Titlebook: Quantal Density Functional Theory II; Approximation Method Viraht Sahni Book 2009 Springer-Verlag Berlin Heidelberg 2009 Atom.Atomic physic

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Quantal Density Functional Theory of the Density Amplitude: Application to Atoms,ne of a model system of . – the . system – with equivalent density .(.). Thus, via Q-DFT, an interacting system in a . or . state can be mapped into a model . system whose density is the same. The state of the . system is ., in that it could be in a . or . state (see Chap. 5). For an interacting sys

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Application of the Irrotational Component Approximation to Nonspherical Density Atoms,degenerate sublevels. However, in most calculations of atomic structure, such atoms are treated in the central field modelwherein their densities are sphericalized by ensemble averaging the different orientations (see e.g. Appendix D). Thus, in order that these atoms be represented in a more physica

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Application of Q-DFT to Atoms in Excited States, Q-DFT mapping from an interacting system of electrons to a model . system of noninteracting fermions with equivalent density, is . in that it is the . for both the . and . states of the real system. Hence, all the equations governing Q-DFT and consequently all the approximation schemes, are equally

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Application of the Q-DFT Fully Correlated Approximation to the Hydrogen Molecule,udy the properties of this molecule from the perspective of Q-DFT, i.e. from the view point of the representation of all different electron correlations present in terms of the corresponding quantal sources, and of the resulting fields, potential energies and total energy components.We apply [1] the

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