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1 | (36) |
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1 | (4) |
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Time-independent Schrodinger equation |
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5 | (2) |
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The Born-Oppenheimer model |
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7 | (2) |
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9 | (2) |
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11 | (3) |
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14 | (2) |
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16 | (2) |
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18 | (1) |
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19 | (4) |
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23 | (1) |
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24 | (3) |
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Standard Notation for Quantum Chemistry |
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27 | (10) |
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27 | (1) |
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28 | (1) |
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Many-electron wavefunctions |
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29 | (1) |
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29 | (1) |
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Linear expansions for the spatial orbitals |
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30 | (1) |
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31 | (1) |
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Single determinant energy expression |
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32 | (1) |
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Notation for repulsion integrals |
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33 | (1) |
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Spatial orbital repulsion integrals |
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34 | (1) |
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Basis function repulsion integrals |
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35 | (2) |
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37 | (38) |
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37 | (1) |
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38 | (2) |
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The differential Hartree-Fock equation |
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40 | (7) |
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47 | (2) |
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49 | (1) |
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50 | (1) |
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Direct parametric minimisation |
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51 | (2) |
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53 | (1) |
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Single-determinant energy expression |
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54 | (21) |
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54 | (2) |
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The normalisation integral |
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56 | (5) |
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61 | (4) |
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65 | (5) |
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70 | (5) |
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75 | (40) |
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75 | (2) |
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77 | (1) |
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78 | (2) |
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80 | (1) |
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The numerator: Hamiltonian mean value |
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81 | (3) |
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The denominator: normalisation condition |
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84 | (2) |
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The Hartree-Fock equation |
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86 | (1) |
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``Normalisation'': the Lagrangian |
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87 | (1) |
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88 | (1) |
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Some technical manipulations |
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89 | (3) |
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92 | (3) |
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95 | (1) |
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96 | (1) |
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97 | (3) |
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100 | (3) |
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Properties of the J and K matrices |
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103 | (5) |
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103 | (3) |
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106 | (1) |
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107 | (1) |
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108 | (2) |
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Lowest state of a given symmetry |
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108 | (2) |
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Single determinant: choice of orbitals |
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110 | (5) |
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110 | (2) |
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112 | (1) |
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113 | (1) |
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``Zeroth-order'' perturbed orbitals |
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113 | (2) |
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A special case: closed shells |
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115 | (8) |
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115 | (1) |
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Notation for the closed-shell case |
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116 | (1) |
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116 | (1) |
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The closed-shell ``HF'' equation |
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117 | (4) |
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121 | (2) |
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Implementation of the closed-shell case |
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123 | (76) |
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124 | (1) |
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Vectors, matrices and arrays |
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125 | (6) |
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The implementation: getting started |
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131 | (17) |
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The implementation: repulsion integral access |
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148 | (10) |
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Building a testbench: conventional SCF |
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158 | (7) |
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Another testbench: direct SCF |
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165 | (8) |
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173 | (1) |
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174 | (1) |
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175 | (9) |
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175 | (1) |
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176 | (1) |
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177 | (2) |
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179 | (3) |
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Other diagonalisation methods |
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182 | (2) |
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184 | (6) |
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184 | (2) |
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186 | (1) |
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187 | (3) |
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190 | (4) |
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Coding the standard index loops |
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194 | (5) |
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Improvements: tools and methods |
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199 | (18) |
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199 | (1) |
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Versions: conditional compilation |
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200 | (7) |
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207 | (3) |
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210 | (2) |
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Improving the formation of G(R) |
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212 | (3) |
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215 | (2) |
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Molecular integrals: an introduction |
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217 | (38) |
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218 | (1) |
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219 | (2) |
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AOs and atom-centred-functions |
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221 | (1) |
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Multi-dimensional integral evaluation |
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222 | (1) |
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Molecular integrals over STOs |
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223 | (9) |
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Basis functions of convenience |
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232 | (2) |
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234 | (17) |
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The contraction technique |
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251 | (4) |
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Molecular integrals: implementation |
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255 | (42) |
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256 | (1) |
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256 | (4) |
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260 | (3) |
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Overview; the general structure |
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263 | (6) |
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Complex code management: the WEB system |
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269 | (7) |
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276 | (11) |
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287 | (1) |
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288 | (1) |
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Source for the WEB of fmch |
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289 | (8) |
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Repulsion integral storage |
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297 | (14) |
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297 | (1) |
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298 | (2) |
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300 | (7) |
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A partner for putint; getint |
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307 | (2) |
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309 | (2) |
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311 | (20) |
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311 | (1) |
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Virtual orbitals in practice |
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312 | (5) |
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The virtual space in LCAO |
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317 | (5) |
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322 | (1) |
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323 | (8) |
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323 | (1) |
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324 | (5) |
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Perturbation theory for matrix equations |
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329 | (2) |
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331 | (12) |
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331 | (4) |
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335 | (2) |
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The Revision Control System: RCS |
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337 | (2) |
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339 | (4) |
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339 | (1) |
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340 | (1) |
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341 | (2) |
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Open shells: implementing UHF |
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343 | (56) |
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344 | (1) |
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344 | (3) |
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347 | (1) |
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Integrals over the spin-basis |
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348 | (2) |
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350 | (1) |
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351 | (6) |
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357 | (3) |
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Interpreting the MO coefficients |
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360 | (3) |
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363 | (1) |
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Version 1 of the SCF code |
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363 | (5) |
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WEB output for function scf |
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368 | (8) |
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376 | (1) |
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WEB Source for the scf code |
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377 | (5) |
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Blocking the Hartree-Fock matrix |
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382 | (12) |
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The block form of the HF matrix |
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382 | (2) |
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384 | (10) |
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394 | (5) |
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394 | (1) |
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395 | (1) |
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Special case: a single excitation |
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396 | (3) |
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399 | (10) |
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399 | (1) |
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Densities and spin-densities |
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400 | (1) |
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Basis representations: charges |
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401 | (3) |
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404 | (2) |
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406 | (1) |
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407 | (1) |
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408 | (1) |
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The general MO functional |
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409 | (32) |
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409 | (1) |
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410 | (2) |
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412 | (4) |
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A single ``Hartree-Fock'' operator |
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416 | (3) |
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419 | (1) |
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Choice of the arbitrary matrices |
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420 | (2) |
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Implementation: stacks of matrices |
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422 | (11) |
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Projection operators and SCF |
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433 | (8) |
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Introduction: optimum single determinant |
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433 | (2) |
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Alternative SCF conditions |
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435 | (1) |
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R matrices as projection operators |
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436 | (5) |
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Spin-restricted open shell |
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441 | (32) |
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441 | (1) |
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442 | (2) |
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444 | (1) |
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A WEB for spin-restricted open shell |
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445 | (28) |
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Banana skins: unexpected disasters |
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473 | (6) |
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474 | (1) |
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475 | (2) |
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477 | (1) |
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478 | (1) |
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479 | (26) |
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479 | (1) |
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Symmetry and the HF method |
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480 | (3) |
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Permutational symmetry of the basis |
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483 | (5) |
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488 | (16) |
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Permutation symmetry: summary |
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504 | (1) |
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Symmetry orbital transformations |
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505 | (10) |
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505 | (4) |
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509 | (3) |
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Generation of symmetry orbitals |
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512 | (2) |
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514 | (1) |
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A symmetry-adapted SCF method |
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515 | (26) |
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515 | (3) |
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518 | (10) |
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Full implementation; linear combinations |
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528 | (5) |
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533 | (1) |
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Kronecker product notation |
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534 | (7) |
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534 | (1) |
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Basis-product transformations |
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535 | (1) |
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Density matrix transformations |
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536 | (1) |
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Transformations in the HF matrix |
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537 | (2) |
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539 | (2) |
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Linear multi-determinant methods |
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541 | (30) |
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Correlation and the Hartree-Fock model |
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541 | (2) |
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The configuration interaction method |
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543 | (1) |
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544 | (1) |
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545 | (5) |
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550 | (3) |
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553 | (1) |
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Nesbet's method for large matrices |
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554 | (6) |
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560 | (5) |
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565 | (1) |
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The ``orthogonal VB'' model |
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566 | (2) |
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568 | (3) |
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571 | (16) |
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Non-orthogonality in expansions |
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571 | (2) |
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573 | (3) |
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Spin eigenfunctions and permutations |
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576 | (5) |
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581 | (4) |
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585 | (2) |
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587 | (18) |
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Introduction: natural orbitals |
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588 | (2) |
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590 | (5) |
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595 | (1) |
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Partial Paired-Excitations; GVB |
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596 | (3) |
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599 | (5) |
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604 | (1) |
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Interpreting the McWeenyan |
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605 | (6) |
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605 | (2) |
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607 | (1) |
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608 | (2) |
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610 | (1) |
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611 | (26) |
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612 | (2) |
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614 | (1) |
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Transforming the Hartree-Fock equation |
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615 | (3) |
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618 | (3) |
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Arbitrariness in the pseudo-orbital |
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621 | (3) |
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Modelling atomic pseudopotentials |
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624 | (2) |
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Modelling atomic core potentials |
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626 | (3) |
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Several valence electrons |
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629 | (4) |
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Atomic cores in molecules |
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633 | (1) |
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634 | (3) |
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Practical core potentials |
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637 | (16) |
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637 | (1) |
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Forms for the core potentials |
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638 | (3) |
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641 | (10) |
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651 | (2) |
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653 | (16) |
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654 | (1) |
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Two forms for the HF equations |
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654 | (3) |
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Self-consistent perturbation theory |
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657 | (2) |
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659 | (8) |
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667 | (2) |
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Time-dependent perturbations: RPA |
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669 | (14) |
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669 | (1) |
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Time-dependent Hartree-Fock theory |
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670 | (1) |
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Oscillatory time-dependent perturbations |
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671 | (4) |
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675 | (1) |
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676 | (2) |
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``Random phase approximation'' |
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678 | (2) |
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Time-dependent variation principle |
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680 | (3) |
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Transitions and stability |
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683 | (8) |
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683 | (1) |
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684 | (1) |
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The transition frequencies |
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685 | (1) |
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Finite perturbations; oscillations |
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686 | (2) |
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Stability; the time-independent case |
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688 | (1) |
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689 | (2) |
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Two-electron transformations |
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691 | (32) |
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691 | (2) |
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693 | (2) |
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Transformation without sorting |
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695 | (10) |
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Transformations with sorting |
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705 | (3) |
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708 | (1) |
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709 | (14) |
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709 | (3) |
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712 | (11) |
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Geometry optimisation: derivatives |
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723 | (16) |
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724 | (1) |
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Derivatives and perturbation theory |
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725 | (2) |
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Derivatives of variational solutions |
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727 | (2) |
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Parameter-dependent basis functions |
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729 | (1) |
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The derivative of the SCF energy |
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730 | (4) |
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Derivatives of molecular integrals |
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734 | (1) |
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Derivatives of non-variational energies |
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735 | (2) |
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737 | (1) |
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737 | (2) |
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The Semi-empirical approach |
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739 | (24) |
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739 | (2) |
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741 | (1) |
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742 | (2) |
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Simulation or calibration? |
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744 | (1) |
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745 | (3) |
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748 | (2) |
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Hohenberg and Kohn's proofs |
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750 | (5) |
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Kohn-Sham equations: introduction |
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755 | (2) |
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757 | (3) |
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Non-local operators in orbital theories |
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760 | (3) |
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Implementing the Kohn-Sham equations |
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763 | (16) |
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A precursor: The Hartree-Fock-Slater model |
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764 | (2) |
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Implementation of the Kohn-Sham method |
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766 | (5) |
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The kinetic energy density |
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771 | (1) |
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Gradients in the exchange-correlation energy |
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772 | (1) |
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Numerical integration of densities |
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773 | (3) |
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776 | (3) |
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779 | (12) |
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Non-variational expansions |
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779 | (3) |
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The pseudospectral methods |
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782 | (4) |
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The discrete variational method |
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786 | (5) |
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Additional reading and other material |
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791 | |
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791 | (3) |
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Additional material by ftp |
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794 | |