
Quantum Theory and Its Stochastic Limit
By:Â Luigi Accardi, Yun Gang Lu, Igor Volovich
Hardcover | 7 August 2002
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500 Pages
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Industry Reviews
"The authors have produced a very important and detailed book on the subject of the stochastic limit of quantum field theory. In particular, they formulate the stochastic limit in the framework of an algebraic central limit theory using the sort of scaling limits encountered in quantum transport phenomena. [...] The book is well written and covers many related problems [...] The audience will be mathematical and theoretical physicists. The authors are to be congratulated for showing the power and range of application of quantum probability to quantum physics." (Mathematical Reviews 2003h)
Statement of the Problem and Simplest Models | |
Notations and Statement of the Problem | p. 3 |
The Schrödinger Equation | p. 3 |
White Noise Approximation for a Free Particle: The Basic Formula | p. 5 |
The Interaction Representation: Propagators | p. 9 |
The Heisenberg Equation | p. 10 |
Dynamical Systems and Their Perturbations | p. 11 |
Asymptotic Behaviour of Dynamical Systems: The Stochastic Limit | p. 12 |
Slow and Fast Degrees of Freedom | p. 13 |
The Quantum Transport Coefficient: Why Just the t/2 Scaling? | p. 15 |
Emergence of White Noise Hamiltonian Equations from the Stochastic Limit | p. 18 |
From Interaction to Heisenberg Evolutions: Conditions on the State | p. 21 |
From Interaction to Heisenberg Evolutions: Conditions on the Observable | p. 22 |
Forward and Backward Langevin Equations | p. 23 |
The Open System Approach to Dissipation and Irreversibility: Master Equation | p. 24 |
Classical Processes Driving Quantum Phenomena | p. 27 |
The Basic Steps ofthe Stochastic Limit | p. 27 |
Connection with the Central Limit Theorems | p. 30 |
Classical Systems | p. 32 |
The Backward Transport Coefficient and the Arrow of Time | p. 33 |
The Master and Fokker-Planck Equations: Projection Techniques | p. 34 |
The Master Equation in Open Systems: an Heuristic Derivation | p. 36 |
The Semiclassical Approximation for the Master Equation | p. 38 |
Beyond the Master Equation | p. 40 |
On the Meaning of the Decomposition H = H0 + HI: Discrete Spectrum | p. 42 |
Other Rescalings when the Time Correlations Are not Integrable | p. 44 |
Connections with the Classical Homogeneization Problem | p. 45 |
Algebraic Formulation of the Stochastic Limit | p. 46 |
Notes | p. 49 |
Quantum Fields | p. 57 |
Creation and Annihilation Operators | p. 57 |
Gaussianity | p. 59 |
Types of Gaussian States: Gauge-Invariant, Squeezed, Fock and Anti-Fock | p. 60 |
Free Evolutions of Quantum Fields | p. 61 |
States Invariant Under Free Evolutions | p. 63 |
Existence of Squeezed Stationary Fields | p. 65 |
Positivity of the Covariance | p. 67 |
Dynamical Systems in Equilibrium: the KMS Condition | p. 68 |
Equilibrium States: the KMS Condition | p. 69 |
q-Gaussian Equilibrium States | p. 70 |
Boson Gaussianity | p. 71 |
Boson Fock Fields | p. 72 |
Free Hamiltonians for Boson Fock Fields | p. 75 |
White Noises | p. 76 |
Boson Fock White Noises and Classical White Noises | p. 76 |
Boson Fock White Noises and Classical Wiener Processes | p. 77 |
Boson Thermal Statistics and Thermal White Noises | p. 77 |
Canonical Representation of the Boson Thermal States | p. 79 |
Spectral Representation of Quantum White Noise | p. 81 |
Locality of Quantum Fields and Ultralocality of Quantum White Noises | p. 83 |
Those Kinds of Fields We Call Noises | p. 85 |
Convergence of Fields in the Sense of Correlators | p. 85 |
Generalized White Noises as the Stochastic Limit ofGaussian Fields | p. 86 |
Existence of Fock, Temperature and Squeezed White Noises | p. 90 |
Convergence of the Field Operator to a Classical White Noise | p. 92 |
Beyond the Master Equation: The Master Field | p. 93 |
Discrete Spectrum Embedded in theContinuum | p. 94 |
The Stochastic Limit of a Classical Gaussian Random Field | p. 97 |
Semiclassical Versus Semiquantum Approximation | p. 98 |
An Historical Example: The Damped Harmonic Oscillator | p. 100 |
Emergence of the White Noise: A Traditional Derivation | p. 102 |
Heuristic Origins of Quantum White Noise | p. 103 |
Relativistic Quantum White Noises | p. 104 |
Space-Time Rescalings: Multidimensional White Noises | p. 106 |
The Chronological Stochastic Limit | p. 108 |
Notes | p. 111 |
Open Systems | p. 113 |
The Nonrelativistic QED Hamiltonian | p. 113 |
The Dipole Approximation | p. 116 |
The Rotating-Wave Approximation | p. 117 |
Composite Systems | p. 118 |
Assumptions on the Environment (Field, Gas, Reservoir, etc.) | p. 119 |
Assumptions on the System Hamiltonian | p. 120 |
The Free Hamiltonian | p. 121 |
Multiplicative (Dipole-Type) Interactions: Canonical Form | p. 121 |
Approximations of the Multiplicative Hamiltonian | p. 122 |
Rotating-Wave Approximation Hamiltonians | p. 123 |
No Rotating-Wave Approximation Hamiltonians with Cutoff | p. 123 |
Neither Dipole nor Rotating-Wave Approximation Hamiltonians Without Cutoff | p. 124 |
The Generalized Rotating-WaveApproximation | p. 125 |
The Stochastic Limit of the Multiplicative Interaction | p. 126 |
The Normal Form of the White Noise Hamiltonian Equation | p. 127 |
Invariance of the Ito Correction Term Under Free System Evolution | p. 128 |
The Stochastic Golden Rule: Langevin and Master Equations | p. 129 |
Classical Stochastic Processes Underlying Quantum Processes | p. 132 |
The Fluctuation-Dissipation Relation | p. 133 |
Vacuum Transition Amplitudes | p. 134 |
Mass Gap of D+ D and Speed of Decay | p. 136 |
How to Avoid Decoherence | p. 137 |
The Energy Shell Scalar Product: Linewidths | p. 138 |
Dispersion Relations and the Ito Correction Term | p. 140 |
The Case: H1 = k2 | p. 141 |
Multiplicative Coupling with the Rotating Wave Approximation: ArbitraryGaussianState | p. 142 |
Multiplicative Coupling with RWA: Gauge Invariant State1 | p. 43 |
RedShifts and Blue Shifts | p. 144 |
The Free Evolution of the Master Field | p. 145 |
Algebras Invariant Under the Flow | p. 147 |
Notes | p. 148 |
Spin-Boson Systems | p. 153 |
Dropping the Rotating-Wave Approximation | p. 154 |
The Master Field | p. 154 |
The White Noise Hamiltonian Equation | p. 157 |
The Operator Transport Coefficient: no Rotating-Wave Approximation, Arbitrary Gaussian Reference State | p. 158 |
Different Roles of the Positive and Negative Bohr Frequencies | p. 159 |
No Rotating-Wave Approximation with Cutoff: Gauge Invariant States | p. 161 |
No Rotating-Wave Approximation with Cutoff: Squeezing States | p. 161 |
The Stochastic Golden Rule for Dipole Type Interactions and Gauge-Invariant States | p. 162 |
The Stochastic GoldenRule | p. 164 |
The Langevin Equation | p. 170 |
Subalgebras Invariant Under the Generator | p. 172 |
The Langevin Equation: Generic Systems | p. 173 |
The Stochastic Golden Rule Versus Standard Perturbation Theory | p. 176 |
Spin-Boson Hamiltonian | p. 178 |
The Damping and Oscillating Regimes: Fock Case | p. 181 |
The Damping and the Oscillating Regimes: Nonzero Temperature | p. 183 |
No Rotating-Wave Approximation Without Cutoff | p. 184 |
The Drift Term for Gauge-Invariant States | p. 185 |
The Free Evolution of the Master Field | p. 187 |
The Stochastic Limit of the Generalized Spin-Boson Hamiltonian | p. 187 |
The Langevin Equation | p. 190 |
Convergence to Equilibrium: Connections with Quantum Measurement | p. 191 |
Control of Coherence | p. 194 |
Dynamics of Spin Systems | p. 196 |
Nonstationary White Noises | p. 201 |
Notes | p. 202 |
Measurements and Filtering Theory | p. 205 |
Input-Output Channels | p. 205 |
The Filtering Problem in Classical Probability | p. 206 |
Field Measurements | p. 207 |
Properties of the Input and Output Processes | p. 210 |
The Filtering Problem in Quantum Theory | p. 213 |
Filtering of a Quantum System Over a Classical Process | p. 214 |
Nondemolition Processes | p. 215 |
Standard Scheme to Construct Examples of Nondemolition Measurements | p. 217 |
Discrete Time Nondemolition Processes | p. 217 |
Notes | p. 218 |
Idea of the Proof and Causal Normal Order | p. 219 |
Term-by-Term Convergence of the Series | p. 219 |
Vacuum Transition Amplitude: The Fourth-Order Term | p. 220 |
Vacuum Transition Amplitude: Non-Time-ConsecutiveDiagrams | p. 223 |
The Causal -Function and the Time-Consecutive Principle | p. 225 |
Theory of Distributions on the Standard Simplex | p. 227 |
The Second-Order Term of the Limit Vacuum Amplitude | p. 230 |
The Fourth-Order Term of the Limit Vacuum Amplitude | p. 230 |
Higher-Order Terms of the Vacuum-Vacuum Amplitude | p. 231 |
Proof of the Normal Form of the White Noise Hamiltonian Equation | p. 231 |
The Unitarity Condition for the Limit Equation | p. 233 |
Normal Form ofthe Thermal White Noise Equation: Boson Case | p. 234 |
From White Noise Calculus to Stochastic Calculus | p. 235 |
Chronological Product Approach to the Stochastic Limit | p. 237 |
Chronological Products | p. 237 |
Chronological Product Approach to the Stochastic Limit | p. 238 |
The Limit of the nth Term, Time-Ordered Product Approach: Vacuum Expectation | p. 242 |
The Stochastic Limit, Time-Ordered Product Approach: General Case | p. 244 |
Functional Integral Approach to the Stochastic Limit | p. 247 |
Statement of the Problem | p. 247 |
The StochasticLimit of the Free Massive Scalar Field | p. 248 |
The StochasticLimit of the Free Massless Scalar Field | p. 250 |
Polynomial Interactions | p. 251 |
The StochasticLimit of the Electromagnetic Field | p. 253 |
Low-Density Limit: The Basic Idea | p. 255 |
The Low-Density Limit: Fock Case, NoSystem | p. 255 |
The Low-Density Limit: Fock Case, Arbitrary System Operator | p. 257 |
Comparison of the Distribution and the Stochastic Approach | p. 258 |
LDL General, Fock Case, No System Operator, = 0 | p. 259 |
Six Basic Principles of the Stochastic Limit | p. 261 |
Polynomial Interactions with Cutoff | p. 262 |
Assumptions on the Dynamics: Standard Models | p. 263 |
Polynomial Interactions: Canonical Forms, FockCase | p. 266 |
Polynomial Interactions: Canonical Forms, Gauge-Invariant Case | p. 269 |
The Stochastic Universality Class Principle | p. 275 |
The Case of Many Independent Fields | p. 277 |
The Block Principle: Fock Case | p. 278 |
The Stochastic Resonance Principle | p. 280 |
The Orthogonalization Principle | p. 280 |
The Stochastic Bosonization Principle | p. 280 |
The Time-Consecutive Principle | p. 282 |
Strongly Nonlinear Regimes | |
Particles Interacting with a Boson Field | p. 285 |
A Single Particle Interacting with a Boson Field | p. 287 |
Dynamical q-Deformation: Emergence of the Entangled Commutation Relations | p. 289 |
The Two-Point and Four-Point Correlators | p. 291 |
The Stochastic Limit of the N-Point Correlator | p. 293 |
The q-Deformed Module Wick Theorem | p. 296 |
The Wick Theorem for the QED Module | p. 301 |
The Limit White Noise Hamiltonian Equation | p. 302 |
Free Independence of the Increments of the Master Field | p. 304 |
Boltzmannian White Noise Hamiltonian Equations: Normal Form | p. 306 |
Unitarity Conditions | p. 309 |
Matrix Elements of the Solution | p. 310 |
Normal Form of the QED Module Hamiltonian Equation | p. 312 |
Unitarity ofthe Solution: Direct Proof | p. 313 |
Matrix Elements of the Limit Evolution Operator | p. 314 |
Nonexponential Decays | p. 317 |
Equilibrium States | p. 321 |
The Master Field321 | |
Proof of the Result for the Two-and Four-Point Correlators | p. 322 |
The Vanishing ofthe Crossing Diagrams | p. 324 |
The Hot Free Algebra | p. 333 |
Interaction of the QEM Field with a Nonfree Particle | p. 335 |
The Limit Two-Point Function | p. 338 |
The Limit Four-Point Function | p. 342 |
The Limit Hilbert Module | p. 344 |
The Limit Stochastic Process | p. 347 |
The Stochastic Differential Equation | p. 348 |
Notes | p. 349 |
The Anderson Model | p. 351 |
Non relativistic Fermions in External Potential: The Anderson Model | p. 352 |
The Limit of the Connected Correlators | p. 355 |
The Four-Point Function | p. 356 |
The Limit of the Connected Transition Amplitude | p. 359 |
Proof of(13.4.3) | p. 362 |
Solution of the Nonlinear Equation(13.4.2) | p. 365 |
Notes | p. 367 |
Field-Field Interactions | p. 369 |
Interacting Commutation Relations | p. 369 |
The Tri-linear Hamiltonian with Momentum Conservation | p. 373 |
Proof of Theorem 14.2.1 | p. 375 |
Example: Four Internal Lines | p. 379 |
The Stochastic Limit for Green Functions | p. 380 |
Second Quantized Representation of the Nonrelativistic QED Hamiltonian | p. 381 |
Interacting Commutation Relations and QED Module Algebra | p. 383 |
Decay and the Universality Class of the QED Hamiltonian | p. 384 |
Photon Splitting Cascades and New Statistics | p. 386 |
Estimates and Proofs | |
Analytical Theory of Feynman Diagrams | p. 393 |
The Connected Component Theorem | p. 395 |
The Factorization Theorem | p. 402 |
The Caseof Many Independent Fields | p. 411 |
The Fermi Block Theorem | p. 411 |
Non-Time-Consecutive Terms: The First Vanishing Theorem | p. 416 |
Non-Time Consecutive Terms: The Second Vanishing Theorem | p. 419 |
The Type-I Term Theorem | p. 423 |
The Double Integral Lemma | p. 431 |
The Multiple-Simplex Theorem | p. 435 |
The Multiple Integral Lemma | p. 438 |
The Second Multiple-Simplex Theorem | p. 439 |
Some Combinatorial Facts and the Block Normal Ordering Theorem | p. 446 |
Term-by-Term Convergence | p. 453 |
The Universality Class Principle and Effective Interaction Hamiltonians | p. 455 |
Block and Orthogonalization Principles | p. 458 |
The Stochastic Resonance Principle | p. 459 |
References | p. 461 |
Index | p. 469 |
Table of Contents provided by Publisher. All Rights Reserved. |
ISBN: 9783540419280
ISBN-10: 3540419284
Published: 7th August 2002
Format: Hardcover
Language: English
Number of Pages: 500
Audience: Professional and Scholarly
Publisher: Springer Nature B.V.
Country of Publication: DE
Dimensions (cm): 23.39 x 15.6 x 2.69
Weight (kg): 0.84
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