The ground-state density amplitude r for atoms and molecules Ž . satisfies a Schrodinger equation in which the customary one-body potential energy V r ¨Ž . of density functional theory is supplemented by the addition of the Pauli potential V r . p Since neither the exchange᎐correlation potential V o
Force-balance and differential equation for the ground-state electron density in atoms and molecules
✍ Scribed by C. Amovilli; N. H. March; T. Gál; Á. Nagy
- Publisher
- John Wiley and Sons
- Year
- 2000
- Tongue
- English
- Weight
- 165 KB
- Volume
- 77
- Category
- Article
- ISSN
- 0020-7608
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✦ Synopsis
Holas and March (1995)
established a force-balance equation from the many-electron Schrödinger equation. Here, we propose this as a basis for the construction of a (usually approximate) differential equation for the ground-state electron density. By way of example we present the simple case of two-electron systems with different external potentials but with weak electron-electron Coulomb repulsion λe 2 /r 12 . In this case first-order Rayleigh-Schrödinger (RS) perturbation theory of the ground-state wave function is known to lead to a compact expression for the first-order density matrix γ (r, r ) in terms of its diagonal density ρ(r) and the density corresponding to λ = 0. This result allows the force-balance equation to be written as a third-order linear, differential homogeneous equation for the ground-state electron density ρ(r). The example of the two-electron Hookean atom is treated: For this case one can also transcend the first-order RS perturbation theory and get exact results for discrete choices of force constants (external potential).
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