2017
DOI: 10.1063/1.4984777
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Communication: Density functional theory embedding with the orthogonality constrained basis set expansion procedure

Abstract: Communication: A novel implementation to compute MP2 correlation energies without basis set superposition errors and complete basis set extrapolation

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Cited by 47 publications
(62 citation statements)
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“…MCP, methylenecyclopropene; LUMO, lowest unoccupied molecular orbital basis-set expansion used in the embedding context to keep orbitals of different subsystems orthogonal. [43] Transforming the embedded Fock matrix of subsystem A (F A(Env) ) in the space spanned by the selected virtual orbitals…”
Section: Theoretical Backgroundmentioning
confidence: 99%
See 1 more Smart Citation
“…MCP, methylenecyclopropene; LUMO, lowest unoccupied molecular orbital basis-set expansion used in the embedding context to keep orbitals of different subsystems orthogonal. [43] Transforming the embedded Fock matrix of subsystem A (F A(Env) ) in the space spanned by the selected virtual orbitals…”
Section: Theoretical Backgroundmentioning
confidence: 99%
“…Because of the fact that the intra‐subsystem Fock matrix is not diagonalized by the rotated orbitals, an additional diagonalization is necessary. Note that this procedure is similar to the orthogonality‐constrained basis‐set expansion used in the embedding context to keep orbitals of different subsystems orthogonal 43 . Transforming the embedded Fock matrix of subsystem A ( F A(Env) ) in the space spanned by the selected virtual orbitals FA=boldCfalse˜virtnormalA,TFnormalA()EnvboldCfalse˜virtA yields a new set of eigenvectors CA and eigenvalues via diagonalization of FA.…”
Section: Theoretical Backgroundmentioning
confidence: 99%
“…1, red). Errors associated with finite values of µ can also be avoided by enforcing the projection via explicit orthogonalization [52][53][54][55][56] of the subsystem orbitals, at some cost to the simplicity of the implementation.…”
Section: Dft-in-dft Embeddingmentioning
confidence: 99%
“…The orthogonality of the P and Q spaces reflects in the orthogonality of the original χ i and Qξ functions, but that orthogonality is lost when we act on χ i and on Qξ with Θ 1 2 (µ−H) in Eqs. (14), (16). Further note that, as mentioned, the same overall Hamiltonian (and therefore the same Θ 1 2 (µ − H) ) is used in preparing both the stochastic and deterministic orbitals, i.e., they are treated on equal footing.…”
Section: B Dft Embeddingmentioning
confidence: 99%