On the Ranks of HS and Mclon the Ranks of the Conway Groups Co2
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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. -
Finite Groups, Designs and Codes
Abstract Introduction Terminology and notation Group Actions and Permutation Characters Method 1 References Finite Groups, Designs and Codes J Moori School of Mathematical Sciences, University of KwaZulu-Natal Pietermaritzburg 3209, South Africa ASI, Opatija, 31 May –11 June 2010 J Moori, ASI 2010, Opatija, Croatia Groups, Designs and Codes Abstract Introduction Terminology and notation Group Actions and Permutation Characters Method 1 References Finite Groups, Designs and Codes J Moori School of Mathematical Sciences, University of KwaZulu-Natal Pietermaritzburg 3209, South Africa ASI, Opatija, 31 May –11 June 2010 J Moori, ASI 2010, Opatija, Croatia Groups, Designs and Codes Abstract Introduction Terminology and notation Group Actions and Permutation Characters Method 1 References Outline 1 Abstract 2 Introduction 3 Terminology and notation 4 Group Actions and Permutation Characters Permutation and Matrix Representations Permutation Characters 5 Method 1 Janko groups J1 and J2 Conway group Co2 6 References J Moori, ASI 2010, Opatija, Croatia Groups, Designs and Codes Abstract Introduction Terminology and notation Group Actions and Permutation Characters Method 1 References Abstract Abstract We will discuss two methods for constructing codes and designs from finite groups (mostly simple finite groups). This is a survey of the collaborative work by the author with J D Key and B Rorigues. In this talk (Talk 1) we first discuss background material and results required from finite groups, permutation groups and representation theory. Then we aim to describe our first method of constructing codes and designs from finite groups. J Moori, ASI 2010, Opatija, Croatia Groups, Designs and Codes Abstract Introduction Terminology and notation Group Actions and Permutation Characters Method 1 References Abstract Abstract We will discuss two methods for constructing codes and designs from finite groups (mostly simple finite groups). -
RIGID LOCAL SYSTEMS with MONODROMY GROUP the CONWAY GROUP Co2
RIGID LOCAL SYSTEMS WITH MONODROMY GROUP THE CONWAY GROUP Co2 NICHOLAS M. KATZ, ANTONIO ROJAS-LEON,´ AND PHAM HUU TIEP Abstract. We first develop some basic facts about hypergeometric sheaves on the multi- plicative group Gm in characteristic p > 0. Certain of their Kummer pullbacks extend to irreducible local systems on the affine line in characteristic p > 0. One of these, of rank 23 in characteristic p = 3, turns out to have the Conway group Co2, in its irreducible orthogonal representation of degree 23, as its arithmetic and geometric monodromy groups. Contents Introduction 1 1. The basic set up, and general results 1 2. The criterion for finite monodromy 10 3. Theorems of finite monodromy 11 4. Determination of the monodromy groups 17 References 18 Introduction In the first two sections, we give the general set up. In the third section, we apply known criteria to show that certain local systems of rank 23 over the affine line in characteristic 3 have finite (arithmetic and geometric) monodromy groups. In the final section, we show that the finite monodromy groups in question are the Conway group Co2 in its 23-dimensional irreducible orthogonal representation. 1. The basic set up, and general results × We fix a prime number p, a prime number ` 6= p, and a nontrivial Q` -valued additive character of Fp. For k=Fp a finite extension, we denote by k the nontrivial additive character of k given by k := ◦ Tracek=Fp . In perhaps more down to earth terms, we fix a × nontrivial Q(µp) -valued additive character of Fp, and a field embedding of Q(µp) into Q` for some ` 6= p. -
The Cohomologies of the Sylow 2-Subgroups of a Symplectic Group of Degree Six and of the Third Conway Group
THE COHOMOLOGIES OF THE SYLOW 2-SUBGROUPS OF A SYMPLECTIC GROUP OF DEGREE SIX AND OF THE THIRD CONWAY GROUP JOHN MAGINNIS Abstract. The third Conway group Co3 is one of the twenty-six sporadic finite simple groups. The cohomology of its Sylow 2-subgroup S is computed, an important step in calculating the mod 2 cohomology of Co3. The spectral sequence for the central extension of S is described and collapses at the sixth page. Generators are described in terms of the Evens norm or transfers from subgroups. The central quotient S0 = S=2 is the Sylow 2-subgroup of the symplectic group Sp6(F2) of six by six matrices over the field of two elements. The cohomology of S0 is computed, and is detected by restriction to elementary abelian 2-subgroups. 1. Introduction A presentation for the Sylow 2-subgroup S of the sporadic finite simple group Co3 is given by Benson [1]. We will use a different presentation, with generators which can be described in terms of Benson's generators fa1; a2; a3; a4; b1; b2; c1; c2; eg as follows. w = c3; x = b2c1c2; y = ec3; z = a4; a = a3a4c2; b = a3a4b1c2; c = a3; t = a4c1; u = a2; v = a1: We have the following set of relations for the generators fw; x; y; z; a; b; c; t; u; vg. w2 = x2 = y2 = z2 = c2 = u2 = v2 = [w; y] = [w; z] = [w; c] = [w; v] = [x; z] = [x; u] = [x; v] = [y; c] = [y; u] = [y; v] = [a; z] = [c; z] = [u; z] = [v; z] = [c; t] = [c; u] = [c; v] = [a; u] = [a; v] = [b; c] = [b; t] = [b; u] = [b; v] = [t; u] = [t; v] = [u; v] = 1; tu = [a; y]; t = [w; b]; av = [w; x]; b = [x; y]; c = [y; z] u = b2 = [x; c] = [b; z] = [b; y] = [b; x]; uv = [t; x] = [a; b]; v = t2 = a2 = [w; u] = [a; c] = [t; z] = [a; w] = [t; w] = [t; a] = [t; y] = [a; x]: The group S has order 1024 and a center Z(S) of order two, generated by v = a1. -
Jhep07(2019)026
Published for SISSA by Springer Received: January 18, 2019 Revised: May 3, 2019 Accepted: June 26, 2019 Published: July 4, 2019 JHEP07(2019)026 Monster anatomy Jin-Beom Bae, Kimyeong Lee and Sungjay Lee Korea Institute for Advanced Study, 85 Hoegiro, Dongdaemun-Gu, Seoul 02455, Korea E-mail: [email protected], [email protected], [email protected] Abstract: 47 We investigate the two-dimensional conformal field theories (CFTs) of c = 2 , 116 c = 5 and c = 23 `dual' to the critical Ising model, the three state Potts model and the tensor product of two Ising models, respectively. We argue that these CFTs exhibit moonshines for the double covering of the baby Monster group, 2 · B, the triple covering 0 of the largest Fischer group, 3 · Fi24 and multiple-covering of the second largest Conway 1+22 group, 2 · 2 · Co2. Various twined characters are shown to satisfy generalized bilinear relations involving Mckay-Thompson series. We also rediscover that the `self-dual' two- dimensional bosonic conformal field theory of c = 12 has the Conway group Co0 ' 2 · Co1 as an automorphism group. Keywords: Conformal and W Symmetry, Field Theories in Lower Dimensions ArXiv ePrint: 1811.12263 Open Access, c The Authors. https://doi.org/10.1007/JHEP07(2019)026 Article funded by SCOAP3. Contents 1 Introduction1 2 Dual of the Ising model and the Baby Monster3 0 3 Dual of the three-state Potts model and 3 · Fi24 6 2 1+22 4 Dual of the critical Ising and 2 · 2 · Co2 9 JHEP07(2019)026 5 Self-dual RCFT and 2 · Co1 11 6 Discussion 13 A Dimension of the irreducible representations 15 B 0 B Character tables of 2 · and 3 · Fi24 16 C Generalized bilinear relations 18 C.1 2 · B 18 0 C.2 3 · Fi24 18 1 Introduction Mckay and Thompson's remarkable observation between the monster group M and the modular objects, especially, the j-invariant, motivated the study of the so-called `Monstrous Moonshine' in [1]. -
2 Cohomology Ring of the Third Conway Groupis Cohen--Macaulay
Algebraic & Geometric Topology 11 (2011) 719–734 719 The mod–2 cohomology ring of the third Conway group is Cohen–Macaulay SIMON AKING DAVID JGREEN GRAHAM ELLIS By explicit machine computation we obtain the mod–2 cohomology ring of the third Conway group Co3 . It is Cohen–Macaulay, has dimension 4, and is detected on the maximal elementary abelian 2–subgroups. 20J06; 20-04, 20D08 1 Introduction There has been considerable work on the mod–2 cohomology rings of the finite simple groups. Every finite simple group of 2–rank at most three has Cohen–Macaulay mod–2 cohomology by Adem and Milgram [2]. There are eight sporadic finite simple groups of 2–rank four. For six of these, Adem and Milgram already determined the mod–2 cohomology ring, at least as a module over a polynomial subalgebra [3, VIII.5]. In most cases the cohomology is not Cohen–Macaulay. For instance, the Mathieu groups M22 and M23 each have maximal elementary abelian 2–subgroups of ranks 3 and 4, meaning that the cohomology cannot be Cohen–Macaulay: see [3, page 269]. The two outstanding cases have the largest Sylow 2–subgroups. The Higman–Sims group HS has size 29 Sylow subgroup, and the cohomology of this 2–group is known 10 by Adem et al [1]. The third Conway group Co3 has size 2 Sylow subgroup. In this paper we consider Co3 . It stands out for two reasons, one being that it has the largest Sylow 2–subgroup. The second reason requires a little explanation. The Mathieu group M12 has 2–rank three. -
Extended Near Hexagons and Line Systems
Extended near hexagons and line systems Hans Cuypers Department of Mathematics Eindhoven University of Technology P.O. Box 513, 5600 MB Eindhoven The Netherlands email: [email protected] October 2, 2002 Abstract In this paper we study extended near hexagons, and classify a class of line systems in which two lines are either perpendicular, or make an angle α with cos α = 1=3. Among the examples we encounter a set of 2300 lines in R23 ± 24 related to the second Conway group Co2 and a set of 2048 lines in R related 1+11 to the group 2 :M24. The other line systems under consideration in this paper are all subsystems of these. MSC classification: 51E30, 05B99, 51E12, 20D8 Keywords: Extended near hexagons, line systems, spherical designs. 1. Introduction In [34], Shult and Yanushka studied a class of line systems in Rn, equipped with the standard inner product ( ), in which any pair of distinct lines is either per- pendicular or makes an angle· jα · with cos α = 1=3. A nice and simple example of such a line system is the set of 4 lines in R3±passing through the vertices of a regular tetrahedron centered at the origin. Other examples considered by Shult and Yanushka include a system of 2300 lines in R23 related to the Leech lattice and the 24 second Conway group Co2 and a system of 2048 lines in R related to the binary 1+11 Golay code and the group 2 :M24. These line systems are all tetrahedrally closed, i.e., given three lines of the system passing through three of the four vertices of a regular tetrahedron centered at the origin, then also the line passing through the fourth vertex of the tetrahedron is present in the line system. -
The Moonshine Module for Conway's Group
Forum of Mathematics, Sigma (2015), Vol. 3, e10, 52 pages 1 doi:10.1017/fms.2015.7 THE MOONSHINE MODULE FOR CONWAY’S GROUP JOHN F. R. DUNCAN and SANDER MACK-CRANE Department of Mathematics, Applied Mathematics and Statistics, Case Western Reserve University, Cleveland, OH 44106, USA; email: [email protected], [email protected] Received 26 September 2014; accepted 30 April 2015 Abstract We exhibit an action of Conway’s group – the automorphism group of the Leech lattice – on a distinguished super vertex operator algebra, and we prove that the associated graded trace functions are normalized principal moduli, all having vanishing constant terms in their Fourier expansion. Thus we construct the natural analogue of the Frenkel–Lepowsky–Meurman moonshine module for Conway’s group. The super vertex operator algebra we consider admits a natural characterization, in direct analogy with that conjectured to hold for the moonshine module vertex operator algebra. It also admits a unique canonically twisted module, and the action of the Conway group naturally extends. We prove a special case of generalized moonshine for the Conway group, by showing that the graded trace functions arising from its action on the canonically twisted module are constant in the case of Leech lattice automorphisms with fixed points, and are principal moduli for genus-zero groups otherwise. 2010 Mathematics Subject Classification: 11F11, 11F22, 17B69, 20C34 1. Introduction Taking the upper half-plane H τ C (τ/ > 0 , together with the Poincare´ 2 2 2 2 VD f 2 j = g metric ds y− .dx dy /, we obtain the Poincare´ half-plane model of the D C hyperbolic plane. -
Iiiiiiiumiiiiuuiiiuiiii~Iuumiiniuii
r.~M CBM ~~~y R ``' ~~o~~o~~`~~~~~~~~~ J~~~~o~ ~;~~~~~ 7626 J~~~~.~~ Qo5 ~oo ~~~, u 1990 iiiiiiiumiiiiuuiiiuiiii~iuumiini ii 458 ! A DESIGN AND A CODE INVARIANT UNDER THE SIMPLE GROUP Co3 Willem H. Haemers, Christopher Parker Vera Pless and Vladimir D. Tonchev r. 4 ~ ~,~' FEw 458 .J ~ ~ ~ A DESIGN AND A CODE INVARIANT UNDER THE SIMPLE GROUP Cos Willem H. Haemers Department of Economics, Tilburg University, P.O.Box 90153, 5000 LE Tilburg, The Netherlands, r Christopher Parker ) Department of Mathematics, University of Wisconsin-Parkside, Box 2000, Kenosha, Wisconsin 53141-2000, USA, Vera Pless, Department of Mathematics, University of Illinois at Chicago, Box 4348, Chicago, Illinois 60680, USA, and Vladimir D. Tonchev~) Institute of Mathematics, P.O. Box 373, 1090 Sofia, Bulgaria In memory of Professor Marshall Hall ABSTRACT A self-orthogonal doubly-even (276,23) code invariant under the Conway simple group Coa is constructed. The minimum weight codewords form a 2-(2~6,100,2. 3)~ doubly-transitive block-primitive design with block sta- bilizer isomorphic to the Higman-Sims simple group HS. More generally, the codewords of any given weight are single orbits stabilized by maximal subgroups of Cos. The restriction of the code on the complement of a mini- mum weight codeword is the (1~6,22) code discovered by Calderbank and Wales as a code invariant under HS. ~) Part of this work was done while these two authors were at the Univer- sity of Giessen, W. Germany, the first as a NATO Research Fellow, and the second as a Research Fellow of the Alexander von Humboldt Foundation. -
Quaternions Over Q(&)
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Elsevier - Publisher Connector JOCRNAL OF ALGEBRA 63, 56-75 (I 980) Quaternions over Q(&), Leech’s Lattice and the Sporadic Group of Hall-lank0 J. TITS CollSge de France, I1 Place Marc&n-Berthelot, 75231 Paris Cedex 0.5, France Communicated by I. N. Herstein Received April 24, 1979 TO MY FRIEND NATHAN JACOBSON ON HIS 70TH BIRTHDAY INTRODUCTION It was observed long ago by J. Thompson that the automorphism group of Leech’s lattice A-Conway’s group *O-contains a subgroup X, isomorphic to the double cover &, of the alternating group ‘SI, . Furthermore, if we denote by X,3X,3 **. r) Xs the decreasing sequence of subgroups of Xs charac- terized up to conjugacy by Xi g ‘& , the centralizers Ci = C.,(XJ form a remarkable sequence: C, = .O is the double cover of Conway’s group ‘1, Cs the sextuple cover c, of Suzuki’s sporadic group, C, the double cover of Ga(F,), C’s the double cover J, of the sporadic group of Hall-Janko, . (cf. [4, p. 2421). This suggests a variety of interesting ways of looking at A, namely, as a module over its endomorphism ring Ri generated by Xi , for i = 2, 3, 4,...: indeed, the automorphism group of that module (endowed with a suitable form) is precisely the group Ci . For i = 2, R, = Z and one simply has Leech’s and Conway’s original approaches to the lattice [2, 10, 111. For i = 3, Rd = Z[$‘i] and A appears as the R,-module of rank 12 investigated by Lindsey [13] (cf. -
Octonions and the Leech Lattice
Journal of Algebra 322 (2009) 2186–2190 Contents lists available at ScienceDirect Journal of Algebra www.elsevier.com/locate/jalgebra Octonions and the Leech lattice Robert A. Wilson School of Mathematical Sciences, Queen Mary, University of London, Mile End Road, London E1 4NS, United Kingdom article info abstract Article history: We give a new, elementary, description of the Leech lattice in Received 18 December 2008 terms of octonions, thereby providing the first real explanation Availableonline27March2009 of the fact that the number of minimal vectors, 196560, can be Communicated by Gernot Stroth expressed in the form 3 × 240 × (1 + 16 + 16 × 16).Wealsogive an easy proof that it is an even self-dual lattice. Keywords: © Octonions 2009 Elsevier Inc. All rights reserved. Leech lattice Conway group 1. Introduction The Leech lattice occupies a special place in mathematics. It is the unique 24-dimensional even self-dual lattice with no vectors of norm 2, and defines the unique densest lattice packing of spheres in 24 dimensions. Its automorphism group is very large, and is the double cover of Conway’s group Co1 [2], one of the most important of the 26 sporadic simple groups. This group plays a crucial role in the construction of the Monster [14,4], which is the largest of the sporadic simple groups, and has connections with modular forms (so-called ‘Monstrous Moonshine’) and many other areas, including theoretical physics. The book by Conway and Sloane [5] is a good introduction to this lattice and its many applications. It is not surprising therefore that there is a huge literature on the Leech lattice, not just within mathematics but in the physics literature too. -
The Leech Lattice Λ and the Conway Group ·O Revisited
TRANSACTIONS OF THE AMERICAN MATHEMATICAL SOCIETY Volume 362, Number 3, March 2010, Pages 1351–1369 S 0002-9947(09)04726-6 Article electronically published on October 20, 2009 THE LEECH LATTICE Λ AND THE CONWAY GROUP ·O REVISITED JOHN N. BRAY AND ROBERT T. CURTIS Dedicated to John Horton Conway as he approaches his seventieth birthday. Abstract. We give a new, concise definition of the Conway group ·Oasfol- lows. The Mathieu group M24 acts quintuply transitively on 24 letters and so acts transitively (but imprimitively) on the set of 24 tetrads. We use this 4 24 action to define a progenitor P of shape 2 4 :M24; that is, a free product of cyclic groups of order 2 extended by a group of permutations of the involutory generators. A simple lemma leads us directly to an easily described, short relator, and factoring P by this relator results in ·O. Consideration of the lowest dimension in which ·O can act faithfully produces Conway’s elements ξT and the 24–dimensional real, orthogonal representation. The Leech lattice is obtained as the set of images under ·O of the integral vectors in R24. 1. Introduction The Leech lattice Λ was discovered by Leech [14] in 1965 in connection with the packing of non-overlapping identical spheres into the 24–dimensional space R24 so that their centres lie at the lattice points; see Conway and Sloane [9]. Its con- struction relies heavily on the rich combinatorial structure underlying the Mathieu group M24. The full group of symmeries of Λ is, of course, infinite, as it contains all translations by a lattice vector.