
Quaternionic Quantum Mechanics and Quantum Fields
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Content
- Intro
- Contents
- I: INTRODUCTION AND GENERAL FORMALISM
- 1 Introduction
- 1.1. Classical Versus Quantum Mechanics
- 1.2. Number Systems Used for Probability Amplitudes
- 1.3. Alternative Formulations of Quantum Mechanics
- 1.4. Notation and Introduction to Quaternionic Arithmetic
- 2 General Framework of Quaternionic Quantum Mechanics
- 2.1. States, Operators, Wave Functions, and Inner Products
- 2.2. Observables and Self-adjoint Operators
- 2.3. Symmetry Transformations and Anti-self-adjoint Operators
- 2.4. Time Development
- 2.5. Relationships Between Quaternionic, Complex, and Real Quantum Mechanics
- 2.6. Energy Eigenstates in Quaternionic, Complex, and Real Quantum Mechanics, and the Complex Embedding of Real Quantum Mechanics
- 2.7. Nonextendability to Octonionic Quantum Mechanics
- 3 Further General Results in Quaternionic Quantum Mechanics
- 3.1. Space Translations and Momentum
- 3.2. Rotations and Angular Momentum
- 3.3. Time Translations, Evolution of Expectation Values, and the Heisenberg Picture
- 3.4. The Uncertainty Principle in Quaternionic Quantum Mechanics
- 3.5. Representation of Symmetries of H
- 3.6. Simultaneous Diagonalization of Mutually Commuting Self-adjoint and Anti-self-adjoint Operators
- 3.7. Spin Angular Momentum and Hamiltonian Structure
- II: NONRELATIVISTIC QUATERNIONIC QUANTUM MECHANICS
- 4 One-Particle Quantum Mechanics - General Formalism
- 4.1. Restrictions on the Form of H from Translational, Rotational, and Galilean Invariance
- 4.2. Simplification of the Schrödinger Equation by Choice of Ray Representative
- 4.3. Projective Group Representations and the Quaternionic Schur's Lemma
- 4.4. Dynamics of Densities and Expectation Values
- 4.5. The Feynman Path Integral Formula: A Partial Analog
- 4.6. Time Reversal Invariance for Spin Zero Systems
- 4.7. Time Reversal Invariance with Spin
- 4.8. The Quaternionic Harmonic Oscillator
- 5 Stationary State Methods and Phase Methods
- 5.1. Reduction of |H| to a Complex Hermitian Operator
- 5.2. Reduction to an Optical Potential
- 5.3. Stationary State Perturbation Theory - Introduction
- 5.4. A Perturbation Theory Application - Leading Order Calculation of I[sub(H)],J[sub(H)],K[sub(H)], and |H|
- 5.5. Stationary State Perturbation Theory - Second-Order Expansion, the Degenerate Case, and Zero-Energy States
- 5.6. Variational Principles
- 5.7. The Adiabatic Approximation and the Geometric Phase
- 5.8. The Nonadiabatic Geometric Phase
- 5.9. The Quaternionic WKB Approximation
- 6 Scattering Theory and Bound States
- 6.1. One-Dimensional Scattering and Bound States - the Delta Function Potential Model
- 6.2. Spherically Symmetric Potentials
- 6.3. General Three-Dimensional Potentials: The S-Matrix Is C(l, i), but Time Reversal Violating
- 6.4. Bound-State-Associated Scattering Resonances
- 6.5. Analyticity Properties
- 6.6. General One-Dimensional Scattering
- 7 Methods for Time Development
- 7.1. Time-Dependent Perturbation Theory
- 7.2. Scattering Theory and the T-Matrix
- 7.3. Decay Theory for H[sub(0)] Energy Eigenstates
- 7.4. Use of the Interaction and Heisenberg Pictures, and the Quaternionic Forced Harmonic Oscillator
- 7.5. A Quaternionic Model for Time Reversal Violation in Particle Physics
- 8 Single-Channel Time-Dependent Formal Scattering Theory
- 8.1. Time Development of the State Vector and Green's Functions
- 8.2. The Möller Wave Operators and Their Properties
- 8.3. The S-Matrix
- 8.4. Symmetries of the S-Malrix
- 9 Multiparticle and Multichannel Methods
- 9.1. Restrictions on H from Translational, Rotational, and Galilean Invariance
- 9.2. Identical Particles
- Separation of Center of Mass Motion
- 9.3. The Tensor Product Problem and the Failure of Clustering
- 9.4. Asymptotic State Structure
- 9.5. Multichannel Time-Dependent Formal Scattering Theory
- 10 Further Multiparticle Topics
- 10.1. Fock Space and Second Quantization
- 10.2. Quasiparticle Transformation for a Particle-Number-Conserving One-Body Hamiltonian
- 10.3. Statistical Mechanics
- 10.4. An Optical Potential Analysis of Clustering
- III: RELATIVISTIC QUATERNIONIC QUANTUM MECHANICS
- 11 Relativistic Single-Particle Wave Equations: Spin-0 and Spin-1/2
- 11.1. The Quaternionic Free Klein-Gordon Equation
- 11.2. The Interacting Klein-Gordon Equation
- 11.3. Nonrelativistic Limit of the Klein-Gordon Equation
- 11.4. The Quaternionic Free Dirac Equation
- 11.5. The Interacting Dirac Equation and Its Nonrelativistic Reduction
- 11.6. Semirelativistic Reduction of the Interacting Klein-Gordon and Dirac Equations
- 11.7. A Survey of Properties of the Semirelativistic Equation
- 12 More on Relativistic Wave Equations: The Spin-1 Gauge Potential, Lagrangian Formulations, and the Poincaré Group
- 12.1. The Quaternionic Gauge Potential B[sub(µ)]
- 12.2. Lagrangians and C(l, i ) Structure and Symmetries
- 12.3. Representations of the Poincaré Group
- 13 Quaternionic Quantum Field Theory
- 13.1. The Klein Paradox and the Necessity for Quantum Field Theory
- 13.2. Quaternionic Embeddings of Complex Quantum Field Theories
- 13.3. Quaternionic Free Fields Formed as Superpositions of Formally Real or Complex Canonical Fields
- 13.4. Quaternionic Irreducible Representations of Compact Groups
- 13.5. Operator Gauge Invariant Total Trace Lagrangian Formulation of Quantum Dynamics
- 13.6. Operator Gauge Invariant Total Trace Lagrangian Formulation of Complex Quantum Mechanics
- 13.7. Operator Gauge Invariant Quaternionic Field Theories
- 13.8. Quaternionic Determinants and Gaussian Integrals
- 14 Outlook
- 14.1. Why Quaternionic Quantum Mechanics?
- 14.2. Experimental Tests and Measurement Theory Issues
- 14.3. Open Questions
- Appendix A. Proof of the Jacobi Identity for the Generalized Poisson Bracket
- Appendix B. Derivation of Gaussian Integral Formulas
- References
- Index
- A
- B
- C
- D
- E
- F
- G
- H
- I
- J
- K
- L
- M
- N
- O
- P
- Q
- R
- S
- T
- U
- V
- W
- Y
- Z
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