Cover image for ADVANCED QUANTUM MECHANICS.
ADVANCED QUANTUM MECHANICS.
Title:
ADVANCED QUANTUM MECHANICS.
Author:
Dyson, Freeman.
ISBN:
9789814383424
Personal Author:
Physical Description:
1 online resource (316 pages)
Contents:
Contents -- Foreword -- Notes -- Preface -- Preface to First Edition -- Generally used Notation -- 1 Introduction -- 1.1 Books -- 1.2 Subject Matter -- 1.3 Detailed Program -- 1.4 One-Particle Theories -- 2 The Dirac Theory -- 2.1 The Form of the Dirac Equation -- 2.2 Lorentz Invariance of the Dirac Equation -- 2.3 To Find the S -- 2.4 The Covariant Notation -- 2.5 Conservation Laws. Existence of Spin -- 2.6 Elementary Solutions -- 2.7 The Hole Theory -- 2.8 Positron States -- 2.9 Electromagnetic Properties of the Electron -- 2.10 The Hydrogen Atom -- 2.11 Solution of Radial Equation -- 2.12 Behaviour of an Electron in a Non-Relativistic Approximation -- 2.13 Summary of Matrices in the Dirac Theory in Our Notation -- 2.14 Summary of Matrices in the Dirac Theory in the Feynman Notation -- 3 Scattering Problems and Born Approximation -- 3.1 General Discussion -- 3.2 Projection Operators -- 3.3 Calculation of Traces -- 3.4 Scattering of Two Electrons in Born Approximation. The Møller Formula -- 3.5 Relation of Cross-sections to Transition Amplitudes -- 3.6 Results for Møller Scattering -- 3.7 Note on the Treatment of Exchange Effects -- 3.8 Relativistic Treatment of Several Particles -- 4 Field Theory -- 4.1 Classical Relativistic Field Theory -- 4.2 Quantum Relativistic Field Theory -- 4.3 The Feynman Method of Quantization -- 4.4 The Schwinger Action Principle -- 4.4.1 The Field Equations -- 4.4.2 The Schrodinger Equation for the State-function -- 4.4.3 Operator Form of the Schwinger Principle -- 4.4.4 The Canonical Commutation Laws -- 4.4.5 The Heisenberg Equation of Motion for the Operators -- 4.4.6 General Covariant Commutation Laws -- 4.4.7 Anticommuting Fields -- 5 Examples of Quantized Field Theories -- 5.1 The Maxwell Field -- 5.1.1 Momentum Representations -- 5.1.2 Fourier Analysis of Operators -- 5.1.3 Emission and Absorption Operators.

5.1.4 Gauge-Invariance of the Theory -- 5.1.5 The Vacuum State -- 5.1.6 The Gupta-Bleuler Method -- 5.1.7 Example: Spontaneous Emission of Radiation -- 5.1.8 The Hamiltonian Operator -- 5.1.9 Fluctuations of the Fields -- 5.1.10 Fluctuation of Position of an Electron in a Quantized Electromagnetic Field. The Lamb Shift -- 5.2 Theory of Line Shift and Line Width -- 5.2.1 The Interaction Representation -- 5.2.2 The Application of the Interaction Representation to the Theory of Line-Shift and Line-Width -- 5.2.3 Calculation of Line-Shift, Non-Relativistic Theory -- 5.2.4 The Idea of Mass Renormalization -- 5.3 Field Theory of the Dirac Electron, Without Interaction -- 5.3.1 Covariant Commutation Rules -- 5.3.2 Momentum Representations -- 5.3.3 Fourier Analysis of Operators -- 5.3.4 Emission and Absorption Operators -- 5.3.5 Charge-Symmetrical Representation -- 5.3.6 The Hamiltonian -- 5.3.7 Failure of Theory with Commuting Fields -- 5.3.8 The Exclusion Principle -- 5.3.9 The Vacuum State -- 5.4 Field Theory of Dirac Electron in External Field -- 5.4.1 Covariant Commutation Rules -- 5.4.2 The Hamiltonian -- 5.4.3 Antisymmetry of the States -- 5.4.4 Polarization of the Vacuum -- 5.4.5 Calculation of Momentum Integrals -- 5.4.6 Physical Meaning of the Vacuum Polarization -- 5.4.7 Vacuum Polarization for Slowly Varying Weak Fields. The Uehling Effect -- 5.5 Field Theory of Dirac and Maxwell Fields in Interaction -- 5.5.1 The Complete Relativistic Quantum Electrodynamics -- 5.5.2 Free Interaction Representation -- 6 Free Particle Scattering Problems -- 6.1 Møller Scattering of Two Electrons -- 6.1.1 Properties of the DF Function -- 6.1.2 The Møller Formula, Conclusion -- 6.1.3 Electron-Positron Scattering -- 6.2 Scattering of a Photon by an Electron. The Compton Effect. Klein-Nishina Formula -- 6.2.1 Calculation of the Cross-Section -- 6.2.2 Sum Over Spins.

6.3 Two Quantum Pair Annihilation -- 6.4 Bremsstrahlung and Pair Creation in the Coulomb Field of an Atom -- 7 General Theory of Free Particle Scattering -- 7.1 The Reduction of an Operator to Normal Form -- 7.2 Feynman Graphs -- 7.3 Feynman Rules of Calculation -- 7.4 The Self-Energy of the Electron -- 7.5 Second-Order Radiative Corrections to Scattering -- 7.6 The Treatment of Low-Frequency Photons. The Infra-Red Catastrophe -- 8 Scattering by a Static Potential. Comparison with Experimental Results -- 8.1 The Magnetic Moment of the Electron -- 8.2 Relativistic Calculation of the Lamb Shift -- 8.2.1 Covariant Part of the Calculation -- 8.2.2 Discussion and the Nature of the -Representation -- 8.2.3 Concluding Non-Covariant Part of the Calculation -- 8.2.4 Accuracy of the Lamb Shift Calculation -- Notes -- Appendices -- Appendix A -- A.1 Particle Mechanics and Field Mechanics -- A.2 Classical Particle Mechanics -- A.3 Classical Relativistic Field Theory -- A.4 Particle Quantum Mechanics -- A.5 Huyghens' Principle and the Feynman Method of Quantization -- A.6 The Feynman Quantization for Field Theory -- A.7 The Schwinger Action Principle for Particle Mechanics -- A.8 Equivalence of the Schwinger Action Principle with Ordinary Quantum Mechanics -- A.8.1. The Operator Equations of Motion -- A.8.2. The Commutation Rules -- A.8.3. The Schrodinger Equation -- A.9 Transition to Field Theory -- Appendix B -- Appendix C -- C.1 The Interaction Representation -- C.2 Contribution of the Interaction (9, 2) -- C.3 Calculation of the Term (1, 6) -- C.4 Gauge Invariance in the Theory -- C.5 Consequences of the Invariance -- C.6 Possibility of Renormalization to All Orders -- C.7 Types of Divergence -- C.8 The Self-Energy of the Vacuum: Diagrams of the Form etc. (G1) -- C.9 Furry's Theorem2 -- C.10 (A) Self-Energy of the Photon.

C.11 (B) Scattering of Light by Light -- C.12 (C) The Vertex Part -- C.13 (D) Self-Energy of the Electron -- C.14 (D) Last Tasks -- C.14.1 First Case -- C.14.2 Second Case -- C.14.3 Calculation of the Renormalized Diagrams of Order Ae(A)4 -- Notes -- References -- Index.
Abstract:
Renowned physicist and mathematician Freeman Dyson is famous for his work in quantum mechanics, nuclear weapons policy and bold visions for the future of humanity. In the 1940s, he was responsible for demonstrating the equivalence of the two formulations of quantum electrodynamics - Richard Feynman's diagrammatic path integral formulation and the variational methods developed by Julian Schwinger and Sin-Itiro Tomonoga - showing the mathematical consistency of QED. This invaluable volume comprises the legendary lectures on quantum electrodynamics first given by Dyson at Cornell University in 1951. The late theorist Edwin Thompson Jaynes once remarked, "For a generation of physicists they were the happy medium: clearer and better motivated than Feynman, and getting to the point faster than Schwinger". This edition has been printed on the 60th anniversary of the Cornell lectures, and includes a foreword by science historian David Kaiser, as well as notes from Dyson's lectures at the Les Houches Summer School of Theoretical Physics in 1954. The Les Houches lectures, described as a supplement to the original Cornell notes, provide a more detailed look at field theory, a careful and rigorous derivation of Fermi's Golden Rule, and a masterful treatment of renormalization and Ward's Identity. Future generations of physicists are bound to read these lectures with pleasure, benefiting from the lucid style that is so characteristic of Dyson's exposition.
Local Note:
Electronic reproduction. Ann Arbor, Michigan : ProQuest Ebook Central, 2017. Available via World Wide Web. Access may be limited to ProQuest Ebook Central affiliated libraries.
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