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1 | (14) |
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12 | (3) |
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2 Schrodinger Theory from the `Newtonian' Perspective of `Classical' Fields Derived from Quantal Sources |
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15 | (52) |
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2.1 Time-Dependent Schrodinger Theory |
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16 | (1) |
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2.2 Definitions of Quantal Sources |
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17 | (5) |
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2.2.1 Electron Density ρ(rt) |
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18 | (1) |
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2.2.2 Spinless Single--Particle Density Matrix γ(Rr't) |
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18 | (1) |
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2.2.3 Pair--Correlation Density g(rr't), and Fermi--Coulomb Hole ρxc(rr't) |
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19 | (2) |
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2.2.4 Current Density j(rt) |
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21 | (1) |
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2.3 Definitions of `Classical' Fields |
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22 | (3) |
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2.3.1 Electron--Interaction Field Eee(rt) |
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22 | (1) |
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2.3.2 Differential Density Field D(rt) |
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23 | (1) |
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2.3.3 Kinetic Field Z(rt) |
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23 | (1) |
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2.3.4 Current Density Field J(rt) |
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24 | (1) |
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2.4 Energy Components in Terms of Quantal Sources and Fields |
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25 | (2) |
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2.4.1 Electron--Interaction Potential Energy Eee(t) |
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25 | (1) |
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2.4.2 Kinetic Energy T(t) |
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26 | (1) |
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2.4.3 External Potential Energy Eext(t) |
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27 | (1) |
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2.5 Schrodinger Theory and the `Quantal Newtonian' Second Law |
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27 | (2) |
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2.6 Integral Virial Theorem |
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29 | (2) |
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2.7 The Quantum--Mechanical `Hydrodynamical' Equations |
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31 | (1) |
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2.8 The Internal Field of the Electrons and Ehrenfest's Theorem |
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32 | (4) |
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2.9 The Harmonic Potential Theorem |
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36 | (2) |
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2.10 Time-Independent Schrodinger Theory: Ground and Bound Excited States |
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38 | (6) |
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2.10.1 The `Quantal Newtonian' First Law |
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38 | (2) |
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2.10.2 Coalescence Constraints |
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40 | (2) |
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2.10.3 Asymptotic Structure of Wavefunction and Density |
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42 | (2) |
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2.11 Examples of the `Newtonian' Perspective: The Ground and First Excited Singlet State of the Hooke's Atom |
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44 | (15) |
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44 | (2) |
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2.11.2 Wavefunction, Orbital Function, and Density |
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46 | (5) |
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2.11.3 Fermi--Coulomb Hole Charge Distribution ρxc(rr') |
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51 | (2) |
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2.11.4 Hartree, Pauli--Coulomb, and Electron--Interaction Fields EH(r), Exc(r), Eee(r) and Energies EH, Exc, Eee |
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53 | (3) |
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2.11.5 Kinetic Field Z(r) and Kinetic Energy T |
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56 | (1) |
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2.11.6 Differential Density Field D(r) |
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57 | (1) |
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2.11.7 Total Energy E and Ionization Potential I |
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57 | (2) |
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2.11.8 Expectations of Other Single--Particle Operators |
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59 | (1) |
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2.12 Schrodinger Theory and Quantum Fluid Dynamics |
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59 | (8) |
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2.12.1 Single--Electron Case |
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60 | (1) |
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2.12.2 Many--Electron Case |
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61 | (4) |
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65 | (2) |
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3 Quantal Density Functional Theory |
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67 | (68) |
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3.1 Time-Dependent Quantal Density Functional Theory: Part I |
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71 | (15) |
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72 | (3) |
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75 | (3) |
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3.1.3 Total Energy and Components in Terms of Quantal Sources and Fields |
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78 | (3) |
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3.1.4 The S System `Quantal Newtonian' Second Law |
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81 | (2) |
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3.1.5 Effective Field Feff(rt) and Electron-Interaction Potential Energy υee(rt) |
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83 | (3) |
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86 | (3) |
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3.2.1 Integral Virial Theorem |
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86 | (1) |
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3.2.2 Ehrenfest's Theorem and the Zero Force Sum Rule |
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86 | (1) |
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87 | (2) |
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3.3 Time-Dependent Quantal Density Functional Theory: Part II |
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89 | (2) |
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3.4 Time-Independent Quantal Density Functional Theory |
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91 | (9) |
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3.4.1 The Interacting System and the `Quantal Newtonian' First Law |
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91 | (1) |
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3.4.2 The S System and Its `Quantal Newtonian' First Law |
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92 | (1) |
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93 | (1) |
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94 | (1) |
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3.4.5 Total Energy and Components |
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94 | (2) |
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3.4.6 Effective Field Feff(r) and Electron--Interaction Potential Energy υee(r) |
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96 | (1) |
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97 | (1) |
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3.4.8 Highest Occupied Eigenvalue εm |
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98 | (1) |
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3.4.9 Proof that Nonuniqueness of Effective Potential Energy Is Solely Due to Correlation-Kinetic Effects |
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99 | (1) |
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3.5 Application of Q-DFT to the Ground and First Excited Singlet State of the Hooke's Atom |
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100 | (15) |
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3.5.1 S System Wavefunction, Spin--Orbitals, and Density |
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101 | (1) |
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3.5.2 Pair--Correlation Density; Fermi and Coulomb Hole Charge Distributions |
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102 | (4) |
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3.5.3 Hartree, Pauli, and Coulomb Fields EH(r), Ex(r), Ec(r) and Energies EH, Ex, Ec |
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106 | (2) |
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3.5.4 Hartree WH(r), Pauli Wx(r), and Coulomb Wc(r) Potential Energies |
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108 | (2) |
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3.5.5 Correlation--Kinetic Field Ztc(r), Energy Tc, and Potential Energy Wtc(r) |
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110 | (4) |
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3.5.6 Total Energy and Ionization Potential |
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114 | (1) |
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3.5.7 Endnote on the Multiplicity of Potentials |
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114 | (1) |
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3.6 Quantal Density Functional Theory of Degenerate States |
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115 | (1) |
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3.7 Application of Q-DFT to the Wigner High-Electron-Correlation Regime of Nonuniform Density Systems |
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116 | (2) |
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3.8 Quantal Density Functional Theory of Hartree--Fock and Hartree Theories |
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118 | (17) |
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3.8.1 Hartree--Fock Theory |
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119 | (3) |
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3.8.2 The Slater--Bardeen Interpretation of Hartree--Fock Theory |
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122 | (2) |
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3.8.3 Theorems in Hartree--Fock Theory |
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124 | (1) |
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3.8.4 Q--DFT of Hartree--Fock Theory |
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124 | (3) |
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127 | (3) |
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3.8.6 Q--DFT of Hartree Theory |
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130 | (2) |
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132 | (3) |
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4 Hohenberg--Kohn, Kohn--Sham, and Runge--Gross Density Functional Theories |
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135 | (50) |
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4.1 The Hohenberg--Kohn Theorems |
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140 | (8) |
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4.1.1 The First Hohenberg-Kohn Theorem |
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141 | (2) |
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4.1.2 Implications of the First Hohenberg-Kohn Theorem |
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143 | (2) |
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4.1.3 The Second Hohenberg-Kohn Theorem |
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145 | (1) |
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4.1.4 The Primacy of the Electron Number in Hohenberg-Kohn Theory |
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146 | (2) |
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4.2 Generalization of the Fundamental Theorem of Hohenberg-Kohn |
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148 | (6) |
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4.2.1 The Unitary Transformation |
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149 | (2) |
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4.2.2 New Insights as a Consequence of the Generalization |
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151 | (3) |
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154 | (1) |
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4.4 The Percus-Levy-Lieb Constrained-Search Path |
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155 | (3) |
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4.5 Kohn--Sham Density Functional Theory |
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158 | (6) |
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4.6 Runge-Gross Time-Dependent Density Functional Theory |
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164 | (3) |
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4.7 Generalization of the Runge-Gross Theorem |
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167 | (3) |
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4.8 Corollary to the Hohenberg--Kohn and Runge-Gross Theorems |
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170 | (15) |
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4.8.1 Corrollary to the Hohenberg-Kohn Theorem |
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172 | (6) |
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4.8.2 Corollary to the Runge-Gross Theorem |
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178 | (2) |
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180 | (2) |
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182 | (3) |
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5 Physical Interpretation of Kohn--Sham Density Functional Theory via Quantal Density Functional Theory |
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185 | (30) |
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5.1 Interpretation of the Kohn--Sham Electron--Interaction Energy Functional EKSee[ ρ] and Its Derivative υee(r) |
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187 | (4) |
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5.2 Adiabatic Coupling Constant Scheme |
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191 | (7) |
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5.2.1 Q--DFT Within Adiabatic Coupling Constant Framework |
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192 | (2) |
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5.2.2 KS--DFT Within Adiabatic Coupling Constant Framework |
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194 | (2) |
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5.2.3 Q--DFT and KS--DFT in Terms of the Adiabatic Coupling Constant Perturbation Expansion |
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196 | (2) |
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5.3 Interpretation of the Kohn--Sham `Exchange' Energy Functional EKSx[ ρ] and Its Derivative υx(r) |
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198 | (1) |
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5.4 Interpretation of the Kohn--Sham `Correlation' Energy Functional EKSc[ ρ] and Its Derivative υc(r) |
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199 | (1) |
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5.5 Interpretation of the KS--DFT of Hartree--Fock Theory |
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200 | (1) |
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5.6 Interpretation of the KS--DFT of Hartree Theory |
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201 | (1) |
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5.7 The Optimized Potential Method |
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202 | (6) |
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5.7.1 The `Exchange--Only' Optimized Potential Method |
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203 | (5) |
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5.8 Physical Interpretation of the Optimized Potential Method |
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208 | (7) |
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5.8.1 Interpretation of `Exchange--Only' OPM |
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208 | (1) |
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5.8.2 A. Derivation via Q--DFT |
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208 | (3) |
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5.8.3 B. Derivation via the XO--OPM Integral Equation |
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211 | (1) |
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212 | (3) |
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6 Quantal Density Functional Theory of the Density Amplitude |
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215 | (16) |
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6.1 Density Functional Theory of the B System |
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217 | (4) |
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6.1.1 DFT Definitions of the Pauli Kinetic and Potential Energies |
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220 | (1) |
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6.2 Derivation of the Differential Equation for the Density Amplitude from the Schrodinger Equation |
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221 | (3) |
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6.3 Quantal Density Functional Theory of the B System |
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224 | (5) |
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6.3.1 Q--DFT Definitions of the Pauli Kinetic and Potential Energy |
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228 | (1) |
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229 | (2) |
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230 | (1) |
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7 Quantal Density Functional Theory of the Discontinuity in the Electron--Interaction Potential Energy |
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231 | (22) |
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7.1 Origin of the Discontinuity of the Electron--Interaction Potential Energy |
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232 | (4) |
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7.2 Expression for Discontinuity Δ in Terms of S System Eigenvalues |
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236 | (3) |
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7.3 Correlations Contributing to the Discontinuity According To Kohn--Sham Theory |
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239 | (1) |
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7.4 Quantal Density Functional Theory of the Discontinuity |
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239 | (11) |
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7.4.1 Correlations Contributing to the Discontinuity According To Q--DFT: Analytical Proof |
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242 | (2) |
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244 | (6) |
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250 | (3) |
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251 | (2) |
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8 Generalized Hohenberg-Kohn Theorems in Electrostatic and Magnetostatic Fields |
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253 | (30) |
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8.1 The Classical Hamiltonian and Properties |
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256 | (3) |
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256 | (3) |
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8.2 The Quantum-Mechanical Hamiltonian and Properties |
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259 | (6) |
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8.3 Generalized Hohenberg-Kohn Theorems |
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265 | (12) |
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8.3.1 Proof of Generalized Hohenberg-Kohn Theorems: Case I: Spinless Electrons |
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266 | (6) |
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8.3.2 Proof of Generalized Hohenberg-Kohn Theorems: Case II: Electrons with Spin |
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272 | (5) |
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8.4 Remarks on Spin and Current Density Functional Theories |
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277 | (4) |
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8.4.1 Remarks on Spin Density Functional Theory |
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277 | (2) |
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8.4.2 Remarks on Paramagnetic Current Density Functional Theory |
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279 | (2) |
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281 | (2) |
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281 | (2) |
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9 Quantal-Density Functional Theory in the Presence of a Magnetostatic Field |
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283 | (30) |
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9.1 Schrodinger Theory and the `Quantal Newtonian' First Law |
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285 | (6) |
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9.2 Quantal Density Functional Theory |
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291 | (4) |
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9.3 Application of Quantal Density Functional Theory to a Quantum Dot |
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295 | (18) |
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296 | (5) |
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9.3.2 Fields and Energies |
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301 | (4) |
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305 | (5) |
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310 | (1) |
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9.3.5 Single-Particle Expectations |
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310 | (1) |
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310 | (1) |
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311 | (2) |
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10 Physical Interpretation of the Local Density Approximation and Slater Theory via Quantal Density Functional Theory |
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313 | (28) |
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10.1 The Local Density Approximation in Kohn--Sham Theory |
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316 | (14) |
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10.1.1 Derivation and Interpretation of Electron Correlations via Kohn--Sham Theory |
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316 | (3) |
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10.1.2 Derivation and Interpretation of Electron Correlations via Quantal Density Functional Theory |
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319 | (5) |
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10.1.3 Structure of the Fermi Hole in the Local Density Approximation |
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324 | (5) |
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329 | (1) |
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330 | (11) |
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10.2.1 Derivation of the Exact `Slater Potential' |
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330 | (3) |
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10.2.2 Why the `Slater Exchange Potential' Does Not Represent the Potential Energy of an Electron |
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333 | (3) |
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10.2.3 Correctly Accounting for the Dynamic Nature of the Fermi Hole |
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336 | (2) |
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10.2.4 The Local Density Approximation in Slater Theory |
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338 | (1) |
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338 | (3) |
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341 | (8) |
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347 | (2) |
Appendix A A Derivation of the `Quantal Newtonian' Second Law |
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349 | (6) |
Appendix B Derivation of the Harmonic Potential Theorem |
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355 | (10) |
Appendix C Analytical Expressions for the Properties of the Ground and First Excited Singlet States of the Hooke's Atom |
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365 | (10) |
Appendix D Derivation of the Kinetic--Energy--Density Tensor for Hooke's Atom in Its Ground State |
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375 | (4) |
Appendix E Derivation of the S System `Quantal Newtonian' Second Law |
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379 | (4) |
Appendix F Derivation of the `Quantal Newtonian' First Law in the Presence of a Magnetic Field |
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383 | (8) |
Appendix G Analytical Expressions for the Ground State Properties of the Hooke's Atom in a Magnetic Field |
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391 | (6) |
Appendix H Derivation of the Kinetic-Energy-Density Tensor for the Ground State of Hooke's Atom in a Magnetic Field |
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397 | (4) |
Appendix I Derivation of the Pair--Correlation Density in the Local Density Approximation for Exchange |
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401 | (6) |
Index |
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407 | |