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| nuclear-electronic_orbital_method [2025/05/21 12:15] – [Density fitting NEO-Hartree-Fock] rmata | nuclear-electronic_orbital_method [2025/05/21 12:36] (current) – [Density fitting NEO-DFT] rmata | ||
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| Line 14: | Line 14: | ||
| < | < | ||
| - | DF-NEO-RHF, | + | DF-NEO-RHF, options |
| </ | </ | ||
| Line 31: | Line 31: | ||
| ===== Density fitting NEO-DFT ===== | ===== Density fitting NEO-DFT ===== | ||
| - | The NEO-DFT program with density fitting for electron-repulsion integrals is available through | + | The spin-restricted |
| < | < | ||
| - | {grid, | ||
| DF-NEO-RKS, | DF-NEO-RKS, | ||
| NEOEPC, | NEOEPC, | ||
| </ | </ | ||
| + | Currently only standard grids are supported ('' | ||
| + | |||
| + | The definition of the quantum nuclei as well as the thresholds for the convergence of the nuclear cycles follows the same procedure as NEO-HF. | ||
| ===== NEO specific options ===== | ===== NEO specific options ===== | ||
| Line 173: | Line 175: | ||
| </ | </ | ||
| - | The second example shows the input of a **'' | + | The second |
| + | |||
| + | < | ||
| + | memory, | ||
| + | gdirect | ||
| + | nosym | ||
| + | noextra | ||
| + | geometry={ | ||
| + | 3 | ||
| + | |||
| + | H1 -3.5008791 | ||
| + | H2 -4.9109791 | ||
| + | O | ||
| + | } | ||
| + | charge=0 | ||
| + | basis={ | ||
| + | default=cc-pvdz | ||
| + | set, | ||
| + | default=neo-basis | ||
| + | H1=pb4-D | ||
| + | H2=pb4-D | ||
| + | set,nucfit, context=JKFIT | ||
| + | default=cc-pvdz | ||
| + | H1=10s10p10d10f | ||
| + | H2=10s10p10d10f | ||
| + | } | ||
| + | {grid, | ||
| + | {df-rks, | ||
| + | qnuc, | ||
| + | {df-neo-rks, | ||
| + | NEOEPC, | ||
| + | } | ||
| + | </ | ||
| + | |||
| + | The following | ||
| < | < | ||
| Line 287: | Line 323: | ||
| H1=10s10p10d10f | H1=10s10p10d10f | ||
| } | } | ||
| + | |||
| + | {rhf} | ||
| qnuc,H1 | qnuc,H1 | ||