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Part I Classical Kinetic Concepts |
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3 | (8) |
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3 | (2) |
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1.2 Virial corrections to the kinetic equation |
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5 | (3) |
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1.2.1 Classical gas of hard spheres |
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6 | (1) |
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1.2.2 Hard-sphere corrections to the quantum Boltzmann equation |
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7 | (1) |
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1.2.3 Quantum nonlocal corrections in gases |
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7 | (1) |
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1.3 Quantum nonlocal corrections in dense Fermi systems |
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8 | (1) |
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1.4 Quantum nonlocal corrections to kinetic theory |
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9 | (2) |
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11 | (33) |
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11 | (5) |
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2.1.1 Principle of motion |
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11 | (1) |
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2.1.2 Principle of finite-range forces |
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12 | (4) |
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16 | (1) |
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2.2 Random versus deterministic |
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16 | (7) |
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17 | (1) |
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2.2.2 Velocity distribution |
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18 | (5) |
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2.3 Information versus chaos |
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23 | (3) |
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2.3.1 Entropy as a measure of negative information or disorder |
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23 | (2) |
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2.3.2 Maximum entropy and equilibrium thermodynamics |
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25 | (1) |
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2.4 Collisions versus drift |
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26 | (10) |
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27 | (2) |
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29 | (2) |
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2.4.3 Equivalence of low-angle collisions and momentum drift |
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31 | (5) |
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36 | (1) |
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2.5 Explicit versus hidden forces |
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36 | (8) |
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38 | (1) |
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39 | (2) |
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41 | (2) |
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43 | (1) |
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3 Classical Kinetic Theory |
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44 | (39) |
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3.1 Nonlocal and non-instant binary collisions |
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45 | (8) |
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45 | (1) |
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3.1.2 Sticky point particles |
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45 | (1) |
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3.1.3 Realistic particles |
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46 | (5) |
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3.1.4 Kinetic equation without a mean field |
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51 | (2) |
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53 | (1) |
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3.2 Effect of the mean field on collisions |
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53 | (4) |
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54 | (1) |
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55 | (2) |
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57 | (1) |
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3.3 Internal mechanism of energy conversion |
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57 | (1) |
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3.4 Equation of continuity |
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58 | (3) |
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58 | (3) |
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61 | (5) |
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3.5.1 Partial pressure of effective molecules |
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63 | (1) |
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3.5.2 Inaccessible volume |
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63 | (1) |
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3.5.3 Mean-field contribution to pressure |
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64 | (2) |
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66 | (2) |
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68 | (1) |
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3.8 Nonequilibrium hydrodynamic equations |
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69 | (2) |
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3.9 Two concepts of quasiparticles |
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71 | (7) |
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72 | (1) |
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3.9.2 Landau's quasiparticle concept |
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72 | (1) |
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3.9.3 Quasiparticle pressure |
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73 | (1) |
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3.9.4 Quasiparticle energy |
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74 | (4) |
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3.9.5 Two forms of quasiparticles |
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78 | (1) |
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78 | (5) |
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Part II Inductive Ways to Quantum Transport |
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4 Scattering on a Single Impurity |
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83 | (13) |
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83 | (4) |
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85 | (1) |
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4.1.2 Resolvent of the host crystal |
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86 | (1) |
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4.2 Scattering and Lippmann--Schwinger equation |
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87 | (3) |
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4.2.1 Born approximation of the scattered wave |
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88 | (2) |
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90 | (1) |
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90 | (2) |
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92 | (3) |
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4.4.1 Scattering on two impurities |
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94 | (1) |
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95 | (1) |
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5 Multiple Impurity Scattering |
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96 | (26) |
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5.1 Divergence of multiple scattering expansion 9 |
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7 | (91) |
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5.2 Averaged wave function |
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98 | (5) |
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101 | (1) |
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102 | (1) |
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5.2.3 Born approximation of selfenergy |
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102 | (1) |
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5.3 Selfconsistent Born approximation |
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103 | (2) |
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5.4 Averaged T-matrix approximation |
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105 | (2) |
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5.4.1 Double counts in the averaged T-matrix approximation |
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106 | (1) |
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107 | (4) |
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5.5.1 Averaged T-matrix approximation in the virtual crystal |
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107 | (3) |
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5.5.2 Averaged T-matrix approximation in the selfconsistent effective crystal |
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110 | (1) |
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5.6 Coherent potential approximation |
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111 | (3) |
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5.6.1 Lorentz-Lorenz local-field correction |
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112 | (1) |
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5.6.2 Coherent potential approximation as the local-field correction |
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113 | (1) |
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114 | (8) |
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5.7.1 Densities of states |
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115 | (1) |
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5.7.2 Bottom of allowed energies in the main band |
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116 | (1) |
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117 | (1) |
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5.7.4 Effect of the collision delay on the density of states |
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118 | (1) |
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5.7.5 Test of approximations in the atomic limit |
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119 | (3) |
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122 | (1) |
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6.1 Averaged amplitude of wave function |
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122 | (1) |
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6.2 Straightforward perturbative expansion |
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122 | (2) |
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6.2.1 Transport vertex in the non-selfconsistent Born approximation |
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123 | (1) |
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6.3 Generalised Kadanoff and Baym formalism |
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124 | (4) |
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126 | (1) |
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6.3.2 Transport vertex in the Born approximation |
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126 | (1) |
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6.3.3 Transport vertex in the selfconsistent averaged T-matrix approximation |
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127 | (1) |
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6.3.4 Coherent potential approximation of the transport vertex |
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128 | (1) |
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128 | (1) |
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129 | (1) |
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6.6 Elimination of surrounding interaction channels-secular equation |
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130 | (3) |
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6.6.1 Wave function renormalisation |
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131 | (1) |
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131 | (1) |
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6.6.3 Two actions of selfenergy |
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132 | (1) |
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133 | (5) |
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Part III Deductive Way to Quantum Transport |
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7 Nonequilibrium Green's Functions |
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137 | (140) |
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7.1 Method of equation of motion |
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137 | (5) |
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7.1.1 Enclosure of hierarchy |
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139 | (3) |
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7.2 Quantum transport equation |
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142 | (2) |
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7.3 Information contained in Green's functions |
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144 | (8) |
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7.3.1 Density and current |
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145 | (1) |
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7.3.2 Total energy content |
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145 | (1) |
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146 | (1) |
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7.3.4 Equilibrium information |
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147 | (2) |
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7.3.5 Matsubara technique |
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149 | (2) |
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7.3.6 Equilibrium pressure |
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151 | (1) |
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152 | (1) |
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153 | (11) |
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153 | (2) |
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8.1.1 Causality and Kramers-Kronig relation |
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153 | (1) |
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154 | (1) |
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8.2 Quasiparticle and extended quasiparticle picture |
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155 | (3) |
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8.3 Comparison with equilibrium |
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158 | (2) |
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8.4 The problem of ansatz |
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160 | (4) |
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8.4.1 Further spectral functions |
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162 | (1) |
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162 | (2) |
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9 Quantum Kinetic Equations |
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164 | (30) |
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9.1 Kadanoff and Baym equation in quasiclassical limit |
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164 | (8) |
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164 | (1) |
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9.1.2 Quasiclassical Kadanoff and Baym equation |
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165 | (2) |
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9.1.3 Collision-less Landau equation |
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167 | (1) |
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9.1.4 Landau equation with collisions |
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168 | (1) |
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169 | (1) |
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9.1.6 Causality and gradient corrections |
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170 | (2) |
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9.1.7 Conclusion from off-shell contributions |
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172 | (1) |
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9.2 Separation of on-shell and off-shell motion |
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172 | (2) |
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9.3 Differential transport equation |
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174 | (3) |
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9.3.1 Quasiclassical limit |
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176 | (1) |
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9.4 Extended quasiparticle picture |
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177 | (5) |
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9.4.1 Precursor of kinetic equation |
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180 | (2) |
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9.5 Numerical examples for equilibrium |
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182 | (3) |
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9.6 Direct gradient expansion of non-Markovian equation |
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185 | (6) |
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9.6.1 Connection between the Wigner and quasiparticle distributions |
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188 | (1) |
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9.6.2 Landau--Silin equation |
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188 | (3) |
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9.7 Alternative approaches to the kinetic equation |
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191 | (3) |
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9.7.1 First quasiclassical approximation |
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91 | (101) |
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9.7.2 Thermo field dynamics approach |
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192 | (2) |
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10 Approximations for the Selfenergy |
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194 | (36) |
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194 | (3) |
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10.2 Random phase approximation |
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197 | (9) |
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10.2.1 Long-range Coulomb interaction |
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197 | (1) |
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10.2.2 Density-density fluctuations |
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198 | (5) |
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10.2.3 Lenard-Balescu collision integral |
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203 | (3) |
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10.3 Selfenergy and effective mass in quasi two-dimensional systems |
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206 | (6) |
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10.3.1 Polarisation function in 2D |
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206 | (2) |
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10.3.2 Integrals over dielectric functions |
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208 | (1) |
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10.3.3 Selfenergy and effective mass |
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208 | (4) |
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10.4 Vertex correction to RPA polarisation |
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212 | (1) |
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10.5 Suucture factor and pair-correlation function |
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213 | (5) |
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10.5.1 Fock approximation |
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214 | (1) |
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10.5.2 Born approximation |
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215 | (1) |
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10.5.3 Collision integral in Born approximation |
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216 | (1) |
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10.5.4 Pair-correlation function in equilibrium |
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217 | (1) |
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10.6 Ladder approximation |
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218 | (8) |
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220 | (1) |
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221 | (1) |
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10.6.3 Scattering T-matrix |
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222 | (1) |
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10.6.4 Missing particle-hole channels |
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222 | (4) |
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10.7 Bethe--Salpeter equation in quasiparticle approximation |
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226 | (2) |
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10.8 Local and instant quantum Boltzmann kinetic equation |
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228 | (2) |
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11 Variational Techniques of Many-Body Theory |
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230 | (37) |
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11.1 Dyson time ordering and Dirac interaction representation |
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230 | (2) |
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11.2 Representation of Green's functions |
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232 | (4) |
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11.2.1 Screening for Coulomb systems |
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235 | (1) |
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236 | (3) |
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11.3.1 Under which conditions does RPA become exact in the high-density limit of fermions? |
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238 | (1) |
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239 | (1) |
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11.5 Asymmetric and cummulant expansion |
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240 | (12) |
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11.5.1 Binary collision approximation |
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244 | (1) |
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11.5.2 Three-particle approximations |
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244 | (1) |
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11.5.3 Screened-ladder approximation |
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245 | (3) |
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11.5.4 Maximally crossed diagrams |
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248 | (1) |
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249 | (1) |
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11.5.6 Pair-pair correlation |
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250 | (2) |
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252 | (4) |
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252 | (1) |
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11.6.2 Connection to diagrammatic expansions |
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252 | (2) |
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11.6.3 Schema for constructing higher-order diagrams |
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254 | (1) |
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11.6.4 Linearising kinetic equations |
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255 | (1) |
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11.7 Response in finite systems |
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256 | (3) |
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11.8 Renormalisation techniques |
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259 | (8) |
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11.8.1 Low-energy degrees of freedom |
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259 | (3) |
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11.8.2 Results for separable interaction |
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262 | (3) |
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11.8.3 Functional renormalisation |
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265 | (2) |
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12 Systems with Condensates and Pairing |
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267 | (48) |
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12.1 Condensation phenomena in correlated systems |
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267 | (4) |
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12.1.1 Bose-Einstein condensation in correlated systems |
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267 | (1) |
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12.1.2 Measurement of the quasiparticle spectrum |
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268 | (1) |
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12.1.3 Quasi-classical approach to superfluidity |
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269 | (1) |
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12.1.4 Quasi-classical approach to superconductivity |
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270 | (1) |
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12.2 Cold interacting Bose gas |
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271 | (7) |
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271 | (1) |
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12.2.2 Bogoliubov transformation for a cold interacting Bose gas |
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272 | (5) |
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12.2.3 Popov approximation |
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277 | (1) |
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12.3 Generalised Soven scheme |
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278 | (6) |
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12.3.1 Missing pole structure |
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278 | (2) |
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12.3.2 Link to anomalous propagators |
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280 | (3) |
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12.3.3 Bogoliubov-DeGennes equation |
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283 | (1) |
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284 | (6) |
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12.4.1 Generalised Soven scheme of coherent potential approximation |
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287 | (3) |
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12.5 Interacting Bose gas at finite temperatures |
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290 | (7) |
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292 | (5) |
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12.6 Comparison of approximations |
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297 | (3) |
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298 | (2) |
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300 | (1) |
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12.7.1 Critical temperature and density of states |
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301 | (1) |
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12.8 Stability of the pairing condensate |
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301 | (7) |
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12.8.1 Galitskii T-matrix |
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306 | (1) |
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12.8.2 Kadanoff-Martin theory |
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307 | (1) |
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12.9 Excitation of Cooper pairs from the condensate |
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308 | (7) |
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12.9.1 Galitskii T-matrix and Kadanoff-Martin theory |
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308 | (1) |
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309 | (1) |
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12.9.3 Relation of pairing density to correlated density |
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310 | (5) |
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Part IV Nonlocal Kinetic Theory |
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13 Nonlocal Collision Integral |
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315 | (11) |
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315 | (4) |
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13.1.1 Two-particle matrix products |
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316 | (1) |
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13.1.2 Convolution of initial states |
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317 | (1) |
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13.1.3 Convolution of T-matrix and hole Green's function |
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318 | (1) |
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13.2 Binary and ternary collisions |
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319 | (2) |
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13.3 Complete kinetic equation |
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321 | (2) |
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13.4 Particle-hole versus space-time symmetry |
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323 | (2) |
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13.4.1 Kinetic equation for Monte-Carlo simulations |
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325 | (1) |
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325 | (1) |
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14 Properties of Non-Instant and Nonlocal Corrections |
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326 | (16) |
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14.1 Recovering classical Δ's from quantum formulae |
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327 | (2) |
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14.1.1 Collision delay Δt |
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327 | (1) |
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14.1.2 Hard-sphere displacement |
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328 | (1) |
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14.2 Invariances of the nonlocal scattering integral |
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329 | (3) |
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329 | (2) |
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14.2.2 Galilean invariance |
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331 | (1) |
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14.3 Quantum Δ's for isolated particles |
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332 | (9) |
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14.3.1 Gauge transformation to a system free of mean field |
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332 | (1) |
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14.3.2 Galilean transformation to the barycentric coordinate framework |
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333 | (1) |
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14.3.3 Rotational symmetry |
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334 | (1) |
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14.3.4 Energy conservation and time-reversal symmetry |
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335 | (1) |
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14.3.5 Classical-like parametrisation |
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336 | (1) |
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14.3.6 Representation in partial waves |
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337 | (1) |
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14.3.7 Numerical results for nuclear matter |
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338 | (3) |
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341 | (1) |
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15 Nonequilibrium Quantum Hydrodynamics |
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342 | (29) |
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15.1 Local conservation laws |
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342 | (1) |
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15.2 Symmetries of collisions |
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343 | (4) |
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343 | (1) |
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344 | (1) |
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15.2.3 Symmetrisation of collision term |
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345 | (2) |
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15.3 Drift contributions to balance equations |
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347 | (4) |
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15.3.1 Density balance from drift |
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347 | (1) |
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15.3.2 Energy balance from the drift |
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348 | (1) |
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15.3.3 Balance of forces from the drift |
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349 | (1) |
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350 | (1) |
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15.4 Molecular contributions to observables from collision integral |
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351 | (8) |
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15.4.1 Expansion properties |
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351 | (1) |
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15.4.2 Correlated observables |
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352 | (3) |
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15.4.3 Molecular current contributions from collision integral |
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355 | (3) |
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358 | (1) |
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15.5 Balance equations and proof of H-theorem |
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359 | (5) |
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15.5.1 Equation of continuity |
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359 | (1) |
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360 | (1) |
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15.5.3 Navier-Stokes equation |
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361 | (1) |
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361 | (1) |
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15.5.5 Proof of H-theorem |
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362 | (2) |
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15.6 Equivalence to extended quasiparticle picture |
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364 | (2) |
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15.6.1 Generalised Beth--Uhlenbeck formula |
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364 | (1) |
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15.6.2 Correlated density in terms of the collision delay |
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365 | (1) |
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15.7 Limit of Landau theory |
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366 | (1) |
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367 | (4) |
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Part V Selected Applications |
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16 Diffraction on a Barrier |
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371 | (21) |
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16.1 One-dimensional barrier |
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371 | (2) |
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16.1.1 Convenient formulation of the boundary problem |
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371 | (2) |
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16.2 Matrix inversion with surface Green's functions |
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373 | (5) |
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16.2.1 Summary of the method |
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377 | (1) |
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16.3 Reflection and transmission |
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378 | (2) |
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16.3.1 Current and current fluctuations |
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379 | (1) |
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16.4 Transport coefficients: parallel stacked organic molecules |
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380 | (3) |
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383 | (5) |
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16.5.1 Configurational averaging |
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383 | (1) |
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384 | (2) |
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16.5.3 Dissipative diffraction: example GaAs/A1As layer |
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386 | (2) |
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16.6 Three-dimensional barrier in a multi-band crystal |
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388 | (4) |
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16.6.1 Diffraction in multi-band crystals |
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390 | (2) |
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17 Deep Impurities with Collision Delay |
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392 | (10) |
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17.1 Transport properties |
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392 | (3) |
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395 | (2) |
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17.3 Compensation of virial and quasiparticle corrections |
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397 | (5) |
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17.3.1 Long wave-length limit |
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397 | (1) |
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17.3.2 Virial correction to Fermi momentum |
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398 | (1) |
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399 | (3) |
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18 Relaxation-Time Approximation |
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402 | (13) |
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402 | (2) |
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18.2 Transport coefficients |
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404 | (1) |
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18.3 Transport coefficients for metals |
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405 | (1) |
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18.4 Transport coefficients in high-temperature gases |
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406 | (3) |
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18.4.1 Stress or momentum current-density tensor |
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408 | (1) |
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18.5 Exact solution of a linearised Boltzmann equation |
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409 | (6) |
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415 | (26) |
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19.1 Formation of correlations |
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417 | (5) |
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417 | (2) |
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19.1.2 Formation of correlations in plasma |
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419 | (2) |
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19.1.3 Formation of correlations in nuclear matter |
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421 | (1) |
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19.2 Quantum quenches and sudden switching |
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422 | (7) |
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19.2.1 Atoms in a lattice after sudden quench |
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424 | (2) |
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19.2.2 Femtosecond laser response |
|
|
426 | (3) |
|
19.3 Failure of memory-kinetic equations |
|
|
429 | (5) |
|
|
429 | (2) |
|
19.3.2 Double count of correlation energy explained by extended quasiparticle picture |
|
|
431 | (3) |
|
19.4 Initial correlations |
|
|
434 | (6) |
|
19.4.1 Formation of correlations with initial correlations |
|
|
438 | (2) |
|
|
440 | (1) |
|
20 Field-Dependent Transport |
|
|
441 | (17) |
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|
441 | (2) |
|
20.1.1 Equation for Wigner distribution |
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|
442 | (1) |
|
20.1.2 Spectral function and ansatz |
|
|
442 | (1) |
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20.2 Kinetic equation in dynamically screened approximation |
|
|
443 | (3) |
|
20.3 Feedback and relaxation effects |
|
|
446 | (2) |
|
20.4 Conductivity with electron-electron interaction |
|
|
448 | (2) |
|
20.5 Isothermal conductivity |
|
|
450 | (3) |
|
20.5.1 Quasi two-dimensional example |
|
|
450 | (3) |
|
20.6 Adiabatic conductivity |
|
|
453 | (1) |
|
20.6.1 Quasi two-dimensional example |
|
|
453 | (1) |
|
20.7 Debye--Onsager relaxation effect |
|
|
454 | (4) |
|
20.7.1 Thermally averaged dynamically screened result |
|
|
455 | (1) |
|
20.7.2 Asymmetric dynamically screened result |
|
|
456 | (2) |
|
21 Kinetic Theory of Systems with SU(2) Structure |
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|
458 | (31) |
|
21.1 Transport in electric and magnetic fields |
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|
458 | (4) |
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|
458 | (1) |
|
|
459 | (1) |
|
21.1.3 Conductivity for crossed electric and magnetic fields: orbital motion |
|
|
460 | (2) |
|
21.2 Systems with electro-magnetic fields and spin-orbit coupling |
|
|
462 | (1) |
|
21.2.1 Various spin-orbit coupling as SU(2) structure |
|
|
462 | (1) |
|
21.3 Meanfield kinetic equations |
|
|
463 | (8) |
|
21.3.1 Gradient expansion |
|
|
463 | (1) |
|
|
464 | (2) |
|
|
466 | (2) |
|
21.3.4 Coupled kinetic equations |
|
|
468 | (1) |
|
21.3.5 Quasi stationary solution |
|
|
469 | (2) |
|
21.4 Normal and anomal currents |
|
|
471 | (1) |
|
|
472 | (4) |
|
21.5.1 Linearisation to external electric field |
|
|
472 | (1) |
|
21.5.2 Conductivities without magnetic fields |
|
|
473 | (1) |
|
|
474 | (2) |
|
21.6 Response with magnetic fields |
|
|
476 | (7) |
|
21.6.1 Retardation subtleties by magnetic field |
|
|
479 | (1) |
|
21.6.2 Classical-Hall effect |
|
|
480 | (1) |
|
21.6.3 Quantum-Hall effect |
|
|
481 | (2) |
|
21.7 Spin-Hall effect, conductivity of graphene |
|
|
483 | (6) |
|
21.7.1 Dirac (Weyl) dispersion |
|
|
483 | (1) |
|
|
483 | (3) |
|
|
486 | (1) |
|
21.7.4 Pseudo-spin conductivity |
|
|
487 | (2) |
|
22 Relativistic Transport |
|
|
489 | (15) |
|
22.1 Model and basic equations |
|
|
489 | (2) |
|
22.2 Coupled Green's functions for meson and baryons |
|
|
491 | (5) |
|
22.3 Equilibrium and saturation thermodynamic properties |
|
|
496 | (3) |
|
|
499 | (5) |
|
23 Simulations of Heavy-Ion Reactions with Nonlocal Collisions |
|
|
504 | (15) |
|
23.1 Scenario of low-energy heavy-ion reactions |
|
|
504 | (1) |
|
23.1.1 Numerical simulations of heavy-ion reactions |
|
|
505 | (1) |
|
23.2 Instant nonlocal approximation |
|
|
505 | (5) |
|
23.2.1 Displacements from the on-shell shifts |
|
|
507 | (2) |
|
23.2.2 Realistic displacements |
|
|
509 | (1) |
|
23.3 Numerical simulation results |
|
|
510 | (5) |
|
23.4 Quasiparticle renormalisation |
|
|
515 | (4) |
|
23.4.1 Experimental charge density distribution |
|
|
517 | (2) |
|
Appendix A Density-Operator Technique |
|
|
519 | (8) |
|
|
519 | (1) |
|
A.2 Derivation of the Levinson equation and non-Markovian energy conservation |
|
|
520 | (2) |
|
A.3 Debye-Onsager relaxation effect from classical hierarchy |
|
|
522 | (5) |
|
A.3.1 With background friction |
|
|
524 | (2) |
|
|
526 | (1) |
|
Appendix B Complex Time Path |
|
|
527 | (4) |
|
Appendix C Derived Optical Theorem |
|
|
531 | (6) |
|
Appendix D Proof of Drift and Gain Compensation into the Rate of Quasiparticles |
|
|
537 | (8) |
|
Appendix E Separable Interactions |
|
|
545 | (6) |
|
E.1 Yamaguchi form factor |
|
|
546 | (5) |
References |
|
551 | (16) |
Index |
|
567 | |