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occ
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Classes | |
| struct | SubshellOccupation |
| One subshell of a neutral atom's minimal-basis configuration. More... | |
Functions | |
| std::vector< SubshellOccupation > | minimal_basis_subshell_occupations (int Z) |
| A neutral atom's minimal-basis configuration, in filling order. | |
| int | ground_state_multiplicity (int Z) |
| Spin multiplicity 2S+1 of the neutral atom's ground state, for Z in 1..118; 0 for anything outside that range. | |
| Mat | compute_sap_matrix (const std::vector< occ::core::Atom > &atoms, const AOBasis &basis) |
Superposition of atomic potentials, as a one-electron matrix in basis. | |
| Mat occ::qm::guess::compute_sap_matrix | ( | const std::vector< occ::core::Atom > & | atoms, |
| const AOBasis & | basis | ||
| ) |
Superposition of atomic potentials, as a one-electron matrix in basis.
Uses whichever fit AOBasis::load_sap_basis provides; there is no choice to make here, and the parameter this once took named a basis it did not actually load.
| int occ::qm::guess::ground_state_multiplicity | ( | int | Z | ) |
Spin multiplicity 2S+1 of the neutral atom's ground state, for Z in 1..118; 0 for anything outside that range.
These are the experimental ground-state terms, so they include the cases Hund's rule alone gets wrong – chromium and copper take an electron from the s shell to half-fill or fill the d shell, palladium empties its s shell entirely. An effective core potential removes only closed shells, so the same multiplicity applies to the valence-only atom: gold keeps its one unpaired 6s electron whether or not its core is replaced.
| std::vector< SubshellOccupation > occ::qm::guess::minimal_basis_subshell_occupations | ( | int | Z | ) |
A neutral atom's minimal-basis configuration, in filling order.
Labelled by (n, l) rather than left as a flat vector, because the minimal basis does not list its shells in filling order: STO-3G gives iron 1s 2s 2p 3s 3p 4s 4p 3d, with the d shell last. Anything that places these occupations has to match them up by subshell, not by position.