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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. -
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. -
Sporadic Sics and Exceptional Lie Algebras
Sporadic SICs and Exceptional Lie Algebras Blake C. Staceyy yQBism Group, Physics Department, University of Massachusetts Boston, 100 Morrissey Boulevard, Boston MA 02125, USA November 13, 2019 Abstract Sometimes, mathematical oddities crowd in upon one another, and the exceptions to one classification scheme reveal themselves as fellow-travelers with the exceptions to a quite different taxonomy. 1 Preliminaries A set of equiangular lines is a set of unit vectors in a d-dimensional vector space such that the magnitude of the inner product of any pair is constant: 1; j = k; jhv ; v ij = (1) j k α; j 6= k: The maximum number of equiangular lines in a space of dimension d (the so-called Gerzon bound) is d(d+1)=2 for real vector spaces and d2 for complex. In the real case, the Gerzon bound is only known to be attained in dimensions 2, 3, 7 and 23, and we know it can't be attained in general. If you like peculiar alignments of mathematical topics, the appearance of 7 and 23 might make your ears prick up here. If you made the wild guess that the octonions and the Leech lattice are just around the corner. you'd be absolutely right. Meanwhile, the complex case is of interest for quantum information theory, because a set of d2 equiangular lines in Cd specifies a measurement that can be performed upon a quantum-mechanical system. These measurements are highly symmetric, in that the lines which specify them are equiangular, and they are \informationally complete" in a sense that quantum theory makes precise. -
12.6 Further Topics on Simple Groups 387 12.6 Further Topics on Simple Groups
12.6 Further Topics on Simple groups 387 12.6 Further Topics on Simple Groups This Web Section has three parts (a), (b) and (c). Part (a) gives a brief descriptions of the 56 (isomorphism classes of) simple groups of order less than 106, part (b) provides a second proof of the simplicity of the linear groups Ln(q), and part (c) discusses an ingenious method for constructing a version of the Steiner system S(5, 6, 12) from which several versions of S(4, 5, 11), the system for M11, can be computed. 12.6(a) Simple Groups of Order less than 106 The table below and the notes on the following five pages lists the basic facts concerning the non-Abelian simple groups of order less than 106. Further details are given in the Atlas (1985), note that some of the most interesting and important groups, for example the Mathieu group M24, have orders in excess of 108 and in many cases considerably more. Simple Order Prime Schur Outer Min Simple Order Prime Schur Outer Min group factor multi. auto. simple or group factor multi. auto. simple or count group group N-group count group group N-group ? A5 60 4 C2 C2 m-s L2(73) 194472 7 C2 C2 m-s ? 2 A6 360 6 C6 C2 N-g L2(79) 246480 8 C2 C2 N-g A7 2520 7 C6 C2 N-g L2(64) 262080 11 hei C6 N-g ? A8 20160 10 C2 C2 - L2(81) 265680 10 C2 C2 × C4 N-g A9 181440 12 C2 C2 - L2(83) 285852 6 C2 C2 m-s ? L2(4) 60 4 C2 C2 m-s L2(89) 352440 8 C2 C2 N-g ? L2(5) 60 4 C2 C2 m-s L2(97) 456288 9 C2 C2 m-s ? L2(7) 168 5 C2 C2 m-s L2(101) 515100 7 C2 C2 N-g ? 2 L2(9) 360 6 C6 C2 N-g L2(103) 546312 7 C2 C2 m-s L2(8) 504 6 C2 C3 m-s -
A Natural Representation of the Fischer-Griess Monster
Proc. Nati. Acad. Sci. USA Vol. 81, pp. 3256-3260, May 1984 Mathematics A natural representation of the Fischer-Griess Monster with the modular function J as character (vertex operators/finite simple group Fl/Monstrous Moonshine/affine Lie algebras/basic modules) I. B. FRENKEL*t, J. LEPOWSKY*t, AND A. MEURMANt *Department of Mathematics, Rutgers University, New Brunswick, NJ 08903; and tMathematical Sciences Research Institute, Berkeley, CA 94720 Communicated by G. D. Mostow, February 3, 1984 ABSTRACT We announce the construction of an irreduc- strange discoveries could make sense. However, instead of ible graded module V for an "affine" commutative nonassocia- illuminating the mysteries, he added a new one, by con- tive algebra S. This algebra is an "affinization" of a slight structing a peculiar commutative nonassociative algebra B variant R of the conMnutative nonassociative algebra B de- and proving directly that its automorphism group contains fined by Griess in his construction of the Monster sporadic F1. group F1. The character of V is given by the modular function The present work started as an attempt to explain the ap- J(q) _ q' + 0 + 196884q + .... We obtain a natural action of pearance of J(q) as well as the structure of B. Our under- the Monster on V compatible with the action of R, thus con- standing of these phenomena has now led us to conceptual ceptually explaining a major part of the numerical observa- constructions of several objects: V; a variant a of B; an "af- tions known as Monstrous Moonshine. Our construction starts finization" 9a of@a; and F1, which appears as a group of oper- from ideas in the theory of the basic representations of affine ators on V and at the sajne time as a group of algebra auto- Lie algebras and develops further the cadculus of vertex opera- morphisms of R and of 9a. -
Arxiv:1911.10534V3 [Math.AT] 17 Apr 2020 Statement
THE ANDO-HOPKINS-REZK ORIENTATION IS SURJECTIVE SANATH DEVALAPURKAR Abstract. We show that the map π∗MString ! π∗tmf induced by the Ando-Hopkins-Rezk orientation is surjective. This proves an unpublished claim of Hopkins and Mahowald. We do so by constructing an E1-ring B and a map B ! MString such that the composite B ! MString ! tmf is surjective on homotopy. Applications to differential topology, and in particular to Hirzebruch's prize question, are discussed. 1. Introduction The goal of this paper is to show the following result. Theorem 1.1. The map π∗MString ! π∗tmf induced by the Ando-Hopkins-Rezk orientation is surjective. This integral result was originally stated as [Hop02, Theorem 6.25], but, to the best of our knowledge, no proof has appeared in the literature. In [HM02], Hopkins and Mahowald give a proof sketch of Theorem 1.1 for elements of π∗tmf of Adams-Novikov filtration 0. The analogue of Theorem 1.1 for bo (namely, the statement that the map π∗MSpin ! π∗bo induced by the Atiyah-Bott-Shapiro orientation is surjective) is classical [Mil63]. In Section2, we present (as a warmup) a proof of this surjectivity result for bo via a technique which generalizes to prove Theorem 1.1. We construct an E1-ring A with an E1-map A ! MSpin. The E1-ring A is a particular E1-Thom spectrum whose mod 2 homology is given by the polynomial subalgebra 4 F2[ζ1 ] of the mod 2 dual Steenrod algebra. The Atiyah-Bott-Shapiro orientation MSpin ! bo is an E1-map, and so the composite A ! MSpin ! bo is an E1-map. -
Our Mathematical Universe: I. How the Monster Group Dictates All of Physics
October, 2011 PROGRESS IN PHYSICS Volume 4 Our Mathematical Universe: I. How the Monster Group Dictates All of Physics Franklin Potter Sciencegems.com, 8642 Marvale Drive, Huntington Beach, CA 92646. E-mail: [email protected] A 4th family b’ quark would confirm that our physical Universe is mathematical and is discrete at the Planck scale. I explain how the Fischer-Greiss Monster Group dic- tates the Standard Model of leptons and quarks in discrete 4-D internal symmetry space and, combined with discrete 4-D spacetime, uniquely produces the finite group Weyl E8 x Weyl E8 = “Weyl” SO(9,1). The Monster’s j-invariant function determines mass ratios of the particles in finite binary rotational subgroups of the Standard Model gauge group, dictates Mobius¨ transformations that lead to the conservation laws, and connects interactions to triality, the Leech lattice, and Golay-24 information coding. 1 Introduction 5. Both 4-D spacetime and 4-D internal symmetry space are discrete at the Planck scale, and both spaces can The ultimate idea that our physical Universe is mathematical be telescoped upwards mathematically by icosians to at the fundamental scale has been conjectured for many cen- 8-D spaces that uniquely combine into 10-D discrete turies. In the past, our marginal understanding of the origin spacetime with discrete Weyl E x Weyl E symmetry of the physical rules of the Universe has been peppered with 8 8 (not the E x E Lie group of superstrings/M-theory). huge gaps, but today our increased understanding of funda- 8 8 mental particles promises to eliminate most of those gaps to 6. -
The Mathieu Groups (Simple Sporadic Symmetries)
The Mathieu Groups (Simple Sporadic Symmetries) Scott Harper (University of St Andrews) Tomorrow's Mathematicians Today 21st February 2015 Scott Harper The Mathieu Groups 21st February 2015 1 / 15 The Mathieu Groups (Simple Sporadic Symmetries) Scott Harper (University of St Andrews) Tomorrow's Mathematicians Today 21st February 2015 Scott Harper The Mathieu Groups 21st February 2015 2 / 15 1 2 A symmetry is a structure preserving permutation of the underlying set. A group acts faithfully on an object if it is isomorphic to a subgroup of the 4 3 symmetry group of the object. Symmetry group: D4 The stabiliser of a point in a group G is Group of rotations: the subgroup of G which fixes x. ∼ h(1 2 3 4)i = C4 Subgroup fixing 1: h(2 4)i Symmetry Scott Harper The Mathieu Groups 21st February 2015 3 / 15 A symmetry is a structure preserving permutation of the underlying set. A group acts faithfully on an object if it is isomorphic to a subgroup of the symmetry group of the object. The stabiliser of a point in a group G is Group of rotations: the subgroup of G which fixes x. ∼ h(1 2 3 4)i = C4 Subgroup fixing 1: h(2 4)i Symmetry 1 2 4 3 Symmetry group: D4 Scott Harper The Mathieu Groups 21st February 2015 3 / 15 A group acts faithfully on an object if it is isomorphic to a subgroup of the symmetry group of the object. The stabiliser of a point in a group G is Group of rotations: the subgroup of G which fixes x. -
Braids, 3-Manifolds, Elementary Particles: Number Theory and Symmetry in Particle Physics
S S symmetry Article Braids, 3-Manifolds, Elementary Particles: Number Theory and Symmetry in Particle Physics Torsten Asselmeyer-Maluga German Aeorspace Center, Rosa-Luxemburg-Str. 2, 10178 Berlin, Germany; [email protected]; Tel.: +49-30-67055-725 Received: 25 July 2019; Accepted: 2 October 2019; Published: 15 October 2019 Abstract: In this paper, we will describe a topological model for elementary particles based on 3-manifolds. Here, we will use Thurston’s geometrization theorem to get a simple picture: fermions as hyperbolic knot complements (a complement C(K) = S3 n (K × D2) of a knot K carrying a hyperbolic geometry) and bosons as torus bundles. In particular, hyperbolic 3-manifolds have a close connection to number theory (Bloch group, algebraic K-theory, quaternionic trace fields), which will be used in the description of fermions. Here, we choose the description of 3-manifolds by branched covers. Every 3-manifold can be described by a 3-fold branched cover of S3 branched along a knot. In case of knot complements, one will obtain a 3-fold branched cover of the 3-disk D3 branched along a 3-braid or 3-braids describing fermions. The whole approach will uncover new symmetries as induced by quantum and discrete groups. Using the Drinfeld–Turaev quantization, we will also construct a quantization so that quantum states correspond to knots. Particle properties like the electric charge must be expressed by topology, and we will obtain the right spectrum of possible values. Finally, we will get a connection to recent models of Furey, Stoica and Gresnigt using octonionic and quaternionic algebras with relations to 3-braids (Bilson–Thompson model). -
Arxiv:1305.5974V1 [Math-Ph]
INTRODUCTION TO SPORADIC GROUPS for physicists Luis J. Boya∗ Departamento de F´ısica Te´orica Universidad de Zaragoza E-50009 Zaragoza, SPAIN MSC: 20D08, 20D05, 11F22 PACS numbers: 02.20.a, 02.20.Bb, 11.24.Yb Key words: Finite simple groups, sporadic groups, the Monster group. Juan SANCHO GUIMERA´ In Memoriam Abstract We describe the collection of finite simple groups, with a view on physical applications. We recall first the prime cyclic groups Zp, and the alternating groups Altn>4. After a quick revision of finite fields Fq, q = pf , with p prime, we consider the 16 families of finite simple groups of Lie type. There are also 26 extra “sporadic” groups, which gather in three interconnected “generations” (with 5+7+8 groups) plus the Pariah groups (6). We point out a couple of physical applications, in- cluding constructing the biggest sporadic group, the “Monster” group, with close to 1054 elements from arguments of physics, and also the relation of some Mathieu groups with compactification in string and M-theory. ∗[email protected] arXiv:1305.5974v1 [math-ph] 25 May 2013 1 Contents 1 Introduction 3 1.1 Generaldescriptionofthework . 3 1.2 Initialmathematics............................ 7 2 Generalities about groups 14 2.1 Elementarynotions............................ 14 2.2 Theframeworkorbox .......................... 16 2.3 Subgroups................................. 18 2.4 Morphisms ................................ 22 2.5 Extensions................................. 23 2.6 Familiesoffinitegroups ......................... 24 2.7 Abeliangroups .............................. 27 2.8 Symmetricgroup ............................. 28 3 More advanced group theory 30 3.1 Groupsoperationginspaces. 30 3.2 Representations.............................. 32 3.3 Characters.Fourierseries . 35 3.4 Homological algebra and extension theory . 37 3.5 Groupsuptoorder16.......................... -
Finite Groups Whose Element Orders Are Consecutive Integers
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Elsevier - Publisher Connector JOURNAL OF ALGEBRA 143, 388X)0 (1991) Finite Groups Whose Element Orders Are Consecutive Integers ROLF BRANDL Mathematisches Institui, Am Hubland 12, D-W-8700 Wiirzberg, Germany AND SHI WUJIE Mathematics Department, Southwest-China Teachers University, Chongqing, China Communicated by G. Glauberman Received February 28, 1986 DEDICATED TO PROFESSORB. H. NEUMANN ON HIS 80~~ BIRTHDAY There are various characterizations of groups by conditions on the orders of its elements. For example, in [ 8, 1] the finite groups all of whose elements have prime power order have been classified. In [2, 16-181 some simple groups have been characterized by conditions on the orders of its elements and B. H. Neumann [12] has determined all groups whose elements have orders 1, 2, and 3. The latter groups are OC3 groups in the sense of the following. DEFINITION. Let n be a positive integer. Then a group G is an OC, group if every element of G has order <n and for each m <n there exists an element of G having order m. In this paper we give a complete classification of finite OC, groups. The notation is standard; see [S, 111. In addition, for a prime q, a Sylow q-sub- group of the group G is denoted by P,. Moreover Z{ stands for the direct product of j copies of Zj and G = [N] Q denotes the split extension of a normal subgroup N of G by a complement Q. -
§2. Elliptic Curves: J-Invariant (Jan 31, Feb 4,7,9,11,14) After
24 JENIA TEVELEV §2. Elliptic curves: j-invariant (Jan 31, Feb 4,7,9,11,14) After the projective line P1, the easiest algebraic curve to understand is an elliptic curve (Riemann surface of genus 1). Let M = isom. classes of elliptic curves . 1 { } We are going to assign to each elliptic curve a number, called its j-invariant and prove that 1 M1 = Aj . 1 1 So as a space M1 A is not very interesting. However, understanding A ! as a moduli space of elliptic curves leads to some breath-taking mathemat- ics. More generally, we introduce M = isom. classes of smooth projective curves of genus g g { } and M = isom. classes of curves C of genus g with points p , . , p C . g,n { 1 n ∈ } We will return to these moduli spaces later in the course. But first let us recall some basic facts about algebraic curves = compact Riemann surfaces. We refer to [G] and [Mi] for a rigorous and detailed exposition. §2.1. Algebraic functions, algebraic curves, and Riemann surfaces. The theory of algebraic curves has roots in analysis of Abelian integrals. An easiest example is the elliptic integral: in 1655 Wallis began to study the arc length of an ellipse (X/a)2 + (Y/b)2 = 1. The equation for the ellipse can be solved for Y : Y = (b/a) (a2 X2), − and this can easily be differentiated !to find bX Y ! = − . a√a2 X2 − 2 This is squared and put into the integral 1 + (Y !) dX for the arc length. Now the substitution x = X/a results in " ! 1 e2x2 s = a − dx, 1 x2 # $ − between the limits 0 and X/a, where e = 1 (b/a)2 is the eccentricity.