1971
DOI: 10.1063/1.3022743
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Methods of Molecular Quantum Mechanics

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Cited by 472 publications
(398 citation statements)
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“…A restricted Slater determinant is always an eigenfunction of Ŝ z with eigenvalue M S h ¼ ðN a À N b Þh=2. [60,58] If all singly occupied orbitals are either a-or b-spin orbitals, then it is also an eigenfunction of Ŝ 2 with S ¼ |M S |. In all other cases, an eigenfunction of Ŝ 2 can be constructed as a linear combination of (degenerate) determinants in which the same orbitals are singly occupied and which correspond to the same value of M S .…”
Section: Spin-restricted Kohn-sham Dftmentioning
confidence: 99%
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“…A restricted Slater determinant is always an eigenfunction of Ŝ z with eigenvalue M S h ¼ ðN a À N b Þh=2. [60,58] If all singly occupied orbitals are either a-or b-spin orbitals, then it is also an eigenfunction of Ŝ 2 with S ¼ |M S |. In all other cases, an eigenfunction of Ŝ 2 can be constructed as a linear combination of (degenerate) determinants in which the same orbitals are singly occupied and which correspond to the same value of M S .…”
Section: Spin-restricted Kohn-sham Dftmentioning
confidence: 99%
“…Such determinants-which can only differ in the spin of the singly occupied orbitals-are degenerate with respect to the noninteracting Hamiltonian of Eq. (60).…”
Section: Spin-restricted Kohn-sham Dftmentioning
confidence: 99%
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“…For two-component relativistic calculations, the e-e interaction needs to be transformed to two-component form. In order c −2 , the corresponding terms are well known [2,109]. The leadingorder relativistic corrections to r −1 kl can be written as…”
Section: Many-electron Systemsmentioning
confidence: 99%