Classical and Quantum Mechanics Via Lie Algebras, Cambridge University Press, to Appear (2009?)

Total Page:16

File Type:pdf, Size:1020Kb

Classical and Quantum Mechanics Via Lie Algebras, Cambridge University Press, to Appear (2009?) Classical and quantum mechanics via Lie algebras Arnold Neumaier Dennis Westra University of Vienna, Austria April 14, 2011 arXiv:0810.1019v2 [quant-ph] 14 Apr 2011 This is the draft of a book. The manuscript has not yet full book quality. Please refer to the book once it is published. Until then, we’d appreciate suggestions for improvements; please send them to [email protected] copyright c by Arnold Neumaier and Dennis Westra Contents Preface ix I An invitation to quantum mechanics 1 1 Motivation 3 1.1 Classicalmechanics................................ 3 1.2 Relativitytheory ................................. 5 1.3 Statistical mechanics and thermodynamics . ... 7 1.4 Hamiltonianmechanics.............................. 8 1.5 Quantummechanics ............................... 10 1.6 Quantumfieldtheory............................... 13 1.7 TheSchr¨odingerpicture . .. .. 13 1.8 TheHeisenbergpicture.............................. 15 1.9 Outlineofthebook................................ 17 2 The simplest quantum system 25 2.1 Matrices, relativity and quantum theory . .. 26 2.2 Continuousmotionsandmatrixgroups . 28 2.3 Infinitesimal motions and matrix Lie algebras . 29 2.4 Uniform motions and the matrix exponential . .. 31 2.5 Volume preservation and special linear groups . ... 33 2.6 The vector product, quaternions, and SL(2, C)................. 35 i ii CONTENTS 2.7 The Hamiltonian form of a Lie algebra . 38 2.8 Atomic energy levels and unitary groups . 39 2.9 QubitsandBlochsphere ............................. 40 2.10 Polarized light and beam transformations . ... 41 2.11 Spinandspincoherentstates . 44 2.12 Particles and detection probabilities . .. 47 2.13Photonsondemand................................ 48 2.14 Unitary representations of SU(2) ........................ 53 3 The symmetries of the universe 57 3.1 Rotations and SO(n)............................... 57 3.2 3-dimensional rotations and SO(3) ....................... 60 3.3 Rotationsandquaternions . .. .. .. 63 3.4 Rotations and SU(2)............................... 65 3.5 Angularvelocity.................................. 66 3.6 Rigid motions and Euclidean groups . 68 3.7 Connected subgroups of SL(2, R) ........................ 70 3.8 Connected subgroups of SL(3, R) ........................ 70 3.9 Classical mechanics and Heisenberg groups . ... 70 3.10 Angularmomentum,isospin,quarks. .. 70 3.11 Connected subgroups of SL(4, R) ........................ 71 3.12TheGalileangroup ................................ 71 3.13 The Lorentz groups O(1, 3), SO(1, 3), SO(1, 3)0 ................ 72 3.14 The Poincare group ISO(1, 3).......................... 75 3.15 ALorentzinvariantmeasure . 77 3.16 Kepler’s laws, the hydrogen atom, and SO(4) ................. 78 3.17 The periodic systemand the conformal group SO(2, 4)............. 78 3.18 The interacting boson model and U(6) ..................... 78 CONTENTS iii 3.19Casimirs...................................... 78 3.20 Unitary representations of the Poincar´egroup . ....... 79 3.21 Some representations of the Poincare group. ...... 80 3.22Elementaryparticles ............................... 80 3.23 Thepositionoperator............................... 81 4 From the theoretical physics FAQ 83 4.1 Tobedone .................................... 83 4.2 Postulates for the formal core of quantum mechanics . ...... 84 4.3 LiegroupsandLiealgebras ........................... 90 4.4 The Galilei group as contraction of the Poincare group . .... 92 4.5 RepresentationsofthePoincaregroup . ... 92 4.6 Forms of relativistic dynamics . 94 4.7 Is there a multiparticle relativistic quantum mechanics? . .... 98 4.8 Whatisaphoton? ................................ 99 4.9 Particle positions and the position operator . 105 4.10 Localization and position operators . 111 4.11 SO(3) = SU(2)/Z2 ................................114 5 Classical oscillating systems 119 5.1 Systemsofdampedoscillators . 119 5.2 The classical anharmonic oscillator . 123 5.3 Harmonic oscillators and linear field equations . 126 5.4 Alpharays.....................................128 5.5 Betarays .....................................130 5.6 Lightraysandgammarays ...........................133 6 Spectral analysis 137 6.1 Thequantumspectrum..............................137 iv CONTENTS 6.2 Probingthespectrumofasystem . 141 6.3 Theearlyhistoryofquantummechanics . 144 6.4 Thespectrumofmany-particlesystems . .148 6.5 Blackbodyradiation ...............................150 6.6 Derivation of Planck’s law . 152 6.7 Stefan’s law and Wien’s displacement law . 156 II Statistical mechanics 159 7 Phenomenological thermodynamics 161 7.1 Standardthermodynamicalsystems . .161 7.2 Thelawsofthermodynamics. .. .. .. .167 7.3 Consequencesofthefirstlaw. 169 7.4 Consequencesofthesecondlaw . 171 7.5 The approach to equilibrium . 175 7.6 Description levels . 176 8 Quantities, states, and statistics 179 8.1 Quantities .....................................180 8.2 Gibbsstates....................................187 8.3 Kuboproductandgeneratingfunctional . .190 8.4 Limit resolution and uncertainty . 195 9 The laws of thermodynamics 201 9.1 Thezerothlaw:Thermalstates . 201 9.2 Theequationofstate...............................205 9.3 Thefirstlaw:Energybalance . .. .. .. .210 9.4 The second law: Extremal principles . 214 9.5 The third law: Quantization . 215 CONTENTS v 10 Models, statistics, and measurements 219 10.1 Description levels . 219 10.2 Local, microlocal, and quantum equilibrium . 226 10.3 Statistics and probability . 230 10.4 Classicalmeasurements. 233 10.5Quantumprobability ...............................236 10.6 Entropyandinformationtheory . 240 10.7 Subjective probability . 244 III Lie algebras and Poisson algebras 247 11 Lie algebras 249 11.1Basicdefinitions..................................250 11.2 Lie algebras from derivations . 253 11.3 Linear groups and their Lie algebras . 255 11.4 Classical Lie groups and their Lie algebras . 258 11.5 Heisenberg algebras and Heisenberg groups . .263 11.6 Lie -algebras ...................................268 ∗ 12 Mechanics in Poisson algebras 273 12.1Poissonalgebras..................................273 12.2 Rotating rigid bodies . 276 12.3 Rotationsandangularmomentum. 277 12.4 Classical rigid body dynamics . 280 12.5Lie–Poissonalgebras ...............................282 12.6 Classical symplectic mechanics . 286 12.7Molecularmechanics ...............................288 12.8 Anoutlooktoquantumfieldtheory . 290 vi CONTENTS 13 Representation and classification 293 13.1 Poissonrepresentations. 293 13.2 Linearrepresentations . .. .. .. 295 13.3 Finite-dimensional representations . .297 13.4 RepresentationsofLiegroups . 298 13.5 Finite-dimensional semisimple Lie algebras . 300 13.6 Automorphismsandcoadjointorbits . 304 IV Nonequilibrium thermodynamics 305 14 Markov Processes 307 14.1Activities .....................................308 14.2Processes .....................................312 14.3 Forward morphisms and quantum dynamical semigroups . .315 14.4Forwardderivations................................ 316 14.5 Single-time, autonomous Markov processes . .319 14.6tobedone.....................................321 15 Diffusion processes 323 15.1 Stochastic differential equations . .323 15.2 Closeddiffusionprocesses . 327 15.3 Ornstein-Uhlenbeckprocesses . .331 15.4 Linearprocesseswithmemory . 333 15.5 Dissipative Hamiltonian Systems . 335 16 Collective Processes 339 16.1Themasterequation ...............................339 16.2 Canonical form and thermodynamic limit . 345 16.3 Stirredchemicalreactions . 350 CONTENTS vii 16.4 Linearresponsetheory . .. .. 352 16.5Opensystem ...................................354 16.6 Somephilosophicalafterthoughts . .356 V Mechanics and differential geometry 357 17 Fields, forms, and derivatives 359 17.1 Scalarfieldsandvectorfields. 360 17.2 Multilinear forms . 363 17.3Exteriorcalculus .................................367 17.4 Manifolds as differential geometries . 370 17.5 Manifolds as topological spaces . 371 17.6 Noncommutativegeometry. 375 17.7Liegroupsasmanifolds..............................376 18 Conservative mechanics on manifolds 379 18.1 Poissonalgebrasfromclosed2-forms . .379 18.2 Conservative Hamiltonian dynamics . 382 18.3 Constrained Hamiltonian dynamics . 385 18.4 Lagrangianmechanics ..............................388 19 Hamiltonian quantum mechanics 393 19.1 Quantum dynamics as symplectic motion . 393 19.2 Quantum-classicaldynamics . 395 19.3 Deformationquantization . 398 19.4TheWignertransform ..............................401 VI Representations and spectroscopy 411 20 Harmonic oscillators and coherent states 413 viii CONTENTS 20.1 The classical harmonic oscillator . 414 20.2 Quantizing the harmonic oscillator . 415 20.3 Representations oftheHeisenberg algebra . .418 20.4BrasandKets...................................420 20.5BosonFockspace .................................423 20.6 Bargmann–Fockrepresentation . .425 20.7 Coherent states for the harmonic oscillator . .426 20.8 Monochromatic beamsandcoherent states . .432 21 Spin and fermions 435 21.1FermionFockspace................................435 21.2 Extensiontomanydegreesoffreedom . .438 21.3 Exterioralgebrarepresentation . .441 21.4 Spin and metaplectic representation . .443 22 Highest weight representations 447 22.1 Triangular decompositions . 447 22.2 Triangulated Lie algebras of rank and degree one . .450 22.3 Unitary representations of SU(2) and SO(3)..................451 22.4 Some unitary highest weight representations . .453 23 Spectroscopy and spectra 455 23.1 Introductionandhistoricalbackground
Recommended publications
  • The Unitary Representations of the Poincaré Group in Any Spacetime
    The unitary representations of the Poincar´e group in any spacetime dimension Xavier Bekaert a and Nicolas Boulanger b a Institut Denis Poisson, Unit´emixte de Recherche 7013, Universit´ede Tours, Universit´ed’Orl´eans, CNRS, Parc de Grandmont, 37200 Tours (France) [email protected] b Service de Physique de l’Univers, Champs et Gravitation Universit´ede Mons – UMONS, Place du Parc 20, 7000 Mons (Belgium) [email protected] An extensive group-theoretical treatment of linear relativistic field equa- tions on Minkowski spacetime of arbitrary dimension D > 2 is presented in these lecture notes. To start with, the one-to-one correspondence be- tween linear relativistic field equations and unitary representations of the isometry group is reviewed. In turn, the method of induced representa- tions reduces the problem of classifying the representations of the Poincar´e group ISO(D 1, 1) to the classification of the representations of the sta- − bility subgroups only. Therefore, an exhaustive treatment of the two most important classes of unitary irreducible representations, corresponding to massive and massless particles (the latter class decomposing in turn into the “helicity” and the “infinite-spin” representations) may be performed via the well-known representation theory of the orthogonal groups O(n) (with D 4 <n<D ). Finally, covariant field equations are given for each − unitary irreducible representation of the Poincar´egroup with non-negative arXiv:hep-th/0611263v2 13 Jun 2021 mass-squared. Tachyonic representations are also examined. All these steps are covered in many details and with examples. The present notes also include a self-contained review of the representation theory of the general linear and (in)homogeneous orthogonal groups in terms of Young diagrams.
    [Show full text]
  • 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.
    [Show full text]
  • Invariant Differential Operators 1. Derivatives of Group Actions
    (October 28, 2010) Invariant differential operators Paul Garrett [email protected] http:=/www.math.umn.edu/~garrett/ • Derivatives of group actions: Lie algebras • Laplacians and Casimir operators • Descending to G=K • Example computation: SL2(R) • Enveloping algebras and adjoint functors • Appendix: brackets • Appendix: proof of Poincar´e-Birkhoff-Witt We want an intrinsic approach to existence of differential operators invariant under group actions. n n The translation-invariant operators @=@xi on R , and the rotation-invariant Laplacian on R are deceptively- easily proven invariant, as these examples provide few clues about more complicated situations. For example, we expect rotation-invariant Laplacians (second-order operators) on spheres, and we do not want to write a formula in generalized spherical coordinates and verify invariance computationally. Nor do we want to be constrained to imbedding spheres in Euclidean spaces and using the ambient geometry, even though this succeeds for spheres themselves. Another basic example is the operator @2 @2 y2 + @x2 @y2 on the complex upper half-plane H, provably invariant under the linear fractional action of SL2(R), but it is oppressive to verify this directly. Worse, the goal is not merely to verify an expression presented as a deus ex machina, but, rather to systematically generate suitable expressions. An important part of this intention is understanding reasons for the existence of invariant operators, and expressions in coordinates should be a foregone conclusion. (No prior acquaintance with Lie groups or Lie algebras is assumed.) 1. Derivatives of group actions: Lie algebras For example, as usual let > SOn(R) = fk 2 GLn(R): k k = 1n; det k = 1g act on functions f on the sphere Sn−1 ⊂ Rn, by (k · f)(m) = f(mk) with m × k ! mk being right matrix multiplication of the row vector m 2 Rn.
    [Show full text]
  • Matrix Lie Groups
    Maths Seminar 2007 MATRIX LIE GROUPS Claudiu C Remsing Dept of Mathematics (Pure and Applied) Rhodes University Grahamstown 6140 26 September 2007 RhodesUniv CCR 0 Maths Seminar 2007 TALK OUTLINE 1. What is a matrix Lie group ? 2. Matrices revisited. 3. Examples of matrix Lie groups. 4. Matrix Lie algebras. 5. A glimpse at elementary Lie theory. 6. Life beyond elementary Lie theory. RhodesUniv CCR 1 Maths Seminar 2007 1. What is a matrix Lie group ? Matrix Lie groups are groups of invertible • matrices that have desirable geometric features. So matrix Lie groups are simultaneously algebraic and geometric objects. Matrix Lie groups naturally arise in • – geometry (classical, algebraic, differential) – complex analyis – differential equations – Fourier analysis – algebra (group theory, ring theory) – number theory – combinatorics. RhodesUniv CCR 2 Maths Seminar 2007 Matrix Lie groups are encountered in many • applications in – physics (geometric mechanics, quantum con- trol) – engineering (motion control, robotics) – computational chemistry (molecular mo- tion) – computer science (computer animation, computer vision, quantum computation). “It turns out that matrix [Lie] groups • pop up in virtually any investigation of objects with symmetries, such as molecules in chemistry, particles in physics, and projective spaces in geometry”. (K. Tapp, 2005) RhodesUniv CCR 3 Maths Seminar 2007 EXAMPLE 1 : The Euclidean group E (2). • E (2) = F : R2 R2 F is an isometry . → | n o The vector space R2 is equipped with the standard Euclidean structure (the “dot product”) x y = x y + x y (x, y R2), • 1 1 2 2 ∈ hence with the Euclidean distance d (x, y) = (y x) (y x) (x, y R2).
    [Show full text]
  • Minimal Dark Matter Models with Radiative Neutrino Masses
    Master’s thesis Minimal dark matter models with radiative neutrino masses From Lagrangians to observables Simon May 1st June 2018 Advisors: Prof. Dr. Michael Klasen, Dr. Karol Kovařík Institut für Theoretische Physik Westfälische Wilhelms-Universität Münster Contents 1. Introduction 5 2. Experimental and observational evidence 7 2.1. Dark matter . 7 2.2. Neutrino oscillations . 14 3. Gauge theories and the Standard Model of particle physics 19 3.1. Mathematical background . 19 3.1.1. Group and representation theory . 19 3.1.2. Tensors . 27 3.2. Representations of the Lorentz group . 31 3.2.1. Scalars: The (0, 0) representation . 35 1 1 3.2.2. Weyl spinors: The ( 2 , 0) and (0, 2 ) representations . 36 1 1 3.2.3. Dirac spinors: The ( 2 , 0) ⊕ (0, 2 ) representation . 38 3.2.4. Majorana spinors . 40 1 1 3.2.5. Lorentz vectors: The ( 2 , 2 ) representation . 41 3.2.6. Field representations . 42 3.3. Two-component Weyl spinor formalism and van der Waerden notation 44 3.3.1. Definition . 44 3.3.2. Correspondence to the Dirac bispinor formalism . 47 3.4. The Standard Model . 49 3.4.1. Definition of the theory . 52 3.4.2. The Lagrangian . 54 4. Component notation for representations of SU(2) 57 4.1. SU(2) doublets . 59 4.1.1. Basic conventions and transformation of doublets . 60 4.1.2. Dual doublets and scalar product . 61 4.1.3. Transformation of dual doublets . 62 4.1.4. Adjoint doublets . 63 4.1.5. The question of transpose and conjugate doublets .
    [Show full text]
  • LECTURE 12: LIE GROUPS and THEIR LIE ALGEBRAS 1. Lie
    LECTURE 12: LIE GROUPS AND THEIR LIE ALGEBRAS 1. Lie groups Definition 1.1. A Lie group G is a smooth manifold equipped with a group structure so that the group multiplication µ : G × G ! G; (g1; g2) 7! g1 · g2 is a smooth map. Example. Here are some basic examples: • Rn, considered as a group under addition. • R∗ = R − f0g, considered as a group under multiplication. • S1, Considered as a group under multiplication. • Linear Lie groups GL(n; R), SL(n; R), O(n) etc. • If M and N are Lie groups, so is their product M × N. Remarks. (1) (Hilbert's 5th problem, [Gleason and Montgomery-Zippin, 1950's]) Any topological group whose underlying space is a topological manifold is a Lie group. (2) Not every smooth manifold admits a Lie group structure. For example, the only spheres that admit a Lie group structure are S0, S1 and S3; among all the compact 2 dimensional surfaces the only one that admits a Lie group structure is T 2 = S1 × S1. (3) Here are two simple topological constraints for a manifold to be a Lie group: • If G is a Lie group, then TG is a trivial bundle. n { Proof: We identify TeG = R . The vector bundle isomorphism is given by φ : G × TeG ! T G; φ(x; ξ) = (x; dLx(ξ)) • If G is a Lie group, then π1(G) is an abelian group. { Proof: Suppose α1, α2 2 π1(G). Define α : [0; 1] × [0; 1] ! G by α(t1; t2) = α1(t1) · α2(t2). Then along the bottom edge followed by the right edge we have the composition α1 ◦ α2, where ◦ is the product of loops in the fundamental group, while along the left edge followed by the top edge we get α2 ◦ α1.
    [Show full text]
  • Representations of the Euclidean Group and Its Applications to the Kinematics of Spatial Chains
    REPRESENTATIONS OF THE EUCLIDEAN GROUP AND ITS APPLICATIONS TO THE KINEMATICS OF SPATIAL CHAINS By JOSE MARIA RICO MARTINEZ A DISSERTATION PRESENTED TO THE GRADUATE SCHOOL OF THE UNIVERSITY OF FLORIDA IN PARTIAL FULFILLMENT OF THE REQUIREMENTS FOR THE DEGREE OF DOCTOR OF PHILOSOPHY UNIVERSITY OF FLORIDA 1988 LIBRARIES v ||miyBRSlTY_OF FLORIDA Copyright 1988 by Jose Maria Rico Martinez ACKNOWLEDGMENTS The author wishes to thank firstly his advisor Dr. Joseph Duffy for his guidance during the selection and development of the contents of this dissertation. Without his encouragement, in times when nothing fruitful seemed to evolve from the approaches followed, without his geometrical insight, and his quest for clarity, this dissertation would have plenty of errors. Nonetheless, the author is to blame for the remaining ones. Secondly, deep felt thanks go to the members of the supervisory committee for their invaluable criticism and for their teachings in the classroom. The faculty of the Mechanical Engineering Department, and in particular the faculty of the Center for Intelligent Machines and Robotics, must be thanked for the development of an atmosphere conductive to research. The contributions of the faculty of this center, including the visiting professors, can be found in many parts of this work. Special gratitude is owed to visiting professors Eric Primrose and Kenneth H. Hunt for their insightful comments. My thanks go also to my fellow students for their friendship and kindness. The economic support from the Mexican Ministry of Public Education and the Consejo Nacional de Ciencia y Tecnologia (CONACYT) is dutifully acknowledged. Finally, the author thanks his wife iii .
    [Show full text]
  • Lecture 7 - Complete Reducibility of Representations of Semisimple Algebras
    Lecture 7 - Complete Reducibility of Representations of Semisimple Algebras September 27, 2012 1 New modules from old A few preliminaries are necessary before jumping into the representation theory of semisim- ple algebras. First a word on creating new g-modules from old. Any Lie algebra g has an action on a 1-dimensional vector space (or F itself), given by the trivial action. Second, any action on spaces V and W can be extended to an action on V ⊗ W by forcing the Leibnitz rule: for any basis vector v ⊗ w 2 V ⊗ W we define x:(v ⊗ w) = x:v ⊗ w + v ⊗ x:w (1) One easily checks that x:y:(v ⊗ w) − y:x:(v ⊗ w) = [x; y]:(v ⊗ w). Assuming g has an action on V , it has an action on its dual V ∗ (recall V ∗ is the vector space of linear functionals V ! F), given by (v:f)(x) = −f(x:v) (2) for any functional f : V ! F in V ∗. This is in fact a version of the \forcing the Leibnitz rule." That is, recalling that we defined x:(f(v)) = 0, we define x:f 2 V ∗ implicitly by x: (f(v)) = (x:f)(v) + f(x:v): (3) For any vector spaces V , W , we have an isomorphism Hom(V; W ) ≈ V ∗ ⊗ W; (4) so Hom(V; W ) is a g-module whenever V and W are. This can be defined using the above rules for duals and tensor products, or, equivalently, by again forcing the Leibnitz rule: for F 2 Hom(V; W ), we define x:F 2 Hom(V; W ) implicitly by x:(F (v)) = (x:F )(v) + F (x:v): (5) 1 2 Schur's lemma and Casimir elements Theorem 2.1 (Schur's Lemma) If g has an irreducible representation on gl(V ) and if f 2 End(V ) commutes with every x 2 g, then f is multiplication by a constant.
    [Show full text]
  • An Identity Crisis for the Casimir Operator
    An Identity Crisis for the Casimir Operator Thomas R. Love Department of Mathematics and Department of Physics California State University, Dominguez Hills Carson, CA, 90747 [email protected] April 16, 2006 Abstract 2 P ij The Casimir operator of a Lie algebra L is C = g XiXj and the action of the Casimir operator is usually taken to be C2Y = P ij g XiXjY , with ordinary matrix multiplication. With this defini- tion, the eigenvalues of the Casimir operator depend upon the repre- sentation showing that the action of the Casimir operator is not well defined. We prove that the action of the Casimir operator should 2 P ij be interpreted as C Y = g [Xi, [Xj,Y ]]. This intrinsic definition does not depend upon the representation. Similar results hold for the higher order Casimir operators. We construct higher order Casimir operators which do not exist in the standard theory including a new type of Casimir operator which defines a complex structure and third order intrinsic Casimir operators for so(3) and so(3, 1). These opera- tors are not multiples of the identity. The standard theory of Casimir operators predicts neither the correct operators nor the correct num- ber of invariant operators. The quantum theory of angular momentum and spin, Wigner’s classification of elementary particles as represen- tations of the Poincar´eGroup and quark theory are based on faulty mathematics. The “no-go theorems” are shown to be invalid. PACS 02.20S 1 1 Introduction Lie groups and Lie algebras play a fundamental role in classical mechan- ics, electrodynamics, quantum mechanics, relativity, and elementary particle physics.
    [Show full text]
  • Advances in Quantum Field Theory
    ADVANCES IN QUANTUM FIELD THEORY Edited by Sergey Ketov Advances in Quantum Field Theory Edited by Sergey Ketov Published by InTech Janeza Trdine 9, 51000 Rijeka, Croatia Copyright © 2012 InTech All chapters are Open Access distributed under the Creative Commons Attribution 3.0 license, which allows users to download, copy and build upon published articles even for commercial purposes, as long as the author and publisher are properly credited, which ensures maximum dissemination and a wider impact of our publications. After this work has been published by InTech, authors have the right to republish it, in whole or part, in any publication of which they are the author, and to make other personal use of the work. Any republication, referencing or personal use of the work must explicitly identify the original source. As for readers, this license allows users to download, copy and build upon published chapters even for commercial purposes, as long as the author and publisher are properly credited, which ensures maximum dissemination and a wider impact of our publications. Notice Statements and opinions expressed in the chapters are these of the individual contributors and not necessarily those of the editors or publisher. No responsibility is accepted for the accuracy of information contained in the published chapters. The publisher assumes no responsibility for any damage or injury to persons or property arising out of the use of any materials, instructions, methods or ideas contained in the book. Publishing Process Manager Romana Vukelic Technical Editor Teodora Smiljanic Cover Designer InTech Design Team First published February, 2012 Printed in Croatia A free online edition of this book is available at www.intechopen.com Additional hard copies can be obtained from [email protected] Advances in Quantum Field Theory, Edited by Sergey Ketov p.
    [Show full text]
  • A Quantum Group in the Yang-Baxter Algebra
    A Quantum Group in the Yang-Baxter Algebra Alexandros Aerakis December 8, 2013 Abstract In these notes we mainly present theory on abstract algebra and how it emerges in the Yang-Baxter equation. First we review what an associative algebra is and then introduce further structures such as coalgebra, bialgebra and Hopf algebra. Then we discuss the con- struction of an universal enveloping algebra and how by deforming U[sl(2)] we obtain the quantum group Uq[sl(2)]. Finally, we discover that the latter is actually the Braid limit of the Yang-Baxter alge- bra and we use our algebraic knowledge to obtain the elements of its representation. Contents 1 Algebras 1 1.1 Bialgebra and Hopf algebra . 1 1.2 Universal enveloping algebra . 4 1.3 The quantum Uq[sl(2)] . 7 2 The Yang-Baxter algebra and the quantum Uq[sl(2)] 10 1 Algebras 1.1 Bialgebra and Hopf algebra To start with, the most familiar algebraic structure is surely that of an asso- ciative algebra. Definition 1 An associative algebra A over a field C is a linear vector space V equipped with 1 • Multiplication m : A ⊗ A ! A which is { bilinear { associative m(1 ⊗ m) = m(m ⊗ 1) that pictorially corresponds to the commutative diagram A ⊗ A ⊗ A −−−!1⊗m A ⊗ A ? ? ? ?m ym⊗1 y A ⊗ A −−−!m A • Unit η : C !A which satisfies the axiom m(η ⊗ 1) = m(1 ⊗ η) = 1: =∼ =∼ A ⊗ C A C ⊗ A ^ m 1⊗η > η⊗1 < A ⊗ A By reversing the arrows we get another structure which is called coalgebra.
    [Show full text]
  • Super-Exceptional Embedding Construction of the Heterotic M5
    Super-exceptional embedding construction of the heterotic M5: Emergence of SU(2)-flavor sector Domenico Fiorenza, Hisham Sati, Urs Schreiber June 2, 2020 Abstract A new super-exceptional embedding construction of the heterotic M5-brane’s sigma-model was recently shown to produce, at leading order in the super-exceptional vielbein components, the super-Nambu-Goto (Green- Schwarz-type) Lagrangian for the embedding fields plus the Perry-Schwarz Lagrangian for the free abelian self-dual higher gauge field. Beyond that, further fields and interactions emerge in the model, arising from probe M2- and probe M5-brane wrapping modes. Here we classify the full super-exceptional field content and work out some of its characteristic interactions from the rich super-exceptional Lagrangian of the model. We show that SU(2) U(1)-valued scalar and vector fields emerge from probe M2- and M5-branes wrapping × the vanishing cycle in the A1-type singularity; together with a pair of spinor fields of U(1)-hypercharge 1 and each transforming as SU(2) iso-doublets. Then we highlight the appearance of a WZW-type term in± the super-exceptional PS-Lagrangian and find that on the electromagnetic field it gives the first-order non-linear DBI-correction, while on the iso-vector scalar field it has the form characteristic of the coupling of vector mesons to pions via the Skyrme baryon current. We discuss how this is suggestive of a form of SU(2)-flavor chiral hadrodynamics emerging on the single (N = 1) M5 brane, different from, but akin to, holographiclarge-N QCD.
    [Show full text]