Time-dependent Internal DFT formalism and Kohn-Sham scheme
arXiv:0908.1028 · doi:10.1103/PhysRevC.80.054614
Abstract
We generalize to the time-dependent case the stationary Internal DFT / Kohn-Sham formalism presented in Ref. [14]. We prove that, in the time-dependent case, the internal properties of a self-bound system (as an atomic nuclei) are all defined by the internal one-body density and the initial state. We set-up a time-dependent Internal Kohn-Sham scheme as a practical way to compute the internal density. The main difference with the traditional DFT / Kohn-Sham formalism is the inclusion of the center-of-mass correlations in the functional.
13 pages. To be published in Phys. Rev. C
References in corpus (6)
- On the "Causality Paradox" of Time-Dependent Density Functional Theory
- Intrinsic-Density Functionals
- Density functional theory and Kohn-Sham scheme for self-bound systems
- Density functional theory for self-bound systems
- Existence of a Density Functional for an Intrinsic State
- Center-of-mass motion and cross-channel coupling in time-dependent Hartree-Fock theory
Cited by in corpus (6)
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- Generalization of internal Density Functional Theory and Kohn-Sham scheme to multicomponent systems, and link with traditional DFT
- Density Functional Theory with Spatial-Symmetry Breaking and Configuration Mixing
- An alternate well-founded way to treat the center-of-mass correlations: use of a local center-of-mass correlations potential
- Local energy density functional for superfluid Fermi gases from effective field theory