I PROBABILITY IN CLASSICAL AND QUANTUM PHYSIC'S |
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Classical probability theory and stochastic processes |
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3 | (56) |
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3 | (2) |
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3 | (1) |
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Probability measures and Kolmogorov axioms |
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4 | (1) |
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Conditional probabilities and independence |
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5 | (1) |
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5 | (6) |
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Definition of random variables |
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6 | (2) |
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Transformation of random variables |
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8 | (1) |
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Expectation values and characteristic function |
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9 | (2) |
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11 | (3) |
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Formal definition of a stochastic process |
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11 | (1) |
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The hierarchy of, joint probability distributions |
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12 | (2) |
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14 | (18) |
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The Chapman-Kolmogorov equation |
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14 | (3) |
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Differential Chapman-Kolmogorov equation |
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17 | (2) |
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Deterministic processes and Liouville equation |
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19 | (2) |
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Jump processes and the master equation |
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21 | (7) |
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Diffusion processes and Fokker-Planck equation |
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28 | (4) |
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Piecewise deterministic processes |
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32 | (13) |
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The Liouville master equation |
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33 | (1) |
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Waiting time distribution and sample paths |
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33 | (4) |
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Path integral representation of PDPs |
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37 | (2) |
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Stochastic calculus for PDPs |
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39 | (6) |
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45 | (14) |
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Translation invariant processes |
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46 | (1) |
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The Levy-Khintchine formula |
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47 | (4) |
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51 | (6) |
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57 | (2) |
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59 | (50) |
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The statistical interpretation of quantum mechanics |
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59 | (15) |
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Self-adjoint operators and the spectral theorem |
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59 | (4) |
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Observables and random variables |
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63 | (2) |
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Pure states and statistical mixtures |
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65 | (5) |
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Joint, probabilities in quantum mechanics |
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70 | (4) |
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Composite quantum systems |
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74 | (5) |
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75 | (2) |
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Schmidt decomposition and entanglement |
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77 | (2) |
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79 | (4) |
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79 | (2) |
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81 | (1) |
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82 | (1) |
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The theory of quantum measurement |
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83 | (26) |
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Ideal quantum measurements |
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83 | (2) |
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85 | (2) |
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Representation theorem for quantum operations |
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87 | (5) |
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Quantum measurement and entropy |
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92 | (1) |
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93 | (3) |
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Indirect quantum measurements |
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96 | (6) |
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Quantum non-demolition measurements |
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102 | (2) |
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104 | (5) |
II DENSITY MATRIX THEORY |
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109 | (110) |
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Closed and open quantum systems |
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110 | (7) |
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The Liouville-von Neumann equation |
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110 | (2) |
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Heisenberg and interaction picture |
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112 | (3) |
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115 | (2) |
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117 | (13) |
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Quantum dynamical semigroups |
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117 | (2) |
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The Markovian quantum master equation |
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119 | (5) |
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The adjoint quantum master equation |
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124 | (1) |
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Multi-time correlation functions |
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125 | (3) |
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Irreversibility and entropy production |
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128 | (2) |
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130 | (11) |
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130 | (7) |
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Relaxation to equilibrium |
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137 | (1) |
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138 | (1) |
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139 | (2) |
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The quantum optical master equation |
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141 | (25) |
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Matter in quantized radiation fields |
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141 | (5) |
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Decay of a two-level system |
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146 | (3) |
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Decay into a squeezed field vacuum |
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149 | (3) |
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152 | (2) |
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154 | (6) |
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The damped harmonic oscillator |
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160 | (6) |
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Non-selective, continuous measurements |
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166 | (6) |
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166 | (1) |
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167 | (5) |
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172 | (29) |
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The Caldeira-Leggett model |
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172 | (1) |
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High-temperature master equation |
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173 | (9) |
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The exact, Heisenberg equations of motion |
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182 | (10) |
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192 | (9) |
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Non-linear quantum master equations |
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201 | (18) |
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Quantum Boltzmann equation |
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201 | (2) |
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Mean field master equations |
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203 | (2) |
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Mean field laser equations |
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205 | (3) |
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Non-linear Schrodinger equation |
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208 | (2) |
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210 | (6) |
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216 | (3) |
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219 | (64) |
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220 | (5) |
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An exactly solvable model |
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225 | (7) |
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Time evolution of the total system |
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225 | (2) |
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Decay of coherences and the decoherence factor |
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227 | (4) |
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Coherent subspaces and system-size dependence |
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231 | (1) |
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Markovian mechanisms of decoherence |
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232 | (10) |
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233 | (1) |
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234 | (1) |
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Internal degrees of freedom |
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235 | (2) |
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237 | (5) |
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The damped harmonic oscillator |
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242 | (9) |
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242 | (4) |
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246 | (5) |
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Electromagnetic field states |
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251 | (11) |
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Atoms interacting with a cavity field mode |
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251 | (6) |
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257 | (5) |
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262 | (7) |
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General decoherence formula |
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263 | (2) |
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265 | (4) |
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Decoherence and quantum measurement |
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269 | (14) |
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Dynamical selection of a pointer basis |
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270 | (5) |
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Dynamical model for a quantum measurement |
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275 | (3) |
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278 | (5) |
III STOCHASTIC PROCESSES IN HILBERT SPACE |
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Probability distributions on Hilbert space |
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283 | (20) |
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The state vector as a random variable in Hilbert space |
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283 | (8) |
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A new type of quantum mechanical ensemble |
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283 | (5) |
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288 | (3) |
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Probability density functionals on Hilbert space |
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291 | (8) |
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Probability measures on Hilbert space |
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291 | (3) |
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Distributions on projective Hilbert, space |
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294 | (3) |
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297 | (2) |
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299 | (4) |
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Probability density functionals on state space |
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299 | (2) |
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Description of selective quantum measurements |
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301 | (1) |
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302 | (1) |
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Stochastic dynamics in Hilbert space |
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303 | (58) |
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Dynamical semigroups and PDPs in Hilbert space |
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304 | (16) |
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Reduced system dynamics as a PDP |
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304 | (7) |
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The Hilbert space path integral |
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311 | (3) |
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314 | (2) |
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Multi-time correlation functions |
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316 | (4) |
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Stochastic: representation of continuous measurements |
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320 | (4) |
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Stochastic time evolution of εP-ensembles |
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321 | (1) |
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Short-time behaviour of the propagator |
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322 | (2) |
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324 | (11) |
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324 | (6) |
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330 | (5) |
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335 | (7) |
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Derivation of the; PDP for homodyne detection |
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336 | (4) |
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Stochastic Schrodinger equation |
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340 | (2) |
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Heterodyne photodetection |
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342 | (6) |
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Stochastic Schrodinger equation |
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342 | (3) |
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Stochastic collapse models |
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345 | (3) |
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Stochastic density matrix equations |
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348 | (2) |
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Photodetection on a field mode |
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350 | (11) |
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The photocounting formula |
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354 | (1) |
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QND measurement of a field mode |
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354 | (4) |
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358 | (3) |
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The stochastic simulation method |
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361 | (29) |
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Numerical simulation algorithms for PDPs |
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362 | (5) |
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Estimation of expectation values |
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362 | (1) |
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Generation of realizations of the process |
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363 | (1) |
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Determination of the waiting time |
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364 | (3) |
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367 | (1) |
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Algorithms for stochastic Schrodinger equations |
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367 | (6) |
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General remarks on convergence |
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368 | (2) |
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370 | (1) |
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370 | (1) |
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The fourth-order Runge-Kutta scheme |
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370 | (2) |
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A second-order weak scheme |
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372 | (1) |
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373 | (7) |
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The damped harmonic oscillator |
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373 | (4) |
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The driven two-level system |
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377 | (3) |
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A case study on numerical performance |
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380 | (10) |
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Numerical efficiency and scaling laws |
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381 | (2) |
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The damped driven Morse oscillator |
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383 | (6) |
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389 | (1) |
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Applications to quantum optical systems |
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390 | (51) |
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Continuous measurements in QED |
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391 | (10) |
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Constructing the microscopic Hamiltonian |
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391 | (2) |
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Determination of the QED operation |
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393 | (3) |
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Stochastic dynamics of multipole radiation |
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396 | (2) |
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Representation of incomplete measurements |
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398 | (3) |
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401 | (8) |
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Waiting time distribution and trapping state |
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401 | (4) |
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Measurement schemes and stochastic evolution |
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405 | (4) |
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Laser cooling and Levy processes |
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409 | (19) |
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Dynamics of the atomic wave function |
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410 | (6) |
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Coherent population trapping |
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416 | (5) |
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Waiting times and momentum distributions |
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421 | (7) |
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Strong field interaction and the Floquet picture |
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428 | (13) |
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429 | (2) |
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Stochastic dynamics in the Floquet picture |
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431 | (3) |
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Spectral detection and the dressed atom |
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434 | (3) |
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437 | (4) |
IV NON-MARKOVIAN QUANTUM PROCESSES |
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Projection operator techniques |
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441 | (19) |
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The Nakajima-Zwanzig projection operator technique |
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442 | (3) |
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442 | (1) |
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The Nakajima-Zwanzig equation |
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443 | (2) |
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The time-convolutionless projection operator method |
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445 | (11) |
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The time-local master equation |
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446 | (1) |
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Perturbation expansion of the TCL generator |
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447 | (4) |
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451 | (1) |
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Perturbation expansion of the inhomogeneity |
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452 | (3) |
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455 | (1) |
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Stochastic unravelling in the doubled Hilbert space |
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456 | (4) |
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458 | (2) |
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Non-Markovian dynamics in physical systems |
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460 | (41) |
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Spontaneous decay of a two-level system |
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461 | (13) |
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Exact master equation and TCL generator |
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461 | (5) |
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Jaynes-Cummings model on resonance |
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466 | (5) |
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Jaynes-Cummings model with detuning |
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471 | (3) |
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Spontaneous decay into a photonic band gap |
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474 | (1) |
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The damped harmonic oscillator |
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474 | (16) |
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The model and frequency renormalization |
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475 | (2) |
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Factorizing initial conditions |
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477 | (4) |
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481 | (2) |
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Non-factorizing initial conditions |
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483 | (5) |
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Disregarding the inhomogeneity |
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488 | (2) |
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490 | (11) |
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490 | (1) |
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Relaxation of an initially factorizing state |
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491 | (4) |
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Equilibrium correlation functions |
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495 | (1) |
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Transition from coherent to incoherent motion |
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496 | (1) |
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497 | (4) |
V RELATIVISTIC QUANTUM PROCESSES |
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Measurements in relativistic quantum mechanics |
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501 | (67) |
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The Schwinger-Tomonaga equation |
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502 | (5) |
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States as functionals of spacelike hypersurfaces |
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502 | (4) |
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506 | (1) |
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The measurement of local observables |
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507 | (19) |
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The operation for a local measurement |
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508 | (3) |
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Relativistic state reduction |
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511 | (3) |
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Multivalued space-time amplitudes |
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514 | (3) |
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The consistent hierarchy of joint probabilities |
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517 | (4) |
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521 | (2) |
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523 | (3) |
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Non-local measurements and causality |
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526 | (31) |
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527 | (3) |
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Non-local measurement by EPR probes |
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530 | (6) |
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Quantum state verification |
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536 | (2) |
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Non-local operations and the causality principle |
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538 | (6) |
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Restrictions on the measurability of operators |
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544 | (6) |
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QND verification of non-local states |
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550 | (4) |
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Preparation of non-local states |
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554 | (1) |
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555 | (2) |
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557 | (11) |
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Coherent transfer of quantum states |
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557 | (3) |
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Teleportation and I3e11-state measurement |
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560 | (2) |
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562 | (3) |
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565 | (3) |
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Open quantum electrodynamics |
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568 | (51) |
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Density matrix theory for QED |
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569 | (8) |
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Field equations and correlation functions |
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569 | (7) |
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The reduced density matrix |
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576 | (1) |
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The influence functional of QED |
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577 | (11) |
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Elimination of the radiation degrees of freedom |
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577 | (6) |
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Vacuum-to-vacuum amplitude |
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583 | (2) |
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Second-order equation of motion |
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585 | (3) |
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Decoherence by emission of bremsstrahlung |
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588 | (26) |
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Introducing the decoherence functional |
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589 | (4) |
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593 | (3) |
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Evaluation of the decoherence functional |
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596 | (11) |
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607 | (7) |
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Decoherence of many-particle states |
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614 | (5) |
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617 | (2) |
Index |
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619 | |