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Spin component scaled approximation

Figure 10.90. N — 14 and 15 rotational levels of CrF in its X 6X1 state, with the spin splitting and spin component transitions observed. This diagram is approximately to scale. Figure 10.90. N — 14 and 15 rotational levels of CrF in its X 6X1 state, with the spin splitting and spin component transitions observed. This diagram is approximately to scale.
In order to test the various approximations of the Coulomb matrix, all electron basis set and numerical scalar scaled ZORA calculations have been performed on the xenon and radon atom. The numerical results have been taken from a previous publication [7], where it should be noted that the scalar orbital energies presented here are calculated by averaging, over occupation numbers, of the two component (i.e. spin orbit split) results. Tables (1) and (2) give the orbital energies for the numerical (s.o. averaged) and basis set calculations for the various Coulomb matrix approximations. The results from table... [Pg.256]

Jung et al. [81] reported a variant of this approach that used the multiplicative factor of zero for the SS component and 1.3 for the OS component. This calculation, SOS-MP2 (scaled opposite-spin MP2), can be performed with only an 0(n4) operation cost when combined with Almlof s Laplace transform technique [82], The SOS approximation can be applied to CIS(D) [69], A similar simplification was often adopted in the GW method under the name COHSEX approximation [32] also partly from an operation cost consideration. [Pg.38]


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See also in sourсe #XX -- [ Pg.38 ]




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Spin-scaling

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