ON FINITE SIMPLE GROUPS of P-LOCAL RANK TWO
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Subgroups of Division Rings in Characteristic Zero Are Characterized
Subgroups of Division Rings Mark Lewis Murray Schacher June 27, 2018 Abstract We investigate the finite subgroups that occur in the Hamiltonian quaternion algebra over the real subfield of cyclotomic fields. When possible, we investigate their distribution among the maximal orders. MSC(2010): Primary: 16A39, 12E15; Secondary: 16U60 1 Introduction Let F be a field, and fix a and b to be non-0 elements of F . The symbol algebra A =(a, b) is the 4-dimensional algebra over F generated by elements i and j that satisfy the relations: i2 = a, j2 = b, ij = ji. (1) − One usually sets k = ij, which leads to the additional circular relations ij = k = ji, jk = i = kj, ki = j = ki. (2) − − − arXiv:1806.09654v1 [math.RA] 25 Jun 2018 The set 1, i, j, k forms a basis for A over F . It is not difficult to see that A is a central{ simple} algebra over F , and using Wedderburn’s theorem, we see that A is either a 4-dimensional division ring or the ring M2(F ) of2 2 matrices over F . It is known that A is split (i.e. is the ring of 2 2 matrices× over F ) if and only if b is a norm from the field F (√a). Note that×b is a norm over F (√a) if and only if there exist elements x, y F so that b = x2 y2a. This condition is symmetric in a and b. ∈ − More generally, we have the following isomorphism of algebras: (a, b) ∼= (a, ub) (3) 1 where u = x2 y2a is a norm from F (√a); see [4] or [6]. -
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. -
Generalized Quaternions
GENERALIZED QUATERNIONS KEITH CONRAD 1. introduction The quaternion group Q8 is one of the two non-abelian groups of size 8 (up to isomor- phism). The other one, D4, can be constructed as a semi-direct product: ∼ ∼ × ∼ D4 = Aff(Z=(4)) = Z=(4) o (Z=(4)) = Z=(4) o Z=(2); where the elements of Z=(2) act on Z=(4) as the identity and negation. While Q8 is not a semi-direct product, it can be constructed as the quotient group of a semi-direct product. We will see how this is done in Section2 and then jazz up the construction in Section3 to make an infinite family of similar groups with Q8 as the simplest member. In Section4 we will compare this family with the dihedral groups and see how it fits into a bigger picture. 2. The quaternion group from a semi-direct product The group Q8 is built out of its subgroups hii and hji with the overlapping condition i2 = j2 = −1 and the conjugacy relation jij−1 = −i = i−1. More generally, for odd a we have jaij−a = −i = i−1, while for even a we have jaij−a = i. We can combine these into the single formula a (2.1) jaij−a = i(−1) for all a 2 Z. These relations suggest the following way to construct the group Q8. Theorem 2.1. Let H = Z=(4) o Z=(4), where (a; b)(c; d) = (a + (−1)bc; b + d); ∼ The element (2; 2) in H has order 2, lies in the center, and H=h(2; 2)i = Q8. -
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. -
The Centre of a Block
THE CENTRE OF A BLOCK A thesis submitted to the University of Manchester for the degree of Doctor of Philosophy in the Faculty of Engineering and Physical Sciences 2016 Inga Schwabrow School of Mathematics 2 Contents Abstract 5 Declaration 7 Copyright Statement 9 Acknowledgements 11 Introduction 13 1 Modular Representation Theory 17 1.1 Basic notation and setup . 17 1.2 Conjugacy class sums, characters and Burnside's formula . 18 1.3 Blocks . 22 1.4 Defect and defect groups . 25 1.5 Jacobson radical and Loewy length . 28 1.6 The Reynolds ideal . 35 2 Equivalences of blocks 37 2.1 Brauer correspondence . 37 2.2 Morita equivalence . 38 2.3 Derived equivalence . 38 2.4 Stable equivalence of Morita type . 40 2.5 Properties of blocks with TI defect groups . 41 2.6 On using the centre to show no derived equivalence exists . 43 3 Blocks with trivial intersection defect groups 44 3 3.1 The Mathieu group M11 with p =3.................... 45 3.2 The McLaughlin group McL, and Aut(McL), with p = 5 . 49 3.3 The Janko group J4 with p =11...................... 52 3.4 The projective special unitary groups . 54 3.5 A question of Rickard . 60 3.6 On the existence of perfect isometries in blocks with TI defect groups . 62 4 On the Loewy length of the Suzuki groups and the small Ree groups in defining characteristic 68 4.1 Relating structure constants . 68 4.2 Suzuki Groups . 70 4.3 The Ree groups . 76 5 More sporadic simple groups 108 5.1 Mathieu groups . -
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. -
Math.AG] 17 Mar 2001 Ebro Uhafml Mle H Og Ojcuefrinfin field 5-Dimensional for Such with Identify Type Conjecture to Weil Hope Hodge We of the Algebra
QUATERNIONIC PRYMS AND HODGE CLASSES B. VAN GEEMEN AND A. VERRA Abstract. Abelian varieties of dimension 2n on which a definite quaternion algebra acts are parametrized by symmetrical domains of dimension n(n 1)/2. Such abelian varieties have primitive Hodge classes in the middle dimensional cohomolo−gy group. In general, it is not clear that these are cycle classes. In this paper we show that a particular 6-dimensional family of such 8-folds are Prym varieties and we use the method of C. Schoen to show that all Hodge classes on the general abelian variety in this family are algebraic. We also consider Hodge classes on certain 5-dimensional subfamilies and relate these to the Hodge conjecture for abelian 4-folds. In this paper we study abelian varieties of dimension 8 whose endomorphism ring is a definite quaternion algebra over Q, we refer to these as abelian 8-folds of quaternion type. Such abelian varieties are interesting since their Hodge rings are not generated by divisor classes [M] and the Hodge conjecture is still open for most of them. The moduli space of 8-folds of quaternion type, with fixed discrete data, is 6-dimensional. One such moduli space was investigated recently by Freitag and Hermann [FrHe]. In [KSTT] a 6-dimensional family of K3 surfaces is studied whose Kuga-Satake varieties have simple factors of dimension 8 which are of quaternion type. Our first result, in section 3, is that one of these moduli spaces parametrizes Prym varieties of unramified 2:1 covers C˜ Cˆ, actually the genus 17 curves C˜ are 8:1 unramified covers of genus 3 curves with Galois→ group Q generated by the quaternions i and j. -
A Note on the Quaternion Group As Galois Group
proceedings of the american mathematical society Volume 108, Number 3, March 1990 A NOTE ON THE QUATERNION GROUP AS GALOIS GROUP ROGER WARE (Communicated by Louis J. Ratliff, Jr.) Abstract. The occurrence of the quaternion group as a Galois group over cer- tain fields is investigated. A theorem of Witt on quaternionic Galois extensions plays a key role. In [9, §6] Witt proved a theorem characterizing quaternionic Galois exten- sions. Namely, he showed that if F is a field of characteristic not 2 then an extension L = F(y/ä,y/b), a,b e F, of degree 4 over F can be embedded in a Galois extension A" of 7 with Gal(K/F) = 77g (the quaternion group 7 7 7 of order 8) if and only if the quadratic form ax + by + abz is isomorphic to x 2 + y 2 + z 2 .In addition he showed how to explicitly construct the Galois extension from the isometry. An immediate and interesting consequence of this is the fact that 77g cannot be a Galois group over any Pythagorean field. In this note Witt's theorem is used to obtain additional results about the existence of 77g as a Galois group over certain fields. If 7 is a field (of char- acteristic not 2) with at most one (total) ordering such that 77g does not oc- cur as a Galois group over F then the structure of the pro-2-Galois groups GF(2) = Gal(7(2)/7), Gpy = Gal(7py/7) (where 7(2) and Fpy are the quadratic and Pythagorean closures of F) are completely determined. -
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.