Symmetric Presentations of Non-Abelian Simple Groups
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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. -
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. -
An Alternative Existence Proof of the Geometry of Ivanov–Shpectorov for O'nan's Sporadic Group
Innovations in Incidence Geometry Volume 15 (2017), Pages 73–121 ISSN 1781-6475 An alternative existence proof of the geometry of Ivanov–Shpectorov for O’Nan’s sporadic group Francis Buekenhout Thomas Connor In honor of J. A. Thas’s 70th birthday Abstract We provide an existence proof of the Ivanov–Shpectorov rank 5 diagram geometry together with its boolean lattice of parabolic subgroups and es- tablish the structure of hyperlines. Keywords: incidence geometry, diagram geometry, Buekenhout diagrams, O’Nan’s spo- radic group MSC 2010: 51E24, 20D08, 20B99 1 Introduction We start essentially but not exclusively from: • Leemans [26] giving the complete partially ordered set ΛO′N of conjugacy classes of subgroups of the O’Nan group O′N. This includes 581 classes and provides a structure name common for all subgroups in a given class; • the Ivanov–Shpectorov [24] rank 5 diagram geometry for the group O′N, especially its diagram ∆ as in Figure 1; ′ • the rank 3 diagram geometry ΓCo for O N due to Connor [15]; • detailed data on the diagram geometries for the groups M11 and J1 [13, 6, 27]. 74 F. Buekenhout • T. Connor 4 1 5 0 1 3 P h 1 1 1 2 Figure 1: The diagram ∆IvSh of the geometry ΓIvSh Our results are the following: • we get the Connor geometry ΓCo as a truncation of the Ivanov–Shpectorov geometry ΓIvSh (see Theorem 7.1); • using the paper of Ivanov and Shpectorov [24], we establish the full struc- ture of the boolean lattice LIvSh of their geometry as in Figure 17 (See Section 8); • conversely, within ΛO′N we prove the existence and uniqueness up to fu- ′ sion in Aut(O N) of a boolean lattice isomorphic to LIvSh. -
Infinite Groups with Large Balls of Torsion Elements and Small Entropy
INFINITE GROUPS WITH LARGE BALLS OF TORSION ELEMENTS AND SMALL ENTROPY LAURENT BARTHOLDI, YVES DE CORNULIER Abstract. We exhibit infinite, solvable, abelian-by-finite groups, with a fixed number of generators, with arbitrarily large balls consisting of torsion elements. We also provide a sequence of 3-generator non-nilpotent-by-finite polycyclic groups of algebraic entropy tending to zero. All these examples are obtained by taking ap- propriate quotients of finitely presented groups mapping onto the first Grigorchuk group. The Burnside Problem asks whether a finitely generated group all of whose ele- ments have finite order must be finite. We are interested in the following related question: fix n sufficiently large; given a group Γ, with a finite symmetric generating subset S such that every element in the n-ball is torsion, is Γ finite? Since the Burn- side problem has a negative answer, a fortiori the answer to our question is negative in general. However, it is natural to ask for it in some classes of finitely generated groups for which the Burnside Problem has a positive answer, such as linear groups or solvable groups. This motivates the following proposition, which in particularly answers a question of Breuillard to the authors. Proposition 1. For every n, there exists a group G, generated by a 3-element subset S consisting of elements of order 2, in which the n-ball consists of torsion elements, and satisfying one of the additional assumptions: (1) G is solvable, virtually abelian, and infinite (more precisely, it has a free abelian normal subgroup of finite 2-power index); in particular it is linear. -
Kernels of Linear Representations of Lie Groups, Locally Compact
Kernels of Linear Representations of Lie Groups, Locally Compact Groups, and Pro-Lie Groups Markus Stroppel Abstract For a topological group G the intersection KOR(G) of all kernels of ordinary rep- resentations is studied. We show that KOR(G) is contained in the center of G if G is a connected pro-Lie group. The class KOR(C) is determined explicitly if C is the class CONNLIE of connected Lie groups or the class ALMCONNLIE of almost con- nected Lie groups: in both cases, it consists of all compactly generated abelian Lie groups. Every compact abelian group and every connected abelian pro-Lie group occurs as KOR(G) for some connected pro-Lie group G. However, the dimension of KOR(G) is bounded by the cardinality of the continuum if G is locally compact and connected. Examples are given to show that KOR(C) becomes complicated if C contains groups with infinitely many connected components. 1 The questions we consider and the answers that we have found In the present paper we study (Hausdorff) topological groups. Ifall else fails, we endow a group with the discrete topology. For any group G one tries, traditionally, to understand the group by means of rep- resentations as groups of matrices. To this end, one studies the continuous homomor- phisms from G to GLnC for suitable positive integers n; so-called ordinary representa- tions. This approach works perfectly for finite groups because any such group has a faithful ordinary representation but we may face difficulties for infinite groups; there do exist groups admitting no ordinary representations apart from the trivial (constant) one. -
Representation Theory
M392C NOTES: REPRESENTATION THEORY ARUN DEBRAY MAY 14, 2017 These notes were taken in UT Austin's M392C (Representation Theory) class in Spring 2017, taught by Sam Gunningham. I live-TEXed them using vim, so there may be typos; please send questions, comments, complaints, and corrections to [email protected]. Thanks to Kartik Chitturi, Adrian Clough, Tom Gannon, Nathan Guermond, Sam Gunningham, Jay Hathaway, and Surya Raghavendran for correcting a few errors. Contents 1. Lie groups and smooth actions: 1/18/172 2. Representation theory of compact groups: 1/20/174 3. Operations on representations: 1/23/176 4. Complete reducibility: 1/25/178 5. Some examples: 1/27/17 10 6. Matrix coefficients and characters: 1/30/17 12 7. The Peter-Weyl theorem: 2/1/17 13 8. Character tables: 2/3/17 15 9. The character theory of SU(2): 2/6/17 17 10. Representation theory of Lie groups: 2/8/17 19 11. Lie algebras: 2/10/17 20 12. The adjoint representations: 2/13/17 22 13. Representations of Lie algebras: 2/15/17 24 14. The representation theory of sl2(C): 2/17/17 25 15. Solvable and nilpotent Lie algebras: 2/20/17 27 16. Semisimple Lie algebras: 2/22/17 29 17. Invariant bilinear forms on Lie algebras: 2/24/17 31 18. Classical Lie groups and Lie algebras: 2/27/17 32 19. Roots and root spaces: 3/1/17 34 20. Properties of roots: 3/3/17 36 21. Root systems: 3/6/17 37 22. Dynkin diagrams: 3/8/17 39 23. -
Abstract Algebra I (1St Exam) Solution 2005
Abstract Algebra I (1st exam) Solution 2005. 3. 21 1. Mark each of following true or false. Give some arguments which clarify your answer (if your answer is false, you may give a counterexample). a. (5pt) The order of any element of a ¯nite cyclic group G is a divisor of jGj. Solution.True. Let g be a generator of G and n = jGj. Then any element ge of n G has order gcd(e;n) which is a divisor of n = jGj. b. (5pt) Any non-trivial cyclic group has exactly two generators. Solution. False. For example, any nonzero element of Zp (p is a prime) is a generator. c. (5pt) If a group G is such that every proper subgroup is cyclic, then G is cyclic. Solution. False. For example, any proper subgroup of Klein 4-group V = fe; a; b; cg is cyclic, but V is not cyclic. d. (5pt) If G is an in¯nite group, then any non-trivial subgroup of G is also an in¯nite group. Solution. False. For example, hC¤; ¢i is an in¯nite group, but the subgroup n ¤ Un = fz 2 C ¤ jz = 1g is a ¯nite subgroup of C . 2. (10pt) Show that a group that has only a ¯nite number of subgroups must be a ¯nite group. Solution. We show that if any in¯nite group G has in¯nitely many subgroups. (case 1) Suppose that G is an in¯nite cyclic group with a generator g. Then the n subgroups Hn = hg i (n = 1; 2; 3;:::) are all distinct subgroups of G. -
Jhep09(2015)035
Published for SISSA by Springer Received: July 17, 2015 Accepted: August 19, 2015 Published: September 7, 2015 Higher S-dualities and Shephard-Todd groups JHEP09(2015)035 Sergio Cecottia and Michele Del Zottob aScuola Internazionale Superiore di Studi Avanzati, via Bonomea 265, 34100 Trieste, Italy bJefferson Physical Laboratory, Harvard University, Cambridge, MA 02138, U.S.A. E-mail: [email protected], [email protected] Abstract: Seiberg and Witten have shown that in = 2 SQCD with N = 2N = 4 N f c the S-duality group PSL(2, Z) acts on the flavor charges, which are weights of Spin(8), by triality. There are other = 2 SCFTs in which SU(2) SYM is coupled to strongly- N interacting non-Lagrangian matter: their matter charges are weights of E6, E7 and E8 instead of Spin(8). The S-duality group PSL(2, Z) acts on these weights: what replaces Spin(8) triality for the E6,E7,E8 root lattices? In this paper we answer the question. The action on the matter charges of (a finite central extension of) PSL(2, Z) factorizes trough the action of the exceptional Shephard- Todd groups G4 and G8 which should be seen as complex analogs of the usual triality group S Weyl(A ). Our analysis is based on the identification of S-duality for SU(2) gauge 3 ≃ 2 SCFTs with the group of automorphisms of the cluster category of weighted projective lines of tubular type. Keywords: Supersymmetry and Duality, Extended Supersymmetry, Duality in Gauge Field Theories ArXiv ePrint: 1507.01799 Open Access, c The Authors. -
Abstract the P-PERIOD of an INFINITE GROUP
Publicacions Matemátiques, Vol 36 (1992), 241-250 . THE p-PERIOD OF AN INFINITE GROUP YINING XIA Abstract For r a group of finite virtual cohomological dimension and a prime p, the p-period of r is defined to be the least positive integer d such that Farrell cohomology groups H'(F ; M) and Í3 i+d (r ; M) have naturally isomorphic p-primary componente for all integers i and Zr-modules M. We generalize a result of Swan on the p-period of a finite p-periodic group to a p-periodic infinite group, i.e ., we prove that the p-period of a p-periodic group r of finite ved is 2LCM(IN((x))1C((x))J) if the r has a finite quotient whose a p- Sylow subgroup is elementary abelian or cyclic, and the kernel is torsion free, where N(-) and C(-) denote normalizer and central- izer, (x) ranges over all conjugacy classes of Z/p subgroups . We apply this result to the computation of the p-period of a p-periodic mapping clase group. Also, we give an example to illustrate this formula is false without our assumption . For F a group of virtual finite cohomological dimension (vcd) and a prime p, the p-period of F is defined to be the least positive integer d ; such that the Farrell cohomology groups H'(F; M) and Hi+d(F M) have natually isomorphic p-primary components for all i E Z and ZF-modules M [3] . The following classical result for a finite group G was showed by Swan in 1960 [9] . -
Product of the Symmetric Group with the Alternating Group on Seven Letters
Quasigroups and Related Systems 9 (2002), 33 ¡ 44 Product of the symmetric group with the alternating group on seven letters Mohammad R. Darafsheh Abstract We will nd the structure of groups G = AB where A and B are subgroups of G with A isomorphic to the alternating group on 7 letters and B isomorphic to the symmetric group on n > 5 letters. 1. Introduction If A and B are subgroups of the group G and G = AB, then G is called a factorizable group and A and B are called factors of the factorization. We also say that G is the product of its subgroups A and B. If any of A or B is a non-proper subgroup of G, then G = AB is called a trivial factorization of G, and by a non-trivial or a proper factorization we mean G = AB with both A and B are proper subgroups of G. It is an interesting problem to know the groups with proper factorization. Of course not every group has a proper factorization, for example an innite group with all proper subgroups nite has no proper factorization, also the Janko simple group J1 of order 175 560 has no proper factorization. In what follows G is assumed to be a nite group. Now we recall some research papers towards the problem of factorization of groups under additional conditions on A and B. In [8] factorization of the simple group L2(q) are obtained and in [1] simple groups G with proper factorizations G = AB such that (jAj; jBj) = 1 are given. -
Polytopes Derived from Sporadic Simple Groups
Volume 5, Number 2, Pages 106{118 ISSN 1715-0868 POLYTOPES DERIVED FROM SPORADIC SIMPLE GROUPS MICHAEL I. HARTLEY AND ALEXANDER HULPKE Abstract. In this article, certain of the sporadic simple groups are analysed, and the polytopes having these groups as automorphism groups are characterised. The sporadic groups considered include all with or- der less than 4030387201, that is, all up to and including the order of the Held group. Four of these simple groups yield no polytopes, and the highest ranked polytopes are four rank 5 polytopes each from the Higman-Sims group, and the Mathieu group M24. 1. Introduction The finite simple groups are the building blocks of finite group theory. Most fall into a few infinite families of groups, but there are 26 (or 27 if 2 0 the Tits group F4(2) is counted also) which these infinite families do not include. These sporadic simple groups range in size from the Mathieu group 53 M11 of order 7920, to the Monster group M of order approximately 8×10 . One key to the study of these groups is identifying some geometric structure on which they act. This provides intuitive insight into the structure of the group. Abstract regular polytopes are combinatorial structures that have their roots deep in geometry, and so potentially also lend themselves to this purpose. Furthermore, if a polytope is found that has a sporadic group as its automorphism group, this gives (in theory) a presentation of the sporadic group over some generating involutions. In [6], a simple algorithm was given to find all polytopes acted on by a given abstract group.