Foreword |
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vii | |
Preface |
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ix | |
Participants |
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xx | |
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1 Mathematical elements of density functional theory |
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1 | (56) |
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1 | (1) |
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2 Elements of quantum mechanics of electrons |
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2 | (7) |
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2.1 Electronic Hilbert spaces |
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2 | (1) |
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3 | (1) |
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2.3 Creation and annihilation operators |
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4 | (2) |
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2.4 Reduced densities and density matrices |
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6 | (1) |
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7 | (1) |
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2.5.1 The number operator |
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7 | (1) |
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2.5.2 The electronic Hamiltonian |
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8 | (1) |
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3 The Hohenberg-Kohn theorem |
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9 | (4) |
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4 Some results on concrete density functionals |
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13 | (28) |
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13 | (1) |
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4.1.1 Definition and basic properties |
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13 | (12) |
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4.1.2 Asymptotic exactness of Thomas-Fermi theory |
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25 | (6) |
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4.2 The Thomas-Fermi-Weizsacker functional |
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31 | (3) |
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4.3 The Engel-Dreizler functional |
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34 | (2) |
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4.4 Density functionals in phase space |
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36 | (1) |
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4.4.1 Marginal functionals: The position space |
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37 | (1) |
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4.4.2 Marginal functions: The momentum space |
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38 | (1) |
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4.4.3 Time-dependent equations |
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39 | (2) |
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5 Functionals of the one-particle density matrix |
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41 | (6) |
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5.1 The Hartree-Fock functional |
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41 | (4) |
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5.2 The Miiller functional |
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45 | (2) |
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Appendix: Maximal functions of powers and Thomas-Fermi energy of exchange holes |
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47 | (2) |
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49 | (1) |
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49 | (8) |
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2 A statistical theory of heavy atoms: Energy and excess charge |
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57 | (12) |
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57 | (2) |
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59 | (3) |
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59 | (1) |
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59 | (1) |
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2.2.1 The Weizsacker energy |
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59 | (1) |
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2.2.2 The potential energy |
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59 | (1) |
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2.2.3 The Thomas-Fermi term |
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60 | (1) |
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2.2.4 The exchange energy |
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60 | (1) |
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61 | (1) |
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3 Application to the excess charge problem |
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62 | (6) |
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68 | (1) |
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68 | (1) |
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3 Relativistic strong Scott conjecture: A short proof |
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69 | (12) |
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69 | (3) |
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2 Proof of the convergence |
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72 | (2) |
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74 | (4) |
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78 | (1) |
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79 | (2) |
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4 Direct methods to Lieb-Thirring kinetic inequalities |
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81 | (36) |
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81 | (4) |
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85 | (12) |
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2.1 A simple proof of Sobolev inequality |
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85 | (2) |
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2.2 Lieb-Thirring kinetic inequality |
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87 | (3) |
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2.3 Eigenvalue bounds for Schrodinger operators |
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90 | (4) |
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2.4 Best known constant for kinetic inequality |
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94 | (3) |
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97 | (1) |
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3 Lundholm-Solovej method |
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97 | (14) |
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3.1 Kinetic inequality via local exclusion principle |
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97 | (7) |
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3.2 Kinetic inequality with semiclassical constant and error term |
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104 | (3) |
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3.3 Kinetic inequality for functions vanishing on diagonal set |
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107 | (2) |
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3.4 Lieb-Thirring inequality for interacting systems |
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109 | (2) |
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111 | (1) |
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111 | (1) |
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112 | (5) |
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5 Dynamics of interacting bosons: A compact review |
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117 | (38) |
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117 | (6) |
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117 | (1) |
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118 | (2) |
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1.3 Types of approximation |
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120 | (3) |
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123 | (1) |
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2 Ground state properties |
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123 | (3) |
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2.1 Leading order approximation for the ground state |
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123 | (1) |
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2.2 Second order correction |
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124 | (2) |
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3 Leading order approximation |
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126 | (10) |
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3.1 Results for different scaling regimes |
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127 | (1) |
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127 | (2) |
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129 | (1) |
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130 | (1) |
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131 | (1) |
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3.2.1 The BBGKY hierarchy |
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132 | (1) |
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3.2.2 Quantitative approaches |
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133 | (3) |
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136 | (7) |
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5 Fock space approximation |
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143 | (3) |
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146 | (1) |
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146 | (9) |
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6 Corrections to the mean-field description for the dynamics of Bose gases |
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155 | (24) |
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155 | (1) |
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2 The microscopic system and the effective system |
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156 | (1) |
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157 | (3) |
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160 | (8) |
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5 Corrections to the mean-field description |
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168 | (5) |
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173 | (3) |
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176 | (1) |
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177 | (2) |
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7 Semiclassics: The hidden theory behind the success of DFT |
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179 | (72) |
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180 | (5) |
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185 | (2) |
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187 | (7) |
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194 | (5) |
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199 | (4) |
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203 | (4) |
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207 | (2) |
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209 | (2) |
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211 | (5) |
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216 | (2) |
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218 | (4) |
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222 | (2) |
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224 | (4) |
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228 | (1) |
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229 | (7) |
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236 | (4) |
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240 | (1) |
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241 | (10) |
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8 Density-potential functional theory for fermions in one dimension |
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251 | (18) |
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251 | (2) |
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2 Density-potential functional theory in a nutshell |
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253 | (4) |
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3 Airy-averaged densities in ID |
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257 | (2) |
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4 DPFT densities for the Morse potential |
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259 | (3) |
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262 | (2) |
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264 | (1) |
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264 | (1) |
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265 | (4) |
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9 Remarks on the density functional theory of relativistic many-particle systems |
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269 | (18) |
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269 | (1) |
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2 Nonrelativistic systems |
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270 | (3) |
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3 Relativistic systems on the basis of the Dirac equation |
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273 | (4) |
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4 Relativistic systems on the basis of field theory |
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277 | (7) |
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284 | (1) |
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284 | (3) |
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10 Energy functionals of single-particle densities: A unified view |
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287 | (22) |
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287 | (1) |
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288 | (5) |
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3 Configuration-space functionals |
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293 | (5) |
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4 Momentum-space functionals |
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298 | (2) |
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5 Thomas-Fermi atoms in configuration and momentum space |
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300 | (2) |
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6 Single-particle-exact functionals |
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302 | (1) |
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Appendix: Semiclassical eigenvalues |
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303 | (3) |
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306 | (1) |
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306 | (3) |
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11 Spin-density functional theory through spin-free wave functions |
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309 | (10) |
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309 | (2) |
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2 The spin-free N-electron wave function |
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311 | (3) |
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2.1 The conventional definition of the universal functional by constrained search |
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312 | (1) |
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2.2 The spin-free definition of the universal functional by constrained search |
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312 | (2) |
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3 The spin-free constrained search from the spin-free iV-electron variational principle |
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314 | (1) |
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4 Spin-free coordinate-scaling constraints on the universal functional and the correlation-energy functional |
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315 | (1) |
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316 | (1) |
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317 | (1) |
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317 | (2) |
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12 Advances in rectangular collocation for solution of the Schrodinger equation: From obviating integrals to machine learning |
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319 | (26) |
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1 Introduction: The big picture |
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319 | (2) |
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2 Similarities and differences between the electronic and the nuclei Schrodinger equations |
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321 | (3) |
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3 Rectangular collocation method to solve the Schrodinger equation |
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324 | (2) |
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4 Rectangular collocation for the vibrational Schrodinger equation |
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326 | (6) |
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4.1 Treatment of the kinetic energy operator |
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329 | (1) |
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4.2 Use of non-integrable basis functions |
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330 | (1) |
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4.3 Advantage of rectangularity |
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331 | (1) |
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5 Rectangular collocation for the electronic Schrodinger equation |
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332 | (5) |
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6 Shaping the collocation point distribution |
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337 | (2) |
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6.1 Physical intuition based collocation point placement |
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337 | (1) |
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6.2 Machine learning guided collocation point placement |
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338 | (1) |
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7 Conclusions and perspectives |
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339 | (2) |
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341 | (4) |
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13 FLEIM: A stable, accurate and robust extrapolation method at infinity for computing the ground state of electronic Hamiltonian |
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345 | |
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345 | (2) |
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345 | (2) |
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1.2 Objective and structure of the paper |
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347 | (1) |
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347 | (5) |
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2.1 The model Schrodinger equation |
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347 | (2) |
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2.2 The correction to the model |
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349 | (1) |
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349 | (1) |
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2.2.2 Approaching the Coulomb interaction |
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349 | (1) |
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2.2.3 Choice of the basis functions |
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350 | (1) |
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2.2.4 Reducing the basis set |
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350 | (2) |
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2.3 Computing other physical properties |
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352 | (1) |
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352 | (5) |
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352 | (1) |
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3.2 General behavior of errors |
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353 | (1) |
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3.3 Possibility of error estimates |
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353 | (3) |
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3.4 Expectation values with FLEIM: (r12) and (r2 12) for harmonium |
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356 | (1) |
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357 | (1) |
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4 Conclusion and perspectives |
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357 | (2) |
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359 | (1) |
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A On density functional approximations |
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359 | (1) |
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360 | (1) |
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C The empirical interpolation method |
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361 | (2) |
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362 | (1) |
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C.2 The forward looking empirical interpolation method (FLEIM) |
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363 | (1) |
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D Numerical details of the calculations |
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363 | (5) |
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D.1 Testing EIM and FLEIM with E(μ) = 1 + xj.(μ) |
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363 | (1) |
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D.2 Discretization for FLEIM |
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363 | (3) |
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366 | (1) |
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D.4 Obtaining the model energy |
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366 | (2) |
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E Change of coordinates in harmonium |
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368 | (1) |
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369 | (1) |
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369 | |