Sporadic Groups and Where to Find Them
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Discussion on Some Properties of an Infinite Non-Abelian Group
International Journal of Mathematics Trends and Technology (IJMTT) – Volume 48 Number 2 August 2017 Discussion on Some Then A.B = Properties of an Infinite Non-abelian = Group Where = Ankur Bala#1, Madhuri Kohli#2 #1 M.Sc. , Department of Mathematics, University of Delhi, Delhi #2 M.Sc., Department of Mathematics, University of Delhi, Delhi ( 1 ) India Abstract: In this Article, we have discussed some of the properties of the infinite non-abelian group of matrices whose entries from integers with non-zero determinant. Such as the number of elements of order 2, number of subgroups of order 2 in this group. Moreover for every finite group , there exists such that has a subgroup isomorphic to the group . ( 2 ) Keywords: Infinite non-abelian group, Now from (1) and (2) one can easily say that is Notations: GL(,) n Z []aij n n : aij Z. & homomorphism. det( ) = 1 Now consider , Theorem 1: can be embedded in Clearly Proof: If we prove this theorem for , Hence is injective homomorphism. then we are done. So, by fundamental theorem of isomorphism one can Let us define a mapping easily conclude that can be embedded in for all m . Such that Theorem 2: is non-abelian infinite group Proof: Consider Consider Let A = and And let H= Clearly H is subset of . And H has infinite elements. B= Hence is infinite group. Now consider two matrices Such that determinant of A and B is , where . And ISSN: 2231-5373 http://www.ijmttjournal.org Page 108 International Journal of Mathematics Trends and Technology (IJMTT) – Volume 48 Number 2 August 2017 Proof: Let G be any group and A(G) be the group of all permutations of set G. -
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. -
Group Theory in Particle Physics
Group Theory in Particle Physics Joshua Albert Phy 205 http://en.wikipedia.org/wiki/Image:E8_graph.svg Where Did it Come From? Group Theory has it©s origins in: ● Algebraic Equations ● Number Theory ● Geometry Some major early contributers were Euler, Gauss, Lagrange, Abel, and Galois. What is a group? ● A group is a collection of objects with an associated operation. ● The group can be finite or infinite (based on the number of elements in the group. ● The following four conditions must be satisfied for the set of objects to be a group... 1: Closure ● The group operation must associate any pair of elements T and T© in group G with another element T©© in G. This operation is the group multiplication operation, and so we write: – T T© = T©© – T, T©, T©© all in G. ● Essentially, the product of any two group elements is another group element. 2: Associativity ● For any T, T©, T©© all in G, we must have: – (T T©) T©© = T (T© T©©) ● Note that this does not imply: – T T© = T© T – That is commutativity, which is not a fundamental group property 3: Existence of Identity ● There must exist an identity element I in a group G such that: – T I = I T = T ● For every T in G. 4: Existence of Inverse ● For every element T in G there must exist an inverse element T -1 such that: – T T -1 = T -1 T = I ● These four properties can be satisfied by many types of objects, so let©s go through some examples... Some Finite Group Examples: ● Parity – Representable by {1, -1}, {+,-}, {even, odd} – Clearly an important group in particle physics ● Rotations of an Equilateral Triangle – Representable as ordering of vertices: {ABC, ACB, BAC, BCA, CAB, CBA} – Can also be broken down into subgroups: proper rotations and improper rotations ● The Identity alone (smallest possible group). -
Group Theory
Appendix A Group Theory This appendix is a survey of only those topics in group theory that are needed to understand the composition of symmetry transformations and its consequences for fundamental physics. It is intended to be self-contained and covers those topics that are needed to follow the main text. Although in the end this appendix became quite long, a thorough understanding of group theory is possible only by consulting the appropriate literature in addition to this appendix. In order that this book not become too lengthy, proofs of theorems were largely omitted; again I refer to other monographs. From its very title, the book by H. Georgi [211] is the most appropriate if particle physics is the primary focus of interest. The book by G. Costa and G. Fogli [102] is written in the same spirit. Both books also cover the necessary group theory for grand unification ideas. A very comprehensive but also rather dense treatment is given by [428]. Still a classic is [254]; it contains more about the treatment of dynamical symmetries in quantum mechanics. A.1 Basics A.1.1 Definitions: Algebraic Structures From the structureless notion of a set, one can successively generate more and more algebraic structures. Those that play a prominent role in physics are defined in the following. Group A group G is a set with elements gi and an operation ◦ (called group multiplication) with the properties that (i) the operation is closed: gi ◦ g j ∈ G, (ii) a neutral element g0 ∈ G exists such that gi ◦ g0 = g0 ◦ gi = gi , (iii) for every gi exists an −1 ∈ ◦ −1 = = −1 ◦ inverse element gi G such that gi gi g0 gi gi , (iv) the operation is associative: gi ◦ (g j ◦ gk) = (gi ◦ g j ) ◦ gk. -
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. -
Verification of Dade's Conjecture for Janko Group J3
JOURNAL OF ALGEBRA 187, 579]619Ž. 1997 ARTICLE NO. JA966836 Verification of Dade's Conjecture for Janko Group J3 Sonja KotlicaU Department of Mathematics, Uni¨ersity of Illinois at Urbana-Champaign, 1409 West Green Street, Urbana, Illinois 61801 View metadata, citation and similar papersCommunicated at core.ac.uk by Walter Feit brought to you by CORE provided by Elsevier - Publisher Connector Received July 5, 1996 Inwx 3 Dade made a conjecture expressing the number kBŽ.,d of characters of a given defect d in a given p-block B of a finite group G in terms of the corresponding numbers kbŽ.,d for blocks b of certain p-local subgroups of G. Several different forms of this conjecture are given inwx 5 . Dade claims that the most complicated form of this conjecture, called the ``Inductive Conjecture 5.8'' inwx 5 , will hold for all finite groups if it holds for all covering groups of finite simple groups. In this paper we verify the inductive conjecture for all covering groups of the third Janko group J3 Žin the notation of the Atlaswx 1. This is one step in the inductive proof of the conjecture for all finite groups. Certain properties of J33simplify our task. The Schur Multiplier of J is cyclic of order 3Ž seewx 1, p. 82. Hence, there are just two covering groups of J33, namely J itself and a central extension 3 ? J33of J by a cyclic group Z of order 3. We treat these two covering groups separately. The outer automorphism group OutŽ.J33of J is cyclic of order 2 Ž seewx 1, p. -
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. -
Crystal Symmetry Groups
X-Ray and Neutron Crystallography rational numbers is a group under Crystal Symmetry Groups multiplication, and both it and the integer group already discussed are examples of infinite groups because they each contain an infinite number of elements. ymmetry plays an important role between the integers obey the rules of In the case of a symmetry group, in crystallography. The ways in group theory: an element is the operation needed to which atoms and molecules are ● There must be defined a procedure for produce one object from another. For arrangeds within a unit cell and unit cells example, a mirror operation takes an combining two elements of the group repeat within a crystal are governed by to form a third. For the integers one object in one location and produces symmetry rules. In ordinary life our can choose the addition operation so another of the opposite hand located first perception of symmetry is what that a + b = c is the operation to be such that the mirror doing the operation is known as mirror symmetry. Our performed and u, b, and c are always is equidistant between them (Fig. 1). bodies have, to a good approximation, elements of the group. These manipulations are usually called mirror symmetry in which our right side ● There exists an element of the group, symmetry operations. They are com- is matched by our left as if a mirror called the identity element and de- bined by applying them to an object se- passed along the central axis of our noted f, that combines with any other bodies. -
Symmetric Generation and Existence of J3:2, the Automorphism Group of the Third Janko Group
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Elsevier - Publisher Connector Journal of Algebra 304 (2006) 256–270 www.elsevier.com/locate/jalgebra Symmetric generation and existence of J3:2, the automorphism group of the third Janko group J.D. Bradley, R.T. Curtis ∗ School of Mathematics, University of Birmingham, Edgbaston, Birmingham B15 2TT, UK Received 27 June 2005 Available online 28 February 2006 Communicated by Jan Saxl Abstract We make use of the primitive permutation action of degree 120 of the automorphism group of L2(16), the special linear group of degree 2 over the field of order 16, to give an elementary definition of the automorphism group of the third Janko group J3 and to prove its existence. This definition enables us to construct the 6156-point graph which is preserved by J3:2, to obtain the order of J3 and to prove its simplicity. A presentation for J3:2 follows from our definition, which also provides a concise notation for the elements of the group. We use this notation to give a representative of each of the conjugacy classes of J3:2. © 2006 Elsevier Inc. All rights reserved. 1. Introduction The group J3 was predicted by Janko in a paper in 1968 [10]. He considered a finite simple group with a single class of involutions in which the centraliser of an involution 1+4 was isomorphic to 2 :A5. The following year Higman and McKay, using an observation of Thompson that J3 must contain a subgroup isomorphic to L2(16):2, constructed the group on a computer [9]. -
Expansion in Finite Simple Groups of Lie Type
Expansion in finite simple groups of Lie type Terence Tao Department of Mathematics, UCLA, Los Angeles, CA 90095 E-mail address: [email protected] In memory of Garth Gaudry, who set me on the road Contents Preface ix Notation x Acknowledgments xi Chapter 1. Expansion in Cayley graphs 1 x1.1. Expander graphs: basic theory 2 x1.2. Expansion in Cayley graphs, and Kazhdan's property (T) 20 x1.3. Quasirandom groups 54 x1.4. The Balog-Szemer´edi-Gowers lemma, and the Bourgain- Gamburd expansion machine 81 x1.5. Product theorems, pivot arguments, and the Larsen-Pink non-concentration inequality 94 x1.6. Non-concentration in subgroups 127 x1.7. Sieving and expanders 135 Chapter 2. Related articles 157 x2.1. Cayley graphs and the algebra of groups 158 x2.2. The Lang-Weil bound 177 x2.3. The spectral theorem and its converses for unbounded self-adjoint operators 191 x2.4. Notes on Lie algebras 214 x2.5. Notes on groups of Lie type 252 Bibliography 277 Index 285 vii Preface Expander graphs are a remarkable type of graph (or more precisely, a family of graphs) on finite sets of vertices that manage to simultaneously be both sparse (low-degree) and \highly connected" at the same time. They enjoy very strong mixing properties: if one starts at a fixed vertex of an (two-sided) expander graph and randomly traverses its edges, then the distribution of one's location will converge exponentially fast to the uniform distribution. For this and many other reasons, expander graphs are useful in a wide variety of areas of both pure and applied mathematics. -
CHAPTER 4 Representations of Finite Groups of Lie Type Let Fq Be a Finite
CHAPTER 4 Representations of finite groups of Lie type Let Fq be a finite field of order q and characteristic p. Let G be a finite group of Lie type, that is, G is the Fq-rational points of a connected reductive group G defined over Fq. For example, if n is a positive integer GLn(Fq) and SLn(Fq) are finite groups of Lie type. 0 In Let J = , where In is the n × n identity matrix. Let −In 0 t Sp2n(Fq) = { g ∈ GL2n(Fq) | gJg = J }. Then Sp2n(Fq) is a symplectic group of rank n and is a finite group of Lie type. For G = GLn(Fq) or SLn(Fq) (and some other examples), the standard Borel subgroup B of G is the subgroup of G consisting of the upper triangular elements in G.A standard parabolic subgroup of G is a subgroup of G which contains the standard Borel subgroup B. If P is a standard parabolic subgroup of GLn(Fq), then there exists a partition (n1, . , nr) of n (a set of positive integers nj such that n1 + ··· + nr = n) such that P = P(n1,...,nr ) = M n N, where M ' GLn1 (Fq) × · · · × GLnr (Fq) has the form A 0 ··· 0 1 0 A2 ··· 0 M = | A ∈ GL ( ), 1 ≤ j ≤ r . . .. .. j nj Fq . 0 ··· 0 Ar and In1 ∗ · · · ∗ 0 In2 · · · ∗ N = , . .. .. . 0 ··· 0 Inr where ∗ denotes arbitary entries in Fq. The subgroup M is called a (standard) Levi sub- group of P , and N is called the unipotent radical of P . Note that the partition (1, 1,..., 1) corresponds to B and (n) corresponds to G.