GENERATING SETS 1. Introduction in Rn, Every Vector Can Be Written As A
Total Page:16
File Type:pdf, Size:1020Kb
Load more
Recommended publications
-
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. -
Lecture 1 – Symmetries & Conservation
LECTURE 1 – SYMMETRIES & CONSERVATION Contents • Symmetries & Transformations • Transformations in Quantum Mechanics • Generators • Symmetry in Quantum Mechanics • Conservations Laws in Classical Mechanics • Parity Messages • Symmetries give rise to conserved quantities . Symmetries & Conservation Laws Lecture 1, page1 Symmetry & Transformations Systems contain Symmetry if they are unchanged by a Transformation . This symmetry is often due to an absence of an absolute reference and corresponds to the concept of indistinguishability . It will turn out that symmetries are often associated with conserved quantities . Transformations may be: Active: Active • Move object • More physical Passive: • Change “description” Eg. Change Coordinate Frame • More mathematical Passive Symmetries & Conservation Laws Lecture 1, page2 We will consider two classes of Transformation: Space-time : • Translations in (x,t) } Poincaré Transformations • Rotations and Lorentz Boosts } • Parity in (x,t) (Reflections) Internal : associated with quantum numbers Translations: x → 'x = x − ∆ x t → 't = t − ∆ t Rotations (e.g. about z-axis): x → 'x = x cos θz + y sin θz & y → 'y = −x sin θz + y cos θz Lorentz (e.g. along x-axis): x → x' = γ(x − βt) & t → t' = γ(t − βx) Parity: x → x' = −x t → t' = −t For physical laws to be useful, they should exhibit a certain generality, especially under symmetry transformations. In particular, we should expect invariance of the laws to change of the status of the observer – all observers should have the same laws, even if the evaluation of measurables is different. Put differently, the laws of physics applied by different observers should lead to the same observations. It is this principle which led to the formulation of Special Relativity. -
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. -
The Homology Theory of the Closed Geodesic Problem
J. DIFFERENTIAL GEOMETRY 11 (1976) 633-644 THE HOMOLOGY THEORY OF THE CLOSED GEODESIC PROBLEM MICHELINE VIGUE-POIRRIER & DENNIS SULLIVAN The problem—does every closed Riemannian manifold of dimension greater than one have infinitely many geometrically distinct periodic geodesies—has received much attention. An affirmative answer is easy to obtain if the funda- mental group of the manifold has infinitely many conjugacy classes, (up to powers). One merely needs to look at the closed curve representations with minimal length. In this paper we consider the opposite case of a finite fundamental group and show by using algebraic calculations and the work of Gromoll-Meyer [2] that the answer is again affirmative if the real cohomology ring of the manifold or any of its covers requires at least two generators. The calculations are based on a method of the second author sketched in [6], and he wishes to acknowledge the motivation provided by conversations with Gromoll in 1967 who pointed out the surprising fact that the available tech- niques of algebraic topology loop spaces, spectral sequences, and so forth seemed inadequate to handle the "rational problem" of calculating the Betti numbers of the space of all closed curves on a manifold. He also acknowledges the help given by John Morgan in understanding what goes on here. The Gromoll-Meyer theorem which uses nongeneric Morse theory asserts the following. Let Λ(M) denote the space of all maps of the circle S1 into M (not based). Then there are infinitely many geometrically distinct periodic geodesies in any metric on M // the Betti numbers of Λ(M) are unbounded. -
10 Group Theory and Standard Model
Physics 129b Lecture 18 Caltech, 03/05/20 10 Group Theory and Standard Model Group theory played a big role in the development of the Standard model, which explains the origin of all fundamental particles we see in nature. In order to understand how that works, we need to learn about a new Lie group: SU(3). 10.1 SU(3) and more about Lie groups SU(3) is the group of special (det U = 1) unitary (UU y = I) matrices of dimension three. What are the generators of SU(3)? If we want three dimensional matrices X such that U = eiθX is unitary (eigenvalues of absolute value 1), then X need to be Hermitian (real eigenvalue). Moreover, if U has determinant 1, X has to be traceless. Therefore, the generators of SU(3) are the set of traceless Hermitian matrices of dimension 3. Let's count how many independent parameters we need to characterize this set of matrices (what is the dimension of the Lie algebra). 3 × 3 complex matrices contains 18 real parameters. If it is to be Hermitian, then the number of parameters reduces by a half to 9. If we further impose traceless-ness, then the number of parameter reduces to 8. Therefore, the generator of SU(3) forms an 8 dimensional vector space. We can choose a basis for this eight dimensional vector space as 00 1 01 00 −i 01 01 0 01 00 0 11 λ1 = @1 0 0A ; λ2 = @i 0 0A ; λ3 = @0 −1 0A ; λ4 = @0 0 0A (1) 0 0 0 0 0 0 0 0 0 1 0 0 00 0 −i1 00 0 01 00 0 0 1 01 0 0 1 1 λ5 = @0 0 0 A ; λ6 = @0 0 1A ; λ7 = @0 0 −iA ; λ8 = p @0 1 0 A (2) i 0 0 0 1 0 0 i 0 3 0 0 −2 They are called the Gell-Mann matrices. -
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. -
Spin in Relativistic Quantum Theory∗
Spin in relativistic quantum theory∗ W. N. Polyzou, Department of Physics and Astronomy, The University of Iowa, Iowa City, IA 52242 W. Gl¨ockle, Institut f¨urtheoretische Physik II, Ruhr-Universit¨at Bochum, D-44780 Bochum, Germany H. Wita la M. Smoluchowski Institute of Physics, Jagiellonian University, PL-30059 Krak´ow,Poland today Abstract We discuss the role of spin in Poincar´einvariant formulations of quan- tum mechanics. 1 Introduction In this paper we discuss the role of spin in relativistic few-body models. The new feature with spin in relativistic quantum mechanics is that sequences of rotationless Lorentz transformations that map rest frames to rest frames can generate rotations. To get a well-defined spin observable one needs to define it in one preferred frame and then use specific Lorentz transformations to relate the spin in the preferred frame to any other frame. Different choices of the preferred frame and the specific Lorentz transformations lead to an infinite number of possible observables that have all of the properties of a spin. This paper provides a general discussion of the relation between the spin of a system and the spin of its elementary constituents in relativistic few-body systems. In section 2 we discuss the Poincar´egroup, which is the group relating inertial frames in special relativity. Unitary representations of the Poincar´e group preserve quantum probabilities in all inertial frames, and define the rel- ativistic dynamics. In section 3 we construct a large set of abstract operators out of the Poincar´egenerators, and determine their commutation relations and ∗During the preparation of this paper Walter Gl¨ockle passed away. -
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.