Division Algebras That Generalize Dickson Semifields 3
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An Introduction to Quantum Field Theory
AN INTRODUCTION TO QUANTUM FIELD THEORY By Dr M Dasgupta University of Manchester Lecture presented at the School for Experimental High Energy Physics Students Somerville College, Oxford, September 2009 - 1 - - 2 - Contents 0 Prologue....................................................................................................... 5 1 Introduction ................................................................................................ 6 1.1 Lagrangian formalism in classical mechanics......................................... 6 1.2 Quantum mechanics................................................................................... 8 1.3 The Schrödinger picture........................................................................... 10 1.4 The Heisenberg picture............................................................................ 11 1.5 The quantum mechanical harmonic oscillator ..................................... 12 Problems .............................................................................................................. 13 2 Classical Field Theory............................................................................. 14 2.1 From N-point mechanics to field theory ............................................... 14 2.2 Relativistic field theory ............................................................................ 15 2.3 Action for a scalar field ............................................................................ 15 2.4 Plane wave solution to the Klein-Gordon equation ........................... -
The Quaternionic Commutator Bracket and Its Implications
S S symmetry Article The Quaternionic Commutator Bracket and Its Implications Arbab I. Arbab 1,† and Mudhahir Al Ajmi 2,* 1 Department of Physics, Faculty of Science, University of Khartoum, P.O. Box 321, Khartoum 11115, Sudan; [email protected] 2 Department of Physics, College of Science, Sultan Qaboos University, P.O. Box 36, P.C. 123, Muscat 999046, Sultanate of Oman * Correspondence: [email protected] † Current address: Department of Physics, College of Science, Qassim University, Qassim 51452, Saudi Arabia. Received: 11 August 2018; Accepted: 9 October 2018; Published: 16 October 2018 Abstract: A quaternionic commutator bracket for position and momentum shows that the i ~ quaternionic wave function, viz. ye = ( c y0 , y), represents a state of a particle with orbital angular momentum, L = 3 h¯ , resulting from the internal structure of the particle. This angular momentum can be attributed to spin of the particle. The vector y~ , points in an opposite direction of~L. When a charged particle is placed in an electromagnetic field, the interaction energy reveals that the magnetic moments interact with the electric and magnetic fields giving rise to terms similar to Aharonov–Bohm and Aharonov–Casher effects. Keywords: commutator bracket; quaternions; magnetic moments; angular momentum; quantum mechanics 1. Introduction In quantum mechanics, particles are described by relativistic or non-relativistic wave equations. Each equation associates a spin state of the particle to its wave equation. For instance, the Schrödinger equation applies to the spinless particles in the non-relativistic domain, while the appropriate relativistic equation for spin-0 particles is the Klein–Gordon equation. -
Formal Power Series - Wikipedia, the Free Encyclopedia
Formal power series - Wikipedia, the free encyclopedia http://en.wikipedia.org/wiki/Formal_power_series Formal power series From Wikipedia, the free encyclopedia In mathematics, formal power series are a generalization of polynomials as formal objects, where the number of terms is allowed to be infinite; this implies giving up the possibility to substitute arbitrary values for indeterminates. This perspective contrasts with that of power series, whose variables designate numerical values, and which series therefore only have a definite value if convergence can be established. Formal power series are often used merely to represent the whole collection of their coefficients. In combinatorics, they provide representations of numerical sequences and of multisets, and for instance allow giving concise expressions for recursively defined sequences regardless of whether the recursion can be explicitly solved; this is known as the method of generating functions. Contents 1 Introduction 2 The ring of formal power series 2.1 Definition of the formal power series ring 2.1.1 Ring structure 2.1.2 Topological structure 2.1.3 Alternative topologies 2.2 Universal property 3 Operations on formal power series 3.1 Multiplying series 3.2 Power series raised to powers 3.3 Inverting series 3.4 Dividing series 3.5 Extracting coefficients 3.6 Composition of series 3.6.1 Example 3.7 Composition inverse 3.8 Formal differentiation of series 4 Properties 4.1 Algebraic properties of the formal power series ring 4.2 Topological properties of the formal power series -
An Introduction to Operad Theory
AN INTRODUCTION TO OPERAD THEORY SAIMA SAMCHUCK-SCHNARCH Abstract. We give an introduction to category theory and operad theory aimed at the undergraduate level. We first explore operads in the category of sets, and then generalize to other familiar categories. Finally, we develop tools to construct operads via generators and relations, and provide several examples of operads in various categories. Throughout, we highlight the ways in which operads can be seen to encode the properties of algebraic structures across different categories. Contents 1. Introduction1 2. Preliminary Definitions2 2.1. Algebraic Structures2 2.2. Category Theory4 3. Operads in the Category of Sets 12 3.1. Basic Definitions 13 3.2. Tree Diagram Visualizations 14 3.3. Morphisms and Algebras over Operads of Sets 17 4. General Operads 22 4.1. Basic Definitions 22 4.2. Morphisms and Algebras over General Operads 27 5. Operads via Generators and Relations 33 5.1. Quotient Operads and Free Operads 33 5.2. More Examples of Operads 38 5.3. Coloured Operads 43 References 44 1. Introduction Sets equipped with operations are ubiquitous in mathematics, and many familiar operati- ons share key properties. For instance, the addition of real numbers, composition of functions, and concatenation of strings are all associative operations with an identity element. In other words, all three are examples of monoids. Rather than working with particular examples of sets and operations directly, it is often more convenient to abstract out their common pro- perties and work with algebraic structures instead. For instance, one can prove that in any monoid, arbitrarily long products x1x2 ··· xn have an unambiguous value, and thus brackets 2010 Mathematics Subject Classification. -
Commutator Groups of Monomial Groups
Pacific Journal of Mathematics COMMUTATOR GROUPS OF MONOMIAL GROUPS CALVIN VIRGIL HOLMES Vol. 10, No. 4 December 1960 COMMUTATOR GROUPS OF MONOMIAL GROUPS C. V. HOLMES This paper is a study of the commutator groups of certain general- ized permutation groups called complete monomial groups. In [2] Ore has shown that every element of the infinite permutation group is itsself a commutator of this group. Here it is shown that every element of the infinite complete monomial group is the product of at most two commutators of the infinite complete monomial group. The commutator subgroup of the infinite complete monomial group is itself, as is the case in the infinite symmetric group, [2]. The derived series is determined for a wide class of monomial groups. Let H be an arbitrary group, and S a set of order B, B ^ d, cZ = ^0. Then one obtains a monomial group after the manner described in [1], A monomial substitution over H is a linear transformation mapping each element x of S in a one-to-one manner onto some element of S multi- plied by an element h of H, the multiplication being formal. The ele- ment h is termed a factor of the substitution. If substitution u maps xi into hjXj, while substitution v maps xό into htxt, then the substitution uv maps xt into hόhtxt. A substitution all of whose factor are the iden- tity β of H is called a permutation and the set of all permutations is a subgroup which is isomorphic to the symmetric group on B objects. -
Commutator Theory for Congruence Modular Varieties Ralph Freese
Commutator Theory for Congruence Modular Varieties Ralph Freese and Ralph McKenzie Contents Introduction 1 Chapter 1. The Commutator in Groups and Rings 7 Exercise 10 Chapter 2. Universal Algebra 11 Exercises 19 Chapter 3. Several Commutators 21 Exercises 22 Chapter 4. One Commutator in Modular Varieties;Its Basic Properties 25 Exercises 33 Chapter 5. The Fundamental Theorem on Abelian Algebras 35 Exercises 43 Chapter 6. Permutability and a Characterization ofModular Varieties 47 Exercises 49 Chapter 7. The Center and Nilpotent Algebras 53 Exercises 57 Chapter 8. Congruence Identities 59 Exercises 68 Chapter 9. Rings Associated With Modular Varieties: Abelian Varieties 71 Exercises 87 Chapter 10. Structure and Representationin Modular Varieties 89 1. Birkhoff-J´onsson Type Theorems For Modular Varieties 89 2. Subdirectly Irreducible Algebras inFinitely Generated Varieties 92 3. Residually Small Varieties 97 4. Chief Factors and Simple Algebras 102 Exercises 103 Chapter 11. Joins and Products of Modular Varieties 105 Chapter 12. Strictly Simple Algebras 109 iii iv CONTENTS Chapter 13. Mal’cev Conditions for Lattice Equations 115 Exercises 120 Chapter 14. A Finite Basis Result 121 Chapter 15. Pure Lattice Congruence Identities 135 1. The Arguesian Equation 139 Related Literature 141 Solutions To The Exercises 147 Chapter 1 147 Chapter 2 147 Chapter 4 148 Chapter 5 150 Chapter 6 152 Chapter 7 156 Chapter 8 158 Chapter 9 161 Chapter 10 165 Chapter 13 165 Bibliography 169 Index 173 Introduction In the theory of groups, the important concepts of Abelian group, solvable group, nilpotent group, the center of a group and centraliz- ers, are all defined from the binary operation [x, y]= x−1y−1xy. -
Commutator Formulas
Commutator formulas Jack Schmidt This expository note mentions some interesting formulas using commutators. It touches on Hall's collection process and the associated Hall polynomials. It gives an alternative expression that is linear in the number of commutators and shows how to find such a formula using staircase diagrams. It also shows the shortest possible such expression. Future versions could touch on isoperimetric inequalities in geometric group theory, powers of commutators and Culler's identity as well as its effect on Schur's inequality between [G : Z(G)] and jG0j. 1 Powers of products versus products of powers In an abelian group one has (xy)n = xnyn so in a general group one has (xy)n = n n x y dn(x; y) for some product of commutators dn(x; y). This section explores formulas for dn(x; y). 1.1 A nice formula in a special case is given by certain binomial coefficients: n (n) (n) (n) (n) (n) (n) (xy) = x 1 y 1 [y; x] 2 [[y; x]; x] 3 [[[y; x]; x]; x] 4 ··· [y; n−1x] n The special case is G0 is abelian and commutes with y. The commutators involved are built inductively: From y and x, one gets [y; x]. From [y; x] and x, one gets [[y; x]; x]. From [y; n−2x] and x, one gets [y; n−1; x]. In general, one would also need to consider [y; x] and [[y; x]; x], but the special case assumes commutators commute, so [[y; x]; [[y; x]; x]] = 1. In general, one would also need to consider [y; x] and y, but the special case assumes commutators commute with y, so [[y; x]; y] = 1. -
Ring (Mathematics) 1 Ring (Mathematics)
Ring (mathematics) 1 Ring (mathematics) In mathematics, a ring is an algebraic structure consisting of a set together with two binary operations usually called addition and multiplication, where the set is an abelian group under addition (called the additive group of the ring) and a monoid under multiplication such that multiplication distributes over addition.a[›] In other words the ring axioms require that addition is commutative, addition and multiplication are associative, multiplication distributes over addition, each element in the set has an additive inverse, and there exists an additive identity. One of the most common examples of a ring is the set of integers endowed with its natural operations of addition and multiplication. Certain variations of the definition of a ring are sometimes employed, and these are outlined later in the article. Polynomials, represented here by curves, form a ring under addition The branch of mathematics that studies rings is known and multiplication. as ring theory. Ring theorists study properties common to both familiar mathematical structures such as integers and polynomials, and to the many less well-known mathematical structures that also satisfy the axioms of ring theory. The ubiquity of rings makes them a central organizing principle of contemporary mathematics.[1] Ring theory may be used to understand fundamental physical laws, such as those underlying special relativity and symmetry phenomena in molecular chemistry. The concept of a ring first arose from attempts to prove Fermat's last theorem, starting with Richard Dedekind in the 1880s. After contributions from other fields, mainly number theory, the ring notion was generalized and firmly established during the 1920s by Emmy Noether and Wolfgang Krull.[2] Modern ring theory—a very active mathematical discipline—studies rings in their own right. -
Hamilton Equations, Commutator, and Energy Conservation †
quantum reports Article Hamilton Equations, Commutator, and Energy Conservation † Weng Cho Chew 1,* , Aiyin Y. Liu 2 , Carlos Salazar-Lazaro 3 , Dong-Yeop Na 1 and Wei E. I. Sha 4 1 College of Engineering, Purdue University, West Lafayette, IN 47907, USA; [email protected] 2 College of Engineering, University of Illinois at Urbana-Champaign, Urbana, IL 61820, USA; [email protected] 3 Physics Department, University of Illinois at Urbana-Champaign, Urbana, IL 61820, USA; [email protected] 4 College of Information Science and Electronic Engineering, Zhejiang University, Hangzhou 310058, China; [email protected] * Correspondence: [email protected] † Based on the talk presented at the 40th Progress In Electromagnetics Research Symposium (PIERS, Toyama, Japan, 1–4 August 2018). Received: 12 September 2019; Accepted: 3 December 2019; Published: 9 December 2019 Abstract: We show that the classical Hamilton equations of motion can be derived from the energy conservation condition. A similar argument is shown to carry to the quantum formulation of Hamiltonian dynamics. Hence, showing a striking similarity between the quantum formulation and the classical formulation. Furthermore, it is shown that the fundamental commutator can be derived from the Heisenberg equations of motion and the quantum Hamilton equations of motion. Also, that the Heisenberg equations of motion can be derived from the Schrödinger equation for the quantum state, which is the fundamental postulate. These results are shown to have important bearing for deriving the quantum Maxwell’s equations. Keywords: quantum mechanics; commutator relations; Heisenberg picture 1. Introduction In quantum theory, a classical observable, which is modeled by a real scalar variable, is replaced by a quantum operator, which is analogous to an infinite-dimensional matrix operator. -
Universit¨At Stuttgart Fachbereich Mathematik
Universitat¨ Fachbereich Stuttgart Mathematik Heisenberg Groups, Semifields, and Translation Planes Norbert Knarr, Markus J. Stroppel Preprint 2013/006 Universitat¨ Fachbereich Stuttgart Mathematik Heisenberg Groups, Semifields, and Translation Planes Norbert Knarr, Markus J. Stroppel Preprint 2013/006 Fachbereich Mathematik Fakultat¨ Mathematik und Physik Universitat¨ Stuttgart Pfaffenwaldring 57 D-70 569 Stuttgart E-Mail: [email protected] WWW: http://www.mathematik.uni-stuttgart.de/preprints ISSN 1613-8309 c Alle Rechte vorbehalten. Nachdruck nur mit Genehmigung des Autors. LATEX-Style: Winfried Geis, Thomas Merkle Heisenberg Groups, Semifields, and Translation Planes Norbert Knarr, Markus J. Stroppel Abstract For Heisenberg groups constructed over semifields (i.e., not neccessarily associative divi- sion rings), we solve the isomorphism problem and determine the automorphism groups. We show that two Heisenberg groups over semifields are isomorphic precisely if the semi- fields are isotopic or anti-isotopic to each other. This condition means that the corre- sponding translation are isomorphic or dual to each other. Mathematics Subject Classification: 12K10 17A35 20D15 20F28 51A35 51A10 Keywords: Heisenberg group, nilpotent group, automorphism, translation plane, semi- field, division algebra, isotopism, autotopism In [7], Heisenberg’s example of a step 2 nilpotent group has been generalized, replacing the ground field by an arbitrary associative ring S with 2 2 S×. The main focus of [7] was on the group of automorphisms of such a Heisenberg group. In the present note we extend this further (see 1.2 below), dropping the restriction on invertibility of 2 and allowing the multiplication in S to be non-associative. The main results of the present paper require that S is a semifield. -
Hilbert's Basis Theorem for Non-Associative and Hom
HILBERT’S BASIS THEOREM FOR NON-ASSOCIATIVE AND HOM-ASSOCIATIVE ORE EXTENSIONS PER BACK¨ AND JOHAN RICHTER Abstract. We prove a hom-associative version of Hilbert’s basis theorem, which includes as special cases both a non-associative version and the classi- cal associative Hilbert’s basis theorem for Ore extensions. Along the way, we develop hom-module theory, including the introduction of corresponding iso- morphism theorems and a notion of being hom-noetherian. We conclude with some examples of both non-associative and hom-associative Ore extensions which are all noetherian by our theorem. 1. Introduction Hom-associative algebras are not necessarily associative algebras, the associativ- ity condition being replaced by α(a) · (b · c) = (a · b) · α(c), where α is a linear map referred to as a twisting map, and a,b,c arbitrary elements in the algebra. Both as- sociative algebras and non-associative algebras can thus be seen as hom-associative algebras; in the first case, by taking α equal to the identity map, and in the latter case by taking α equal to the zero map. Historically hom-associative algebras originate in the development of hom-Lie al- gebras, the latter introduced by Hartwig, Larsson and Silvestrov as generalizations of Lie algebras, the Jacobi identity now twisted by a vector space homomorphism; the “hom” referring to this homomorphism [6]. The introduction of these gener- alizations of Lie algebras was mainly motivated by an attempt to study so-called q-deformations of the Witt and Virasoro algebras within a common framework. Makhlouf and Silvestrov then introduced hom-associative algebras as the natural counterparts to associative algebras; taking a hom-associative algebra and defining the commutator as a new multiplication gives a hom-Lie algebra, just as with the classical relation between associative algebras and Lie algebras [7]. -
Special Unitary Group - Wikipedia
Special unitary group - Wikipedia https://en.wikipedia.org/wiki/Special_unitary_group Special unitary group In mathematics, the special unitary group of degree n, denoted SU( n), is the Lie group of n×n unitary matrices with determinant 1. (More general unitary matrices may have complex determinants with absolute value 1, rather than real 1 in the special case.) The group operation is matrix multiplication. The special unitary group is a subgroup of the unitary group U( n), consisting of all n×n unitary matrices. As a compact classical group, U( n) is the group that preserves the standard inner product on Cn.[nb 1] It is itself a subgroup of the general linear group, SU( n) ⊂ U( n) ⊂ GL( n, C). The SU( n) groups find wide application in the Standard Model of particle physics, especially SU(2) in the electroweak interaction and SU(3) in quantum chromodynamics.[1] The simplest case, SU(1) , is the trivial group, having only a single element. The group SU(2) is isomorphic to the group of quaternions of norm 1, and is thus diffeomorphic to the 3-sphere. Since unit quaternions can be used to represent rotations in 3-dimensional space (up to sign), there is a surjective homomorphism from SU(2) to the rotation group SO(3) whose kernel is {+ I, − I}. [nb 2] SU(2) is also identical to one of the symmetry groups of spinors, Spin(3), that enables a spinor presentation of rotations. Contents Properties Lie algebra Fundamental representation Adjoint representation The group SU(2) Diffeomorphism with S 3 Isomorphism with unit quaternions Lie Algebra The group SU(3) Topology Representation theory Lie algebra Lie algebra structure Generalized special unitary group Example Important subgroups See also 1 of 10 2/22/2018, 8:54 PM Special unitary group - Wikipedia https://en.wikipedia.org/wiki/Special_unitary_group Remarks Notes References Properties The special unitary group SU( n) is a real Lie group (though not a complex Lie group).