In this article, we derive the analytical asymptotic structure in the Ž . classically forbidden region of atoms of the Kohn᎐Sham KS theory exchange᎐correlation Ž . KS w x Ž . KS w x potential defined as the functional derivative r s ␦ E r␦ r , where E is xc xc xc Ž . the KS exchange᎐correlation ene
Structure of the correlation–kinetic component of the Kohn–Sham exchange potential in atoms and at metal surfaces
✍ Scribed by Alexander Solomatin; Viraht Sahni
- Publisher
- John Wiley and Sons
- Year
- 1997
- Tongue
- English
- Weight
- 296 KB
- Volume
- 65
- Category
- Article
- ISSN
- 0020-7608
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✦ Synopsis
The Kohn᎐Sham density functional theory ''exchange'' potential v r s x KS w x Ž . KS w x ␦E r␦ r , where E is the ''exchange'' energy functional, is composed of a x x component representative of Pauli correlations and one that constitutes part of the KS Ž . correlation contribution to the kinetic energy. The Pauli term is the work done W r in x KS Ž . the field E E E E E r obtained by Coulomb's law from the Fermi hole charge distribution x constructed from the Kohn᎐Sham orbitals. The correlation᎐kinetic term is the work done Ž1. Ž . Ž1. Ž . W r in the field Z r derived from the kinetic-energy᎐density tensor involving the t t c c
first-order correction to the Kohn᎐Sham single-particle density matrix. The sum of these fields is conservative, so that the total work done is path-independent. There is no KS w x explicit correlation᎐kinetic contribution to the ''exchange'' energy E . Its contribution x Ž . is manifested via the Kohn᎐Sham orbitals generated via the potential v r . The functional x KS w x KS Ž .
📜 SIMILAR VOLUMES
An approximation scheme was developed for the Kohn᎐Sham exchange᎐correlation potential v , making use of a partitioning of v into a long-range screening v and xc x c scr a short-range response v component. For the response part, a model v mod was used, res p res p which represents v as weighted orbi
The long-range asymptotic behavior of the exchange-correlation Ž . Kohn᎐Sham KS potential v and its relation to the exchange-correlation energy E are