An Algebraic Treatment of Mal'cev's Theorems Concerning
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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. -
The Frattini Module and P -Automorphisms of Free Pro-P Groups
Publ. RIMS, Kyoto Univ. (), The Frattini module and p!-automorphisms of free pro-p groups. By Darren Semmen ∗ Abstract If a non-trivial subgroup A of the group of continuous automorphisms of a non- cyclic free pro-p group F has finite order, not divisible by p, then the group of fixed points FixF (A) has infinite rank. The semi-direct product F >!A is the universal p-Frattini cover of a finite group G, and so is the projective limit of a sequence of finite groups starting with G, each a canonical group extension of its predecessor by the Frattini module. Examining appearances of the trivial simple module 1 in the Frattini module’s Jordan-H¨older series arose in investigations ([FK97], [BaFr02] and [Sem02]) of modular towers. The number of these appearances prevents FixF (A) from having finite rank. For any group A of automorphisms of a group Γ, the set of fixed points FixΓ(A) := {g ∈ Γ | α(g) = g, ∀α ∈ A} of Γ under the action of A is a subgroup of Γ. Nielsen [N21] and, for the infinite rank case, Schreier [Schr27] showed that any subgroup of a free discrete group will be free. Tate (cf. [Ser02, I.§4.2, Cor. 3a]) extended this to free pro-p groups. In light of this, it is natural to ask for a free group F , what is the rank of FixF (A)? When F is a free discrete group and A is finite, Dyer and Scott [DS75] demonstrated that FixF (A) is a free factor of F , i.e. -
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. -
A Splitting Theorem for Linear Polycyclic Groups
New York Journal of Mathematics New York J. Math. 15 (2009) 211–217. A splitting theorem for linear polycyclic groups Herbert Abels and Roger C. Alperin Abstract. We prove that an arbitrary polycyclic by finite subgroup of GL(n, Q) is up to conjugation virtually contained in a direct product of a triangular arithmetic group and a finitely generated diagonal group. Contents 1. Introduction 211 2. Restatement and proof 212 References 216 1. Introduction A linear algebraic group defined over a number field K is a subgroup G of GL(n, C),n ∈ N, which is also an affine algebraic set defined by polyno- mials with coefficients in K in the natural coordinates of GL(n, C). For a subring R of C put G(R)=GL(n, R) ∩ G.LetB(n, C)andT (n, C)bethe (Q-defined linear algebraic) subgroups of GL(n, C) of upper triangular or diagonal matrices in GL(n, C) respectively. Recall that a group Γ is called polycyclic if it has a composition series with cyclic factors. Let Q be the field of algebraic numbers in C.Every discrete solvable subgroup of GL(n, C) is polycyclic (see, e.g., [R]). 1.1. Let o denote the ring of integers in the number field K.IfH is a solvable K-defined algebraic group then H(o) is polycyclic (see [S]). Hence every subgroup of a group H(o)×Δ is polycyclic, if Δ is a finitely generated abelian group. Received November 15, 2007. Mathematics Subject Classification. 20H20, 20G20. Key words and phrases. Polycyclic group, arithmetic group, linear group. -
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. -
The Tits Alternative
The Tits Alternative Matthew Tointon April 2009 0 Introduction In 1972 Jacques Tits published his paper Free Subgroups in Linear Groups [Tits] in the Journal of Algebra. Its key achievement was to prove a conjecture of H. Bass and J.-P. Serre, now known as the Tits Alternative for linear groups, namely that a finitely-generated linear group over an arbitrary field possesses either a solvable subgroup of finite index or a non-abelian free subgroup. The aim of this essay is to present this result in such a way that it will be clear to a general mathematical audience. The greatest challenge in reading Tits's original paper is perhaps that the range of mathematics required to understand the theorem's proof is far greater than that required to understand its statement. Whilst this essay is not intended as a platform in which to regurgitate theory it is very much intended to overcome this challenge by presenting sufficient background detail to allow the reader, without too much effort, to enjoy a proof that is pleasing in both its variety and its ingenuity. Large parts of the prime-characteristic proof follow basically the same lines as the characteristic-zero proof; however, certain elements of the proof, particularly where it is necessary to introduce field theory or number theory, can be made more concrete or intuitive by restricting to characteristic zero. Therefore, for the sake of clarity this exposition will present the proof over the complex numbers, although where clarity and brevity are not impaired by considering a step in the general case we will do so. -
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. -
Section I.9. Free Groups, Free Products, and Generators and Relations
I.9. Free Groups, Free Products, and Generators and Relations 1 Section I.9. Free Groups, Free Products, and Generators and Relations Note. This section includes material covered in Fraleigh’s Sections VII.39 and VII.40. We define a free group on a set and show (in Theorem I.9.2) that this idea of “free” is consistent with the idea of “free on a set” in the setting of a concrete category (see Definition I.7.7). We also define generators and relations in a group presentation. Note. To define a free group F on a set X, we will first define “words” on the set, have a way to reduce these words, define a method of combining words (this com- bination will be the binary operation in the free group), and then give a reduction of the combined words. The free group will have the reduced words as its elements and the combination as the binary operation. If set X = ∅ then the free group on X is F = hei. Definition. Let X be a nonempty set. Define set X−1 to be disjoint from X such that |X| = |X−1|. Choose a bijection from X to X−1 and denote the image of x ∈ X as x−1. Introduce the symbol “1” (with X and X−1 not containing 1). A −1 word on X is a sequence (a1, a2,...) with ai ∈ X ∪ X ∪ {1} for i ∈ N such that for some n ∈ N we have ak = 1 for all k ≥ n. The sequence (1, 1,...) is the empty word which we will also sometimes denote as 1.