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Quantum Mechanics and the particles of nature: An outline for mathematicians PDF

369 Pages·1986·44.931 MB·English
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I Quantum mechanics and the particles of nature AN OUTLINE FOR MATHEMATICIANS ANTHONY SUDBERY Department of Mathematics, University of York Th~ ri'ght of thr Uniursil}' of Combridgr to print ond ull of/ manner of books was grontt'd by Henry VIII in JJJ4. The Univtrsit)' has printl'd and publishtd t'ontinU<Jwly Jincr 1584. CAMBRIDGE UNIVERSITY PRESS Cambridge London New York New Rochelle Melbourne Sydney Published by the Press Syndicate of the University of Cambridge The Pitt Building, Trumpington Street, Cambridge CB2 I RP 32 East 57th Street, New York, NY 10022, USA 10 Stamford Road, Oakleigh, Melbourne 3166, Australia 0 Cambridge University Press 1986 First published 1986 Printed in Great Britain at the University Press, Cambridge British Library cataloguing in publication data Sudbery, Anthony Quantum mechanics and the particles of nature. I. Quantum theory I. Title 530.1'2 QC174.12 Library of Congress cataloging-in-publication data Sudbery, Anthony. Quantum mechanics and the particles of nature. Bibliography: p. Includes index. I. Quantum theory. 2. Particles (Nuclear physics) I. Title. QC174.12.S89 1986 530.1'2 85-29124 ISBN 0 521 25891 X hard covers ISBN 0 521 27765 5 paperback MP Contents Preface xi 1 Particles and forces 1 A. THE ANALYSIS OF MATIER 1.1 Molecules and atoms 1 1.2 Electrons, protons and neutrons 3 1.3 Neutrinos 6 1.4 Antiparticles: baryons and leptons 8 Summary: the first four particles 10 1.5 Quarks and leptons 11 1.6 Observation of particles 16 B. THE ANALYSIS OF FORCE 17 I. 7 Kinds of force 1 7 1.8 Particles of force 19 Further reading 35 Problems 35 2 Quantum statics 36 2.1 Some examples 36 A note on probability 41 2.2 State space 43 2.3 The results of experiments 47 2.4 Observables 52 Operators and matrices 53; Hermitian conjugation 54; Statistical properties of observables 56; Compatibility of observables 57 2.5 Observables of a particle moving in space 59 A note on Hilbert space 67 2.6 Combined systems 68 Identical particles 70 Appendix: properties of hermitian and unitary operators 74 Bones of Chapter 2 75 Further reading 75 Problems 75 \'Ill Contents 3 Quantum dynamics 78 3.1 The equations of motion 78 I Rate of change of expectation value 82; The probability current 85; Boundary conditions for tire Sclrrodinger equation 85 3.2 lnvariances and constants of the motion 88 Parity 95; Time reversal 96; Combined systems 98; Transformation of observables 99; Actir;e and passh·e transformations /02 3.3 Groups of operations 103 3.4 The Heisenberg picture 109 3.5 Time-dependent perturbation theory Ill First-order theory 112; The phase-space factor in decay rates 116; Second-order theory 117; Interpretation: transition amplitudes 117: Dyson's form of the perturbation series 119: Exponential decay 120 3.6 Feynman's formulation of quantt,~m mechanics 123 Bones of Chapter 3 127 Further reading 117 Problems 127 4 Some quantum systems 133 4.1 Angular momentum 133 Orbital angular momentum 137: Spin 138; Spin-! particles 139; Rotation operators 139; The rotation group and SU(2) 141; Intrinsic parity 142: Massless particles 143 4.2 Addition of angular momentum 144 The Wigner-Eckart theorem 147 4.3 Two-particle systems 149 4.4 The hydrogen atom 153 Tire periodic table 157 4.5 The harmonic oscillator 158 The three-dimensional harmonic oscillator 160 4.6 Annihilation and creation operators 162 Bosonic systems 162: Fermionic systems 164; Several types of particle 166: Charge conjugation 167; Particle-changing interactions 169 Bones of Chapter 4 173 Further reading 174 Problems 17 4 5 Quantum metaphysics 178 5.1 Statistical formulations of classical and quantum mechanics 178 (a) Classical mechanics 178 (b) Quantum mechanics: the statistical operator 180 Combined systems 185 5.2 Quantum theory of measurement 185 Schrodinger's cat paradox 187; Properties of macroscopic apparatus 189; Continuous observation 191 5.3 Hidden variables and locality 194 The Einstein-Podolsk~Rosen paradox 194; Thede Broglie/Bohm pilot wave theory 196; Belrs inequalities 198 Contents ix 5.4 Alternative formulations of quantum mechanics 201 Algebraic formulations 201: Quantum logic 203; Superse/ection rules 208; Three-valued logic 209 5.5 Interpretations of quantum mechanics 210 Some meta-scientific vocabulary 2 10; The peculiarities of quantum mechanics 210; Nine interprerations 212: Conclusion 224 Bones of Chapter 5 224 Further Reading 225 Problems 225 6 Quantum numbers The properties of particles 227 6.1 Isospin 227 Isospin and charge conjugation 232; Irreducible isospin operators 234; lsospin in electromagnetic and weak interactions 236 6.2 Strangeness 238 Newral K-mesons 241: CP non-conservation 244 6.3 The eightfold way 244 Quark strucwre 250: SU(4, 5 and 6) 255 6.4 Hadron spectroscopy 256 Charm, beauty and truth 261 6.5 The colour force 265 Colour 265: Gluons 268: Asymptotic freedom and confinement 269: The Zweig rule 271 6.6 The electroweak force 273 Non-conservation of parity 273; The Sa/am-Weinberg Hamiltonian 276: Experimental confirmation of the Sa/am-Weinberg theory 280 6.7 Further speculations 281 Grand unification 281: Supersymmetry 283: Substructure 285 Further reading 286 Problems 286 7 Quantum fields 290 7.1 Field operators 290 (a) The electromagnetic field 290 Relativistic formulation 294 (b) Second quantisation 297 The Klein-Gordon equation 300 7.2 The Dirac equation 301 Parity 305: Spinor bilinears 305; Second quantisation 309 7.3 Field dynamics 311 In variances and conserved quantities 314; quantum electrodynamics 317: renormalisation 319 7.4 Gauge theories 320 Quantum chromodynamics 324 7.5 Hidden symmetries 325 Self-interacting fields 325; Global symmetry: Goldstone bosons 326; Hidden local symmetry: the Higgs mechanism 329 X Contents 7.6 Quantum navourdynamics 331 Bones of Chapter 7 334 Further reading 335 Problems 335 Appendix 1: 3-vector and 4-vector algebra 337 Appendix II: Particle properties 340 Appendix Ill: Clebsch--Gordan coefficients 342 Answers to all(/ help with problems 346 Bibliography 350 Index 354 Preface This book is addressed to the reader who wants, as an educated person, to have an outline of the present state of knowledge of the constituents of the material world; who has a logical cast of mind and will follow a mathematical argument; but who may have little knowledge of physics and no intention of becoming deeply involved in the subject. In practice I have imagined this reader as a mathematics student taking a third-year undergraduate course in quantum mechanics such as is commonly offered as a part of the mathematics degree course in British universities. Only a minority of such students will be intending to pursue the subject further, and it seems more appropriate to aim for a wide survey of the interesting bits than to try to provide a sound basis for a training as a quantum mechanic. The emphasis in the book, therefore, is on providing a coherent account of the basic theoretical concepts of quantum mechanics and particle physics. Experimental detail, mathematical rigour and calculational facility are all given lower priority than conceptual coherence. However, I hope that I have given sufficient experimental reason for every major statement of theory; that the mathematics is honest, with gaps acknowledged and without the inconsistencies which can puzzle and dishearten (or arouse the scorn of) mathematics students; and that there are enough problems at the end of chapters to enable readers to test their grasp of the concepts. This approach to the subject has led me to omit several topics which would normally be included in a quantum mechanics course; for example, there is no scattering theory and little discussion of the Schrodinger equation as a differential equation. These topics may be indispensable to anyone who wants to work in the area, but they are not actually needed in explaining the results of the research in which they were tools. On the other hand, there are conceptual problems which can be (and often have been) ignored by the working physicist, but which seem much more important to the spectator who wants to understand more of the game. These metaphysical problems often arouse great interest in students, who find that it is poorly catered for in quantum mechanics textbooks (perhaps because the discussion is likely to be either Xll Preface inconclusive or unconvincing, and quite possibly both). I have devoted a chapter to such problems; it is indeed inconclusive, and may well be unconvmcmg. The reading of mathematics and physics books is hopefully embarked upon more often than it is successfully completed. This fact of human nature is allowed for in the structure of this book, which has several points at which a reader can feel that they have reached the end of a journey. Thereafter the journey is started again, but in a different craft and at a different level. The first chapter is a general description of the structure of matter, leading to the introduction of quarks and leptons, and an account of the first ideas of quantum mechanics. This material will be familiar to many students, but not to all; it is included to make the book accessible to mathematics students who may have studied no physics, or have forgotten what they have studied, and to meet the complaint that books on particle physics always assume that you a!r eady know about particles. At the end of this chapter the reader will know what the particles of matter are, and what forces act between them. The next two chapters contain the theoretical development of quantum mechanics, in the state-vector formalism with its standard interpretation. At the end of Chapter 3 the reader will know the basic assumptions and theoretical apparatus of quantum theory. Chapter 4 continues the study of quantum mechanics, but should perhaps be regarded as a prelude to the remaining chapters, being largely concerned with constructing more apparatus for later use (angular momentum theory, annihilation and creation operators), though it also contains the theory of the hydrogen atom as being of intrinsic interest. The last three chapters provide three independent journeys, which can be taken in any order. Chapter 5 goes over the ground of Chapters 2 and 3 again, examining the concepts of quantum mechanics more critically. This journey ends in a muddy river delta, the mainstream having split into nine mouths. Chapter 6 goes over the ground of Chapter 1, the language of quantum mechanics now being available for a more detailed description of particles. Annihilation and creation operators are used to give a simplified treatment of the forces between particles- a kind of quantum field theory without space and time. Finally, the ideas of quantum field theory proper are described in Chapter 7. The first half of this chapter is a continuation of the formal development of quantum mechanics, and carries on directly from Chapter 4. The second half describes how quantum field theory is applied to particle physics in quantum chromodynamics and quantum flavourdynamics, and constitutes a third passage over the ground of particle physics. Although the development is not formally axiomatic, the book does have a logical skeleton consisting of postulates (stated as such) and a chain of propositi-ons (marked by the symbol e) deduced from them. The bones are listed at the end of each chapter (except Chapters 1 and 6, which are cartilaginous). The. mathematical arguments are not as rigorous as they might Preface XIII be, but the physical arguments are slightly more rigorous than they often are. The mathematical style is mainly algebraic, being based on commutation relations: the notion of a wave function is not needed in this logical skeleton. (The spectrum of the hydrogen atom is found by Pauli's original method, which predates the Schrodinger equation.} However, since it would be an impoverished idea of quantum mechanics that did not include wave functions, and since students arc likely to have met them elsewhere, they are included from the beginning as an example of a type of state vector, and the usual assumptions about them (e.g. boundary conditions for the Schrodinger equation) are justified. Teachers of quantum mechanics arc divided, and no doubt always will be, about the suitability of the state-vector formalism for a first course in quantum mechanics. Those who, like myself, first learnt quantum mechanics by reading Dirac's immortal Pri11ciples have no doubt that the state-vector formalism is the best introduction to the subject.ln deference to the other half of the world I have to say that this book mighr be found difficult by students who have not taken a first course on quantum mechanics based on wave functions. Formally, however, it requires no knowledge of any physics. Formally, also, the only mathematics required is vector algebra and vector calculus; but the reader with no knowledge of linear algebra will probably find it heavy going, and an acquaintance with the idea of a group and the elements of analytical mechanics will be helpful in places. Until Chapter 7 the only fact from special relativity that is used is the energy-momentum relation ( 1.5); for Chapter 7 the reader will need the 4-vector formalism and a knowledge of Maxwell's equations. Bold type is used to indicate that a word or phrase is being defined, and the reader is not expected to know what it means. The symbol • denotes the end of a proof (or a proposition whose proof has already appeared). Complex conjugation is denoted by an overbar (not by an asterisk). I would like to thank Mark Lawson, Chris Clarke, Richard Crossley, Peter Landshoff, Ian Drummond, Jeremy Rogers, Stephen McGahan, Alison Ramsay. Clifford Bishop, Denis Cronin, Roland Hall, Anne Thompson and Steve Roberts, all of whom read parts of the manuscript and made useful suggestions. I am grateful to the Scientific Information Service of CERN, Geneva, for supplying me with photographs and for their permission to use them. Finally, I would like to record my appreciation of the sensitive and patient editorship of Simon Capel in, and the care and forbearance of Sheila Shepherd and the other staff of Cambridge University Press. Tony Sudbery York, July 1985

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