Symmetries in Quantum Physics
|
|
- Lydia Chapman
- 5 years ago
- Views:
Transcription
1 Symmetries in Quantum Physics U. Fano Department of Physics and James Franck Institute University of Chicago Chicago, Illinois A. R. P. Rau Department of Physics and Astronomy louisiana State University Baton Rouge, louisiana Academic Press San Diego New York Boston London Sydney Tokyo Toronto
2 Contents Preface xiii 1 Introduction 1 Transformation Theories: Klein's and Dirac's Symmetry and the Selection of Variables Examples of tensorial equations Algebraic Elements Vectors, tensors, and related quantities Addition and direct product of tensorial sets Linear transformation Reduction Procedure and Irreducible Tensorial Sets An analytical example: Reduction of tensors Further Aspects of Reduction Reduction procedures Labeling of set elements Block diagonalization of the reduction Phase normalization Group theory Reduction as an expansion into eigenfunctions Structure of the Book Alternative sets of commuting invariant operators Quaternions 28 Problems 29 v
3 vi PART A STATE REPRESENTATIVES AND r-transformations: THEIR CONSTRUCTION AND PROPERTIES 2 Infinitesimal Rotations and Angular Momentum Basic Relations Analytical Example: Infinitesimal Transformation of Cartesian Coordinates The Angular Momentum Matrices of Quantum Mechanics Phase normalization Definition of a standard base The Fundamental Representation Significance of half-integer j 47 Problems 49 3 Frame Reversal and Complex Conjugation Analytical Representation and Implications of Frame Reversal Explicit form of the matrix U Properties of the matrix U Contragredience and the Construction of Invariants Contragredient tensorial sets Invariant products Notation Cartesian Base for Integer j > Cartesian-to-standard transformation Phase normalization of spherical harmonics 72 Problems 74 4 Standard r-transformation Matrices and Their Applications Explicit Form and Properties Spinor method 78
4 Vll Algebraic approach First order differential system Second order differential equation Symmetries of the standard r-transformations Integrals r-transformations in the Cartesian frame Macroscopic Applications Applications to Quantum Physics Particle transmission through a Stern-Gerlach magnet Angular distribution of a particle in orbital motion Rotational eigenfunctions and eigenvalues for symmetric-top polyatomic molecules and heteronuclear diatomics Spinor and vector harmonics Coordinate Inversion and Parity Eigenfunctions 93 Problems 97 5 Reduction of Direct Products (Addition of Angular Momenta) Structure and Properties of the Reducing Matrix Spinor approach Normalization Recurrence relations Symmetries Reduction in the Cartesian frame Reduction of r-transformation Products Irreducible Product Sets Special cases Symmetry Products of contragredient sets Wave-mechanical examples Multiple products Coupling diagrams Symmetrization of Wigner Coefficients: Invariant Triple Product and 3-j Coefficients 119 Problems. 123
5 Vlll PART В TENSORIAL ASPECTS OF QUANTUM PHYSICS 6 Tensorial Sets of Quantum Operators The Liouville Representation of Quantum Mechanics Quantum Mechanics of Particles with Spin Base sets of matrices and operators Two-Level Systems Atom in a radiation field Light polarization and Stokes parameters Further applications of two-level systems: Occupation, creation, and annihilation operators Particles with Spin j> : Wigner-Eckart Theorem Density matrix Multipole expansion of operators G Physical implications of the triangular relation к < 2j Systems with 2j + l Levels Transfer of Angular Momentum Calculation of Matrix Elements 150 Problems Recoupling Transformations: 6-j and 9-j Coefficients Transformation Matrices and Their Analysis Diagrams Group properties Factorization of transformations Symmetrized Recoupling: 6-j and 9-j Coefficients j coefficients j coefficients Alternative perspectives Products of Operators Unit operators General operator Commutators Schrödinger equation for a (2j + l)-level system Combining Operators of Different Systems 183
6 IX 7.5 Illustrations Interaction matrix elements Projection of operators Correlations 191 Problems Partially Filled Shells of Atoms or Nuclei Qualitative Discussion Two-particle states States of three or more equivalent particles Quantum numbers for many-particle states Shell-wide Treatment Triple tensors and their matrices Coefficients of fractional parentage Algebra of Triple Tensors and Its Applications Interpretation of Х(*«*.*г) Quasi-spin and seniority Quasiparticles for the / shell Determination of fractional parentage Operator matrices 224 PART С SYMMETRIES OF HIGHER DIMENSIONS 9 Discrete Transformations of Coordinates Point Symmetry Operations and Their Groups Characters of Group Representations and Their Applications Abelian groups Non-Abelian groups Characters of the rotation group 50(3) Reduction of representations Reduction of set products Symmetries of Molecules and Crystals 243
7 X Symmetry combinations Vibrational motions Molecular rotations Stability analysis of nuclear positions 246 Problems Rotation Groups in Higher Dimensions: Multiparticle Problems Four-Dimensional Rotations: The Coulomb-Kepler Problem Spherical and parabolic representations Rotations in four dimensions Hydrogen atom in momentum space Alternative subgroups of 50(4): The hydrogen atom in external fields Clebsch-Gordan coefficients for products of 50(4) Orthogonal Groups in Higher Dimensions Hypersphere in D dimensions Hyperspherical coordinates for multiparticle systems Transformation between alternative schemes Further Developments Invariance and noninvariance groups "Dynamical symmetries" for atoms and nuclei Adjoining an extra degree of freedom Alternative reduction schemes for multiparticle systems Lorentz Transformations and the Lorentz and Poincare Groups Lorentz Transformations Generators and Representations of the Lorentz Group Four-vectors and the Lorentz metric Generators of the proper Lorentz group Lorentz transformations to r-transformations Spinor representations Neutrino and electron spinor states Electromagnetism and its quantum The Inhomogeneous Lorentz (Poincare) Group Generators and commutation relationships 296
8 11.4 Field Representations Massive systems Representations of massless entities Symmetries of the Scattering Continuum Symmetries of Radial Eigenfunctions The Full Noninvariance Group of Hydrogen Alternative decompositions of the noninvariance group Dynamics and Symmetry Transformations 310 Bibliography 313 Index 317
GROUP THEORY IN PHYSICS
GROUP THEORY IN PHYSICS Wu-Ki Tung World Scientific Philadelphia Singapore CONTENTS CHAPTER 1 CHAPTER 2 CHAPTER 3 CHAPTER 4 PREFACE INTRODUCTION 1.1 Particle on a One-Dimensional Lattice 1.2 Representations
More informationLECTURES ON QUANTUM MECHANICS
LECTURES ON QUANTUM MECHANICS GORDON BAYM Unitsersity of Illinois A II I' Advanced Bock Progrant A Member of the Perseus Books Group CONTENTS Preface v Chapter 1 Photon Polarization 1 Transformation of
More informationThe Raman Effect. A Unified Treatment of the Theory of Raman Scattering by Molecules. DerekA. Long
The Raman Effect A Unified Treatment of the Theory of Raman Scattering by Molecules DerekA. Long Emeritus Professor ofstructural Chemistry University of Bradford Bradford, UK JOHN WILEY & SONS, LTD Vll
More informationMOLECULAR SPECTROSCOPY
MOLECULAR SPECTROSCOPY First Edition Jeanne L. McHale University of Idaho PRENTICE HALL, Upper Saddle River, New Jersey 07458 CONTENTS PREFACE xiii 1 INTRODUCTION AND REVIEW 1 1.1 Historical Perspective
More informationGroup Theory and Its Applications in Physics
T. Inui Y Tanabe Y. Onodera Group Theory and Its Applications in Physics With 72 Figures Springer-Verlag Berlin Heidelberg New York London Paris Tokyo Hong Kong Barcelona Contents Sections marked with
More informationNotes on Quantum Mechanics
Notes on Quantum Mechanics K. Schulten Department of Physics and Beckman Institute University of Illinois at Urbana Champaign 405 N. Mathews Street, Urbana, IL 61801 USA (April 18, 2000) Preface i Preface
More informationP. W. Atkins and R. S. Friedman. Molecular Quantum Mechanics THIRD EDITION
P. W. Atkins and R. S. Friedman Molecular Quantum Mechanics THIRD EDITION Oxford New York Tokyo OXFORD UNIVERSITY PRESS 1997 Introduction and orientation 1 Black-body radiation 1 Heat capacities 2 The
More informationQuantum Mechanics: Fundamentals
Kurt Gottfried Tung-Mow Yan Quantum Mechanics: Fundamentals Second Edition With 75 Figures Springer Preface vii Fundamental Concepts 1 1.1 Complementarity and Uncertainty 1 (a) Complementarity 2 (b) The
More informationSymmetries in Physics
W. Ludwig C. Falter Symmetries in Physics Group Theory Applied to Physical Problems With 87 Figures Springer-Verlag Berlin Heidelberg New York London Paris Tokyo Contents 1. Introduction 1 2. Elements
More informationQUANTUM MECHANICS. Franz Schwabl. Translated by Ronald Kates. ff Springer
Franz Schwabl QUANTUM MECHANICS Translated by Ronald Kates Second Revised Edition With 122Figures, 16Tables, Numerous Worked Examples, and 126 Problems ff Springer Contents 1. Historical and Experimental
More informationCoupling of Angular Momenta Isospin Nucleon-Nucleon Interaction
Lecture 5 Coupling of Angular Momenta Isospin Nucleon-Nucleon Interaction WS0/3: Introduction to Nuclear and Particle Physics,, Part I I. Angular Momentum Operator Rotation R(θ): in polar coordinates the
More informationQUANTUM MECHANIC S. Symmetries
Walter Greiner Berndt Müller QUANTUM MECHANIC S Symmetries 1. Symmetries in Quantum Mechanics 1 1.1 Symmetries in Classical Physics 1 1.2 Spatial Translations in Quantum Mechanics 1 9 1.3 The Unitary
More informationQuantum Mechanics: Foundations and Applications
Arno Böhm Quantum Mechanics: Foundations and Applications Third Edition, Revised and Enlarged Prepared with Mark Loewe With 96 Illustrations Springer-Verlag New York Berlin Heidelberg London Paris Tokyo
More informationmsqm 2011/8/14 21:35 page 189 #197
msqm 2011/8/14 21:35 page 189 #197 Bibliography Dirac, P. A. M., The Principles of Quantum Mechanics, 4th Edition, (Oxford University Press, London, 1958). Feynman, R. P. and A. P. Hibbs, Quantum Mechanics
More informationPRINCIPLES OF PHYSICS. \Hp. Ni Jun TSINGHUA. Physics. From Quantum Field Theory. to Classical Mechanics. World Scientific. Vol.2. Report and Review in
LONDON BEIJING HONG TSINGHUA Report and Review in Physics Vol2 PRINCIPLES OF PHYSICS From Quantum Field Theory to Classical Mechanics Ni Jun Tsinghua University, China NEW JERSEY \Hp SINGAPORE World Scientific
More informationPractical Quantum Mechanics
Siegfried Flügge Practical Quantum Mechanics With 78 Figures Springer-Verlag Berlin Heidelberg New York London Paris Tokyo Hong Kong Barcelona Budapest Contents Volume I I. General Concepts 1. Law of probability
More informationSpectra of Atoms and Molecules. Peter F. Bernath
Spectra of Atoms and Molecules Peter F. Bernath New York Oxford OXFORD UNIVERSITY PRESS 1995 Contents 1 Introduction 3 Waves, Particles, and Units 3 The Electromagnetic Spectrum 6 Interaction of Radiation
More informationLecture Notes. Quantum Theory. Prof. Maximilian Kreuzer. Institute for Theoretical Physics Vienna University of Technology. covering the contents of
Lecture Notes Quantum Theory by Prof. Maximilian Kreuzer Institute for Theoretical Physics Vienna University of Technology covering the contents of 136.019 Quantentheorie I and 136.027 Quantentheorie II
More informationTopics for the Qualifying Examination
Topics for the Qualifying Examination Quantum Mechanics I and II 1. Quantum kinematics and dynamics 1.1 Postulates of Quantum Mechanics. 1.2 Configuration space vs. Hilbert space, wave function vs. state
More informationCONTENTS. vii. CHAPTER 2 Operators 15
CHAPTER 1 Why Quantum Mechanics? 1 1.1 Newtonian Mechanics and Classical Electromagnetism 1 (a) Newtonian Mechanics 1 (b) Electromagnetism 2 1.2 Black Body Radiation 3 1.3 The Heat Capacity of Solids and
More informationwhich implies that we can take solutions which are simultaneous eigen functions of
Module 1 : Quantum Mechanics Chapter 6 : Quantum mechanics in 3-D Quantum mechanics in 3-D For most physical systems, the dynamics is in 3-D. The solutions to the general 3-d problem are quite complicated,
More informationQUANTUM MECHANICS SECOND EDITION G. ARULDHAS
QUANTUM MECHANICS SECOND EDITION G. ARULDHAS Formerly, Professor and Head of Physics and Dean, Faculty of Science University of Kerala New Delhi-110001 2009 QUANTUM MECHANICS, 2nd Ed. G. Aruldhas 2009
More informationQuantum. Mechanics. Y y. A Modern Development. 2nd Edition. Leslie E Ballentine. World Scientific. Simon Fraser University, Canada TAIPEI BEIJING
BEIJING TAIPEI Quantum Mechanics A Modern Development 2nd Edition Leslie E Ballentine Simon Fraser University, Canada Y y NEW JERSEY LONDON SINGAPORE World Scientific SHANGHAI HONG KONG CHENNAI Contents
More informationPart I. Many-Body Systems and Classical Field Theory
Part I. Many-Body Systems and Classical Field Theory 1. Classical and Quantum Mechanics of Particle Systems 3 1.1 Introduction. 3 1.2 Classical Mechanics of Mass Points 4 1.3 Quantum Mechanics: The Harmonic
More informationMaxwell s equations. based on S-54. electric field charge density. current density
Maxwell s equations based on S-54 Our next task is to find a quantum field theory description of spin-1 particles, e.g. photons. Classical electrodynamics is governed by Maxwell s equations: electric field
More informationPhysics of atoms and molecules
Physics of atoms and molecules 2nd edition B.H. Bransden and C.J. Joachain Prentice Hall An imprint of Pearson Education Harlow, England London New York Boston San Francisco Toronto Sydney Singapore Hong
More informationLie Algebras in Particle Physics
Lie Algebras in Particle Physics Second Edition Howard Georgi S WieW Advanced Book Program A Member of the Perseus Books Group Contents Why Group Theory? 1 1 Finite Groups 2 1.1 Groups and representations
More informationQuantum Physics II (8.05) Fall 2002 Outline
Quantum Physics II (8.05) Fall 2002 Outline 1. General structure of quantum mechanics. 8.04 was based primarily on wave mechanics. We review that foundation with the intent to build a more formal basis
More informationIntroduction to Modern Physics
SECOND EDITION Introduction to Modern Physics John D. McGervey Case Western Reserve University Academic Press A Subsidiary of Harcourt Brace Jovanovich Orlando San Diego San Francisco New York London Toronto
More informationChemistry 483 Lecture Topics Fall 2009
Chemistry 483 Lecture Topics Fall 2009 Text PHYSICAL CHEMISTRY A Molecular Approach McQuarrie and Simon A. Background (M&S,Chapter 1) Blackbody Radiation Photoelectric effect DeBroglie Wavelength Atomic
More informationMaxwell s equations. electric field charge density. current density
Maxwell s equations based on S-54 Our next task is to find a quantum field theory description of spin-1 particles, e.g. photons. Classical electrodynamics is governed by Maxwell s equations: electric field
More informationAn Introduction to the Standard Model of Particle Physics
An Introduction to the Standard Model of Particle Physics W. N. COTTINGHAM and D. A. GREENWOOD Ж CAMBRIDGE UNIVERSITY PRESS Contents Preface. page xiii Notation xv 1 The particle physicist's view of Nature
More informationLok С. Lew Yan Voon Morten Willatzen. The k-p Method. Electronic Properties of Semiconductors. Springer
Lok С. Lew Yan Voon Morten Willatzen The k-p Method Electronic Properties of Semiconductors Springer Acronyms xxi 1 Introduction 1 1.1 What Is к p Theory? 1 1.2 Electronic Properties of Semiconductors
More informationIntroduction to Modern Quantum Field Theory
Department of Mathematics University of Texas at Arlington Arlington, TX USA Febuary, 2016 Recall Einstein s famous equation, E 2 = (Mc 2 ) 2 + (c p) 2, where c is the speed of light, M is the classical
More informationGROUP REPRESENTATION THEORY FOR PHYSICISTS
GROUP REPRESENTATION THEORY FOR PHYSICISTS JIN-QUAN CHEN Vfe World Scientific wl Singapore New Jersey London Hong Kong Contents Foreword Preface Glossary v vii xix Introduction 1 Chapter 1 Elements of
More informationNuclear models: Collective Nuclear Models (part 2)
Lecture 4 Nuclear models: Collective Nuclear Models (part 2) WS2012/13: Introduction to Nuclear and Particle Physics,, Part I 1 Reminder : cf. Lecture 3 Collective excitations of nuclei The single-particle
More informationIntroduction to Mathematical Physics
Introduction to Mathematical Physics Methods and Concepts Second Edition Chun Wa Wong Department of Physics and Astronomy University of California Los Angeles OXFORD UNIVERSITY PRESS Contents 1 Vectors
More informationTotal Angular Momentum for Hydrogen
Physics 4 Lecture 7 Total Angular Momentum for Hydrogen Lecture 7 Physics 4 Quantum Mechanics I Friday, April th, 008 We have the Hydrogen Hamiltonian for central potential φ(r), we can write: H r = p
More informationLectures on Quantum Mechanics
Lectures on Quantum Mechanics Steven Weinberg The University of Texas at Austin CAMBRIDGE UNIVERSITY PRESS Contents PREFACE page xv NOTATION xviii 1 HISTORICAL INTRODUCTION 1 1.1 Photons 1 Black-body radiation
More informationStudents are required to pass a minimum of 15 AU of PAP courses including the following courses:
School of Physical and Mathematical Sciences Division of Physics and Applied Physics Minor in Physics Curriculum - Minor in Physics Requirements for the Minor: Students are required to pass a minimum of
More informationMODERN PHYSICS Frank J. Blatt Professor of Physics, University of Vermont
MODERN PHYSICS Frank J. Blatt Professor of Physics, University of Vermont McGRAW-HILL, INC. New York St. Louis San Francisco Auckland Bogota Caracas Lisbon London Madrid Mexico Milan Montreal New Delhi
More informationB. PHENOMENOLOGICAL NUCLEAR MODELS
B. PHENOMENOLOGICAL NUCLEAR MODELS B.0. Basic concepts of nuclear physics B.0. Binding energy B.03. Liquid drop model B.04. Spherical operators B.05. Bohr-Mottelson model B.06. Intrinsic system of coordinates
More informationRepresentations of Lorentz Group
Representations of Lorentz Group based on S-33 We defined a unitary operator that implemented a Lorentz transformation on a scalar field: How do we find the smallest (irreducible) representations of the
More informationQuantum Physics in the Nanoworld
Hans Lüth Quantum Physics in the Nanoworld Schrödinger's Cat and the Dwarfs 4) Springer Contents 1 Introduction 1 1.1 General and Historical Remarks 1 1.2 Importance for Science and Technology 3 1.3 Philosophical
More informationCLASSICAL ELECTRICITY
CLASSICAL ELECTRICITY AND MAGNETISM by WOLFGANG K. H. PANOFSKY Stanford University and MELBA PHILLIPS Washington University SECOND EDITION ADDISON-WESLEY PUBLISHING COMPANY Reading, Massachusetts Menlo
More informationPlan for the rest of the semester. ψ a
Plan for the rest of the semester ϕ ψ a ϕ(x) e iα(x) ϕ(x) 167 Representations of Lorentz Group based on S-33 We defined a unitary operator that implemented a Lorentz transformation on a scalar field: and
More informationLecture 10: A (Brief) Introduction to Group Theory (See Chapter 3.13 in Boas, 3rd Edition)
Lecture 0: A (Brief) Introduction to Group heory (See Chapter 3.3 in Boas, 3rd Edition) Having gained some new experience with matrices, which provide us with representations of groups, and because symmetries
More informationQuantum Field Theory
Quantum Field Theory PHYS-P 621 Radovan Dermisek, Indiana University Notes based on: M. Srednicki, Quantum Field Theory 1 Attempts at relativistic QM based on S-1 A proper description of particle physics
More informationAttempts at relativistic QM
Attempts at relativistic QM based on S-1 A proper description of particle physics should incorporate both quantum mechanics and special relativity. However historically combining quantum mechanics and
More informationAPPLIED PARTIAL DIFFERENTIAL EQUATIONS
APPLIED PARTIAL DIFFERENTIAL EQUATIONS AN I N T R O D U C T I O N ALAN JEFFREY University of Newcastle-upon-Tyne ACADEMIC PRESS An imprint of Elsevier Science Amsterdam Boston London New York Oxford Paris
More informationLINEAR ALGEBRA AND iroup THEORY FOR PHYSICISTS
LINEAR ALGEBRA AND iroup THEORY FOR PHYSICISTS K.N. SRINIVASA RAO Professor of Theoretical Physics (Retd) University of Mysore, Mysore, INDIA JOHN WILEY «SONS NEW YORK CHICHESTER BRISBANE TORONTO SINGAPORE
More informationQuantum Field Theory. Kerson Huang. Second, Revised, and Enlarged Edition WILEY- VCH. From Operators to Path Integrals
Kerson Huang Quantum Field Theory From Operators to Path Integrals Second, Revised, and Enlarged Edition WILEY- VCH WILEY-VCH Verlag GmbH & Co. KGaA I vh Contents Preface XIII 1 Introducing Quantum Fields
More informationChemistry 881 Lecture Topics Fall 2001
Chemistry 881 Lecture Topics Fall 2001 Texts PHYSICAL CHEMISTRY A Molecular Approach McQuarrie and Simon MATHEMATICS for PHYSICAL CHEMISTRY, Mortimer i. Mathematics Review (M, Chapters 1,2,3 & 4; M&S,
More informationModern Geometric Structures and Fields
Modern Geometric Structures and Fields S. P. Novikov I.A.TaJmanov Translated by Dmitry Chibisov Graduate Studies in Mathematics Volume 71 American Mathematical Society Providence, Rhode Island Preface
More informationPhysics 221A Fall 2017 Notes 20 Parity
Copyright c 2017 by Robert G. Littlejohn Physics 221A Fall 2017 Notes 20 Parity 1. Introduction We have now completed our study of proper rotations in quantum mechanics, one of the important space-time
More informationLecture 4 Quantum mechanics in more than one-dimension
Lecture 4 Quantum mechanics in more than one-dimension Background Previously, we have addressed quantum mechanics of 1d systems and explored bound and unbound (scattering) states. Although general concepts
More information129 Lecture Notes More on Dirac Equation
19 Lecture Notes More on Dirac Equation 1 Ultra-relativistic Limit We have solved the Diraction in the Lecture Notes on Relativistic Quantum Mechanics, and saw that the upper lower two components are large
More informationLecture #1. Review. Postulates of quantum mechanics (1-3) Postulate 1
L1.P1 Lecture #1 Review Postulates of quantum mechanics (1-3) Postulate 1 The state of a system at any instant of time may be represented by a wave function which is continuous and differentiable. Specifically,
More information11 Spinor solutions and CPT
11 Spinor solutions and CPT 184 In the previous chapter, we cataloged the irreducible representations of the Lorentz group O(1, 3. We found that in addition to the obvious tensor representations, φ, A
More informationAngular Momentum in Quantum Mechanics
Angular Momentum in Quantum Mechanics In classical mechanics the angular momentum L = r p of any particle moving in a central field of force is conserved. For the reduced two-body problem this is the content
More informationParticle Physics. Michaelmas Term 2011 Prof. Mark Thomson. Handout 2 : The Dirac Equation. Non-Relativistic QM (Revision)
Particle Physics Michaelmas Term 2011 Prof. Mark Thomson + e - e + - + e - e + - + e - e + - + e - e + - Handout 2 : The Dirac Equation Prof. M.A. Thomson Michaelmas 2011 45 Non-Relativistic QM (Revision)
More informationAngular momentum. Quantum mechanics. Orbital angular momentum
Angular momentum 1 Orbital angular momentum Consider a particle described by the Cartesian coordinates (x, y, z r and their conjugate momenta (p x, p y, p z p. The classical definition of the orbital angular
More informationPhysics 221A Fall 1996 Notes 14 Coupling of Angular Momenta
Physics 1A Fall 1996 Notes 14 Coupling of Angular Momenta In these notes we will discuss the problem of the coupling or addition of angular momenta. It is assumed that you have all had experience with
More informationAngular Momentum. Classical. J r p. radius vector from origin. linear momentum. determinant form of cross product iˆ xˆ J J J J J J
Angular Momentum Classical r p p radius vector from origin linear momentum r iˆ ˆj kˆ x y p p p x y determinant form of cross product iˆ xˆ ˆj yˆ kˆ ˆ y p p x y p x p y x x p y p y x x y Copyright Michael
More informationTensor Calculus, Relativity, and Cosmology
Tensor Calculus, Relativity, and Cosmology A First Course by M. Dalarsson Ericsson Research and Development Stockholm, Sweden and N. Dalarsson Royal Institute of Technology Stockholm, Sweden ELSEVIER ACADEMIC
More informationIntroduction to Group Theory
Chapter 10 Introduction to Group Theory Since symmetries described by groups play such an important role in modern physics, we will take a little time to introduce the basic structure (as seen by a physicist)
More informationELECTROMAGNETIC FIELDS AND RELATIVISTIC PARTICLES
ELECTROMAGNETIC FIELDS AND RELATIVISTIC PARTICLES Emil J. Konopinski Professor of Physics Indiana University McGraw-Hill Book Company New York St. Louis San Francisco Auckland Bogota Hamburg Johannesburg
More information9 Electron orbits in atoms
Physics 129b Lecture 15 Caltech, 02/22/18 Reference: Wu-Ki-Tung, Group Theory in physics, Chapter 7. 9 Electron orbits in atoms Now let s see how our understanding of the irreps of SO(3) (SU(2)) can help
More informationINTRODUCTION TO THE STRUCTURE OF MATTER
INTRODUCTION TO THE STRUCTURE OF MATTER A Course in Modern Physics John J. Brehm and William J. Mullin University of Massachusetts Amherst, Massachusetts Fachberelch 5?@8hnlsdie Hochschule Darmstadt! HochschulstraSa
More informationParticle Physics Dr. Alexander Mitov Handout 2 : The Dirac Equation
Dr. A. Mitov Particle Physics 45 Particle Physics Dr. Alexander Mitov µ + e - e + µ - µ + e - e + µ - µ + e - e + µ - µ + e - e + µ - Handout 2 : The Dirac Equation Dr. A. Mitov Particle Physics 46 Non-Relativistic
More information3. Quantum Mechanics in 3D
3. Quantum Mechanics in 3D 3.1 Introduction Last time, we derived the time dependent Schrödinger equation, starting from three basic postulates: 1) The time evolution of a state can be expressed as a unitary
More informationAngular Momentum Techniques in Quantum Mechanics
Angular Momentum Techniques in Quantum Mechanics Fundamental Theories of Physics An International Book Series on The Fundamental Theories of Physics: Their Clarification, Development and Application Editor:
More informationQuantum Field Theory 2 nd Edition
Quantum Field Theory 2 nd Edition FRANZ MANDL and GRAHAM SHAW School of Physics & Astromony, The University of Manchester, Manchester, UK WILEY A John Wiley and Sons, Ltd., Publication Contents Preface
More informationPhysics 221A Fall 1996 Notes 21 Hyperfine Structure in Hydrogen and Alkali Atoms
Physics 221A Fall 1996 Notes 21 Hyperfine Structure in Hydrogen and Alkali Atoms Hyperfine effects in atomic physics are due to the interaction of the atomic electrons with the electric and magnetic multipole
More informationProblem 1: Spin 1 2. particles (10 points)
Problem 1: Spin 1 particles 1 points 1 Consider a system made up of spin 1/ particles. If one measures the spin of the particles, one can only measure spin up or spin down. The general spin state of a
More informationHigh Collection Nonimaging Optics
High Collection Nonimaging Optics W. T. WELFORD Optics Section Department of Physics Imperial College of Science, Technology and Medicine University of London London, England R. WINSTON Enrico Fermi Institute
More informationRelativistic Waves and Quantum Fields
Relativistic Waves and Quantum Fields (SPA7018U & SPA7018P) Gabriele Travaglini December 10, 2014 1 Lorentz group Lectures 1 3. Galileo s principle of Relativity. Einstein s principle. Events. Invariant
More informationComparing and Improving Quark Models for the Triply Bottom Baryon Spectrum
Comparing and Improving Quark Models for the Triply Bottom Baryon Spectrum A thesis submitted in partial fulfillment of the requirements for the degree of Bachelor of Science degree in Physics from the
More informationThe 3 dimensional Schrödinger Equation
Chapter 6 The 3 dimensional Schrödinger Equation 6.1 Angular Momentum To study how angular momentum is represented in quantum mechanics we start by reviewing the classical vector of orbital angular momentum
More informationSpin, Isospin and Strong Interaction Dynamics
October, 11 PROGRESS IN PHYSICS Volume 4 Spin, Isospin and Strong Interaction Dynamics Eliahu Comay Charactell Ltd. P.O. Box 3919, Tel Aviv 6139 Israel. E-mail: elicomay@post.tau.ac.il The structure of
More informationPrinciples of Electron Optics
Principles of Electron Optics Volume 1 Basic Geometrical Optics by P. W. HAWKES CNRS Laboratory of Electron Optics, Toulouse, France and E. KASPER Institut für Angewandte Physik Universität Tübingen, Federal
More information16. GAUGE THEORY AND THE CREATION OF PHOTONS
6. GAUGE THEORY AD THE CREATIO OF PHOTOS In the previous chapter the existence of a gauge theory allowed the electromagnetic field to be described in an invariant manner. Although the existence of this
More informationChapter 1. Introduction
Chapter 1 Introduction The book Introduction to Modern Physics: Theoretical Foundations starts with the following two paragraphs [Walecka (2008)]: At the end of the 19th century, one could take pride in
More informationTHEORY OF GROUP REPRESENTATIONS AND APPLICATIONS
THEORY OF GROUP REPRESENTATIONS AND APPLICATIONS ASIM 0. BARUT Institute for Theoretical Physics, University of Colorado, Boulder, Colo., U.S.A. RYSZARD RATJZKA Institute for Nuclear Research, Warszawa,
More informationFYS-6306 QUANTUM THEORY OF MOLECULES AND NANOSTRUCTURES
i FYS-6306 QUANTUM THEORY OF MOLECULES AND NANOSTRUCTURES Credit units: 6 ECTS Lectures: 48 h Tapio Rantala, prof. Tue 10 12 SC203 SG219 8 10 SG312 FirstName.LastName@tut.fi http://www.tut.fi/~trantala/opetus/
More informationAnalytical Mechanics for Relativity and Quantum Mechanics
Analytical Mechanics for Relativity and Quantum Mechanics Oliver Davis Johns San Francisco State University OXPORD UNIVERSITY PRESS CONTENTS Dedication Preface Acknowledgments v vii ix PART I INTRODUCTION:
More informationImplications of Time-Reversal Symmetry in Quantum Mechanics
Physics 215 Winter 2018 Implications of Time-Reversal Symmetry in Quantum Mechanics 1. The time reversal operator is antiunitary In quantum mechanics, the time reversal operator Θ acting on a state produces
More informationSpecial Functions of Mathematical Physics
Arnold F. Nikiforov Vasilii B. Uvarov Special Functions of Mathematical Physics A Unified Introduction with Applications Translated from the Russian by Ralph P. Boas 1988 Birkhäuser Basel Boston Table
More informationSolutions to exam : 1FA352 Quantum Mechanics 10 hp 1
Solutions to exam 6--6: FA35 Quantum Mechanics hp Problem (4 p): (a) Define the concept of unitary operator and show that the operator e ipa/ is unitary (p is the momentum operator in one dimension) (b)
More informationParity P : x x, t t, (1.116a) Time reversal T : x x, t t. (1.116b)
4 Version of February 4, 005 CHAPTER. DIRAC EQUATION (0, 0) is a scalar. (/, 0) is a left-handed spinor. (0, /) is a right-handed spinor. (/, /) is a vector. Before discussing spinors in detail, let us
More informationarxiv:hep-lat/ v2 18 Jul 2006
The Effect of Reduced Spatial Symmetries on Lattice States: Results for Non-zero Linear Momentum David C. Moore, George T. Fleming arxiv:hep-lat/0607005v 8 Jul 006 Sloane Physics Laboratory, Yale University,
More informationPhysics 221A Fall 2005 Homework 11 Due Thursday, November 17, 2005
Physics 221A Fall 2005 Homework 11 Due Thursday, November 17, 2005 Reading Assignment: Sakurai pp. 234 242, 248 271, Notes 15. 1. Show that Eqs. (15.64) follow from the definition (15.61) of an irreducible
More informationRepresentation of Lie Groups and Special Functions
Representation of Lie Groups and Special Functions Recent Advances by N. Ja. Vilenkint formerly of The Correspondence Pedagogical Institute, Moscow, Russia and A.U. Klimyk Institute for Theoretical Physics,
More information2.4 Parity transformation
2.4 Parity transformation An extremely simple group is one that has only two elements: {e, P }. Obviously, P 1 = P, so P 2 = e, with e represented by the unit n n matrix in an n- dimensional representation.
More informationNERS 311 Current Old notes notes Chapter Chapter 1: Introduction to the course 1 - Chapter 1.1: About the course 2 - Chapter 1.
NERS311/Fall 2014 Revision: August 27, 2014 Index to the Lecture notes Alex Bielajew, 2927 Cooley, bielajew@umich.edu NERS 311 Current Old notes notes Chapter 1 1 1 Chapter 1: Introduction to the course
More informationLorentz-covariant spectrum of single-particle states and their field theory Physics 230A, Spring 2007, Hitoshi Murayama
Lorentz-covariant spectrum of single-particle states and their field theory Physics 30A, Spring 007, Hitoshi Murayama 1 Poincaré Symmetry In order to understand the number of degrees of freedom we need
More informationPhysics 221A Fall 1996 Notes 19 The Stark Effect in Hydrogen and Alkali Atoms
Physics 221A Fall 1996 Notes 19 The Stark Effect in Hydrogen and Alkali Atoms In these notes we will consider the Stark effect in hydrogen and alkali atoms as a physically interesting example of bound
More informationCOPYRIGHTED MATERIAL. Index
347 Index a AC fields 81 119 electric 81, 109 116 laser 81, 136 magnetic 112 microwave 107 109 AC field traps see Traps AC Stark effect 82, 84, 90, 96, 97 101, 104 109 Adiabatic approximation 3, 10, 32
More informationPHYSICS-PH (PH) Courses. Physics-PH (PH) 1
Physics-PH (PH) 1 PHYSICS-PH (PH) Courses PH 110 Physics of Everyday Phenomena (GT-SC2) Credits: 3 (3-0-0) Fundamental concepts of physics and elementary quantitative reasoning applied to phenomena in
More informationTheory and Experiment
Theory and Experiment Mark Beck OXPORD UNIVERSITY PRESS Contents Table of Symbols Preface xiii xix 1 MATHEMATICAL PRELIMINARIES 3 1.1 Probability and Statistics 3 1.2 LinearAlgebra 9 1.3 References 17
More information