. Unlike the amenable case, the outer automorphism group is a Polish space in the natural topology (see Section 1) and its topological properties are algebraic invariants of the factor and orbital invariants of the dynamical sys- tem. The first results in this sphere were obtained by A. Connes [Con 2] in 1980 who showed that the outer automorphism group of the Hi-factor of an ICC-group with the T-property is discrete and at most countable. Various ex- amples of factors and ergodic equivalence relations with locally compact groups of outer automorphisms were constructed in [Cho 1] , [EW] , [GGN] , [Gol] , [GG 1] and [GG 2] . In [Gol] and [GG 2] the topological properties of the outer automorphism group were used to construct orbitally nonequivalent Communicated by H. -
IMAGE of FUNCTORIALITY for GENERAL SPIN GROUPS 11 Splits As Two Places in K Or V Is Inert, I.E., There Is a Single Place in K Above the Place V in K
IMAGE OF FUNCTORIALITY FOR GENERAL SPIN GROUPS MAHDI ASGARI AND FREYDOON SHAHIDI Abstract. We give a complete description of the image of the endoscopic functorial transfer of generic automorphic representations from the quasi-split general spin groups to general linear groups over arbitrary number fields. This result is not covered by the recent work of Arthur on endoscopic classification of automorphic representations of classical groups. The image is expected to be the same for the whole tempered spectrum, whether generic or not, once the transfer for all tempered representations is proved. We give a number of applications including estimates toward the Ramanujan conjecture for the groups involved and the characterization of automorphic representations of GL(6) which are exterior square transfers from GL(4); among others. More applications to reducibility questions for the local induced representations of p-adic groups will also follow. 1. Introduction The purpose of this article is to completely determine the image of the transfer of globally generic, automorphic representations from the quasi-split general spin groups to the general linear groups. We prove the image is an isobaric, automorphic representation of a general linear group. Moreover, we prove that the isobaric summands of this representation have the property that their twisted symmetric square or twisted exterior square L-function has a pole at s = 1; depending on whether the transfer is from an even or an odd general spin group. We are also able to determine whether the image is a transfer from a split group, or a quasi-split, non-split group. Arthur's recent book on endoscopic classification of representations of classical groups [Ar] establishes similar results for automorphic representations of orthogonal and symplectic groups, generic or not, but does not cover the case of the general spin groups we consider here. -
1 the Spin Homomorphism SL2(C) → SO1,3(R) a Summary from Multiple Sources Written by Y
1 The spin homomorphism SL2(C) ! SO1;3(R) A summary from multiple sources written by Y. Feng and Katherine E. Stange Abstract We will discuss the spin homomorphism SL2(C) ! SO1;3(R) in three manners. Firstly we interpret SL2(C) as acting on the Minkowski 1;3 spacetime R ; secondly by viewing the quadratic form as a twisted 1 1 P × P ; and finally using Clifford groups. 1.1 Introduction The spin homomorphism SL2(C) ! SO1;3(R) is a homomorphism of classical matrix Lie groups. The lefthand group con- sists of 2 × 2 complex matrices with determinant 1. The righthand group consists of 4 × 4 real matrices with determinant 1 which preserve some fixed real quadratic form Q of signature (1; 3). This map is alternately called the spinor map and variations. The image of this map is the identity component + of SO1;3(R), denoted SO1;3(R). The kernel is {±Ig. Therefore, we obtain an isomorphism + PSL2(C) = SL2(C)= ± I ' SO1;3(R): This is one of a family of isomorphisms of Lie groups called exceptional iso- morphisms. In Section 1.3, we give the spin homomorphism explicitly, al- though these formulae are unenlightening by themselves. In Section 1.4 we describe O1;3(R) in greater detail as the group of Lorentz transformations. This document describes this homomorphism from three distinct per- spectives. The first is very concrete, and constructs, using the language of Minkowski space, Lorentz transformations and Hermitian matrices, an ex- 4 plicit action of SL2(C) on R preserving Q (Section 1.5).