John Conway, My Thoughts After His Passing (28 April, 2020)
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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. -
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. -
ELEMENTARY ABELIAN P-SUBGROUPS of ALGEBRAIC GROUPS
ROBERT L. GRIESS, JR ELEMENTARY ABELIAN p-SUBGROUPS OF ALGEBRAIC GROUPS Dedicated to Jacques Tits for his sixtieth birthday ABSTRACT. Let ~ be an algebraically closed field and let G be a finite-dimensional algebraic group over N which is nearly simple, i.e. the connected component of the identity G O is perfect, C6(G °) = Z(G °) and G°/Z(G °) is simple. We classify maximal elementary abelian p-subgroups of G which consist of semisimple elements, i.e. for all primes p ~ char K. Call a group quasisimple if it is perfect and is simple modulo the center. Call a subset of an algebraic group total if it is in a toms; otherwise nontoral. For several quasisimple algebraic groups and p = 2, we define complexity, and give local criteria for whether an elementary abelian 2-subgroup of G is total. For all primes, we analyze the nontoral examples, include a classification of all the maximal elementary abelian p-groups, many of the nonmaximal ones, discuss their normalizers and fusion (i.e. how conjugacy classes of the ambient algebraic group meet the subgroup). For some cases, we give a very detailed discussion, e.g. p = 3 and G of type E6, E 7 and E 8. We explain how the presence of spin up and spin down elements influences the structure of projectively elementary abelian 2-groups in Spin(2n, C). Examples of an elementary abelian group which is nontoral in one algebraic group but toral in a larger one are noted. Two subsets of a maximal torus are conjugate in G iff they are conjugate in the normalizer of the torus; this observation, with our discussion of the nontoral cases, gives a detailed guide to the possibilities for the embedding of an elementary abelian p-group in G. -
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. -
Sphere Packing, Lattice Packing, and Related Problems
Sphere packing, lattice packing, and related problems Abhinav Kumar Stony Brook April 25, 2018 Sphere packings Definition n A sphere packing in R is a collection of spheres/balls of equal size which do not overlap (except for touching). The density of a sphere packing is the volume fraction of space occupied by the balls. ~ ~ ~ ~ ~ ~ ~ ~ ~ ~ ~ ~ ~ In dimension 1, we can achieve density 1 by laying intervals end to end. In dimension 2, the best possible is by using the hexagonal lattice. [Fejes T´oth1940] Sphere packing problem n Problem: Find a/the densest sphere packing(s) in R . In dimension 2, the best possible is by using the hexagonal lattice. [Fejes T´oth1940] Sphere packing problem n Problem: Find a/the densest sphere packing(s) in R . In dimension 1, we can achieve density 1 by laying intervals end to end. Sphere packing problem n Problem: Find a/the densest sphere packing(s) in R . In dimension 1, we can achieve density 1 by laying intervals end to end. In dimension 2, the best possible is by using the hexagonal lattice. [Fejes T´oth1940] Sphere packing problem II In dimension 3, the best possible way is to stack layers of the solution in 2 dimensions. This is Kepler's conjecture, now a theorem of Hales and collaborators. mmm m mmm m There are infinitely (in fact, uncountably) many ways of doing this! These are the Barlow packings. Face centered cubic packing Image: Greg A L (Wikipedia), CC BY-SA 3.0 license But (until very recently!) no proofs. In very high dimensions (say ≥ 1000) densest packings are likely to be close to disordered. -
ORBITS in the LEECH LATTICE 1. Introduction the Leech Lattice Λ Is a Lattice in 24-Dimensional Euclidean Space with Many Remark
ORBITS IN THE LEECH LATTICE DANIEL ALLCOCK Abstract. We provide an algorithm for determining whether two vectors in the Leech lattice are equivalent under its isometry group, 18 the Conway group Co 0 of order 8 10 . Our methods rely on and develop the work of R. T.∼ Curtis,× and we describe our in- tended applications to the symmetry groups of Lorentzian lattices and the enumeration of lattices of dimension 24 with good prop- erties such as having small determinant. Our≈ algorithm reduces 12 the test of equivalence to 4 tests under the subgroup 2 :M24, ≤ and a test under this subgroup to 12 tests under M24. We also give algorithms for testing equivalence≤ under these two subgroups. Finally, we analyze the performance of the algorithm. 1. Introduction The Leech lattice Λ is a lattice in 24-dimensional Euclidean space with many remarkable properties, for us the most important of which is that its isometry group (modulo I ) is one of the sporadic finite {± } simple groups. The isometry group is called the Conway group Co 0, and our purpose is to present an algorithm for a computer to determine whether two given vectors of Λ are equivalent under Co 0. The group is fairly large, or order > 8 1018, so the obvious try-every-isometry algorithm is useless. Instead,× we use the geometry of Λ to build a faster algorithm; along the way we build algorithms for the problem 24 12 of equivalence of vectors in R under the subgroups 2 :M24 and M24, where M24 is the Mathieu group permuting the 24 coordinates. -
Optimality and Uniqueness of the Leech Lattice Among Lattices
ANNALS OF MATHEMATICS Optimality and uniqueness of the Leech lattice among lattices By Henry Cohn and Abhinav Kumar SECOND SERIES, VOL. 170, NO. 3 November, 2009 anmaah Annals of Mathematics, 170 (2009), 1003–1050 Optimality and uniqueness of the Leech lattice among lattices By HENRY COHN and ABHINAV KUMAR Dedicated to Oded Schramm (10 December 1961 – 1 September 2008) Abstract We prove that the Leech lattice is the unique densest lattice in R24. The proof combines human reasoning with computer verification of the properties of certain explicit polynomials. We furthermore prove that no sphere packing in R24 can 30 exceed the Leech lattice’s density by a factor of more than 1 1:65 10 , and we 8 C give a new proof that E8 is the unique densest lattice in R . 1. Introduction It is a long-standing open problem in geometry and number theory to find the densest lattice in Rn. Recall that a lattice ƒ Rn is a discrete subgroup of rank n; a minimal vector in ƒ is a nonzero vector of minimal length. Let ƒ vol.Rn=ƒ/ j j D denote the covolume of ƒ, i.e., the volume of a fundamental parallelotope or the absolute value of the determinant of a basis of ƒ. If r is the minimal vector length of ƒ, then spheres of radius r=2 centered at the points of ƒ do not overlap except tangentially. This construction yields a sphere packing of density n=2 r Án 1 ; .n=2/Š 2 ƒ j j since the volume of a unit ball in Rn is n=2=.n=2/Š, where for odd n we define .n=2/Š .n=2 1/. -
Octonions and the Leech Lattice
Octonions and the Leech lattice Robert A. Wilson School of Mathematical Sciences, Queen Mary, University of London, Mile End Road, London E1 4NS 18th December 2008 Abstract We give a new, elementary, description of the Leech lattice in terms of octonions, thereby providing the first real explanation of the fact that the number of minimal vectors, 196560, can be expressed in the form 3 × 240 × (1 + 16 + 16 × 16). We also give an easy proof that it is an even self-dual lattice. 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 [13, 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. Many attempts have been made in particular to find simplified constructions (see for example the 23 constructions described in [3] and the four constructions 1 described in [15]). -
A Uniform Construction of the Holomorphic Voas of Central
A Uniform Construction of the 71 Holomorphic VOAs of c = 24 from the Leech Lattice Sven Möller (joint work with Nils Scheithauer) Vertex Operator Algebras, Number Theory, and Related Topics: A Conference in Honor of Geoffrey Mason, California State University, Sacramento 12th June 2018 Schellekens’ List Orbifold Construction and Dimension Formulae A Generalised Deep-Hole Construction Contents 1 Schellekens’ List 2 Orbifold Construction and Dimension Formulae 3 A Generalised Deep-Hole Construction Sven Möller A Uniform Construction of the 71 holomorphic VOAs of c = 24 Schellekens’ List Orbifold Construction and Dimension Formulae A Generalised Deep-Hole Construction Holomorphic VOAs of Small Central Charge Proposition (Consequence of [Zhu96]) Let V be a strongly rational, holomorphic VOA. Then the central charge c of V is in 8Z≥0. + c = 8: VE8 , c = 16: V 2 , V (only lattice theories) [DM04] E8 D16 Theorem ([Sch93, DM04, EMS15]) Let V be a strongly rational, holomorphic VOA of central charge c = 24. Then the Lie algebra V1 is isomorphic to one of the 71 Lie algebras on Schellekens’ list (V \, 24 Niemeier lattice theories, etc. with chV (τ) = j(τ) − 744 + dim(V1)). c = 32: already more than 1 160 000 000 lattice theories Sven Möller A Uniform Construction of the 71 holomorphic VOAs of c = 24 Schellekens’ List Orbifold Construction and Dimension Formulae A Generalised Deep-Hole Construction Classification Orbifold constructions give all 71 cases on Schellekens’ list. [FLM88, DGM90, Don93, DGM96, Lam11, LS12, LS15, Miy13, SS16, EMS15, Mö16, LS16b, LS16a, LL16] Theorem (Classification I) There is a strongly rational, holomorphic VOA V of central charge c = 24 with Lie algebra V1 if and only if V1 is isomorphic to one of the 71 Lie algebras on Schellekens’ list. -
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).