Part I. Statement of the Problem and Simplest Models |
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Notations and Statement of the Problem |
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3 | (54) |
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3 | (2) |
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White Noise Approximation for a Free Particle: The Basic Formula |
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5 | (4) |
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The Interaction Representation: Propagators |
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9 | (1) |
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10 | (1) |
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Dynamical Systems and Their Perturbations |
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11 | (1) |
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Asymptotic Behaviour of Dynamical Systems: The Stochastic Limit |
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12 | (1) |
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Slow and Fast Degrees of Freedom |
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13 | (2) |
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The Quantum Transport Coefficient: Why Just the t/λ2 Scaling? |
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15 | (3) |
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Emergence of White Noise Hamiltonian Equations from the Stochastic Limit |
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18 | (3) |
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From Interaction to Heisenberg Evolutions: Conditions on the State |
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21 | (1) |
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From Interaction to Heisenberg Evolutions: Conditions on the Observable |
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22 | (1) |
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Forward and Backward Langevin Equations |
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23 | (1) |
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The Open System Approach to Dissipation and Irreversibility: Master Equation |
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24 | (3) |
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Classical Processes Driving Quantum Phenomena |
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27 | (1) |
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The Basic Steps of the Stochastic Limit |
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27 | (3) |
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Connection with the Central Limit Theorems |
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30 | (2) |
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32 | (1) |
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The Backward Transport Coefficient and the Arrow of Time |
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33 | (1) |
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The Master and Fokker--Planck Equations: Projection Techniques |
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34 | (2) |
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The Master Equation in Open Systems: an Heuristic Derivation |
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36 | (2) |
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The Semiclassical Approximation for the Master Equation |
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38 | (2) |
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Beyond the Master Equation |
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40 | (2) |
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On the Meaning of the Decomposition H = H0 + H1: Discrete Spectrum |
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42 | (2) |
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Other Rescalings when the Time Correlations Are not Integrable |
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44 | (1) |
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Connections with the Classical Homogeneization Problem |
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45 | (1) |
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Algebraic Formulation of the Stochastic Limit |
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46 | (3) |
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49 | (8) |
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57 | (28) |
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Creation and Annihilation Operators |
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57 | (2) |
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59 | (1) |
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Types of Gaussian States: Gauge-Invariant, Squeezed, Fock and Anti-Fock |
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60 | (1) |
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Free Evolutions of Quantum Fields |
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61 | (2) |
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States Invariant Under Free Evolutions |
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63 | (2) |
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Existence of Squeezed Stationary Fields |
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65 | (2) |
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Positivity of the Covariance |
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67 | (1) |
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Dynamical Systems in Equilibrium: the KMS Condition |
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68 | (1) |
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Equilibrium States: the KMS Condition |
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69 | (1) |
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q-Gaussian Equilibrium States |
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70 | (1) |
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71 | (1) |
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72 | (3) |
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Free Hamiltonians for Boson Fock Fields |
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75 | (1) |
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76 | (1) |
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Boson Fock White Noises and Classical White Noises |
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76 | (1) |
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Boson Fock White Noises and Classical Wiener Processes |
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77 | (1) |
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Boson Thermal Statistics and Thermal White Noises |
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77 | (2) |
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Canonical Representation of the Boson Thermal States |
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79 | (2) |
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Spectral Representation of Quantum White Noise |
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81 | (2) |
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Locality of Quantum Fields and Ultralocality of Quantum White Noises |
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83 | (2) |
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Those Kinds of Fields We Call Noises |
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85 | (28) |
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Convergence of Fields in the Sense of Correlators |
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85 | (1) |
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Generalized White Noises as the Stochastic Limit of Gaussian Fields |
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86 | (4) |
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Existence of Fock, Temperature and Squeezed White Noises |
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90 | (2) |
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Convergence of the Field Operator to a Classical White Noise |
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92 | (1) |
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Beyond the Master Equation: The Master Field |
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93 | (1) |
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Discrete Spectrum Embedded in the Continuum |
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94 | (3) |
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The Stochastic Limit of a Classical Gaussian Random Field |
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97 | (1) |
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Semiclassical Versus Semiquantum Approximation |
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98 | (2) |
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An Historical Example: The Damped Harmonic Oscillator |
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100 | (2) |
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Emergence of the White Noise: A Traditional Derivation |
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102 | (1) |
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Heuristic Origins of Quantum White Noise |
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103 | (1) |
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Relativistic Quantum White Noises |
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104 | (2) |
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Space--Time Rescalings: Multidimensional White Noises |
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106 | (2) |
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The Chronological Stochastic Limit |
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108 | (3) |
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111 | (2) |
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113 | (40) |
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The Nonrelativistic QED Hamiltonian |
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113 | (3) |
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116 | (1) |
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The Rotating-Wave Approximation |
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117 | (1) |
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118 | (1) |
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Assumptions on the Environment (Field, Gas, Reservoir, etc.) |
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119 | (1) |
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Assumptions on the System Hamiltonian |
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120 | (1) |
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121 | (1) |
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Multiplicative (Dipole-Type) Interactions: Canonical Form |
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121 | (1) |
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Approximations of the Multiplicative Hamiltonian |
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122 | (3) |
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Rotating-Wave Approximation Hamiltonians |
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123 | (1) |
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No Rotating-Wave Approximation Hamiltonians with Cutoff |
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123 | (1) |
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Neither Dipole nor Rotating-Wave Approximation Hamiltonians Without Cutoff |
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124 | (1) |
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The Generalized Rotating-Wave Approximation |
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125 | (1) |
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The Stochastic Limit of the Multiplicative Interaction |
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126 | (1) |
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The Normal Form of the White Noise Hamiltonian Equation |
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127 | (1) |
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Invariance of the Ito Correction Term Under Free System Evolution |
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128 | (1) |
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The Stochastic Golden Rule: Langevin and Master Equations |
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129 | (3) |
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Classical Stochastic Processes Underlying Quantum Processes |
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132 | (1) |
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The Fluctuation-Dissipation Relation |
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133 | (1) |
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Vacuum Transition Amplitudes |
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134 | (2) |
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Mass Gap of D+ D and Speed of Decay |
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136 | (1) |
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137 | (1) |
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The Energy Shell Scalar Product: Linewidths |
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138 | (2) |
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Dispersion Relations and the Ito Correction Term |
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140 | (1) |
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141 | (1) |
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Multiplicative Coupling with the Rotating Wave Approximation: Arbitrary Gaussian State |
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142 | (1) |
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Multiplicative Coupling with RWA: Gauge Invariant State |
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143 | (1) |
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Red Shifts and Blue Shifts |
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144 | (1) |
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The Free Evolution of the Master Field |
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145 | (2) |
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Algebras Invariant Under the Flow |
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147 | (1) |
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148 | (5) |
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153 | (52) |
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Dropping the Rotating-Wave Approximation |
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154 | (1) |
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154 | (3) |
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The White Noise Hamiltonian Equation |
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157 | (1) |
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The Operator Transport Coefficient: no Rotating-Wave Approximation, Arbitrary Gaussian Reference State |
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158 | (1) |
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Different Roles of the Positive and Negative Bohr Frequencies |
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159 | (2) |
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No Rotating-Wave Approximation with Cutoff: Gauge Invariant States |
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161 | (1) |
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No Rotating-Wave Approximation with Cutoff: Squeezing States |
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161 | (1) |
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The Stochastic Golden Rule for Dipole Type Interactions and Gauge-Invariant States |
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162 | (2) |
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The Stochastic Golden Rule |
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164 | (6) |
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170 | (2) |
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Subalgebras Invariant Under the Generator |
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172 | (1) |
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The Langevin Equation: Generic Systems |
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173 | (3) |
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The Stochastic Golden Rule Versus Standard Perturbation Theory |
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176 | (2) |
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178 | (3) |
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The Damping and Oscillating Regimes: Fock Case |
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181 | (2) |
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The Damping and the Oscillating Regimes: Nonzero Temperature |
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183 | (1) |
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No Rotating-Wave Approximation Without Cutoff |
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184 | (1) |
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The Drift Term for Gauge-Invariant States |
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185 | (2) |
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The Free Evolution of the Master Field |
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187 | (1) |
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The Stochastic Limit of the Generalized Spin-Boson Hamiltonian |
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187 | (3) |
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190 | (1) |
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Convergence to Equilibrium: Connections with Quantum Measurement |
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191 | (3) |
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194 | (2) |
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196 | (5) |
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Nonstationary White Noises |
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201 | (1) |
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202 | (3) |
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Measurements and Filtering Theory |
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205 | (14) |
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205 | (1) |
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The Filtering Problem in Classical Probability |
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206 | (1) |
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207 | (3) |
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Properties of the Input and Output Processes |
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210 | (3) |
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The Filtering Problem in Quantum Theory |
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213 | (1) |
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Filtering of a Quantum System Over a Classical Process |
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214 | (1) |
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215 | (2) |
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Standard Scheme to Construct Examples of Nondemolition Measurements |
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217 | (1) |
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Discrete Time Nondemolition Processes |
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217 | (1) |
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218 | (1) |
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Idea of the Proof and Causal Normal Order |
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219 | (18) |
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Term-by-Term Convergence of the Series |
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219 | (1) |
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Vacuum Transition Amplitude: The Fourth-Order Term |
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220 | (3) |
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Vacuum Transition Amplitude: Non-Time-Consecutive Diagrams |
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223 | (2) |
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The Causal δ-Function and the Time-Consecutive Principle |
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225 | (2) |
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Theory of Distributions on the Standard Simplex |
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227 | (3) |
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The Second-Order Term of the Limit Vacuum Amplitude |
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230 | (1) |
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The Fourth-Order Term of the Limit Vacuum Amplitude |
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230 | (1) |
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Higher-Order Terms of the Vacuum-Vacuum Amplitude |
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231 | (1) |
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Proof of the Normal Form of the White Noise Hamiltonian Equation |
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231 | (2) |
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The Unitarity Condition for the Limit Equation |
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233 | (1) |
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Normal Form of the Thermal White Noise Equation: Boson Case |
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234 | (1) |
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From White Noise Calculus to Stochastic Calculus |
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235 | (2) |
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Chronological Product Approach to the Stochastic Limit |
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237 | (10) |
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237 | (1) |
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Chronological Product Approach to the Stochastic Limit |
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238 | (4) |
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The Limit of the nth Term, Time-Ordered Product Approach: Vacuum Expectation |
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242 | (2) |
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The Stochastic Limit, Time-Ordered Product Approach: General Case |
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244 | (3) |
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Functional Integral Approach to the Stochastic Limit |
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247 | (8) |
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247 | (1) |
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The Stochastic Limit of the Free Massive Scalar Field |
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248 | (2) |
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The Stochastic Limit of the Free Massless Scalar Field |
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250 | (1) |
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251 | (2) |
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The Stochastic Limit of the Electromagnetic Field |
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253 | (2) |
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Low-Density Limit: The Basic Idea |
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255 | (6) |
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The Low-Density Limit: Fock Case, No System |
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255 | (2) |
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The Low-Density Limit: Fock Case, Arbitrary System Operator |
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257 | (1) |
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Comparison of the Distribution and the Stochastic Approach |
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258 | (1) |
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LDL General, Fock Case, No System Operator, ω = 0 |
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259 | (2) |
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Six Basic Principles of the Stochastic Limit |
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261 | (24) |
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Polynomial Interactions with Cutoff |
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262 | (1) |
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Assumptions on the Dynamics: Standard Models |
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263 | (3) |
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Polynomial Interactions: Canonical Forms, Fock Case |
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266 | (3) |
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Polynomial Interactions: Canonical Forms, Gauge-Invariant Case |
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269 | (6) |
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The Stochastic Universality Class Principle |
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275 | (2) |
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The Case of Many Independent Fields |
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277 | (1) |
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The Block Principle: Fock Case |
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278 | (2) |
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The Stochastic Resonance Principle |
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280 | (1) |
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The Orthogonalization Principle |
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280 | (1) |
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The Stochastic Bosonization Principle |
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280 | (2) |
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The Time-Consecutive Principle |
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282 | (3) |
Part II. Strongly Nonlinear Regimes |
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Particles Interacting with a Boson Field |
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285 | (66) |
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A Single Particle Interacting with a Boson Field |
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287 | (2) |
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Dynamical q-Deformation: Emergence of the Entangled Commutation Relations |
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289 | (2) |
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The Two-Point and Four-Point Correlators |
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291 | (2) |
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The Stochastic Limit of the N-Point Correlator |
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293 | (3) |
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The q-Deformed Module Wick Theorem |
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296 | (5) |
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The Wick Theorem for the QED Module |
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301 | (1) |
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The Limit White Noise Hamiltonian Equation |
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302 | (2) |
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Free Independence of the Increments of the Master Field |
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304 | (2) |
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Boltzmannian White Noise Hamiltonian Equations: Normal Form |
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306 | (3) |
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309 | (1) |
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Matrix Elements of the Solution |
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310 | (2) |
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Normal Form of the QED Module Hamiltonian Equation |
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312 | (1) |
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Unitarity of the Solution: Direct Proof |
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313 | (1) |
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Matrix Elements of the Limit Evolution Operator |
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314 | (3) |
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317 | (4) |
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321 | (1) |
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321 | (1) |
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Proof of the Result for the Two- and Four-Point Correlators |
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322 | (2) |
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The Vanishing of the Crossing Diagrams |
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324 | (9) |
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333 | (2) |
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Interaction of the QEM Field with a Nonfree Particle |
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335 | (3) |
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The Limit Two-Point Function |
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338 | (4) |
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The Limit Four-Point Function |
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342 | (2) |
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344 | (3) |
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The Limit Stochastic Process |
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347 | (1) |
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The Stochastic Differential Equation |
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348 | (1) |
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349 | (2) |
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351 | (18) |
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Nonrelativistic Fermions in External Potential: The Anderson Model |
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352 | (3) |
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The Limit of the Connected Correlators |
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355 | (1) |
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356 | (3) |
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The Limit of the Connected Transition Amplitude |
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359 | (3) |
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362 | (3) |
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Solution of the Nonlinear Equation (13.4.2) |
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365 | (2) |
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367 | (2) |
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Field--Field Interactions |
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369 | (24) |
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Interacting Commutation Relations |
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369 | (4) |
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The Tri-linear Hamiltonian with Momentum Conservation |
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373 | (2) |
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375 | (4) |
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Example: Four Internal Lines |
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379 | (1) |
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The Stochastic Limit for Green Functions |
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380 | (1) |
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Second Quantized Representation of the Nonrelativistic QED Hamiltonian |
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381 | (2) |
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Interacting Commutation Relations and QED Module Algebra |
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383 | (1) |
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Decay and the Universality Class of the QED Hamiltonian |
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384 | (2) |
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Photon Splitting Cascades and New Statistics |
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386 | (7) |
Part III. Estimates and Proofs |
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Analytical Theory of Feynman Diagrams |
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393 | (60) |
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The Connected Component Theorem |
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395 | (7) |
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The Factorization Theorem |
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402 | (9) |
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The Case of Many Independent Fields |
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411 | (1) |
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411 | (5) |
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Non-Time-Consecutive Terms: The First Vanishing Theorem |
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416 | (3) |
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Non-Time Consecutive Terms: The Second Vanishing Theorem |
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419 | (4) |
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423 | (8) |
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The Double Integral Lemma |
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431 | (4) |
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The Multiple-Simplex Theorem |
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435 | (3) |
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The Multiple Integral Lemma |
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438 | (1) |
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The Second Multiple-Simplex Theorem |
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439 | (7) |
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Some Combinatorial Facts and the Block Normal Ordering Theorem |
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446 | (7) |
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453 | (8) |
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The Universality Class Principle and Effective Interaction Hamiltonians |
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455 | (3) |
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Block and Orthogonalization Principles |
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458 | (1) |
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The Stochastic Resonance Principle |
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459 | (2) |
References |
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461 | (8) |
Index |
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469 | |