Atom-Centered Functions in the Optimized Thomas-Fermi Theory
β Scribed by Gary G. Hoffman
- Publisher
- Elsevier Science
- Year
- 1995
- Tongue
- English
- Weight
- 225 KB
- Volume
- 116
- Category
- Article
- ISSN
- 0021-9991
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β¦ Synopsis
In the application of the optimized Thomas-Fermi theory to condensed phase systems, it has proved convenient to introduce a sum of atom-centered functions to represent the most rapidly varying part of the electron density near the nuclei. By extraction of this portion of the density, attention can be focused on the more slowly varying portion, allowing numerical techniques to be employed without being hindered by a prohibitively high density of grid points. Dealing with these atom-centered functions is facilitated by the closed-form evaluation of some nontrivial integrals. For the case of exponential functions, these integrals are evaluated here and specific methods for their computation are presented. (c) 1995 Academic Press, Inc.
π SIMILAR VOLUMES
The self-consistent ThomasαFermi atom satisfying Poisson's equation in D dimensions has a functional derivative of the kinetic energy T with respect to the Ε½ . 2rD 1y2rD ground-state density n r proportional to n . But the Poisson equation relates n to ''reduced'' density derivatives n y1Ε½ d 2 n r d
We investigate a density-functional theory (DFT) approach for an unpolarized trapped dilute Fermi gas in the unitary limit. A reformulation of the recent work of T. Papenbrock [1] in the language of fractional exclusion statistics allows us to obtain an estimate of the universal factor, ΞΎ~3D~, in th