| Dedication | v |
| Preface | vii |
1 | Introduction | 1 |
2 | Phenomenological Equations of Motion for Dissipative Systems | 5 |
2.1 | Frictional Forces Linear Velocity | 5 |
2.2 | Raleigh's Oscillator | 8 |
2.3 | One-Dimensional Motion and Bopp Transformation | 8 |
2.4 | The Classical Theory of Line Width | 11 |
2.5 | Frictional Forces Quadratic in Velocity | 12 |
2.6 | Non-Newtonian and Nonlocal Dissipative Forces | 13 |
3 | Lagrangian Formulations | 15 |
3.1 | Rayleigh and Lur'e Dissipative Functions | 15 |
3.2 | Inverse Problem of Analytical Dynamics | 20 |
3.3 | Some Examples of the Lagrangians for Dissipative Systems | 24 |
3.4 | Non-Uniqueness of the Lagrangian | 27 |
3.5 | Acceptable Lagrangians for Dissipative Systems | 30 |
4 | Hamiltonian Formulation | 33 |
4.1 | Inverse Problem for the Hamiltonian | 33 |
4.2 | Hamiltonians for Simple Dissipative Systems | 36 |
4.3 | Ostrogradsky's Method | 39 |
4.4 | Complex or Leaky Spring Constant | 42 |
4.5 | Dekker's Complex Coordinate Formulation | 42 |
4.6 | Hamiltonian Formulation of the Motion of a Particle with Variable Mass | 44 |
4.7 | Variable Mass Oscillator | 45 |
4.8 | Bateman's Damped-Amplified Harmonic Oscillators | 47 |
4.9 | Dissipative Forces Quadratic in Velocity | 48 |
4.10 | Resistive Forces Proportional to Arbitrary Powers of Velocity | 48 |
4.11 | Universal Lagrangian and Hamiltonian | 49 |
4.12 | Hamiltonian Formulation in Phase Space of N-Dimensions | 52 |
4.13 | Symmetric Phase Space Formulation of the Damped Harmonic Oscillator | 55 |
4.14 | Dynamical Systems Expressible as Linear Difference Equations | 57 |
5 | Hamilton-Jacobi Formulation | 63 |
5.1 | The Hamilton-Jacobi Equation for Linear Damping | 64 |
5.2 | Classical Action for an Oscillator with Leaky Spring Constant | 66 |
5.3 | More About the Hamilton-Jacobi Equation for the Damped Motion | 67 |
6 | Motion of a Charged Particle in an External Electromagnetic Field in the Presence of Damping | 71 |
7 | Noether and Non-Noether Symmetries and Conservation Laws | 77 |
7.1 | Non-Noether Symmetries and Conserved Quantities | 84 |
7.2 | Noether's Theorem for a Scalar Field | 86 |
8 | Dissipative Forces Derived from Many-Body Problems | 91 |
8.1 | The Schrodinger Chain | 91 |
8.2 | A Particle Coupled to a Chain | 93 |
8.3 | Dynamics of a Non-Uniform Chain | 94 |
8.4 | Mechanical System Coupled to a Heat Bath | 98 |
8.5 | Euclidean Lagrangian | 104 |
9 | A Particle Coupled to a Field | 107 |
9.1 | Harmonically Bound Radiating Electron | 107 |
9.2 | An Oscillator Coupled to a String of Finite Length | 109 |
9.3 | An Oscillator Coupled to an Infinite String | 112 |
10 | Damped Motion of the Central Particle | 117 |
10.1 | Diagonalization of the Hamiltonian | 117 |
11 | Classical Microscopic Models of Dissipation and Minimal Coupling Rule | 125 |
12 | Quantization of Dissipative Systems | 129 |
12.1 | Early Attempts to Quantize the Damped Oscillator | 129 |
12.2 | Yang-Feldman Method of Quantization | 136 |
12.3 | Heisenberg's Equations of Motion for Dekker's Formulation | 138 |
12.4 | Quantization of the Bateman Hamiltonian | 139 |
12.5 | Fermi's Nonlinear Equation for Quantized Radiation Reaction | 142 |
12.6 | Attempts to Quantize Systems with a Dissipative Force Quadratic in Velocity | 145 |
12.7 | Solution of the Wave Equation for Linear and Newtonian Damping Forces | 147 |
12.8 | The Classical Limit of the Schrodinger Equation with Velocity-Dependent Forces | 150 |
12.9 | Quadratic Damping as an Externally Applied Force | 151 |
12.10 | Motion in a Viscous Field of Force Proportional to an Arbitrary Power of Velocity | 153 |
12.11 | The Classical Limit and the Van Vleck Determinant | 154 |
13 | Quantization of Explicitly Time-Dependent Hamiltonian | 157 |
13.1 | Wave Equation for the Kanai-Caldirola Hamiltonian | 157 |
13.2 | Coherent States of a Damped Oscillator | 164 |
13.3 | Squeezed State of a Damped Harmonic Oscillator | 167 |
13.4 | Quantization of a System with Variable Mass | 169 |
13.5 | The Schrodinger-Langevin Equation for Linear Damping | 172 |
13.6 | An Extension of the Madelung Formulation | 175 |
13.7 | Quantization of a Modified Hamilton-Jacobi Equation for Damped Systems | 180 |
13.8 | Exactly Solvable Cases of the Schrodinger -Langevin Equation | 184 |
13.9 | Harmonically Bound Radiating Electron and the Schrodinger-Langevin Equation | 187 |
13.10 | Other Phenomenological Nonlinear Potentials for Dissipative Systems | 189 |
13.11 | Scattering in the Presence of Frictional Forces | 192 |
13.12 | Application of the Noether Theorem: Linear and Nonlinear Wave Equations for Dissipative Systems | 193 |
13.13 | Wave Equation for Impulsive Forces Acting at Certain Intervals | 196 |
13.14 | Classical Limit for the Time-Dependent Problems | 197 |
14 | Density Matrix and the Wigner Distribution Function | 201 |
14.1 | Classical Distribution Function for Nonconservative Motions | 201 |
14.2 | The Density Matrix | 205 |
14.3 | Phase Space Quantization of Dekker's Hamiltonian | 207 |
14.4 | Density Operator and the Fokker-Planck Equation | 209 |
14.5 | The Density Matrix Formulation of a Solvable Model | 213 |
14.6 | Wigner Distribution Function for the Damped Oscillator | 216 |
14.7 | Density Operator for a Particle Coupled to a Heat Bath | 219 |
15 | Path Integral Formulation of a Damped Harmonic Oscillator | 223 |
15.1 | Propagator for the Damped Harmonic Oscillator | 224 |
15.2 | Path Integral Quantization of a Harmonic Oscillator with Complex Spring Constant | 230 |
15.3 | Modified Classical Action and the Propagator for the Damped Harmonic Oscillator | 233 |
15.4 | Path Integral Formulation of a System Coupled to a Heat Bath | 235 |
16 | Quantization of the Motion of an Infinite Chain | 239 |
16.1 | Quantum Mechanics of a Uniform Chain | 239 |
16.2 | Ground State of the Central Particle | 242 |
16.3 | Wave Equation for a Non-Uniform Chain | 244 |
16.4 | Connection with Other Phenomenological Frictional Forces | 246 |
16.5 | Fokker-Planck Equation for the Probability Density | 247 |
17 | The Heisenberg Equations of Motion for a Particle Coupled to a Heat Bath | 249 |
17.1 | Heisenberg Equations for a Damped Harmonic Oscillator | 249 |
17.2 | Density Matrix for the Motion of a Particle Coupled to a Field | 260 |
17.3 | Equations of Motion for the Central Particle | 263 |
17.4 | Wave Equation for the Motion of the Central Particle | 264 |
17.5 | Motion of the Center-of-Mass in Viscous Medium | 269 |
17.6 | Invariance Under Galilean Transformation | 272 |
17.7 | Velocity Coupling and Coordinate Coupling | 273 |
17.8 | Equation of Motion for a Harmonically Bound Radiating Electron | 274 |
18 | Quantum Mechanical Models of Dissipative Systems | 279 |
18.1 | Forced Vibration with Damping | 279 |
18.2 | The Wigner-Weisskopf Model | 282 |
18.3 | Quantum Theory of Line Width | 286 |
18.4 | The Optical Potential | 291 |
18.5 | Gisin's Nonlinear Wave Equation | 295 |
18.6 | Nonlinear Generalization of the Wave Equation | 298 |
18.7 | Dissipation Arising from the Motion of the Boundaries | 301 |
18.8 | Decaying States in a Many-Boson System | 308 |
19 | More on the Concept of Optical Potential | 315 |
19.1 | The Classical Analogue of the Nonlocal Interaction | 315 |
19.2 | Minimal and/or Maximal Coupling | 319 |
19.3 | Damped Harmonic Oscillator and Optical Potential | 323 |
19.4 | Quantum Mechanical Analogue of the Raleigh Oscillator | 326 |
| Index | 331 |