1999
DOI: 10.1002/(sici)1096-987x(19990115)20:1<51::aid-jcc7>3.0.co;2-k
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Relativistic all-electron density functional calculations

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Cited by 77 publications
(68 citation statements)
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“…The most of our calculations were performed using M06-L density functional which has been well validated for transition metals [11][12][13]. We have included the relativistic effects using two most popular ways: via Douglass-Kroll-Hess twocomponent (DKH2) Hamiltonian [14,15] or utilizing zeroorder regular approximation (ZORA) [16][17][18]. The computations with DKH2 approach were performed with ORCA 4.0.1 program [19], and the results by ZORA were obtained in ADF 2018 [20][21][22].…”
Section: Methodsmentioning
confidence: 99%
“…The most of our calculations were performed using M06-L density functional which has been well validated for transition metals [11][12][13]. We have included the relativistic effects using two most popular ways: via Douglass-Kroll-Hess twocomponent (DKH2) Hamiltonian [14,15] or utilizing zeroorder regular approximation (ZORA) [16][17][18]. The computations with DKH2 approach were performed with ORCA 4.0.1 program [19], and the results by ZORA were obtained in ADF 2018 [20][21][22].…”
Section: Methodsmentioning
confidence: 99%
“…Among the all-electron relativistic approaches available, the family of Douglas-Kroll-Hess (DKH) transformation-based methods [59][60][61] and zero order regular approximation (ZORA) [62][63][64] are the methods most widely tested and used [65,66]. Different theoretical investigations showed that the ZORA and DKH approaches provide similar results.…”
Section: Methodsmentioning
confidence: 99%
“…If we require to reproduce the length of magnetization instead, this is a noncollinear [' '(nc)' '] approach because the magnetization is a vector field representing a magnetic dipole moment whose direction changes with position. [135,137,139,140,141] Note that these different choices for the noninteracting reference system each implies a different definition of the noninteracting kinetic energy functional, T ðclÞ s ½q; m z and T ðncÞ s ½q; jmj , and thus also of the exchange-correlation energy, E ðclÞ xc ½q; m z and E ðncÞ xc ½q; jmj , respectively. For the choices mentioned here, where in addition to the electron density one additional quantity is reproduced by the KS system, the resulting exchangecorrelation potential has two components.…”
Section: Relativistic Spin-dftmentioning
confidence: 99%